Cauchy’s Theorem and Edge Lengths of Convex
微积分英文专业词汇
微积分词汇第一章函数与极限Chapter1 Function and Limit集合set元素element子集subset空集empty set并集union交集intersection差集difference of set基本集basic set补集complement set直积direct product笛卡儿积Cartesian product开区间open interval闭区间closed interval半开区间half open interval有限区间finite interval区间的长度length of an interval无限区间infinite interval领域neighborhood领域的中心centre of a neighborhood 领域的半径radius of a neighborhood 左领域left neighborhood右领域right neighborhood映射mappingX到Y的映射mapping of X ontoY 满射surjection单射injection一一映射one-to-one mapping双射bijection算子operator变化transformation函数function逆映射inverse mapping复合映射composite mapping自变量independent variable因变量dependent variable定义域domain函数值value of function函数关系function relation值域range自然定义域natural domain 单值函数single valued function多值函数multiple valued function单值分支one-valued branch函数图形graph of a function绝对值函数absolute value符号函数sigh function整数部分integral part阶梯曲线step curve当且仅当if and only if(iff)分段函数piecewise function上界upper bound下界lower bound有界boundedness无界unbounded函数的单调性monotonicity of a function 单调增加的increasing单调减少的decreasing单调函数monotone function函数的奇偶性parity(odevity) of a function 对称symmetry偶函数even function奇函数odd function函数的周期性periodicity of a function周期period反函数inverse function直接函数direct function复合函数composite function中间变量intermediate variable函数的运算operation of function基本初等函数basic elementary function 初等函数elementary function幂函数power function指数函数exponential function对数函数logarithmic function三角函数trigonometric function反三角函数inverse trigonometric function 常数函数constant function双曲函数hyperbolic function双曲正弦hyperbolic sine双曲余弦hyperbolic cosine双曲正切hyperbolic tangent反双曲正弦inverse hyperbolic sine反双曲余弦inverse hyperbolic cosine反双曲正切inverse hyperbolic tangent极限limit数列sequence of number收敛convergence收敛于a converge to a发散divergent极限的唯一性uniqueness of limits收敛数列的有界性boundedness of a convergent sequence子列subsequence函数的极限limits of functions函数当x趋于x0时的极限limit of functions as x approaches x0左极限left limit右极限right limit单侧极限one-sided limits水平渐近线horizontal asymptote无穷小infinitesimal无穷大infinity铅直渐近线vertical asymptote夹逼准则squeeze rule单调数列monotonic sequence高阶无穷小infinitesimal of higher order低阶无穷小infinitesimal of lower order同阶无穷小infinitesimal of the same order作者:新少年特工2007-10-8 18:37 回复此发言--------------------------------------------------------------------------------2 高等数学-翻译等阶无穷小equivalent infinitesimal函数的连续性continuity of a function增量increment函数在x0连续the function is continuous at x0左连续left continuous右连续right continuous区间上的连续函数continuous function函数在该区间上连续function is continuous on an interval 不连续点discontinuity point第一类间断点discontinuity point of the first kind第二类间断点discontinuity point of the second kind初等函数的连续性continuity of the elementary functions定义区间defined interval最大值global maximum value (absolute maximum)最小值global minimum value (absolute minimum)零点定理the zero point theorem介值定理intermediate value theorem第二章导数与微分Chapter2 Derivative and Differential速度velocity匀速运动uniform motion平均速度average velocity瞬时速度instantaneous velocity圆的切线tangent line of a circle切线tangent line切线的斜率slope of the tangent line位置函数position function导数derivative可导derivable函数的变化率问题problem of the change rate of a function导函数derived function左导数left-hand derivative右导数right-hand derivative单侧导数one-sided derivatives在闭区间【a,b】上可导is derivable on the closed interval [a,b]切线方程tangent equation角速度angular velocity成本函数cost function边际成本marginal cost链式法则chain rule隐函数implicit function显函数explicit function二阶函数second derivative三阶导数third derivative高阶导数nth derivative莱布尼茨公式Leibniz formula对数求导法log- derivative参数方程parametric equation相关变化率correlative change rata微分differential可微的differentiable函数的微分differential of function自变量的微分differential of independent variable微商differential quotient间接测量误差indirect measurement error绝对误差absolute error相对误差relative error第三章微分中值定理与导数的应用Chapter3 MeanValue Theorem of Differentials and the Application of Derivatives罗马定理Rolle’s theorem费马引理Fermat’s lemma拉格朗日中值定理Lagrange’s mean value theorem驻点stationary point稳定点stable point临界点critical point辅助函数auxiliary function拉格朗日中值公式Lagrange’s mean value formula柯西中值定理Cauchy’s mean value theorem洛必达法则L’Hospital’s Rule0/0型不定式indeterminate form of type 0/0 不定式indeterminate form泰勒中值定理Taylor’s mean value theorem 泰勒公式Taylor formula余项remainder term拉格朗日余项Lagrange remainder term麦克劳林公式Maclaurin’s formula佩亚诺公式Peano remainder term凹凸性concavity凹向上的concave upward, cancave up凹向下的,向上凸的concave downward’concave down 拐点inflection point函数的极值extremum of function极大值local(relative) maximum最大值global(absolute) mximum极小值local(relative) minimum最小值global(absolute) minimum目标函数objective function曲率curvature弧微分arc differential平均曲率average curvature曲率园circle of curvature曲率中心center of curvature曲率半径radius of curvature渐屈线evolute渐伸线involute根的隔离isolation of root隔离区间isolation interval切线法tangent line method第四章不定积分Chapter4 Indefinite Integrals原函数primitive function(antiderivative)积分号sign of integration被积函数integrand积分变量integral variable积分曲线integral curve积分表table of integrals换元积分法integration by substitution分部积分法integration by parts分部积分公式formula of integration by parts 有理函数rational function真分式proper fraction假分式improper fraction第五章定积分Chapter5 Definite Integrals曲边梯形trapezoid with曲边curve edge窄矩形narrow rectangle曲边梯形的面积area of trapezoid with curved edge积分下限lower limit of integral积分上限upper limit of integral积分区间integral interval分割partition积分和integral sum可积integrable矩形法rectangle method积分中值定理mean value theorem of integrals函数在区间上的平均值average value of a function on an integvals牛顿-莱布尼茨公式Newton-Leibniz formula微积分基本公式fundamental formula of calculus换元公式formula for integration by substitution递推公式recurrence formula反常积分improper integral反常积分发散the improper integral is divergent反常积分收敛the improper integral is convergent无穷限的反常积分improper integral on an infinite interval无界函数的反常积分improper integral of unbounded functions绝对收敛absolutely convergent第六章定积分的应用Chapter6 Applications of the Definite Integrals元素法the element method面积元素element of area平面图形的面积area of a luane figure直角坐标又称“笛卡儿坐标(Cartesian coordinates)”极坐标polar coordinates抛物线parabola椭圆ellipse旋转体的面积volume of a solid of rotation 旋转椭球体ellipsoid of revolution, ellipsoid of rotation曲线的弧长arc length of acurve可求长的rectifiable光滑smooth功work 水压力water pressure引力gravitation变力variable force第七章空间解析几何与向量代数Chapter7 Space Analytic Geometry and Vector Algebra向量vector自由向量free vector单位向量unit vector零向量zero vector相等equal平行parallel向量的线性运算linear poeration of vector三角法则triangle rule平行四边形法则parallelogram rule交换律commutative law结合律associative law负向量negative vector差difference分配律distributive law空间直角坐标系space rectangular coordinates坐标面coordinate plane卦限octant向量的模modulus of vector向量a与b的夹角angle between vector a and b方向余弦direction cosine方向角direction angle向量在轴上的投影projection of a vector onto an axis数量积,外积,叉积scalar product,dot product,inner product曲面方程equation for a surface球面sphere旋转曲面surface of revolution母线generating line轴axis圆锥面cone顶点vertex旋转单叶双曲面revolution hyperboloids of one sheet旋转双叶双曲面revolution hyperboloids oftwo sheets柱面cylindrical surface ,cylinder圆柱面cylindrical surface准线directrix抛物柱面parabolic cylinder二次曲面quadric surface椭圆锥面dlliptic cone椭球面ellipsoid单叶双曲面hyperboloid of one sheet双叶双曲面hyperboloid of two sheets旋转椭球面ellipsoid of revolution椭圆抛物面elliptic paraboloid旋转抛物面paraboloid of revolution双曲抛物面hyperbolic paraboloid马鞍面saddle surface椭圆柱面elliptic cylinder双曲柱面hyperbolic cylinder抛物柱面parabolic cylinder空间曲线space curve空间曲线的一般方程general form equations of a space curve空间曲线的参数方程parametric equations of a space curve螺转线spiral螺矩pitch投影柱面projecting cylinder投影projection平面的点法式方程pointnorm form eqyation of a plane法向量normal vector平面的一般方程general form equation of a plane两平面的夹角angle between two planes点到平面的距离distance from a point to a plane空间直线的一般方程general equation of a line in space方向向量direction vector直线的点向式方程pointdirection form equations of a line方向数direction number直线的参数方程parametric equations of a line两直线的夹角angle between two lines 垂直perpendicular直线与平面的夹角angle between a line and a planes平面束pencil of planes平面束的方程equation of a pencil of planes行列式determinant系数行列式coefficient determinant第八章多元函数微分法及其应用Chapter8 Differentiation of Functions of Several Variables and Its Application一元函数function of one variable多元函数function of several variables内点interior point外点exterior point边界点frontier point,boundary point聚点point of accumulation开集openset闭集closed set连通集connected set开区域open region闭区域closed region有界集bounded set无界集unbounded setn维空间n-dimentional space二重极限double limit多元函数的连续性continuity of function of seveal连续函数continuous function不连续点discontinuity point一致连续uniformly continuous偏导数partial derivative对自变量x的偏导数partial derivative with respect to independent variable x高阶偏导数partial derivative of higher order 二阶偏导数second order partial derivative 混合偏导数hybrid partial derivative全微分total differential偏增量oartial increment偏微分partial differential全增量total increment可微分differentiable必要条件necessary condition充分条件sufficient condition叠加原理superpostition principle全导数total derivative中间变量intermediate variable隐函数存在定理theorem of the existence of implicit function曲线的切向量tangent vector of a curve法平面normal plane向量方程vector equation向量值函数vector-valued function切平面tangent plane法线normal line方向导数directional derivative梯度gradient数量场scalar field梯度场gradient field向量场vector field势场potential field引力场gravitational field引力势gravitational potential曲面在一点的切平面tangent plane to a surface at a point曲线在一点的法线normal line to a surface at a point无条件极值unconditional extreme values条件极值conditional extreme values拉格朗日乘数法Lagrange multiplier method 拉格朗日乘子Lagrange multiplier经验公式empirical formula最小二乘法method of least squares均方误差mean square error第九章重积分Chapter9 Multiple Integrals二重积分double integral可加性additivity累次积分iterated integral体积元素volume element三重积分triple integral直角坐标系中的体积元素volume element in rectangular coordinate system柱面坐标cylindrical coordinates柱面坐标系中的体积元素volume element in cylindrical coordinate system 球面坐标spherical coordinates球面坐标系中的体积元素volume element in spherical coordinate system反常二重积分improper double integral曲面的面积area of a surface质心centre of mass静矩static moment密度density形心centroid转动惯量moment of inertia参变量parametric variable第十章曲线积分与曲面积分Chapter10 Line(Curve)Integrals and Surface Integrals对弧长的曲线积分line integrals with respect to arc hength第一类曲线积分line integrals of the first type对坐标的曲线积分line integrals with respect to x,y,and z第二类曲线积分line integrals of the second type有向曲线弧directed arc单连通区域simple connected region复连通区域complex connected region格林公式Green formula第一类曲面积分surface integrals of the first type对面的曲面积分surface integrals with respect to area有向曲面directed surface对坐标的曲面积分surface integrals with respect to coordinate elements第二类曲面积分surface integrals of the second type有向曲面元element of directed surface高斯公式gauss formula拉普拉斯算子Laplace operator格林第一公式Green’s first formula通量flux散度divergence斯托克斯公式Stokes formula环流量circulation旋度rotation,curl第十一章无穷级数Chapter11 Infinite Series一般项general term部分和partial sum余项remainder term等比级数geometric series几何级数geometric series公比common ratio调和级数harmonic series柯西收敛准则Cauchy convergence criteria, Cauchy criteria for convergence正项级数series of positive terms达朗贝尔判别法D’Alembert test柯西判别法Cauchy test交错级数alternating series绝对收敛absolutely convergent条件收敛conditionally convergent柯西乘积Cauchy product函数项级数series of functions发散点point of divergence收敛点point of convergence收敛域convergence domain和函数sum function幂级数power series幂级数的系数coeffcients of power series阿贝尔定理Abel Theorem收敛半径radius of convergence收敛区间interval of convergence泰勒级数Taylor series麦克劳林级数Maclaurin series二项展开式binomial expansion近似计算approximate calculation舍入误差round-off error,rounding error欧拉公式Euler’s formula魏尔斯特拉丝判别法Weierstrass test三角级数trigonometric series振幅amplitude角频率angular frequency初相initial phase矩形波square wave谐波分析harmonic analysis直流分量direct component 基波fundamental wave二次谐波second harmonic三角函数系trigonometric function system傅立叶系数Fourier coefficient傅立叶级数Forrier series周期延拓periodic prolongation正弦级数sine series余弦级数cosine series奇延拓odd prolongation偶延拓even prolongation傅立叶级数的复数形式complex form of Fourier series第十二章微分方程Chapter12 Differential Equation解微分方程solve a dirrerential equation常微分方程ordinary differential equation偏微分方程partial differential equation,PDE 微分方程的阶order of a differential equation 微分方程的解solution of a differential equation微分方程的通解general solution of a differential equation初始条件initial condition微分方程的特解particular solution of a differential equation初值问题initial value problem微分方程的积分曲线integral curve of a differential equation可分离变量的微分方程variable separable differential equation隐式解implicit solution隐式通解inplicit general solution衰变系数decay coefficient衰变decay齐次方程homogeneous equation一阶线性方程linear differential equation of first order非齐次non-homogeneous齐次线性方程homogeneous linear equation 非齐次线性方程non-homogeneous linear equation常数变易法method of variation of constant 暂态电流transient stata current稳态电流steady state current伯努利方程Bernoulli equation全微分方程total differential equation积分因子integrating factor高阶微分方程differential equation of higher order悬链线catenary高阶线性微分方程linera differential equation of higher order自由振动的微分方程differential equation of free vibration强迫振动的微分方程differential equation of forced oscillation串联电路的振荡方程oscillation equation of series circuit二阶线性微分方程second order linera differential equation线性相关linearly dependence线性无关linearly independce二阶常系数齐次线性微分方程second order homogeneour linear differential equation with constant coefficient二阶变系数齐次线性微分方程second order homogeneous linear differential equation with variable coefficient特征方程characteristic equation无阻尼自由振动的微分方程differential equation of free vibration with zero damping 固有频率natural frequency简谐振动simple harmonic oscillation,simple harmonic vibration微分算子differential operator待定系数法method of undetermined coefficient共振现象resonance phenomenon欧拉方程Euler equation幂级数解法power series solution数值解法numerial solution勒让德方程Legendre equation微分方程组system of differential equations 常系数线性微分方程组system of linera differential equations with constant coefficient。
Unit+2+Literary+Theory+and+Criticism
Unit 2 Literary Theory and CriticismThe practice of literary theory has historical roots that run as far back as ancient Greece and it became a profession in the 20th century. This unit will give you a brief introduction to literary theory and some of the major schools of literary criticism, which is often informed by literary theory.Part I Text ALead-inWhat is literary theory? What is literary criticism? And why do we need them? Write down your answers before reading Text A._____________________________________________________________________ _____________________________________________________________________ _____________________________________________________________________ Now read Text A and compare your answers with the author’s analysis.The reading process and literary theory1Charles E. Bressler The relationship between literary theory and a reader’s personal worldview is best illustrated in the act of reading itself. When reading, we are constantly interacting with the text. According to Louise M. Rosenblatt2’s text The Reader, the Text, the Poem (1978), during the act or event of reading,A reader brings to the text his or her past experience and present personality.Under the magnetism of the ordered symbols of the text, the readermarshals his or her resources and crystallizes out from the stuff of memory,thought, and feeling a new order, a new experience, which he/she sees asthe poem. This becomes part of the ongoing stream of the reader’s lifeexperience, to be reflected on from any angle important to him or her as ahuman being.Accordingly, Rosenblatt declares that the relationship between the reader and the text is not linear, but transactional; that is, it is a process or event that takes place at a particular time and place in which the text and the reader condition each other. The reader and the text transact, creating meaning, for meaning does not exist solely within the reader’s mind or within the text, Rosenblatt maintains, but in the transaction between them. To arrive at an interpretation of a text (what Rosenblatt calls the poem), readers bring their own “temperament and fund of past transactions to the text and live through a process of handling new situations, new attitudes, new personalities, [and] new conflicts in value. They can reject, revise, or assimilate into the resources with which they engage their world.”Through this transactional experience, readers consciously and unconsciously amend their worldview.Because no literary theory can account for all the various factors included in everyone’s conceptual framework, and because we as readers all have differentliterary experiences, there can exist no metatheory–no one overarching literary theory that encompasses all possible interpretations of a text suggested by its readers. And too, there can be no one correct literary theory, for in and of itself, each literary theory asks valid questions of and about a text, and no one theory is capable of exhausting all legitimate questions to be asked about any text.The valid and legitimate questions asked about a text by the various literary theories differ, often widely. Espousing separate critical orientations, each theory focuses primarily on one element of the interpretative process, although in practice different theories may address several areas of concern in interpreting a text. For example, one theory may stress the work itself, believing that the text alone contains all the necessary information to arrive at an interpretation. This theory isolates the text from its historical or sociological setting and concentrates on the literary forms found in the text, such as figures of speech, word choice, and style. Another theory may attempt to place a text in its historical, political, sociological, religious, and economic setting. By placing the text in historical perspective, this theory asserts that its adherents can arrive at an interpretation that both the text’s author and its original audience would support. Still another theory may direct its chief concern toward the text’s audience. It asks how the reader s’emotions and personal backgrounds affect each reader’s interpretation of a particular text. Whether the primary focus of concern is psychological, linguistic, mythical, historical, or from any other critical orientation, each literary theory establishes its own theoretical basis and then proceeds to develop its own methodology whereby readers can apply the particular theory to an actual text.Although each reader’s theory and methodology for arriving at a text’s interpretation differs, sooner or later groups of readers and critics declare allegiance to a similar core of beliefs and band together, thereby founding schools of criticism. For example, critics who believe that social and historical concerns must be highlighted in a text are known as Marxist critics, whereas reader-response critics concentrate on readers’ personal reactions to the text. Because new points of view concerning literary works are continually evolving, new schools of criticism – and therefore new literary theories – will continue to develop. One of the more recent schools to emerge in the 1980s and 1990s, New Historicism or Cultural Poetics, declares that a text must be analyzed through historical research that assumes that history and fiction are inseparable. The members of this school, known as New Historicists, hope to shift the boundaries between history and literature and thereby produce criticism that accurately reflects what they believe to be the proper relationship between the text and its historical context. Still other newly evolving schools of criticism, such as postcolonialism3, African American studies, and gender studies, continue to emerge and challenge previous ways of thinking about and critiquing texts.Because the various schools of criticism (and the theories on which they are based) ask different questions about the same work of literature, these theoretical schools provide an abundance of options from which readers can choose to broaden their understanding not only of texts but also of their society, their culture and their own humanity. By embracing literary theory, we learn about literature, but importantly, we are also taught tolerance for other people’s beliefs. By rejecting or ignoringtheory, we are in danger of canonizing ourselves as literary saints who possess divine knowledge and who can therefore supply the one and only correct interpretation for a given text. When we oppose, disregard or ignore literary theory, we are in danger of blindly accepting our often unquestioned prejudices and assumptions. By embracing literary theory and literary criticism (its practical application), we can participate in that seemingly endless historical conversation about the nature of humanity and of humanity’s concerns as expressed in literature. In the process, we can begin to question our concepts of ourselves, our society, and our culture and how texts themselves help define and continually redefine these concepts. (972 words)New Words and Expressionsmagnetism / / n. a quality that makes sth./ sb. very attractive 吸引力, 魅力marshal / / vt. to bring together or organize people or things in order to achieve a particular aim 集结;排列crystallize / / v. to become definite or easily understood, or to make sth. definite or easily understood 使(思想、计划等)具体化linear / / a. involving ideas or events that are directly connected and follow one after the other 通过单独的若干阶段来发展amend / / vt. to make changes to a document, law, agreement, etc. esp. in order to improve it 修正metatheory / / n. 超理论(用以阐明某一或某类理论而本身又更高超的一种理论) overaching / / a. most important, because including or affecting all other areas首要的encompass / / vt. to include, especially different types of things 包含legitimate / / a. fair and reasonable 合情合理的espouse / / vt. to become involved with or support an activity or opinion 支持,拥护adherent / / n. a supporter of a set of ideas, an organization, or a person支持者,拥护者linguistic / / a. connected with language or the study of language 语言的;语言学的allegiance / / n. strong loyalty to a person, group, idea or country 忠诚critique / / vt. to express one’s opinion about sth. after examining and judging it carefully and in detail 对……发表评论embrace / / vt. to accept sth. enthusiastically 信奉canonize / / vt. to announce officially that someone is a saint正式宣布(某人)为圣徒Notes1. This text is taken from Literary Criticism: An Introduction to Theory and Practice (2003), by Charles E. Bressler, a professor of English at Houghton College.2. Louise M. Rosenblatt (1904-2005): an influential scholar of reading and the teaching of literature. She was an emeritus professor of English education at New York University3. postcolonialism: a specifically intellectual discourse that consists of reactions to, and analysis of, the cultural legacy of colonialism.Critical Reading and ThinkingTask 1 OverviewTask 2 Points for DiscussionDiscuss the following questions with your classmate(s) and referring to the speaking strategies in Part V might be helpful.1.According to Louise M. Rosenblatt, how do the readers interact with the text?2.What does a literary theory account for? Why do we need a theory?3.What is a metatheory? According to Text B, is there any metatheory?4.What is the relationship between literary theory and literary criticism?5.What are the major concerns of the following schools of criticism: Marxistcriticism, reader-response criticism, New Historicism, postcolonialism, African American studies and gender studies?Language Building-upTask 1 Specialized vocabularyThe following terms are selected from Text A. Translate them either from Chinese to English or from English to Chinese.1.文学理论________________________________2.文学批评________________________________3.批评流派________________________________4.修辞________________________________5.选词________________________________6.Marxist critics ________________________________7.New Historicism _______________________________8.Cultural Poetics ________________________________9.Postcolonialism ________________________________10.African American studies __________________________11.gender studies ________________________________Task 2 Signpost languages (cause and effect)There are various expressions and patterns indicating a cause and effect relationship.The following sentences are taken from Text A, and all the sign-post languages indicating cause and effect have been removed. Complete the sentences and then compare your answers with the original sentences in Text A.1.The reader and the text transact, creating meaning, _________ meaning does notexist solely within the reader’s mind or within the text, Rosenblatt maintains, but in the transaction between them. (Paragraph 1)2._________ no literary theory can account for all the various factors included ineveryone’s conceptual framework, and _________ we as readers all have different literary experiences, there can exist no metatheory – no one overarching literary theory that encompasses all possible interpretations of a text suggested by its readers. (Paragraph 2)3.…there can be no one correct literary theory, _________ in and of itself, eachliterary theory asks valid questions of and about a text, and no one theory is capable of exhausting all legitimate questions to be asked about any text.(Paragraph 2)4._________ new points of view concerning literary works are continually evolving,new schools of criticism – and _________ new literary theories – will continue to develop. (Paragraph 4)5.The members of this school, known as New Historicists, hope to shift theboundaries between history and literature and _________ produce criticism that accurately reflects what they believe to be the proper relationship between the text and its historical context. (Paragraph 4)6.By rejecting or ignoring theory, we are in danger of canonizing ourselves asliterary saints who possess divine knowledge and who can _________ supply the one and only correct interpretation for a given text. (Paragraph 5)Task 3 Formal EnglishThe following sentences are selected from Text A. Change the underlined formal words into forms that are neutral or less formal.1.There can exist no metatheory –no one overarching literary theory thatencompasses all possible interpretations of a text suggested by its readers.2.Espousing separate critical orientations, each theory focuses primarily on oneelement of the interpretative process …3.This theory asserts that its adherents can arrive at an interpretation that both thetext’s author and its original audience would support.4.Whether the primary focus of concern is psychological, linguistic, mythical,historical, or from any other critical orientation, each literary theory establishes its own theoretical basis and then proceeds to develop its own methodology whereby readers can apply the particular theory to an actual text.5. Although each reader’s theory and methodology for arriving at a text’sinterpretation differs, sooner or later groups of readers and critics declare allegiance to a similar core of beliefs and band together, thereby founding schools of criticism.Part II Text BLiterary criticism has probably existed for as long as literature, and great critics can be as entertaining and stimulating as great poets and novelists. In this essay, a critic reflects on the meaning of his work.The Will Not to Power, but to Self-Understanding1Adam Kirsch If you are writing poetry, or even fiction, the best response to the “absence of echo” is probably indifference. The echoes that creative work provokes are generally too quiet and internal to be measured by indexes like sales figures. Things are somewhat different for a critic, since the critic is necessarily more conscious than other writers of his own will, of what he wants to happen in the world as a result of his writing. As Alfred Kazin2puts it, “He writes to convince, to argue, to establish his argument.”But if this were a critic’s only purpose, his will would merely be a will to power. And a critic who writes primarily out of a will to power (they do exist; they could be named) is never a great critic, or a lasting one. Increasingly, I feel that argument is only the form of criticism, not the substance, just as passing judgment on a particular book is only the occasion of criticism, not the goal. It’s better —certainly it’s better for the critic — not to see criticism as a means of making things happen, of rewarding and punishing, o r of becoming what Kazin calls a “force.” The critic participates in the world of literature not as a lawgiver or a team captain for this or that school of writing, but as a writer, a colleague of the poet and the novelist. Novelists interpret experience through the medium of plot and character, poets through the medium of rhythm and metaphor, and critics through the medium of other texts.This is my definition of “serious criticism,” and I think it’s essentially the same today as it was 50 years ago: a serious critic is one who says something true about life and the world. The critic’s will is not to power, but to self-understanding, self-expression, truth. A review by Edmund Wilson3 in The New Yorker might once have had the power to drive a book’s sales up or down, but that’s not why we continue to read “The Wound and the Bow4.” Lionel Trilling5 never had that kind of concrete power, but that doesn’t stop us from continuing to read “The Opposing Self6.” These books are classics of criticism because they each show a mind working out its own questions —about psychology, society, politics, morals —through reading. In this sense, Wilson and Trilling and other critics in their tradition, of whom Frank Kermode7 might have been the last example, show us what reading can be: a way of making one’s self, one’s soul.Of course, this is an ideal. Most of the time, depending on the kind of piece she is writing, the critic also has other responsibilities. She is a journalist: a review is, in part, a news story about a new book and why it matters. She is a consumer advocate, giving the reader enough information to decide whether to buy the book. At times — as we saw recently in the discussion of Jonathan Franzen’s8“Freedom”— she is a social commentator, trying to determine what the success (or failure) of a particular book says about America at large, how the nation lives or thinks or imagines.In this way, the role of the critic can shade into that of the public intellectual, and of course many great critics have been intellectuals, too. (So have many novelists and poets — look at George Eliot9and T. S. Eliot10.) Trilling wrote about Jane Austen11, but also about the Kinsey Report12; Kazin wrote about Blake13, but also about John F. Kennedy14. This kind of widening of the purview of criticism is natural, because thinking about literature eventually means thinking about society and politics. For Matthew Arnold15, the inability of his contemporaries to write in what he called the “grand style” led him to a general critiq ue of Victorian society, which he saw as addicted to materialism and utilitarianism.I’m not sure if anyone is writing this kind of criticism today — certainly, the most admired literary critics aren’t —and the reason is probably the one Kazin cited: “th e growing assumption that literature cannot affect our future, that the future is in other hands.” This development, whose beginnings he saw 50 years ago, has now come to pass. It is difficult to recapture the old sense, which Arnold had, that the literary critic is the critic par excellence, that the study of literature gives you the best vantage point from which to understand an entire society.Perhaps this loss of centrality accounts for my own inclination to put the emphasis in the phrase “literary criticism” on the first word, not the second. If you are primarily interested in writing, then you do not need a definite or immediate sense of your audience: you write for an ideal reader, for yourself, for God, or for a combination of the three. If you want criticism to be a lever to move the world, on the other hand, you need to know exactly where you’re standing —that is, how many people are reading, and whether they’re the right people. In short, you must worry about reaching a “general audience,” with a ll the associated worries about fragmentation, the decline of print, and the rise of the Internet and its mental groupuscules.Like everyone, I wonder whether a general audience, made up of what Virginia Woolf16called “common readers,” still exists. If i t does, the readership of The New York Times Book Review is probably it. But measured against the audience for a new movie or video game, or against the population as a whole, even the Book Review reaches only a niche audience. Perhaps the only difference between our situation and Arnold’s is that in Victorian England, the niche that cared about literature also happened to constitute the ruling class, while in democratic, mass-media America, the two barely overlap.What this displacement takes from the critic in terms of confidence and authority, it perhaps restores to him in terms of integrity and freedom. Or maybe it’s just that, as a poet, I am all too used to making excuses for the marginality of a kind of writingthat I continue to feel is important. Whether I am writing verse or prose, I try to believe that what matters is not exercising influence or force, but writing well — that is, truthfully and beautifully; and that maybe, if you seek truth and beauty, all the rest will be added unto you. (1069 words)New Words and Expressionspurview / / n. the limit of someone's responsibility, interest or activity(活动、理解能力等的)范围;权限utilitarianism / / n. the system of thought which states that the best action or decision in a particular situation is the one which brings most advantages tothe most people 功利主义come to pass to happen, to take place 发生par excellence to a degree of excellence 最卓越,超群vantage point a place, especially a high place, which provides a good clear view of an area 有利位置lever / / n.杠杆groupuscule / / n. a small, activist group or faction 小团体;小派别niche audience relatively small audience with specialized interests, tastes, andbackgrounds 一小部分有特殊兴趣、品味的读者、(听)观众displacement / / n. the process of forcing sth. out of its position or space 移位marginality / / n. the property of not being central 边缘性unto / / prep. (now used only in antiquated, formal, or scriptural style) toNotes1. A version of this article appeared in print on January 2, 2011, on page BR10 of theSunday Book Review. Adam Kirsch is the author of several books of poetry and criticism, as well as a biography, Benjamin Disraeli.2. Alfred Kazin (1915 - 1998): an American writer and literary critic.3. Edmund Wilson (1895 - 1972): an American writer and literary and social critic andnoted man of letters.4. The Wound and the Bow: a collection of seven essays on literary themes byEdmund Wilson.5. Lionel Trilling (1905 - 1975): an American literary critic, author, and teacher.6. The Opposing Self: a collection of nine essays in criticism, by Lionel Trilling.7. Frank Kermode (1919 - 2010): a highly regarded British literary critic best knownfor his seminal critical work The Sense of an Ending: Studies in the Theory of Fiction, published in 1967 (revised 2000).8. Jonathan Franzen (1959 - ): an American novelist and essayist. His most recentnovel, Freedom, was published in August 2010.9. George Eliot (1819 - 1880): an English novelist, journalist and translator, and oneof the leading writers of the Victorian era.10. T. S. Eliot (1888 –1965): an American-born English poet, playwright, and literarycritic, arguably the most important English-language poet of the 20th century.11. Jane Austen (1775 - 1817): an English novelist. Her works of romantic fictionearned her a place as one of the most widely read writers in English literature. 12. Kinsey Reports: two books on human sexual behavior, published in 1948 and1953. Kinsey was a zoologist at Indiana University.13. (William) Blake (1757 – 1827): an English poet, painter, and printmaker.14. John F. Kennedy (1917 - 1963): the 35th President of the United States, servingfrom 1961 until his assassination in 1963.15. Matthew Arnold (1822 - 1888): a British poet and cultural critic.16. Virginia Woolf (1882 - 1941): an English author, essayist, publisher, and writer ofshort stories, regarded as one of the foremost modernist literary figures of the twentieth century.Critical Reading and ThinkingTask 1 Major viewsDecide whether the author of Text B agrees with the following statements or not.______1. The goal of criticism is making judgment and convincing others.______2. In some sense, a critic’s work is the same as a novelist’s.______3. A critic is also a journalist and a consumer advocate.______4. Literature can affect our future.______5. People are now more interested in watching movies and playing video games than in reading books.______6. In modern America, the ruling class isn’t interested in literature.______7. What matters in writing verse or prose is exerting influence.Task 2 Points for discussionDiscuss the following questions with your classmate(s) and referring to the speaking strategies in Part V might be helpful.1. How do you understand the title The Will Not to Power, but to Self-Understanding?2. Why does the author put emphasis on the first rather than the second word of “literary criticism”?3. What this displacement takes from the critic in terms of confidence and authority, it perhaps restores to him in terms of integrity and freedom.(Line )What does this sentence mean?ResearchingRead one book review from the latest newspaper and try to understand the critic’s purpose.Part III Text C (For Your Information)First wave of feminist criticism: Woolf and de Beauvoir1Charles E. Bressler In 1919, the British scholar and teacher Virginia Woolf (1882-1941) laid thefoundation for present-day feminist criticism in her seminal work A Room of One’s Own2. In this text, Woolf declares that men have and continue to treat women as inferiors. It is the male, she asserts, who defines what it means to be female and who controls the political, economic, social, and literary structures. Agreeing with Samuel T. Coleridge3, one of the foremost nineteenth-century literary critic, that great minds possess both male and female characteristics, she hypothesizes in her text the existence of Shakespeare’s sister, one who is equally as gifted as a writer as Shakespeare himself. Her gender, however, prevents her from having “a room of her own”. Because she is a woman, she cannot obtain an education or find profitable employment. Her innate artistic talents will therefore never flourish, for she cannot afford her own room, Woolf’s symbol of the solitude and autonomy needed to seclude one’s self from the world and its social constraints in order to find time to think and write. Ultimately, Shakespeare’s sister dies alone without any acknowledgement for her personal genius. Even her grave bears not her name, for she is buried in an unmarked grave simply because she is female.This kind of loss of artistic talent and personal worthiness, says Woolf, is the direct result of society’s opinion of women: to wit, that they are intellectually inferior to men. Women, Woolf argues, must reject this social construct and establish their own identity. Women must challenge the prevailing, false cultural notions about their gender identity and develop a female discourse that will accurately portray their relationship “to the world of reality and not to the world of men.” If women accept this challenge, Woolf believes that Shakespeare’s sister can be resurrected in and through women living today, even those who may be “washing up the dishes and putting the children to bed” right now. Regrettably, the Great Depression of the 1930s and World War II in the 1940s focused humankind’s attention on other matters and delayed the development of such feminist ideals.With the 1949 publication of The Second Sex by the French writer Simone de Beauvoir (1908 - 1986)4, however, feminist interests were once again surfacing. Heralded as the foundational work of twentieth-century feminism, Beauvoir’s text declares that French society (and Western societies in general) are patriarchal, controlled by males. Like Woolf before her, Beauvoir believed that the male in these societies defines what it means to be human, including, therefore, what it means to be female. Since the female is not male, Beauvoir asserted, she becomes the Other, an object whose existence is defined and interpreted by the male, the dominant being in society. Always subordinate to the male, the female finds herself a secondary or nonexistent player in the major social institutions of her culture, such as the church, government, and educational systems. Beauvoir asserts that a woman must break the bonds of her patriarchal society and define herself if she wishes to become a significant human being in her own right and defy male classification as the Other. She must ask herself, “What is a woman?”Beauvoir insists that a woman’s answer must not be “mankind”, for such a term once again allows men to define woman. This generic label must be rejected, for it assumes that “humanity is male and man defines woman not in herself as relative to him.” (576 words)。
Distributed Order Calculus and Equations of Ultraslow Diffusion
Umarov and Gorenflo [39] applied to equations (1.2) Dubinskij’s theory [8] of analytic pseudo-differential operators. This leads to solvability results for (1.2) in the spaces of analytic functions and dual spaces of analytic functionals. Such a theory is very different from the theory of parabolic equations; results obtained this way “do not feel” the difference between the equations (1.2) with B = ∆ and B = −∆. The aim of this paper is to develop a theory of the model equation (1.2) with B = ∆ comparable with the classical theory of the Cauchy problem for the heat equation. In particular, we construct and investigate in detail a fundamental solution of the Cauchy problem for the homogeneous equation (f = 0) and the corresponding kernel appearing in the volume potential solving the inhomogeneous equation, prove their positivity and subordination properties. This leads to a rigorous understanding of a solution of the Cauchy problem – it is important to know, in which sense a solution satisfies the equation. In its turn, this requires a deeper understanding of the distributed order derivative (1.3), the availability of its various forms resembling the classical fractional calculus [36]. We also introduce and study a kind of a distributed order fractional integral corresponding to the derivative (1.3). A Marchaud-type representation of the distributed order derivative (based on a recent result by Samko and Cardoso [35]) is the main tool for obtaining, in the spirit of [19, 9], uniqueness theorems for the Cauchy problem for general equations (1.2) in the class of bounded functions and, for n = 1 and B = d2 /dx2 , in the class of functions of sub-exponential growth. Comparing with the theory of fractional diffusion equation (1.1) we see that the distributed order equations (under reasonable assumptions regarding µ) constitute the limiting case equations, as α → 0. That is readily observed from estimates of fundamental solutions having, 2 as |x| → ∞, the estimate exp −a|x| 2−α , a > 0, for the fractional diffusion equations, and exp(−a|x|) in the case of ultraslow diffusion. In fact, we begin with the “ordinary” equation D(µ) u = λu, λ ∈ R. If λ < 0, already this equation demonstrates a logarithmic decay of solution at infinity; see Theorem 2.3 below. In general, the theory presented here is an interesting example of subtle analysis (with kernels from L1 belonging to no Lp , p > 1, etc) appearing in problems of a direct physical significance.
Cauchy-Schwarzinequality[1]
b2 i
.
Using the induction hypothesis, one has
k+1 k+1 k k 2 a2 i + ak+1 · i=1 k k i=1 2 b2 i + bk+1
a2 i ·
i=1 i=1
b2 i =
≥
i=1 k
a2 i ·
i=1
b2 i + |ak+1 bk+1 |
k+1
≥
i=1
|ai bi | + |ak+1 bk+1 | =
i=1
|ai bi |.
It means that the inequality (1) holds for n = k + 1, we thus conclude that the inequality (1) holds for all natural numbers n. This completes the proof of inequality (1). Proof 7. Let A = {a1 b1 , · · · a1 bn , a2 b1 , · · · , a2 bn , · · · , an b1 , · · · an bn } B = {a1 b1 , · · · a1 bn , a2 b1 , · · · , a2 bn , · · · , an b1 , · · · an bn } C = {a1 b1 , · · · a1 bn , a2 b1 , · · · , a2 bn , · · · , an b1 , · · · an bn } D = {a1 b1 , · · · an b1 , a1 b2 , · · · , an b2 , · · · , a1 bn , · · · an bn } It is easy to observe that the set A and B are similarly sorted, while the set C and D are mixed sorted. Applying the rearrangement inequality, we have (a1 b1 )(a1 b1 ) + · · · + (a1 bn )(a1 bn ) + (a2 b1 )(a2 b1 ) + · · · + (a2 bn )(a2 bn ) + · · · + (an b1 )(an b1 ) + · · · + (an bn )(an bn ) ≥ (a1 b1 )(a1 b1 )+ · · · +(a1 bn )(an b1 )+(a2 b1 )(a1 b2 )+ · · · +(a2 bn )(an b2 )+ · · · +(an b1 )(a1 bn )+ · · · +(an bn )(an bn ), which can be simplified to the inequality
拉马努金
他15岁时,朋友借给他英国数学家卡尔(G. Carr)写的《纯粹数学与应 用数学概要》一书。该书收录了代数、、三角微积分学和解析几何的五 千多个方程,但书中没有给出详细的证明。这正好符合拉马努金的胃口, 他把每一个方程式当成一个研究题,尝试对其进行独特的证明而且还对 其中一些进行推广。这花去了他大约5年的时间,留下了几百页的数学笔 记。他证明了其中的一些方程,而以后他研究的基础却受益于这本书。
除了在纯粹数学方面做出卓越的成就以外,拉马努金的理论还得到了广泛的应 用。他发现的好几个定理在包括粒子物理、统计力学、计算机科学、密码技术 和空间技术等不同领域起着相当重要的作用,甚至晶体和塑料的研制也受到他 创立的整数分拆理论的启发,而他在黎曼ζ函数方面的研究成果,现在已经与齿 轮技术的进步挂上了钩,还被用于测温学及冶金高炉的优化。他生命中的最后 一项成果——模仿θ函数有力地推动了用孤立波理论来研究癌细胞的恶化和扩散 以及海啸的运动;最近有专家认为,这一函数很可能被用来解释宇宙黑洞的部 分奥秘,而令人吃惊的是,当拉马努金首次提出这种函数的时候,人们还不知 道黑洞是什么。
Much of Ramanujan’s work is in number theory, a branch of mathematics that deals with the subtle (难 以捉摸的) laws and relationships that govern numbers. Mathematicians describe his results as elegant and beautiful but they are much too complex to be appreciated by laymen.
机械工程学专业词汇英语翻译(C)1
cable stayed bridge 斜拉桥 cad 计算机辅助设计 calculator 计算机 calculus of approximation 近似计算 calculus of finite differences 差分演算 calibration 校准 calibrator 校准器 calorific capacity 热容量 calorimetric measurement 量热测量 camber changing flap 改变机翼弯度的襟翼 canal 管道 canal vortex 沟渠涡旋 canal wave 沟渠波 canard 鸭翼 canonical coordinate 正则坐标 canonical distribution 正则分布 canonical equation of motion 正则运动⽅程 canonical equations 正则⽅程 canonical form 正则形式 canonical momentum 正则动量 canonical transformation 正则变换 canonical variable 正则变量 cantilever 悬臂梁 caoutchouc elasticity 橡胶弹性 capacitive transducer 电容传感器 capacity 功率 capacity measure 容积量度 capacity strain gage 电容应变计 capillarity ⽑细现象 capillary absorption ⽑细管吸收 capillary action ⽑细酌 capillary attraction ⽑细引⼒ capillary condensation ⽑细凝缩 capillary constant ⽑细常数 capillary energy 表⾯张⼒能 capillary fissure ⽑细裂纹 capillary flow ⽑管流 capillary force ⽑细⼒ capillary gravity wave ⽑细重⼒波 capillary level oscillation ⽑细⾯振动 capillary phenomenon ⽑细现象 capillary pressure ⽑细压⼒ capillary rise ⽑细升⾼ capillary tension ⽑细张⼒ capillary tube ⽑细管 capillary viscosimeter ⽑细管粘度计 capillary waves ⽑细波 capture 俘获 carbon fiber 碳纤维 cardan angle 卡登⾓ cardan rings 卡登环 cardiac dynamics ⼼脏动⼒学 cardiac work ⼼脏的⼯作 cargo 货物 carrier gas ⽓体载体 carrier inertial force 牵连惯性⼒ carrier liquid 载体液体 carrier oscillation 载波振荡 carrier rocket 运载⽕箭 carrier velocity 牵连速度 carrying capacity 负荷量 cartesian coordinates 笛卡⼉坐标 cartesian vector 笛卡⼉⽮量 cascade excitation 级联激发 cascade flow 翼栅怜 cascade of aerofoil 翼型叶栅 cascade tunnel 叶栅风洞 case depth 渗碳层深度 case hardening 表⾯硬化 casing 外壳 castigliano theorem 卡斯蒂利亚诺定理 casting stress 铸造应⼒ catapult 弹射器 catenary 悬链线 catenoid 悬链曲⾯ cauchy deformation tensor 柯挝变张量 cauchy equation of motion 柯嗡动⽅程 cauchy integral theorem 柯锡分定理 cauchy law of similarity 柯梧似性定律 cauchy residue theorem 柯涡数定理 cauchy riemann equations 柯卫杪 匠眺 cauchy stress tensor 柯桅⼒张量 caudad acceleration 尾向加速度 causality 因果律 caving 空泡形成 cavitating flow ⽓⽳流涡空流 cavitation ⽓蚀现象 cavitation bubble 空泡 cavitation damage 空化损坏 cavitation effect 空化效应 cavitation erosion 空蚀 cavitation nucleus 空化核 cavitation number 空化数 cavitation parameter 空化参数 cavitation phenomenon ⽓蚀现象 cavitation shock ⽓蚀冲击 cavitation tunnel 空泡试验筒 cavity 空腔 cavity collapse 空泡破裂 cavity drag 空泡阻⼒ cavity flow ⽓⽳流涡空流 cavity flow theory 空泡另论 cavity formation 空泡形成 cavity pressure 空腔压⼒ cavity resonator 空腔共振器 cavity vibration 共振腔振动 ceiling 上升限度 celestial mechanics 天体⼒学 cell model 笼⼦模型 cell reynolds number 格雷诺数 cellular grid 状栅格 cellular structure 栅格结构 center 中⼼ center line 中⼼线 center line average height 中线平均⾼度 center line of the bar 杆件轴线 center of area ⾯积中⼼ center of buoyancy 浮⼼ center of curvature 曲率中⼼ center of gravity 重⼼ center of inertia 惯性中⼼ center of inertia system 惯性中⼼坐标系 center of inversion 反演中⼼ center of mass 质⼼ center of mass coordinate 质⼼坐标系 center of mass law 质⼼定理 center of mass motion 质⼼运动 center of mass system 质⼼坐标系 center of mass theorem 质⼼定理 center of oscillation 震荡中⼼ center of percussion 撞恍⼼ center of rotation 转动中⼼ center of similarity 相似中⼼ center of twist 扭转中⼼ center of vorticity 涡⼼ center to center distance 中⼼距 center to center spacing 中⼼距 centered compressional wave 有⼼压缩波 centered rarefactional wave 有⼼稀疏波 centi 厘 centigrade temperature 摄⽒温度 centimetre 厘⽶ centimetre gramme second 厘⽶克秒 central 中⼼的 central angle 中⼼⾓;圆⼼⾓ central axis of inertia 惯性中⼼轴 central body 中枢体 central difference method 中⼼差分法 central force 有⼼⼒ central force field 有⼼⼒场 central gas stream 中⼼⽓流 central impact 对⼼碰撞 central limit theorem 中⼼极限定理 central line 中线 central moment 中⼼⼒矩 central point 中⼼点 central potential 有⼼⼒势 central principal axis of inertia 中⼼惯性轴 central principal moment of inertia 中⼼知动惯量 centre 中⼼ centre of buyoncy 浮⼼ centre of curvature 曲率中⼼ centre of force ⼒⼼ centre of gravity 重⼼ centre of gyration 旋转中⼼ centre of inertia 质⼼ centre of mass 质⼼ centre of mass motion 质⼼运动 centre of mass system 质⼼系 centre of percussion 撞恍⼼ centre of pressure 压⼒中⼼ centrifugal 离⼼的 centrifugal acceleration 离⼼加速度 centrifugal effect 离⼼效应 centrifugal field 离⼼⼒场 centrifugal force 离⼼⼒ centrifugal governor 离⼼式蒂器 centrifugal inertial force 惯性离⼼⼒ centrifugal load 离⼼荷载 centrifugal pendulum 离⼼摆 centrifugal potential 离⼼势 centrifugation 离⼼分离 centrifuge 离⼼机 centrifuge modelling 离⼼模拟 centripetal 向⼼的 centripetal acceleration 向⼼加速度 centripetal force 向⼼⼒ centrode 瞬⼼轨迹 centroid 质⼼ centroid axis 重⼼轴线 centroid of area ⾯⼼ centroidal principal axes of inertia 重⼼诌性轴 centrosymmetric 中⼼对称的 cgs system cgs 单位制 chain drive 链条传动 chain graph 链图 chain reaction 连锁反应 chain transmission 链条传动 chance event 随机事件 chance quantity 随机量 chance variable 随机变量 change 变化 change of coordinates 坐标变换 change of form 形态变化 change of state 物态变化 change of the variable 变数更换 change of the wind 风向改变 changing load 交变负载 channel 渠道 channel diffusion 通道扩散 channel flow 渠道怜 chaos 混沌 chaplygin correspondence principle 恰普雷⾦对应原理 chaplygin equation 恰普雷⾦⽅程 chaplygin fluid 恰普雷⾦铃 chaplygin function 恰普雷⾦函数 chapman enskog method 查普曼⾖科格⽅法 chapman enskog solution 查普曼⾖科格解 chapman jouguet condition 查普曼儒盖条件 chapman jouguet hypothesis 查普曼儒盖假设 chapman kolmogoroff equation 查普曼柯尔莫果洛夫⽅程 chapman layer 查普曼层 characteristic 特性 characteristic curve 特性曲线 characteristic datum 特盏 characteristic determinant 特招列式 characteristic diagram 特者图 characteristic einstein temperature 爱因斯坦特章度 characteristic energy 特哲量 characteristic equation 特性⽅程 characteristic frequency 特盏率 characteristic function 特寨数 characteristic hydraulic number 特蘸压数 characteristic length 特栅度 characteristic line 特性线 characteristic matrix 特肇阵 characteristic parameter 特性参数 characteristic plane 特战⾯ characteristic quantity 特性量 characteristic surface 特怔⾯ characteristic surge impedance 特性浪涌阻抗 characteristic temperature 特章度 characteristic value 特盏 characteristic vector 特崭量 characteristic velocity 特召度 characteristic wavelength 特炸长 characteristics 特性 charge 装药 charpy impact machine 却贝冲辉验机 charpy impact test 却贝冲辉验 chatter amplitude 颤动幅度 chatter mark 振颤痕 chatter vibration 颤动 chattering 颤动 check 校验 check analysis 检验分析 chilling 冷硬 choke 扼⼒ choke free ⽆阻塞的 choked nozzle 壅塞式喷管 choked wind tunnel 阻塞式风洞 choking 壅塞 choking coil 扼⼒ choking mach number 壅塞马赫数 choking region 壅柳 choking velocity 壅塞速度 chopped wave 斩波 choppy sea 三⾓浪 chord 翼弦 chord length 弦长 chronometry 测时 ciliary motion 纤⽑运动 circle errors of gyroscope 陀螺盘旋误差 circle of curvature 曲率圆 circle of inertia 惯性圆 circle of inflexions 挠曲圆 circular cone 圆锥 circular cylinder 圆柱 circular function 圆函数 circular motion 圆周运动 circular orbit 圆形轨道 circular pendulum 圆摆 circular shaft 圆轴 circular tube 圆管 circular velocity 圆速度 circular vibration 圆振动 circular vortex 圆涡 circular vorticity 圆涡 circular wave number vector 圆波⽮量 circular whirl 圆涡 circulating air 循环空⽓ circulating flow 环流 circulating water 循环⽔ circulation 循环 circulation branch 环林⽀ circulation coefficient 环恋数 circulation constant 环粒数 circulation free ⽆环聊 circulation index 环粮数 circulation layer 环零 circulation loop 循环管路 circulation of the vector field ⽮量场环路 circulation of water ⽔循环 circulation pattern 环良 circulation preserving motion 环量守恒运动 circulation process 循环过程 circulation theorem 环哩理 circulation water channel 循环⽔槽 circulator sector 扇形 circulatory flow 环流 circulatory integral 循环积分 circulatory motion 环了动 circulatory system 循环系统 circumference 圆周 circumferential component 周缘分量 circumferential direction 周向 circumferential force 切向⼒ circumferential speed 周向速率 circumglobal radiation 球⾯总辐射 circumgyration 回转 circumpolar vorticity 环极涡旋 circumsphere 外接球 cistern barometer 液槽⽓压计 civil engineering ⼟⽊⼯程 clamped beam 固⽀梁 clapeyron elastic body 克拉佩隆弹性体 clapotis 驻波 clapp oscillator 克拉普振荡器 classical mechanics 经典⼒学 classical physics 经典物理学 classical statistical mechanics 经典统计⼒学 classical theory of probability 经典概率论 classical thermodynamics 经典热⼒学 clausius clapeyron equation 克劳修斯克拉佩隆⽅程 clausius clapeyron relation 克劳修斯克拉佩隆⽅程 clausius duhem inequality 克劳修斯迪昂不等式 clausius planck inequality 克劳修斯普朗克不等式 clearance 间隙 cleavage 劈裂 cleavage crack 解理裂纹 cleavage fracture 解理断裂 cleavage fracture strength 解理断裂强度 cleavage plane 裂开⾯ cleavage strength 解理强度 cleft 裂纹 cleft family 裂⼝族 cleftiness 裂隙 climbing 攀移 climbing speed 上升速率 clinoaxis 斜轴 clipper 快速帆船 clockwise 顺时针⽅向的 clockwise rotation 顺时针旋转 closed loop 闭环 closed shell 闭壳 closed system 闭合系 closed wind tunnel 闭式回羚洞 closing pressure 关闭压⼒ co oscillating tides 共振潮 co oscillation 合振荡 co tidal line 等潮线 coagulation 凝聚 coalescence 聚并 coanda effect 柯安达效应 coasting motion 惯性运动 coating thickness 涂层厚度 cockpit 驾驶舱 coefficient of amplification 放⼤系数 coefficient of apparent expansion 表观膨胀系数 coefficient of compressibility 压缩系数 coefficient of condensation 凝结系数 coefficient of consolidation 固结系数 coefficient of contraction 收缩系数 coefficient of cubical expansion 体胀系数 coefficient of diffusion 扩散系数 coefficient of dispersion 弥散系数 coefficient of eddy viscosity 湍脸性系数 coefficient of elasticity 弹性系数 coefficient of elongation 伸长系数 coefficient of expansion 膨胀系数 coefficient of friction 摩擦系数 coefficient of heat conduction 热传导系数 coefficient of heat transmission 传热系数 coefficient of infiltration 浸渗系数 coefficient of internal friction 内摩擦系数 coefficient of kinetic friction 动摩擦系数 coefficient of linear extension 线伸长系数 coefficient of mutual diffusion 相互扩散系数 coefficient of pivoting friction 枢轴摩擦系数 coefficient of pressure diffusion 加压扩散系数 coefficient of regression 回归系数 coefficient of resistance 阻⼒系数 coefficient of restitution 恢复系数 coefficient of rolling friction 滚动摩擦系数 coefficient of sliding friction 滑动摩擦系数 coefficient of stability 稳定性系数 coefficient of static friction 静摩擦系数 coefficient of surface expansion 表⾯膨胀系数 coefficient of thermal conductivity 导热系数 coefficient of thermal expansion 热膨胀系数 coefficient of transmission 透射系数 coefficient of viscosity 粘性系数 coherence distance 相⼲距离 coherence function 相⼲函数 coherence length 相⼲距离 coherence scattering 相⼲散射 coherent structure of turbulence 湍拎⼲结构 coherent wave 相⼲波 cohesion 内聚 cohesion force 内聚⼒ cohesion pressure 内聚压⼒ cohesion strength 内聚强度 cohesionless soil ⽆粘聚性⼟ cohesive energy 内聚能 cohesive soil 粘聚性⼟ coiled spring 螺旋形弹簧 cold bending test 冷弯曲试验 cold brittleness 冷脆性 cold crack 冷裂纹 cold cutting 冷切 cold deformation 冷变形 cold drawing 冷拉 cold energy 冷能 cold flow 冷流 cold plasma 冷等离⼦体 cold pressure 冷压 cold rolling 冷轧 cold wave 冷波 cold working 冷加⼯ collapse 崩溃 collapse mechanism 破坏机构 collapsible tube 可折皱管 collapsing force 破坏⼒ collar vortex 涡环 collateral motion 次级运动 collective mode of motion 集体运动模式 collective motion 集体运动 collimation 视准 collision 碰撞 collision chain 碰撞链 collision cross section 碰撞截⾯ collision diameter 碰撞直径 collision diffusion 碰撞扩散 collision excitation 碰撞激发 collision frequency 碰撞频率 collision heating 碰撞加热 collision integral 碰撞积分 collision invariant 碰撞不变量。
2011滑铁卢竞赛试题答案
1.(a)Since (x +1)+(x +2)+(x +3)=8+9+10,then 3x +6=27or 3x =21and so x =7.(b)Since 25+√x =6,then squaring both sides gives 25+√x =36or √x =11.Since √x =11,then squaring both sides again,we obtain x =112=121.Checking, 25+√121=√25+11=√36=6,as required.(c)Since (a,2)is the point of intersection of the lines with equations y =2x −4and y =x +k ,then the coordinates of this point must satisfy both equations.Using the first equation,2=2a −4or 2a =6or a =3.Since the coordinates of the point (3,2)satisfy the equation y =x +k ,then 2=3+k or k =−1.2.(a)Since the side length of the original square is 3and an equilateral triangle of side length 1is removed from the middle of each side,then each of the two remaining pieces of each side of the square has length 1.Also,each of the two sides of each of the equilateral triangles that are shown has length 1.1111Therefore,each of the 16line segments in the figure has length 1,and so the perimeter of the figure is 16.(b)Since DC =DB ,then CDB is isosceles and ∠DBC =∠DCB =15◦.Thus,∠CDB =180◦−∠DBC −∠DCB =150◦.Since the angles around a point add to 360◦,then∠ADC =360◦−∠ADB −∠CDB =360◦−130◦−150◦=80◦.(c)By the Pythagorean Theorem in EAD ,we have EA 2+AD 2=ED 2or 122+AD 2=132,and so AD =√169−144=5,since AD >0.By the Pythagorean Theorem in ACD ,we have AC 2+CD 2=AD 2or AC 2+42=52,and so AC =√25−16=3,since AC >0.(We could also have determined the lengths of AD and AC by recognizing 3-4-5and 5-12-13right-angled triangles.)By the Pythagorean Theorem in ABC ,we have AB 2+BC 2=AC 2or AB 2+22=32,and so AB =√9−4=√5,since AB >0.3.(a)Solution 1Since we want to make 15−y x as large as possible,then we want to subtract as little as possible from 15.In other words,we want to make y x as small as possible.To make a fraction with positive numerator and denominator as small as possible,wemake the numerator as small as possible and the denominator as large as possible.Since 2≤x ≤5and 10≤y ≤20,then we make x =5and y =10.Therefore,the maximum value of 15−y x is 15−105=13.Solution2Since y is positive and2≤x≤5,then15−yx≤15−y5for any x with2≤x≤5andpositive y.Since10≤y≤20,then15−y5≤15−105for any y with10≤y≤20.Therefore,for any x and y in these ranges,15−yx≤15−105=13,and so the maximumpossible value is13(which occurs when x=5and y=10).(b)Solution1First,we add the two given equations to obtain(f(x)+g(x))+(f(x)−g(x))=(3x+5)+(5x+7)or2f(x)=8x+12which gives f(x)=4x+6.Since f(x)+g(x)=3x+5,then g(x)=3x+5−f(x)=3x+5−(4x+6)=−x−1.(We could alsofind g(x)by subtracting the two given equations or by using the second of the given equations.)Since f(x)=4x+6,then f(2)=14.Since g(x)=−x−1,then g(2)=−3.Therefore,2f(2)g(2)=2×14×(−3)=−84.Solution2Since the two given equations are true for all values of x,then we can substitute x=2to obtainf(2)+g(2)=11f(2)−g(2)=17Next,we add these two equations to obtain2f(2)=28or f(2)=14.Since f(2)+g(2)=11,then g(2)=11−f(2)=11−14=−3.(We could alsofind g(2)by subtracting the two equations above or by using the second of these equations.)Therefore,2f(2)g(2)=2×14×(−3)=−84.4.(a)We consider choosing the three numbers all at once.We list the possible sets of three numbers that can be chosen:{1,2,3}{1,2,4}{1,2,5}{1,3,4}{1,3,5}{1,4,5}{2,3,4}{2,3,5}{2,4,5}{3,4,5} We have listed each in increasing order because once the numbers are chosen,we arrange them in increasing order.There are10sets of three numbers that can be chosen.Of these10,the4sequences1,2,3and1,3,5and2,3,4and3,4,5are arithmetic sequences.Therefore,the probability that the resulting sequence is an arithmetic sequence is410or25.(b)Solution 1Join B to D .AConsider CBD .Since CB =CD ,then ∠CBD =∠CDB =12(180◦−∠BCD )=12(180◦−60◦)=60◦.Therefore, BCD is equilateral,and so BD =BC =CD =6.Consider DBA .Note that ∠DBA =90◦−∠CBD =90◦−60◦=30◦.Since BD =BA =6,then ∠BDA =∠BAD =12(180◦−∠DBA )=12(180◦−30◦)=75◦.We calculate the length of AD .Method 1By the Sine Law in DBA ,we have AD sin(∠DBA )=BA sin(∠BDA ).Therefore,AD =6sin(30◦)sin(75◦)=6×12sin(75◦)=3sin(75◦).Method 2If we drop a perpendicular from B to P on AD ,then P is the midpoint of AD since BDA is isosceles.Thus,AD =2AP .Also,BP bisects ∠DBA ,so ∠ABP =15◦.Now,AP =BA sin(∠ABP )=6sin(15◦).Therefore,AD =2AP =12sin(15◦).Method 3By the Cosine Law in DBA ,AD 2=AB 2+BD 2−2(AB )(BD )cos(∠ABD )=62+62−2(6)(6)cos(30◦)=72−72(√32)=72−36√3Therefore,AD = 36(2−√3)=6 2−√3since AD >0.Solution 2Drop perpendiculars from D to Q on BC and from D to R on BA .AThen CQ =CD cos(∠DCQ )=6cos(60◦)=6×12=3.Also,DQ =CD sin(∠DCQ )=6sin(60◦)=6×√32=3√3.Since BC =6,then BQ =BC −CQ =6−3=3.Now quadrilateral BQDR has three right angles,so it must have a fourth right angle and so must be a rectangle.Thus,RD =BQ =3and RB =DQ =3√3.Since AB =6,then AR =AB −RB =6−3√3.Since ARD is right-angled at R ,then using the Pythagorean Theorem and the fact that AD >0,we obtain AD =√RD 2+AR 2= 32+(6−3√3)2= 9+36−36√3+27= 72−36√3which we can rewrite as AD = 36(2−√3)=6 2−√3.5.(a)Let n be the original number and N be the number when the digits are reversed.Sincewe are looking for the largest value of n ,we assume that n >0.Since we want N to be 75%larger than n ,then N should be 175%of n ,or N =74n .Suppose that the tens digit of n is a and the units digit of n is b .Then n =10a +b .Also,the tens digit of N is b and the units digit of N is a ,so N =10b +a .We want 10b +a =74(10a +b )or 4(10b +a )=7(10a +b )or 40b +4a =70a +7b or 33b =66a ,and so b =2a .This tells us that that any two-digit number n =10a +b with b =2a has the required property.Since both a and b are digits then b <10and so a <5,which means that the possible values of n are 12,24,36,and 48.The largest of these numbers is 48.(b)We “complete the rectangle”by drawing a horizontal line through C which meets they -axis at P and the vertical line through B at Q .x A (0,Since C has y -coordinate 5,then P has y -coordinate 5;thus the coordinates of P are (0,5).Since B has x -coordinate 4,then Q has x -coordinate 4.Since C has y -coordinate 5,then Q has y -coordinate 5.Therefore,the coordinates of Q are (4,5),and so rectangle OP QB is 4by 5and so has area 4×5=20.Now rectangle OP QB is made up of four smaller triangles,and so the sum of the areas of these triangles must be 20.Let us examine each of these triangles:• ABC has area 8(given information)• AOB is right-angled at O ,has height AO =3and base OB =4,and so has area 12×4×3=6.• AP C is right-angled at P ,has height AP =5−3=2and base P C =k −0=k ,and so has area 1×k ×2=k .• CQB is right-angled at Q ,has height QB =5−0=5and base CQ =4−k ,andso has area 12×(4−k )×5=10−52k .Since the sum of the areas of these triangles is 20,then 8+6+k +10−52k =20or 4=32k and so k =83.6.(a)Solution 1Suppose that the distance from point A to point B is d km.Suppose also that r c is the speed at which Serge travels while not paddling (i.e.being carried by just the current),that r p is the speed at which Serge travels with no current (i.e.just from his paddling),and r p +c his speed when being moved by both his paddling and the current.It takes Serge 18minutes to travel from A to B while paddling with the current.Thus,r p +c =d 18km/min.It takes Serge 30minutes to travel from A to B with just the current.Thus,r c =d 30km/min.But r p =r p +c −r c =d 18−d 30=5d 90−3d 90=2d 90=d 45km/min.Since Serge can paddle the d km from A to B at a speed of d 45km/min,then it takes him 45minutes to paddle from A to B with no current.Solution 2Suppose that the distance from point A to point B is d km,the speed of the current of the river is r km/h,and the speed that Serge can paddle is s km/h.Since the current can carry Serge from A to B in 30minutes (or 12h),then d r =12.When Serge paddles with the current,his speed equals his paddling speed plus the speed of the current,or (s +r )km/h.Since Serge can paddle with the current from A to B in 18minutes (or 310h),then d r +s =310.The time to paddle from A to B with no current would be d s h.Since d r =12,then r d =2.Since d r +s =310,then r +s d =103.Therefore,s d =r +s d −r d =103−2=43.Thus,d s =34,and so it would take Serge 34of an hour,or 45minutes,to paddle from A to B with no current.Solution 3Suppose that the distance from point A to point B is d km,the speed of the current of the river is r km/h,and the speed that Serge can paddle is s km/h.Since the current can carry Serge from A to B in 30minutes (or 12h),then d r =12or d =1r .When Serge paddles with the current,his speed equals his paddling speed plus the speed of the current,or (s +r )km/h.Since Serge can paddle with the current from A to B in 18minutes (or 310h),then d r +s =310or d =310(r +s ).Since d =12r and d =310(r +s ),then 12r =310(r +s )or 5r =3r +3s and so s =23r .To travel from A to B with no current,the time in hours that it takes is d s =12r 2r =34,or 45minutes.(b)First,we note that a =0.(If a =0,then the “parabola”y =a (x −2)(x −6)is actuallythe horizontal line y =0which intersects the square all along OR .)Second,we note that,regardless of the value of a =0,the parabola has x -intercepts 2and 6,and so intersects the x -axis at (2,0)and (6,0),which we call K (2,0)and L (6,0).This gives KL =4.Third,we note that since the x -intercepts of the parabola are 2and 6,then the axis ofsymmetry of the parabola has equation x =12(2+6)=4.Since the axis of symmetry of the parabola is a vertical line of symmetry,then if theparabola intersects the two vertical sides of the square,it will intersect these at the same height,and if the parabola intersects the top side of the square,it will intersect it at two points that are symmetrical about the vertical line x =4.Fourth,we recall that a trapezoid with parallel sides of lengths a and b and height h hasarea 12h (a +b ).We now examine three cases.Case1:a<0Here,the parabola opens downwards.Since the parabola intersects the square at four points,it must intersect P Q at points M and N.(The parabola cannot intersect the vertical sides of the square since it gets “narrower”towards the vertex.)xx =4Since the parabola opens downwards,then MN<KL=4.Since the height of the trapezoid equals the height of the square(or8),then the area of the trapezoid is1h(KL+MN)which is less than1(8)(4+4)=32.But the area of the trapezoid must be36,so this case is not possible.Case2:a>0;M and N on P QWe have the following configuration:xx =4Here,the height of the trapezoid is8,KL=4,and M and N are symmetric about x=4.Since the area of the trapezoid is36,then12h(KL+MN)=36or12(8)(4+MN)=36or4+MN=9or MN=5.Thus,M and N are each52units from x=4,and so N has coordinates(32,8).Since this point lies on the parabola with equation y=a(x−2)(x−6),then8=a(32−2)(32−6)or8=a(−12)(−92)or8=94a or a=329.Case3:a>0;M and N on QR and P Oxx =4Here,KL=4,MN=8,and M and N have the same y-coordinate.Since the area of the trapezoid is36,then12h(KL+MN)=36or12h(4+8)=36or6h=36or h=6.Thus,N has coordinates(0,6).Since this point lies on the parabola with equation y=a(x−2)(x−6),then 6=a(0−2)(0−6)or6=12a or a=12.Therefore,the possible values of a are329and12.7.(a)Solution1Consider a population of100people,each of whom is75years old and who behave ac-cording to the probabilities given in the question.Each of the original100people has a50%chance of living at least another10years,so there will be50%×100=50of these people alive at age85.Each of the original100people has a20%chance of living at least another15years,so there will be20%×100=20of these people alive at age90.Since there is a25%(or14)chance that an80year old person will live at least another10years(that is,to age90),then there should be4times as many of these people alive at age80than at age90.Since there are20people alive at age90,then there are4×20=80of the original100 people alive at age80.In summary,of the initial100people of age75,there are80alive at age80,50alive at age85,and20people alive at age90.Because50of the80people alive at age80are still alive at age85,then the probability that an80year old person will live at least5more years(that is,to age85)is50=5,or 62.5%.Solution2Suppose that the probability that a75year old person lives to80is p,the probability that an80year old person lives to85is q,and the probability that an85year old person lives to90is r.We want to the determine the value of q.For a75year old person to live at least another10years,they must live another5years (to age80)and then another5years(to age85).The probability of this is equal to pq. We are told in the question that this is equal to50%or0.5.Therefore,pq=0.5.For a75year old person to live at least another15years,they must live another5years (to age80),then another5years(to age85),and then another5years(to age90).The probability of this is equal to pqr.We are told in the question that this is equal to20% or0.2.Therefore,pqr=0.2Similarly,since the probability that an80year old person will live another10years is25%,then qr=0.25.Since pqr=0.2and pq=0.5,then r=pqrpq=0.20.5=0.4.Since qr=0.25and r=0.4,then q=qrr=0.250.4=0.625.Therefore,the probability that an80year old man will live at least another5years is0.625,or62.5%.(b)Using logarithm rules,the given equation is equivalent to22log10x=3(2·2log10x)+16or(2log10x)2=6·2log10x+16.Set u=2log10x.Then the equation becomes u2=6u+16or u2−6u−16=0.Factoring,we obtain(u−8)(u+2)=0and so u=8or u=−2.Since2a>0for any real number a,then u>0and so we can reject the possibility that u=−2.Thus,u=2log10x=8which means that log10x=3.Therefore,x=1000.8.(a)First,we determine thefirst entry in the50th row.Since thefirst column is an arithmetic sequence with common difference3,then the50th entry in thefirst column(thefirst entry in the50th row)is4+49(3)=4+147=151.Second,we determine the common difference in the50th row by determining the second entry in the50th row.Since the second column is an arithmetic sequence with common difference5,then the 50th entry in the second column(that is,the second entry in the50th row)is7+49(5) or7+245=252.Therefore,the common difference in the50th row must be252−151=101.Thus,the40th entry in the50th row(that is,the number in the50th row and the40th column)is151+39(101)=151+3939=4090.(b)We follow the same procedure as in(a).First,we determine thefirst entry in the R th row.Since thefirst column is an arithmetic sequence with common difference3,then the R th entry in thefirst column(that is,thefirst entry in the R th row)is4+(R−1)(3)or 4+3R−3=3R+1.Second,we determine the common difference in the R th row by determining the second entry in the R th row.Since the second column is an arithmetic sequence with common difference5,then the R th entry in the second column(that is,the second entry in the R th row)is7+(R−1)(5) or7+5R−5=5R+2.Therefore,the common difference in the R th row must be(5R+2)−(3R+1)=2R+1.Thus,the C th entry in the R th row(that is,the number in the R th row and the C th column)is3R+1+(C−1)(2R+1)=3R+1+2RC+C−2R−1=2RC+R+C(c)Suppose that N is an entry in the table,say in the R th row and C th column.From(b),then N=2RC+R+C and so2N+1=4RC+2R+2C+1.Now4RC+2R+2C+1=2R(2C+1)+2C+1=(2R+1)(2C+1).Since R and C are integers with R≥1and C≥1,then2R+1and2C+1are each integers that are at least3.Therefore,2N+1=(2R+1)(2C+1)must be composite,since it is the product of two integers that are each greater than1.9.(a)If n=2011,then8n−7=16081and so √8n−7≈126.81.Thus,1+√8n−72≈1+126.812≈63.9.Therefore,g(2011)=2(2011)+1+8(2011)−72=4022+ 63.9 =4022+63=4085.(b)To determine a value of n for which f(n)=100,we need to solve the equation2n−1+√8n−72=100(∗)Wefirst solve the equation2x−1+√8x−72=100(∗∗)because the left sides of(∗)and(∗∗)do not differ by much and so the solutions are likely close together.We will try integers n in(∗)that are close to the solutions to(∗∗). Manipulating(∗∗),we obtain4x−(1+√8x−7)=2004x−201=√8x−7(4x−201)2=8x−716x2−1608x+40401=8x−716x2−1616x+40408=02x2−202x+5051=0By the quadratic formula,x=202±2022−4(2)(5051)2(2)=202±√3964=101±√992and so x≈55.47or x≈45.53.We try n=55,which is close to55.47:f(55)=2(55)−1+8(55)−72=110−1+√4332Since √433≈20.8,then1+√4332≈10.9,which gives1+√4332=10.Thus,f(55)=110−10=100.Therefore,a value of n for which f(n)=100is n=55.(c)We want to show that each positive integer m is in the range of f or the range of g ,butnot both.To do this,we first try to better understand the “complicated”term of each of the func-tions –that is,the term involving the greatest integer function.In particular,we start witha positive integer k ≥1and try to determine the positive integers n that give 1+√8n −72 =k .By definition of the greatest integer function,the equation 1+√8n −72 =k is equiv-alent to the inequality k ≤1+√8n −72<k +1,from which we obtain the following set of equivalent inequalities 2k ≤1+√8n −7<2k +22k −1≤√8n −7<2k +14k 2−4k +1≤8n −7<4k 2+4k +14k 2−4k +8≤8n <4k 2+4k +812(k 2−k )+1≤n <12(k 2+k )+1If we define T k =1k (k +1)=1(k 2+k )to be the k th triangular number for k ≥0,thenT k −1=12(k −1)(k )=12(k 2−k ).Therefore, 1+√8n −72 =k for T k −1+1≤n <T k +1.Since n is an integer,then 1+√8n −72=k is true for T k −1+1≤n ≤T k .When k =1,this interval is T 0+1≤n ≤T 1(or 1≤n ≤1).When k =2,this interval is T 1+1≤n ≤T 2(or 2≤n ≤3).When k =3,this interval is T 2+1≤n ≤T 3(or 4≤n ≤6).As k ranges over all positive integers,these intervals include every positive integer n and do not overlap.Therefore,we can determine the range of each of the functions f and g by examining the values f (n )and g (n )when n is in these intervals.For each non-negative integer k ,define R k to be the set of integers greater than k 2and less than or equal to (k +1)2.Thus,R k ={k 2+1,k 2+2,...,k 2+2k,k 2+2k +1}.For example,R 0={1},R 1={2,3,4},R 2={5,6,7,8,9},and so on.Every positive integer occurs in exactly one of these sets.Also,for each non-negative integer k define S k ={k 2+2,k 2+4,...,k 2+2k }and define Q k ={k 2+1,k 2+3,...,k 2+2k +1}.For example,S 0={},S 1={3},S 2={6,8},Q 0={1},Q 1={2,4},Q 2={5,7,9},and so on.Note that R k =Q k ∪S k so every positive integer occurs in exactly one Q k or in exactly one S k ,and that these sets do not overlap since no two S k ’s overlap and no two Q k ’s overlap and no Q k overlaps with an S k .We determine the range of the function g first.For T k −1+1≤n ≤T k ,we have 1+√8n −72=k and so 2T k −1+2≤2n ≤2T k 2T k −1+2+k ≤2n + 1+√8n −72 ≤2T k +k k 2−k +2+k ≤g (n )≤k 2+k +k k 2+2≤g (n )≤k 2+2kNote that when n is in this interval and increases by 1,then the 2n term causes the value of g (n )to increase by 2.Therefore,for the values of n in this interval,g (n )takes precisely the values k 2+2,k 2+4,k 2+6,...,k 2+2k .In other words,the range of g over this interval of its domain is precisely the set S k .As k ranges over all positive integers (that is,as these intervals cover the domain of g ),this tells us that the range of g is precisely the integers in the sets S 1,S 2,S 3,....(We could also include S 0in this list since it is the empty set.)We note next that f (1)=2− 1+√8−72 =1,the only element of Q 0.For k ≥1and T k +1≤n ≤T k +1,we have 1+√8n −72=k +1and so 2T k +2≤2n ≤2T k +12T k +2−(k +1)≤2n − 1+√8n −72 ≤2T k +1−(k +1)k 2+k +2−k −1≤f (n )≤(k +1)(k +2)−k −1k 2+1≤f (n )≤k 2+2k +1Note that when n is in this interval and increases by 1,then the 2n term causes the value of f (n )to increase by 2.Therefore,for the values of n in this interval,f (n )takes precisely the values k 2+1,k 2+3,k 2+5,...,k 2+2k +1.In other words,the range of f over this interval of its domain is precisely the set Q k .As k ranges over all positive integers (that is,as these intervals cover the domain of f ),this tells us that the range of f is precisely the integers in the sets Q 0,Q 1,Q 2,....Therefore,the range of f is the set of elements in the sets Q 0,Q 1,Q 2,...and the range of g is the set of elements in the sets S 0,S 1,S 2,....These ranges include every positive integer and do not overlap.10.(a)Suppose that ∠KAB =θ.Since ∠KAC =2∠KAB ,then ∠KAC =2θand ∠BAC =∠KAC +∠KAB =3θ.Since 3∠ABC =2∠BAC ,then ∠ABC =23×3θ=2θ.Since ∠AKC is exterior to AKB ,then ∠AKC =∠KAB +∠ABC =3θ.This gives the following configuration:BNow CAK is similar to CBA since the triangles have a common angle at C and ∠CAK =∠CBA .Therefore,AKBA=CACBordc=baand so d=bca.Also,CKCA=CACBora−xb=baand so a−x=b2aor x=a−b2a=a2−b2a,as required.(b)From(a),bc=ad and a2−b2=ax and so we obtainLS=(a2−b2)(a2−b2+ac)=(ax)(ax+ac)=a2x(x+c) andRS=b2c2=(bc)2=(ad)2=a2d2In order to show that LS=RS,we need to show that x(x+c)=d2(since a>0).Method1:Use the Sine LawFirst,we derive a formula for sin3θwhich we will need in this solution:sin3θ=sin(2θ+θ)=sin2θcosθ+cos2θsinθ=2sinθcos2θ+(1−2sin2θ)sinθ=2sinθ(1−sin2θ)+(1−2sin2θ)sinθ=3sinθ−4sin3θSince∠AKB=180◦−∠KAB−∠KBA=180◦−3θ,then using the Sine Law in AKB givesx sinθ=dsin2θ=csin(180◦−3θ)Since sin(180◦−X)=sin X,then sin(180◦−3θ)=sin3θ,and so x=d sinθsin2θandc=d sin3θsin2θ.This givesx(x+c)=d sinθsin2θd sinθsin2θ+d sin3θsin2θ=d2sinθsin22θ(sinθ+sin3θ)=d2sinθsin22θ(sinθ+3sinθ−4sin3θ)=d2sinθsin22θ(4sinθ−4sin3θ)=4d2sin2θsin22θ(1−sin2θ)=4d2sin2θcos2θsin22θ=4d2sin2θcos2θ(2sinθcosθ)2=4d2sin2θcos2θ4sin2θcos2θ=d2as required.We could have instead used the formula sin A +sin B =2sinA +B 2 cos A −B2 toshow that sin 3θ+sin θ=2sin 2θcos θ,from which sin θ(sin 3θ+sin θ)=sin θ(2sin 2θcos θ)=2sin θcos θsin 2θ=sin 22θMethod 2:Extend ABExtend AB to E so that BE =BK =x and join KE .ENow KBE is isosceles with ∠BKE =∠KEB .Since ∠KBA is the exterior angle of KBE ,then ∠KBA =2∠KEB =2θ.Thus,∠KEB =∠BKE =θ.But this also tells us that ∠KAE =∠KEA =θ.Thus, KAE is isosceles and so KE =KA =d.ESo KAE is similar to BKE ,since each has two angles equal to θ.Thus,KA BK =AE KE or d x =c +x dand so d 2=x (x +c ),as required.Method 3:Use the Cosine Law and the Sine LawWe apply the Cosine Law in AKB to obtainAK 2=BK 2+BA 2−2(BA )(BK )cos(∠KBA )d 2=x 2+c 2−2cx cos(2θ)d 2=x 2+c 2−2cx (2cos 2θ−1)Using the Sine Law in AKB ,we get x sin θ=d sin 2θor sin 2θsin θ=d x or 2sin θcos θsin θ=d x and so cos θ=d 2x.Combining these two equations,d2=x2+c2−2cx2d24x2−1d2=x2+c2−cd2x+2cxd2+cd2x=x2+2cx+c2d2+cd2x=(x+c)2xd2+cd2=x(x+c)2d2(x+c)=x(x+c)2d2=x(x+c)as required(since x+c=0).(c)Solution1Our goal is tofind a triple of positive integers that satisfy the equation in(b)and are the side lengths of a triangle.First,we note that if(A,B,C)is a triple of real numbers that satisfies the equation in(b)and k is another real number,then the triple(kA,kB,kC)also satisfies the equationfrom(b),since(k2A2−k2B2)(k2A2−k2B2+kAkC)=k4(A2−B2)(A2−B2+AC)=k4(B2C2)=(kB)2(kC)2 Therefore,we start by trying tofind a triple(a,b,c)of rational numbers that satisfies the equation in(b)and forms a triangle,and then“scale up”this triple to form a triple (ka,kb,kc)of integers.To do this,we rewrite the equation from(b)as a quadratic equation in c and solve for c using the quadratic formula.Partially expanding the left side from(b),we obtain(a2−b2)(a2−b2)+ac(a2−b2)=b2c2which we rearrange to obtainb2c2−c(a(a2−b2))−(a2−b2)2=0By the quadratic formula,c=a(a2−b2)±a2(a2−b2)2+4b2(a2−b2)22b2=a(a2−b2)±(a2−b2)2(a2+4b2)2b2Since∠BAC>∠ABC,then a>b and so a2−b2>0,which givesc=a(a2−b2)±(a2−b2)√a2+4b22b2=(a2−b2)2b2(a±√a2+4b2)Since a2+4b2>0,then √a2+4b2>a,so the positive root isc=(a2−b2)2b2(a+a2+(2b)2)We try to find integers a and b that give a rational value for c .We will then check to see if this triple (a,b,c )forms the side lengths of a triangle,and then eventually scale these up to get integer values.One way for the value of c to be rational (and in fact the only way)is for a 2+(2b )2to be an integer,or for a and 2b to be the legs of a Pythagorean triple.Since √32+42is an integer,then we try a =3and b =2,which givesc =(32−22)2·22(3+√32+42)=5and so (a,b,c )=(3,2,5).Unfortunately,these lengths do not form a triangle,since 3+2=5.(The Triangle Inequality tells us that three positive real numbers a ,b and c form a triangle if and only if a +b >c and a +c >b and b +c >a .)We can continue to try small Pythagorean triples.Now 152+82=172,but a =15and b =4do not give a value of c that forms a triangle with a and b .However,162+302=342,so we can try a =16and b =15which givesc =(162−152)2·152(16+√162+302)=31450(16+34)=319Now the lengths (a,b,c )=(16,15,319)do form the sides of a triangle since a +b >c and a +c >b and b +c >a .Since these values satisfy the equation from (b),then we can scale them up by a factor of k =9to obtain the triple (144,135,31)which satisfies the equation from (b)and are the side lengths of a triangle.(Using other Pythagorean triples,we could obtain other triples of integers that work.)Solution 2We note that the equation in (b)involves only a ,b and c and so appears to depend only on the relationship between the angles ∠CAB and ∠CBA in ABC .Using this premise,we use ABC ,remove the line segment AK and draw the altitude CF .CBA 3θ2θb aa c os 2θbc os 3θF Because we are only looking for one triple that works,we can make a number of assump-tions that may or may not be true in general for such a triangle,but which will help us find an example.We assume that 3θand 2θare both acute angles;that is,we assume that θ<30◦.In ABC ,we have AF =b cos 3θ,BF =a cos 2θ,and CF =b sin 3θ=a sin 2θ.Note also that c =b cos 3θ+a cos 2θ.One way to find the integers a,b,c that we require is to look for integers a and b and an angle θwith the properties that b cos 3θand a cos 2θare integers and b sin 3θ=a sin 2θ.Using trigonometric formulae,sin 2θ=2sin θcos θcos 2θ=2cos 2θ−1sin 3θ=3sin θ−4sin 3θ(from the calculation in (a),Solution 1,Method 1)cos 3θ=cos(2θ+θ)=cos 2θcos θ−sin 2θsin θ=(2cos 2θ−1)cos θ−2sin 2θcos θ=(2cos 2θ−1)cos θ−2(1−cos 2θ)cos θ=4cos 3θ−3cos θSo we can try to find an angle θ<30◦with cos θa rational number and then integers a and b that make b sin 3θ=a sin 2θand ensure that b cos 3θand a cos 2θare integers.Since we are assuming that θ<30◦,then cos θ>√32≈0.866.The rational number with smallest denominator that is larger than √32is 78,so we try the acute angle θwith cos θ=7.In this case,sin θ=√1−cos 2θ=√158,and sosin 2θ=2sin θcos θ=2×78×√158=7√1532cos 2θ=2cos 2θ−1=2×4964−1=1732sin 3θ=3sin θ−4sin 3θ=3×√158−4×15√15512=33√15128cos 3θ=4cos 3θ−3cos θ=4×343512−3×78=7128To have b sin 3θ=a sin 2θ,we need 33√15128b =7√1532a or 33b =28a .To ensure that b cos 3θand a cos 2θare integers,we need 7128b and 1732a to be integers,andso a must be divisible by 32and b must be divisible by 128.The integers a =33and b =28satisfy the equation 33b =28a .Multiplying each by 32gives a =1056and b =896which satisfy the equation 33b =28a and now have the property that b is divisible by 128(with quotient 7)and a is divisible by 32(with quotient 33).With these values of a and b ,we obtain c =b cos 3θ+a cos 2θ=896×7128+1056×1732=610.We can then check that the triple (a,b,c )=(1056,896,610)satisfies the equation from(b),as required.As in our discussion in Solution 1,each element of this triple can be divided by 2to obtain the “smaller”triple (a,b,c )=(528,448,305)that satisfies the equation too.Using other values for cos θand integers a and b ,we could obtain other triples (a,b,c )of integers that work.。
极限思想外文翻译pdf
极限思想外文翻译pdfBSHM Bulletin, 2014Did Weierstrass’s differential calculus have a limit-avoiding character? His,,,definition of a limit in styleMICHIYO NAKANENihon University Research Institute of Science & Technology, Japan In the 1820s, Cauchy founded his calculus on his original limit concept and,,,developed his the-ory by using inequalities, but he did not apply theseinequalities consistently to all parts of his theory. In contrast, Weierstrass consistently developed his 1861 lectures on differential calculus in terms of epsilonics. His lectures were not based on Cauchy’s limit and are distin-guished bytheir limit-avoiding character. Dugac’s partial publication of the 1861 lecturesmakes these differences clear. But in the unpublished portions of the lectures,,,,Weierstrass actu-ally defined his limit in terms ofinequalities. Weierstrass’slimit was a prototype of the modern limit but did not serve as a foundation of his calculus theory. For this reason, he did not providethe basic structure for the modern e d style analysis. Thus it was Dini’s 1878 text-book that introduced the,,,definition of a limit in terms of inequalities.IntroductionAugustin Louis Cauchy and Karl Weierstrass were two of the most important mathematicians associated with the formalization of analysis on the basis of the e d doctrine. In the 1820s, Cauchy was the first to give comprehensive statements of mathematical analysis that were based from the outset on a reasonably clear definition of the limit concept (Edwards 1979, 310). He introduced various definitions and theories that involved his limit concept. His expressions were mainly verbal, but they could be understood in terms of inequalities: given an e, find n or d (Grabiner 1981, 7). As we show later, Cauchy actually paraphrased his limit concept in terms of e, d, and n0 inequalities, in his more complicated proofs. But it was Weierstrass’s 1861 lectures which used the technique in all proofs and also in his defi-nition (Lutzen? 2003, 185–186).Weierstrass’s adoption of full epsilonic arguments, however, didnot mean that he attained a prototype of the modern theory. Modern analysis theory is founded on limits defined in terms of e d inequalities. His lectures were not founded on Cauchy’s limit or his own original definition of limit (Dugac 1973). Therefore, in order to clarify the formation of the modern theory, it will be necessary toidentify where the e d definition of limit was introduced and used as a foundation.We do not find the word ‘limit’ in the pu blished part of the 1861 lectures.Accord-ingly, Grattan-Guinness (1986, 228) characterizesWeierstrass’s analysis aslimit-avoid-ing. However, Weierstrass actually defined his limit in terms of epsilonics in the unpublished portion of his lectures. Histheory involved his limit concept, although the concept did not function as the foundation of his theory. Based on this discovery, this paper re-examines the formation of e d calculus theory, noting mathematicians’ treat-ments of their limits. We restrict ourattention to the process of defining continuity and derivatives. Nonetheless, this focus provides sufficient information for our purposes.First, we confirm that epsilonics arguments cannot representCauchy’s limit,though they can describe relationships that involved his limit concept. Next, we examine how Weierstrass constructed a novel analysis theory which was not based2013 British Society for the History of Mathematics52 BSHM Bulletinon Cauchy’s limits but could have involved Cauchy’s resu lts. Thenwe confirmWeierstrass’s definition of limit. Finally, we note that Dini organized his analysis textbook in 1878 based on analysis performed inthe e d style.Cauchy’s limit and epsilonic argumentsCauchy’s series of textbooks on calculus, Cours d’analyse (1821), Resume deslecons? donnees a l’Ecole royale polytechnique sur le calcul infinitesimal tomepremier (1823), and Lecons? sur le calcul differentiel (1829), are often considered as the main referen-ces for modern analysis theory, the rigour of which is rooted more in the nineteenth than the twentieth century.At the beginning of his Cours d’analyse, Cauchy defined the limit concept as fol-lows: ‘When the successively attributed values of the same variable indefinitely approach a fixed value, so that finally they differ from it by as little as desired, the last is called the limit of all theothers’ (1821, 19; English translation fromGrabiner 1981, 80). Starting from this concept, Cauchy developed a theory of continuous func-tions, infinite series, derivatives, and integrals, constructing an analysis based on lim-its (Grabiner 1981, 77).When discussing the evolution of the limit concept, Grabiner writes:‘This con-cept, translated into the algebra of inequalities, was exactly what Ca uchy needed for his calculus’ (1981, 80). From the present-day point of view, Cauchy described rather than defined his kinetic concept of limits. According to his ‘definition’—which has the quality of a translation or description—he could develop any aspectof the theory by reducing it to the algebra of inequalities.Next, Cauchy introduced infinitely small quantities into his theory. ‘When the suc-cessive absolute values of a variable decrease indefinitely, in such a way as to become less than any given quantity, that variable becomes what is called an infinitesimal. Such a variable has zero for its limit’ (1821, 19; English translationfrom Birkhoff and Merzbach 1973, 2). That is to say, in Cauchy’s framework ‘thelimit of variable x is c’ is intuitively understood as ‘x indefinitely approaches c’,and is represented as ‘jx cj is as little as desired’ or ‘jx cj is infinitesimal’.Cauchy’s idea of defining infinitesimals as variables of a special kind was original, because Leibniz and Euler, for example, had treated them as constants (Boyer 1989, 575; Lutzen? 2003, 164).In Cours d’analyse Cauchy at first gave a verbal definition of a continuous func-tion. Then, he rewrote it in terms of infinitesimals:[In other words,] the function f ðxÞ will rema in continuous relative to x in a given interval if (in this interval) an infinitesimalincrement in the variable always pro-duces an infinitesimal increment in the function itself. (1821, 43; English transla-tion from Birkhoff and Merzbach 1973, 2).He introduced the infinitesimal-involving definition and adopted a modified version of it in Resume (1823, 19–20) and Lecons? (1829, 278).Following Cauchy’s definition of infinitesimals, a continuous function can be defined as a function f ðxÞ in which ‘the variable f ðx þ aÞ f ðxÞ is an infinitelysmall quantity (as previously defined) whenever the variable a is, that is, that f ðx þ aÞ f ðxÞ approaches to zero as a does’, as notedby Edwards (1979, 311). Thus,the definition can be translated into the language of e dinequalities from a modern viewpoint. Cauchy’s infinitesimals are variables, and we can also takesuch an interpretation.Volume 29 (2014) 53Cauchy himself translated his limit concept in terms of e d inequalities. He changed ‘If the difference f ðx þ 1Þ f ðxÞ converges towards a certain limit k, for increasing values of x, (. . .)’ to‘First suppose that the quantity k has a finitevalue, and denote by e a number as small as we wish. . . . we cangive the number h a value large enough that, when x is equal to orgreater than h, the difference in question is always contained between the limits k e; k þ e’ (1821, 54; Englishtranslation from Bradley and Sandifer 2009, 35).In Resume , Cauchy gave a definition of a derivative: ‘if f ðxÞ is continuous, thenits derivative is the limit of the difference quotient,,yf(x,i),f(x), ,xias i tends to 0’ (1823, 22–23). He also translated the concept of derivative asfollows: ‘Designate by d and e two very small numbers; the first being chosen in such a way that, for numerical values of i less than d, [. . .], the ratio f ðx þ iÞ fðxÞ=i always remains greater than f ’ðx Þ e and less than f ’ðxÞ þ e’ (1823,44–45; English transla-tion from Grabiner 1981, 115).These examples show that Cauchy noted that relationships involving limits or infinitesimals could be rewritten in term of inequalities. Cauchy’s argumentsabout infinite series in Cours d’analyse, which dealt with the relationship betweenincreasing numbers and infinitesimals, had such a character. Laugwitz (1987, 264; 1999, 58) and Lutzen? (2003, 167) have noted Cauchy’s strict use of the e Ncharacterization of convergence in several of his proofs. Borovick and Katz (2012) indicate that there is room to question whether or not our representation using e d inequalities conveys messages different from Cauchy’s original intention. Butthis paper accepts the inter-pretations of Edwards, Laugwitz, and Lutzen?.Cauchy’s lectures mainly discussed properties of series and functions in the limit process, which were represented as relationships between his limits or his infinitesi-mals, or between increasing numbers and infinitesimals. His contemporaries presum-ably recognized the possibility of developing analysis theory in terms of only e, d, and n0 inequalities. With a few notable exceptions, all of Cauchy’s lectures could be rewrit-ten in terms of e d inequalities. Cauchy’s limits and hisinfinitesimals were not func-tional relationships,1 so they were not representable in terms of e d inequalities.Cauchy’s limit concept was the foundation of his theory. Thus, Weierstrass’s fullepsilonic analysis theory has a different foundation from that of Cauchy.Weierstrass’s 1861 lecturesWeierstrass’s consistent use of e d argumentsWeierstrass delivered his lectures ‘On the differential calculus’ at the GewerbeInsti-tut Berlin2 in the summer semester of 1861. Notes of these lectures were taken by1Edwards (1979, 310), Laugwitz (1987, 260–261, 271–272), andFisher (1978, 16–318) point out tha t Cauchy’s infinitesimals equate to a dependent variablefunction or aðhÞ that approaches zero as h ! 0. Cauchy adopted the latter infinitesimals, which can be written in terms of e d arguments, when he intro-duced a concept of degree of infinitesimals (1823, 250; 1829, 325). Every infinitesimal of Cauchy’s is a vari-able in the parts that the present paperdiscusses.2A forerunner of the Technische Universit?at Berlin.54 BSHM BulletinHerman Amandus Schwarz, and some of them have been published in the original German by Dugac (1973). Noting the new aspects related to foundational concepts in analysis, full e d definitions of limit and continuous function, a new definition of derivative, and a modern definition of infinitesimals, Dugac considered that the nov-elty of Weierstrass’s lectures was incontestable (1978, 372, 1976, 6–7).3 After beginning his lectures by defining a variable magnitude, Weierstrass gave the definition of a function using the notion of correspondence. This brought him to the following important definition, which did not directly appear in Cauchy’s theory:(D1) If it is now possible to determine for h a bound d such thatfor all values of h which in their absolute value are smaller than d, f ðx þ hÞ f ðxÞ becomes smaller than any magnitude e, however small, then one says that infinitely small changes of the argument correspond to infinitely small changes of the function. (Dugac 1973, 119; English translation from Calinger 1995, 607)That is, Weierstrass defined not infinitely small changes of variables but ‘infinitelysmall changes of the arguments correspond(ing) to infinitely small changes of function’ that were presented in terms of e d inequalities. He founded his theory on this correspondence.Using this concept, he defined a continuous function as follows: (D2) If now a function is such that to infinitely small changes of the argument there correspond infinitely small changes of the function, one then says that it is a continuous function of the argument, or that it changes continuously with this argument. (Dugac 1973, 119–120; English translation from Calinger 1995, 607)So we see that in accordance with his definition of correspondence, Weierstrass actually defined a continuous function on an interval in terms of epsiloni cs. Since (D2) is derived by merely changing Cauchy’s term ‘produce’ to, it seems that Weierstrass took the idea of this definition from‘correspond’Cauchy. However, Weierstrass’s definition was given in terms of epsilonics, whileCauchy’s definition c an only be interpreted in these terms. Furthermore, Weierstrass achieved it without Cauchy’s limit.Luzten? (2003, 186) indicates that Weierstrass still used the concept of ‘infinitelysmall’ in his lectures. Until giving his definition of derivative, Weierstrass actuallya function continued to use the term ‘infinitesimally small’ and often wrote of ‘which becomes infinitely small with h’. But several instances of‘infinitesimallysmall’ appeared in forms of the relationships involving them. Definition (D1) gives the rela-tionship in terms of e d inequalities. We may therefore assume that Weierstrass’s lectures consistently used e d inequalities, even though his definitions were not directly written in terms of these inequalities.Weierstrass inserted sentences confirming that the relationships involving the term ‘infinitely small’ were defined in terms of e d inequalities as follows:ðhÞ is an (D3) If h denotes a magnitude which can assume infinitely small values, ’arbitrary function of h with the property that for an infinitely small value of h it3The present paper also quotes Kurt Bing’s translation included in Calinger’sClassics of mathematics.Volume 29 (2014) 55also becomes infinitely small (that is, that always, as soon as a definite arbitrary small magnitude e is chosen, a magnitude d can be determined such that for all values of h whose absolute value is smaller than d, ’ðhÞ becomes smaller than e).(Dugac 1973, 120; English translation from Calinger, 1995, 607)As Dugac (1973, 65) in dicates, some modern textbooks describe ’ðhÞ as infinitelysmall or infinitesimal.Weierstrass argued that the whole change of function can in general be decom-posed asDf ðxÞ ? f ðx þ hÞ f ðxÞ ? p:h þ hðhÞ; ð 1Þwhere the factor p is independent of h and ðh Þ is a magnitude that becomes infinitely small with h.4 However, he overlooked that such decomposition is not possible for all functions and inserted the term‘in general’. He rewrote h as dx.One can make the difference between Df ðxÞ and p:dx s maller than any magnitude with decreasing dx. Hence Weierstrass defined ‘differential’ as the changewhich a function undergoes when its argument changes by an infinitesimally small magnitude and denoted it as df ðxÞ. Then, df ðxÞ ? p:dx. Weierstrass pointed outthat the differential coefficient p is a function of x derived from f ðxÞ and called it a derivative (Dugac 1973, 120–121; English translation from Calinger 1995, 607–608). In accordance with Weierstrass’s definitions (D1) and (D3),he largelydefined a derivative in terms of epsilonics.Weierstrass did not adopt the term ‘infinitely small’ but directly used e dinequalities when he discussed properties of infinite seriesinvolving uniform conver-gence (Dugac 1973, 122–124). It may beinferred from the publishedportion of his notes that Cauchy’s limit has no place in Weierstrass’s lectures.Grattan-Guinness’s (1986, 228) description of the limit-avoiding character of his analysis represents this situation well.However, Weierstrass thought that his theory included most of the content of Cauchy’s theory. Cauchy first gave the definition of limits of variables andinfinitesi-mals. Then, he demonstrated notions and theorems that were written in terms of the relationships involving infinitesimals. From Weierstrass’s viewpoint,they were writ-ten in terms of e d inequalities. Analytical theory mainly examines properties of functions and series, which were described in the relationships involving Cauchy’s limits and infinitesimals. Weierstrass recognized this fact and had the idea of consis-tently developing his theory in terms of inequalities. Hence Weierstrass atfirst defined the relationships among infinitesimals in terms of e d inequalities. In accor-dance with this definition, Weierstrass rewrote Cauchy’sresults and naturally imported them into his own theory. This is a process that may be described as fol-lows: ‘Weierstrass completed the transformation away fromthe use of terms such as “infinitely small”’ (Katz 1998, 728).Weierstrass’s definition of limitDugac (1978, 370–372; 1976, 6–7) read (D1) as the first definition of limit withthe help of e d. But (D1) does not involve an endpoint thatvariables or functions4Dugac (1973, 65) indicated that ðhÞ corresponds to the modernnotion of oð1Þ. In addition, hðhÞ corre-sponds to the function that was introduced as ’ðhÞ in theformer quotation from Weierstrass’s sentences.。
Axial crushing behaviors of multi-cell tubes with triangular lattices
Axial crushing behaviors of multi-cell tubes with triangular lattices Wu Hong a,b,Hualin Fan a,c,*,Zhicheng Xia b,Fengnian Jin b,Qing Zhou d,**,Daining Fang e,**a Laboratory of Structural Analysis for Defense Engineering and Equipment,College of Mechanics and Materials,Hohai University,Nanjing210098,Chinab State Key Laboratory for Disaster Prevention&Mitigation of Explosion&Impact,PLA University of Science&Technology,Nanjing210007,Chinac State Key Laboratory of Structural Analysis for Industrial Equipment,Dalian University of Technology,Dalian116023,Chinad State Key Laboratory of Automotive Safety and Energy,Tsinghua University,Beijing100084,Chinae Institute of Engineering,Peking University,Beijing100084,Chinaa r t i c l e i n f oArticle history:Received9April2013 Received in revised form2August2013Accepted11August2013 Available online22August2013Keywords:Multi-cell lattice tubePlastic deformation modeMean crushing forceEnergy absorption a b s t r a c tTo enhance the energy absorbing ability of thin-walled structures,multi-cell tubes with triangular and Kagome lattices were designed and manufactured.Quasi-static axial compression experiments were carried out to reveal the progressive collapse mode and folding mechanism of thin-walled multi-cell bining with the experiments,deformation styles were revealed and classical plastic models were suggested to predict the mean crushing forces of multi-cell pared with anti-crushing behaviors of single-cell tubes,multi-cell lattice tubes have comparable peak loads while much greater mean crushing forces,which indicates that multi-cell lattice tubes are more weight efficient in energy absorption.Ó2013Elsevier Ltd.All rights reserved.1.IntroductionThin-walled tubes have been widely used as energy absorbers. Material property,configuration of the cross-section,wall thick-ness,boundary condition,and other factors of the thin-walled tube could affect the energy absorption.Among these factors,the configuration of the cross-section is one of the most important. Thin-walled tubes with various cross-sections,including square tubes,circular tubes,and other single-cell tubes have been dis-cussed theoretically,experimentally and numerically.Axial crushing of circular tube wasfirstly analyzed by Alexander [1]and found to be an excellent mechanism for energy absorption. Experimental researches and theoretical predictions on axial crushing of circular and square tubes were published by Abramo-wicz and Jones[2,3],Abramowicz and Wierzbicki[4],Andrews et al.[5],Wierzbicki and Abramowicz[6]and others.Hong et al.[7] revealed the energy absorption of triangular tubes,whose collapse modes are quite different.To improve the energy absorbing ability, multi-cell tubes were proposed.Chen and Wierzbicki[8]studied the axial crushing of hollow multi-cell columns.Kim[9]suggested new extruded multi-cell profile based on the idea of adding a square element to the corner part of a cross-section for more crash energy absorption.The analytical solution for calculating the mean crushing force of multi-cell profiles with four square elements at the corner was derived.Specific energy absorption of the multi-cell structure is1.9times greater than conventional square tube.It has been found that severe plastic deformation would develop near the tube corner.Most of the energy would be dissipated by the membrane deformation and the bending deformation along the bending hinge lines,especially at the corner.Therefore,topology and node number of the cross-section would decide the energy absorbing efficiency.Zhang et al.[10]and Zhang and Cheng[11] studied the axial crushing of multi-cell square columns.Based on the super folding element theory,a theoretical solution for the mean crushing force of multi-cell tubes was derived by dividing the profile into3parts:corner,crisscross,and T-shape.It was found that the crisscross part was the most efficient component for en-ergy absorption and the energy absorption efficiency of a single-cell column can be increased by50%when the section was divided into 3Â3cells.Zhang et al.[10]adopted the approach of Chen and Wierzbicki[8]to get a reduced model to predict the mean crushing*Corresponding boratory of Structural Analysis for Defense Engineer-ing and Equipment,College of Mechanics and Materials,Hohai University,Nanjing 210098,China.**Corresponding authors.E-mail addresses:fhl02@(H.Fan),zhouq@ (Q.Zhou),fangdn@(D.Fang).Contents lists available at ScienceDirectInternational Journal of Impact Engineering jo urn al homepag e:/locate/ijimpeng 0734-743X/$e see front matterÓ2013Elsevier Ltd.All rights reserved.International Journal of Impact Engineering63(2014)106e117force,neglecting the energy absorbing mechanism of the toroidal surface.They underestimated the mean crushing force[8].Zhang and Zhang[12,13]improved the model through adding the energy dissipated by rolling hinges.Krolak et al.[14]studied the stability of multi-cell column of triangular cross-section.The multi-cell column buckles at a stress of seven times greater.Hou et al.[15]numerically designed the cross-section of multi-cell columns to maximize the energy ab-sorption and minimize the peak force.Najafiand Rais-Rohani[16] adopted quasi-static nonlinearfinite element method to study the energy absorption of aluminum multi-cell tubes.Tang et al.[17] designed multi-cell cylindrical columns to improve energy absorbing performances.Most of above researches were focused on the theoretical analysis and numerical simulation.Few experiments have been Kagome lattices,as shown in Fig.1,were designed,manufactured, tested and analyzed.2.ManufacturesConfiguration of the tested specimen is shown in Fig.1, including Kagome lattice tube and triangular lattice tube.All specimens were fabricated by mild steel Q235with a yield strength, s s,of230MPa.To keep the integrity,all lattice tubes were wire cut out from solid steel rods.The triangular lattice tube has nine triangular lattices,as shown in Fig.1a.The Kagome lattice tube has one hexagonal lattice and six triangular lattices,as shown in Fig.1b. All specimens have identical wall thickness,t,of1.5mm and tube length,L,of100mm,while the breadth of the tube,B,varies from 90mm,120mm to150mm.The corresponding breadth,c,of the triangular cell varies from30mm,40mm to50mm.Geometrical dimensions of tested tubes were listed in Table1.Tubes KT1,TT1 and ST1,with breadth of90mm,have identical masses.Triangular lattice tubes have identical cross-sectional areas to the corre-sponding single-cell tube of the same breadth.Tubes KT2,TT2and ST2,with breadth of120mm,have identical masses.Tubes KT3,TT3 and ST3,with breadth of150mm,are of the same weight.3.Experiments3.1.MethodQuasi-static axial compression experiments were carried out on a600kN universal testing machine at a loading rate of2.5mm/min. The lower end of the specimen wasfixed on the test machine,while the upper end was constrained by a spherical hinge,as shown in Fig.1c.To reveal the priority of the lattice tube,single-cell trian-gular tubes of the same weight were also tested.3.2.Kagome lattice tubesProgressive collapse modes and corresponding deformationFig.1.Multi-cell tube with(a)triangular,(b)Kagome lattices and(c)the testing setup.Table1Dimensions and experimental data.Tube b(mm)t(mm)Experimental dataP m(kN)P y(kN)P max(kN)EnergyabsorptionstabilityL e(mm)lKT1-190 1.5123.42147.3175.31 1.4271.750.72 KT1-2131.42139.8184.47 1.4071.250.71 KT1-3133.25139.3195.48 1.4671.460.71 KT2-1120 1.5131.29188.5206.42 1.5772.420.72 KT2-2131.96202.5204.24 1.5471.240.71 KT2-3128.27192.5205.92 1.6072.050.72 KT3-1150 1.5140.72238.5241.51 1.7173.590.74 KT3-2138.37255.8246.6 1.8573.510.74 KT3-3132.75217.08217.08 1.7173.220.73 TT1-190 1.5133.55141.4188.45 1.4164.190.64 TT1-2137.39164.0182.04 1.3264.460.64 TT1-3142.26146.3199.46 1.4065.580.66 TT2-1120 1.5140.11206.4207.25 1.4767.160.67 TT2-2152.0205.7215.33 1.4166.570.67 TT3-1150 1.5145.36241.79241.79 1.6769.470.69 TT3-2145.67241.70241.70 1.6669.310.69 TT3-3145.74259.62259.62 1.7869.570.70 ST-190 3.070.01163.9163.9 2.3473.000.73 ST-2120 3.078.52226.2226.2 2.8873.000.73 ST-3150 3.085.93297.7297.7 3.4673.000.73W.Hong et al./International Journal of Impact Engineering63(2014)106e117107KT1tubes have the smallest ratio,20,of cell breadth to wall thickness.Progressive crushing modes and displacement curves of KT1tubes are shown in Fig.2.After the elastic deformation,the tube yielded.The yield forces are 147.3kN,139.8kN and 139.31kN,respectively,as listed in Table 1,which could be predictedaccurately by the area of cross-section,794.412mm 2.Strain hard-ening made the load continuously increase to the peak.The peak loads are 175.31kN,184.47kN and 195.48kN,respectively.After the peak load,plastic buckling let the load drop to 100kN,approximately,companying with the development of the firstfold.Fig.2.(a)Progressive crushing modes and (b)displacement curves of KT1samples.W.Hong et al./International Journal of Impact Engineering 63(2014)106e 117108After that,two folds developed successively,but the load was stable at the level of about 130kN.Three lobes formed in compression.The ratio of effective crushing displacement to tube length is 0.73,which is close to the ratio of the single-cell tube [7].Stress level of the deformation plateau keeps constant,with few fluctuations.The mean crushing forces of KT1tubes are 123.42kN,131.42kN and 133.25kN,respectively,rather close to the yield strength of the ually,the energy absorption stability factor (EASF),x ,de fined by the ratio of the peak force,P max ,to the mean crushing force,P m ,asFig.4.(a)Progressive crushing modes and (b)displacement curves of KT3samples.W.Hong et al./International Journal of Impact Engineering 63(2014)106e 117109x ¼P max m(1)is another important parameter to evaluate the performance of thin-walled structures.Perfect energy absorption material has a x of 1.0.The EASFs are 1.42,1.40and 1.46for KT1tubes,respectively,much smaller than single-cell triangular tube [7].For KT2specimens,the cell breadth increases to 40mm and the yield strengths are 188.5kN,202.5kN and 192.5kN,respectively,as listed in Table 1,whereas the peak loads are 206.42kN,204.24kN and 205.92kN,respectively.Peak loads of KT2specimens are rather greater,contributing to greater area of the cross-section.However,the mean crushing forces of KT2specimens are 131.29kN,131.96kNFig.6.(a)Progressive crushing modes and (b)displacement curves of TT2samples.W.Hong et al./International Journal of Impact Engineering 63(2014)106e 117110and128.27kN,respectively,comparable to those of KT1specimens. For multi-cell tubes,nodes have great contribution to the energy absorption.Increasing the breadth could not enhance the mean crushing force effectively.Furthermore,there are only two folds and the wavelength is longer,as shown in Fig.3.The EASFs of KT2 tubes are1.57,1.54and1.60,respectively,not as good as those of KT1specimens.Different from KT1and KT2specimens,two displacement curves of KT3specimens in Fig.4have only one initial peak force. The peak loads are241.51kN,246.6kN and217.08kN,respectively. However,the mean crushing forces of KT3specimens vary from 140.72kN,138.37kN to132.75kN,respectively.The EASFs of KT3 tubes are1.71,1.85and1.71,respectively,not as good as those of KT1and KT2specimens.The average yield forces of KT1,KT2and KT3tubes are142.1kN, 194.5kN and237.1kN,respectively,with a ratio of1:1.37:1.67, rather close to3:4:5,ratio of the area of the three tubes.The average mean crushing forces of KT1,KT2and KT3tubes are 129.4kN,130.5kN and137.3kN,respectively.The three tubes have comparable mean crushing forces.To the tested samples,increasing the breadth would have faint influence to increase the mean crushing force of Kagome lattice tubes.3.3.Triangular lattice tubesThe progressive collapse mode and the corresponding displacement curve of triangular lattice tubes were displayed in Figs.5e7.TT1specimens have the smallest cell breadth of30mm.After the elastic deformation,the tubes yielded and then were strain-hardened.Similar to the Kagome lattice tube,there are two extremum loads for TT1specimens.Thefirst peak loads for TT1are 141.4kN,164.0kN and146.3kN,respectively,denoting the yield strength.Strain hardening made the loads continuously develop to 188.45kN,182.04kN and199.46kN,respectively,before the occurrence of the plastic buckling,which then led a strain soft-ening.Three folds developed as shown in Fig.5.It is interesting to find axial stacking faults for adjacent lobes.Staggering along the horizontal direction,when one lobe moves inwardly the adjacent usually moves outwardly.In the formation of thefirst fold,plastic folding mechanism made the load drop from200kN to125kN, approximately.After that,deformation curves are stable with little fluctuations.The deformation plateau has a stress level of the yield strength of the steel material.Mean crushing forces vary from 133.55kN,137.39kN to142.26kN.Similar to KTI lattice tubes, deformation of TT1tubes is much more close to the deformation mechanism of the steel material,not that of a thin-walled structure. The EASFs of TT1tubes are1.41,1.32and1.40,respectively.TT1tubes have comparable peak loads with KT1tubes,while the mean crushing forces are a little greater,as listed in Table1.The most notable difference between TT1with KT1specimens is the effective crushing distance.The effective crushing distance for TT1 is0.645,smaller than0.73,which of the single-cell tube and the Kagome lattice tube.The triangular lattice tubes have higher rela-tive density,which increases the mean crushing force and reduces the effective crushing distance at the same time.For TT2specimens,the cell breadth increases to40mm and the yield strengths are206.4kN and205.7kN,respectively,as listed in Table1.With greater areas,the yield strengths of TT2tubes are much greater than those of TT1tubes.After initial yield,strain hardening of TT2tubes was not well developed.Peak loads are just 207.25kN and215.33kN,respectively,as shown in Fig.6.In the formation of thefirst fold,the load would drop from210kN to 130kN,approximately.Two folds formed in the experiments.The forces of TT2specimens are140.11kN and152.00kN,respectively, comparable with those of TT1tubes and a little greater than those of KT2specimens.The EASFs of TT2tubes are 1.47and 1.41, respectively.Compared with TT1and TT2tubes,TT3tubes have only one extremum force without any strain hardening,as shown in Fig.7. The maximum forces are241.79kN,241.70kN and259.62kN, respectively,comparable to the yield strength of the steel material. One curve dropped at the lower bound of the yield strength,while Fig.8.Displacement curves of triangular tubes with breadth of(a)90mm,(b)120mmW.Hong et al./International Journal of Impact Engineering63(2014)106e117111the other curve directly dropped at the critical value of the yield strength.Strain softening maybe induced by a critical state between the elastic buckling and the plastic buckling.Mean crushing forces of TT3specimens are145.36kN,145.67kN and 145.74kN,respec-tively,comparable with those of TT1and TT2tubes and a little greater than those of KT3specimens.The EASFs of TT3tubes are 1.67,1.66and 1.78,respectively.The average yield forces of TT1,TT2and TT3tubes are 150.6kN,206.1kN and 247.7kN,respectively.The ratio of the yield forces of the three tubes is 1:1.37:1.64,rather close to 3:4:5,ratio of the area of the three tubes.The average mean crushing forces of TT1,TT2and TT3tubes are 137.7kN,146.1kN and 145.6kN,respectively.Although the ratio of the cross-section area of the three tubes is 3:4:5,the three tubes have comparable mean crushing forces.Besides the traditional folding mechanism,lattice tubes must have new important energy absorbing mechanism,which has been revealed by the tests of Kagome lattice tubes.Compared with Kagome lattice tubes,triangular lattice tubes could enhance the mean crushing force to some extent,while little in fluence to the peak force.3.4.Single-cell triangular tubesSingle-cell tubes were also tested.The height is 100mm.The wall thickness is 3.0mm.To keep identical mass with the multi-cell tube,breadths of ST1,ST2and ST3tubes are 90mm,120mm and 150mm,respectively,as listed in Table 1.According to Fig.8,strain hardening was not fully developed.After the peak load,load drop is dramatically larger,as shown in Fig.8.Peak loads are 163.9kN,226.2kN and 297.7kN,respectively,even a little greater than those of the multi-cell tubes.On the contrary,the mean crushing forces are 70.01kN,78.52kN and 85.93kN,respectively,much smaller than multi-cell tubes.The EASFs of ST tubes are 2.34,2.88and 3.46,respectively.ST tube has unfavorable weight ef ficiency in energy absorption compared with the multi-cell lattice tube.4.Energy absorption ef ficiencyA ratio,z ,is de fined by the mean crushing force,P m ,of the multi-cell lattice tube to that of the corresponding single-cell tube asz ¼ðP m Þmulti Àcell lattice tubeðP m Þsingle Àcell tube(2)where z suggests the enhancement of the mean crushing force of multi-cell tubes.Divided by the mean crushing force of ST1Table 2Value of coef ficient z .Node/tube zNode V 0.962Node K 0.850Node X 0.803Node Star 0.764Tube KT 0.883Tube TT 0.85780100120140160120180240300Y i e l d f o r c e (k N )B readth (m m )(a)80100120140160120180240300Y i e l d f o r c e (k N )B readth (m m )(b)80100120140160120180240300Y i e l d f o r c e (k N )B readth (m m )(c)Fig.10.Predicted yield forces of (a)multi-cell Kagome lattice tubes,(b)multi-cellFig.9.Simpli fied model of deformation restriction from the neighboring wall.W.Hong et al./International Journal of Impact Engineering 63(2014)106e 117112specimen,enhancements of the mean crushing force,z ,are 176.3%,187.7%and 190.3%for KT1tubes,and 190.7%,196.2%and 203.2%for TT1tubes,respectively.Divided by the mean crushing force of ST2specimen,the enhancements,z ,are 167.20%,168.06%and 163.3%for KT2tubes structures as well as 178.4%and 193.5%for TT2tubes,respectively.Divided by the mean crushing force of ST3specimen,the improvements,z ,are 163.7%,161.0%and 154.4%for KT3tubes as well as 169.2%,169.5%and 169.6%for TT3tubes,respectively.The average mean crushing forces are 129.4kN,130.5kN and 137.3kN for KT1,KT2and KT3tubes,respectively,and 137.7kN,146.1kN and 145.6kN for TT1,TT2and TT3tubes,pared with Kagome lattice tubes,triangular lattice tubes have a little greater mean crushing forces,about 6.4%,12.0%and 6.1%higher,respectively.The average crushing distances are 71.49mm,71.90mm and 73.44mm for KT1,KT2and KT3tubes,respectively,and 64.74mm,66.87mm and 69.45mm for TT1,TT2and TT3tubes,respectively.Triangular lattice tubes have shorter crushing dis-tance,about 9.4%,7.0%and 5.4%smaller,respectively.These two kinds of lattice tubes have identical energy absorptions.With thesame weight,these two multi-cell lattice tubes have the same speci fic energy absorption per unit mass.Due to the cross-section area of the Kagome lattice tube is 1/3greater,the speci fic energy absorption per unit volume of the Kagome lattice tube is about 75%of that of the triangular lattice tube.5.Analysis 5.1.Yield strengthSimply,yield force of the tube,P y ,could be predicted byP y ¼s z S ¼s s S(3)where s s is the initial yield stress of the material and S is the solid area of the cross-section of the multi-cell lattice tube.Symbol s z denotes the compression stress.In ideal one-dimensional stress state,the horizontal stress,s x ,is assumed to be zero and the yield condition is controlledbyFig.11.Deformation modes of Kagome lattice with breadth of (a)90mm,(b)120mm and (c)150mm.W.Hong et al./International Journal of Impact Engineering 63(2014)106e 117113s z ¼s s(4)Eq.(3)always overestimates the yield force.Actually,each flange of the multi-cell tube is not in one-dimensional compression stress state.Neighboring walls have deformation restrictions,which would be strengthened if the node has more connectivities.A simpli fied model of deformation restriction from a neighboring wall is proposed in Fig.9.Under compression stress,s z ,the hori-zontal deformation of side AB,d x ,is de fined byd xc =2¼Àn s z E(5)where E is the Young ’s modulus and n is the Poisson ’s ratio of thematerial.Simultaneously,the horizontal deformation of side BC,d x 0,induced by the horizontal deformation of side AB,a half of the cell breadth,is given byd x 0c =2¼d x cos jc =2¼Àn s z Ecos j (6)Horizontal stress of side BC,s x 0,induced by the horizontal strainiss x 0¼Ed x 0c =2¼Àns z cos j(7)Component of s x 0along side AB restrains the deformation of ABand the constraint stress,s x ,can be calculated from the deforma-tion of the neighboring flange BC,a half of the cell breadth,ass x ¼s x 0cos j ¼Àn cos 2js z(8)With multi-flanges at a node,the horizontal stress would be a summation ass x ¼Àns zXcos 2j(9)The yield condition in two-dimensional stress state iss s ¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiðs x Às z Þ2þs 2x þs 2zs (10)which suggests the critical vertical stress of each node,s z s ,ass z s ¼zs s(11)with a coef ficient z asz ¼1ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi1þn P cos 2j þn 2Pcos 4jp (12)Values of z for node V,node K,node V and node Star were listed in Table 2.For lattice tubes,the critical vertical stress should be averaged by the area ratio of each node,as listed in Table 2.Yield force of the tube,P y ,is given byP y ¼zs s S(13)where S is the solid area of the cross-section of the multi-cell lattice tube.As suggested by Fig.10,one-dimensional analysis greatly overestimates the yield force of the multi-cell lattice tube.Simpli-fied two-dimensional analysis introduced coef ficient z and would give more consistent predictions.To single-cell tubes,predictions suggested by the one-dimensional analysis and the two- 5.2.Mean crushing forceDeformation modes of Kagome and triangular lattice tubes were shown in Figs.11and 12,respectively.The folding style is similar to that of the single-cell tube revealed by Hong et al.[7]and Fan et al.[18].Zhang et al.also stressed the flange interactions at nodes with more connectivities [10e 13].Wierzbicki and Abramowicz [6]offered the method,as shown in Fig.13(a),to calculate the energy absorbed in inextensional mode,E 1,asE 1¼M P16I 1Hb þ2p c þ4I 3H 2(14)withI 1Àj ;a Á¼sin aZb ða Þ0d x ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffitan 2j þcos 2xq À p Àj Àarctancos b ða Þj !(15)(a)(b)PQAMAW.Hong et al./International Journal of Impact Engineering 63(2014)106e 117114andI3Àj;aÁ¼cot jZ acos affiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffitan2jþsin2aqd a(16)where r is the radius of the toroidal shell element in the kinemat-ically admissible velocityfield,t is the wall thickness,2H denotes the initial distance between plastic hinges at top and bottom of a basic folding element.Symbol M P is the fully plastic bending moment per unit width.For the angle j0in this paper,I1¼0.33and I3¼0.61.The external work,2P m H l,is equal to internal work,18E1,dissipated by plastic deformation of the lattice tube with18inextensional ele-ments as2P m H l¼18E1¼18M P16I1Hbtþ2p cþ4I3H2r(17)where l is a ratio of the effective crushing distance to the tube length.The wavelength and the mean crushing force of the lattice tube are given byH¼1:45c2=3t1=3(18) andP mP l¼116:76c 1=3(19) Abramowicz and Jones[2]suggested a method,as shown inFig.13b,to calculate the energy absorbed in extensional mode,E2, asE2¼M Pp Hþ2p cþ2p H2t(20)for square tubes.Hong et al.[7]applied this equation to evaluate the mean crushing force of triangular tubes.To suggest a more reasonable model,Eq.(20)should be improved.Suggested by Abramowicz and Jones[2],the energy absorbed by an extensional element with an angle of pÀ2j0isE2¼4M P HðpÀ2j0Þ=2þp c=2þ2j0H 2t !(21)For triangular tubes,j0¼p3(22) andE2¼M P23p Hþ2p cþ83p H2t(23)The energy equilibrium for a triangular lattice tube,having18 extensional elements,requires2P m H l¼18E2¼M P12p Hþ36p cþ48pH2(24)To determine the wavelength of the folding,it requiresv P m v H ¼0(25)H¼ffiffiffiffiffiffiffi3ctp2(26)The mean crushing force in extensional mode isP mM Pl¼6pþ24pffiffiffiffiffi3ctr(27)a little greater than the mean crushing force predicted by Eq.(20).The fully plastic bending moment per unit width is calculated byM P¼1st2(28)For a material with power law hardeningsðεÞ¼s uεεun(29)as shown in Fig.14a,theflow stress s0can be approximated by anaverage stress over the strain range[0,εu]as[8]s0¼1εuZεus dε(30)0.000.050.100.150.20100200300400500σεσS tra inStress(Mpa)σ=σ(ε/ε)(a)(b)0.000.050.100.150.200.25100200300400S trainStress(Mpa)T ested cu rv eσ=σ(ε/ε)50Unit: mm 10W.Hong et al./International Journal of Impact Engineering63(2014)106e117115where n is the power law exponent and suggested to be 0.165ac-cording to the experiment as shown in Fig.14b.Symbol s u is the ultimate tensile stress and εu is the strain at s u .The tested curve suggests s u ¼400MPa and s 0¼340.7MPa.Thus M P ¼0.1916kN $m/m.Inextensional mode of TT2tube and extensional mode of TT1tube were observed in experiments,as shown in Fig.15,where two star-nodes with six connectivities were cut out from two triangular lattice tubes.The experimental observation supports the potential application of classical theory in predicting the mean crushing force,as shown in Fig.16,where l ¼0.67for triangular lattice tubes and l ¼0.72for Kagome lattice ually,the classical theory includes two deformation modes and could suggest the lower and the upper limits of the mean crushing force of triangular tubes [7].Extensional mode could suggest consistent mean crushing forces with tested data when the cell dimension is smaller,as shown in Fig.16.When the cell dimension increases,predicted mean crushing force is gradually close to the inextensional prediction,as shown in Fig.16.But the inextensional deformation mode suggests smaller mean crushing forces than the tested.It would attribute to the interaction among neighboring flanges,which was not included in the model.Mean crushing forces of tubes with smaller cells are more consistently predicted by the extensional mode,while tubes with larger cells would be crushed mainly at the inextensional mode.The extensional mode and the inextensional mode could suggest the upper limit and the lower one of the mean crushing force,respectively.6.Multi-cell mechanismsAccording to the experiments and the theoretical analysis,the energy absorption of the multi-cell lattice tube would be greatly enhanced through two mechanisms.One is the multi-cell topology,which induces smaller cell dimension and thinner cell wall.Wavelength of each fold is greatly shortened.The other is the constraints from neighboring flanges.Energy dissipated by additional inwardly retracted plastic hinge lines near the node enhances the anti-crushing performance.Multi-cell structure let the lattice cell have much smaller breadth,c ,and smaller wall thickness,t .The wavelength is pro-portional to c 2/3t 1/3or ffiffiffiffict p for lattice tubes,as suggested by Eqs.(18)and (26).In current research,ratio of the wavelength of the single-cell tube to that of the lattice tube,k ,is de fined ask ¼Àffiffiffiffictp Ásingle Àcell tubeÀffiffiffiffict p Ámulti Àcell lattice tube(31)for extensional mode andk ¼c 23t 13single Àcell tubec 23t 13multi Àcell lattice tube(32)for inextensional mode,respectively.For the tested tubes,the ratios are 2.45and 2.62suggested by Eqs.(31)and (32),respectively,suggesting that the folding wavelength of the lattice tube would be nearly one third of that of the single-cell tube.In experiments,KT1and TT1tubes have three folds.The others have two folds.Single-cell tubes have only one fold.Wavelengths were also predicted,as listed in Table ttice tubes have much shorter wavelengths and more folds,theoretically.The folding wavelength is greatly shortened by multi-cell topology,indicating more folds and more plastic lines,which would dissipate more energy and increase the mean crushingforce.Fig.15.Folding styles in experiments for (a)inextensional mode and (b)extensional mode.0.0250.0300.0350.0400.0450.0500.05550100150200250300M e a n c r u s h i n g f o r c e (k N )C ell d im ension (m )Fig.16.Predicted mean crushing forces.W.Hong et al./International Journal of Impact Engineering 63(2014)106e 117116。
1 Introduction to the Galois Theory of Linear Differential Equations
1.2 What is a Linear Differential Equation? I will develop an algebraic setting for the study of linear differential equations. Although there are many interesting questions concerning differential equations in characteristic p [MvdP03a, MvdP03b, dP95, dP96], we will restrict ourselves throughout this paper, without further mention, to fields of characteristic 0. I begin with some basic definitions.
Compactness of solutions to the Yamabe problem. II
Compactness of solutions to the Yamabe problem. II
YanYan Li Department of Mathematics Rutgers University 110 Frelinghuysen Road Piscataway, NJ 08854 Lei Zhang Department of Mathematics University of Florida 358 Little Hall Gainesville, FL 32611-8105
1
IntroducБайду номын сангаасion
Let (M n , g ) be a compact, smooth, connected Riemannian manifold (without boundary) of dimension n ≥ 3. The Yamabe conjecture has been proved through the works of Yamabe [92], Trudinger [91], Aubin [4] and Schoen [79]: There exist constant scalar curvature metrics on M which are pointwise conformal to g . Consider the Yamabe equation and its sub-critical approximations: −Lg u = n(n − 2)up , u > 0, on M, (1)
1
2 Schoen initiated the investigation of the compactness of Mp and proved the following remarkable result in 1991, see [82], under the assumption that (M, g ) is locally conformally flat and is not conformally diffeomorphic to standard spheres: For any +2 1<1+ǫ≤p≤ n and for any non-negative integer k , n−2 u
【完整版】柯西积分定理与柯西积分公式的由来及其应用
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100个世界著名初等数学难题
100个世界著名初等数学难题2005-12-05 19:28, 数学绿园, 11802 字, 0/6, 原创| 引用100个著名初等数学问题(转载)第01题阿基米德分牛问题Archimedes' Problema Bovinu m太阳神有一牛群,由白、黑、花、棕四种颜色的公、母牛组成.在公牛中,白牛数多于棕牛数,多出之数相当于黑牛数的1/2 +1/3;黑牛数多于棕牛数,多出之数相当于花牛数的¼+1/5;花牛数多于棕牛数,多出之数相当于白牛数的1/6+1/7.在母牛中,白牛数是全体黑牛数的1/3+¼;黑牛数是全体花牛数¼+1/5;花牛数是全体棕牛数的1/5+1/6;棕牛数是全体白牛数的1/6+1/7.问这牛群是怎样组成的?第02题德·梅齐里亚克的法码问题The Weight Problem of Bachet de Meziriac一位商人有一个40磅的砝码,由于跌落在地而碎成4块.后来,称得每块碎片的重量都是整磅数,而且可以用这4块来称从1至40磅之间的任意整数磅的重物.问这4块砝码碎片各重多少?第03题牛顿的草地与母牛问题Newton's Problem of the Fields and Cowsa头母牛将b块地上的牧草在c天内吃完了;a'头母牛将b'块地上的牧草在c'天内吃完了;a"头母牛将b"块地上的牧草在c"天内吃完了;求出从a到c"9个数量之间的关系?第04题贝韦克的七个7的问题Berwick's Problem of th e Seven Sevens在下面除法例题中,被除数被除数除尽:* * 7 * * * * * * * ÷* * * * 7 * = * * 7 * ** * * * * ** * * * * 7 ** * * * * * ** 7 * * * ** 7 * * * ** * * * * * ** * * * 7 * ** * * * * ** * * * * *用星号(*)标出的那些数位上的数字偶然被擦掉了,那些不见了的是些什么数字呢?第05题柯克曼的女学生问题Kirkman's Schoolgirl Probl em某寄宿学校有十五名女生,她们经常每天三人一行地散步,问要怎样安排才能使每个女生同其他每个女生同一行中散步,并恰好每周一次?第06题伯努利-欧拉关于装错信封的问题The Bernoulli-Eu ler Problem of the Misaddressed letters求n个元素的排列,要求在排列中没有一个元素处于它应当占有的位置.第07题欧拉关于多边形的剖分问题Euler's Problem of P olygon Division可以有多少种方法用对角线把一个n边多边形(平面凸多边形)剖分成三角形?第08题鲁卡斯的配偶夫妇问题Lucas' Problem of the M arried Couplesn对夫妇围圆桌而坐,其座次是两个妇人之间坐一个男人,而没有一个男人和自己的妻子并坐,问有多少种坐法?第09题卡亚姆的二项展开式Omar Khayyam's Binomial Expansion当n是任意正整数时,求以a和b的幂表示的二项式a+b的n 次幂.第10题柯西的平均值定理Cauchy's Mean Theorem求证n个正数的几何平均值不大于这些数的算术平均值.第11题伯努利幂之和的问题Bernoulli's Power Sum Pro blem确定指数p为正整数时最初n个自然数的p次幂的和S=1p+ 2p+3p+…+np.第12题欧拉数The Euler Number求函数φ(x)=(1+1/x)x及Φ(x)=(1+1/x)x+1当x无限增大时的极限值.第13题牛顿指数级数Newton's Exponential Series将指数函数ex变换成各项为x的幂的级数.第14题麦凯特尔对数级数Nicolaus Mercator's Logarith mic Series不用对数表,计算一个给定数的对数.第15题牛顿正弦及余弦级数Newton's Sine and Cosine Series不用查表计算已知角的正弦及余弦三角函数.第16题正割与正切级数的安德烈推导法Andre's Derivatio n of the Secant and Tangent Series在n个数1,2,3,…,n的一个排列c1,c2,…,cn中,如果没有一个元素ci的值介于两个邻近的值ci-1和ci+1之间,则称c1,c2,…,cn为1,2,3,…,n的一个屈折排列.试利用屈折排列推导正割与正切的级数.第17题格雷戈里的反正切级数Gregory's Arc Tangent S eries已知三条边,不用查表求三角形的各角.第18题德布封的针问题Buffon's Needle Problem在台面上画出一组间距为d的平行线,把长度为l(小于d)的一根针任意投掷在台面上,问针触及两平行线之一的概率如何?第19题费马-欧拉素数定理The Fermat-Euler Prime Nu mber Theorem每个可表示为4n+1形式的素数,只能用一种两数平方和的形式来表示.第20题费马方程The Fermat Equation求方程x2-dy2=1的整数解,其中d为非二次正整数.第21题费马-高斯不可能性定理The Fermat-Gauss Impo ssibility Theorem证明两个立方数的和不可能为一立方数.第22题二次互反律The Quadratic Reciprocity Law(欧拉-勒让德-高斯定理)奇素数p与q的勒让德互反符号取决于公式(p/q)·(q/p)=(-1)[(p-1)/2]·[(q-1)/2].第23题高斯的代数基本定理Gauss' Fundamental Theor em of Algebra每一个n次的方程zn+c1zn-1+c2zn-2+…+cn=0具有n 个根.第24题斯图谟的根的个数问题Sturm's Problem of the Number of Roots求实系数代数方程在已知区间上的实根的个数.第25题阿贝尔不可能性定理Abel's Impossibility Theore m高于四次的方程一般不可能有代数解法.第26题赫米特-林德曼超越性定理The Hermite-Lindema nn Transcedence Theorem系数A不等于零,指数α为互不相等的代数数的表达式A1eα1+A2eα2+A3eα3+…不可能等于零.第27题欧拉直线Euler's Straight Line在所有三角形中,外接圆的圆心,各中线的交点和各高的交点在一直线—欧拉线上,而且三点的分隔为:各高线的交点(垂心)至各中线的交点(重心)的距离两倍于外接圆的圆心至各中线的交点的第28题费尔巴哈圆The Feuerbach Circle三角形中三边的三个中点、三个高的垂足和高的交点到各顶点的线段的三个中点在一个圆上.第29题卡斯蒂朗问题Castillon's Problem将各边通过三个已知点的一个三角形内接于一个已知圆.第30题马尔法蒂问题Malfatti's Problem在一个已知三角形内画三个圆,每个圆与其他两个圆以及三角形的两边相切.第31题蒙日问题Monge's Problem画一个圆,使其与三已知圆正交.第32题阿波洛尼斯相切问题The Tangency Problem of Apollonius.画一个与三个已知圆相切的圆.第33题马索若尼圆规问题Macheroni's Compass Proble m.证明任何可用圆规和直尺所作的图均可只用圆规作出.第34题斯坦纳直尺问题Steiner's Straight-edge Proble m证明任何一个可以用圆规和直尺作出的图,如果在平面内给出一个定圆,只用直尺便可作出.第35题德里安倍立方问题The Deliaii Cube-doubling Pr oblem画出体积为一已知立方体两倍的立方体的一边.第36题三等分一个角Trisection of an Angle把一个角分成三个相等的角.第37题正十七边形The Regular Heptadecagon画一正十七边形.第38题阿基米德π值确定法Archimedes' Determination of the Number Pi设圆的外切和内接正2vn边形的周长分别为av和bv,便依次得到多边形周长的阿基米德数列:a0,b0,a1,b1,a2,b2,…其中av+1是av、bv的调和中项,bv+1是bv、av+1的等比中项. 假如已知初始两项,利用这个规则便能计算出数列的所有项. 这个方法叫作阿基米德算法.第39题富斯弦切四边形问题Fuss' Problem of the Chor d-Tangent Quadrilateral找出半径与双心四边形的外接圆和内切圆连心线之间的关系.(注:一个双心或弦切四边形的定义是既内接于一个圆而同时又外切于另一个圆的四边形)第40题测量附题Annex to a Survey利用已知点的方位来确定地球表面未知但可到达的点的位置.第41题阿尔哈森弹子问题Alhazen's Billiard Problem在一个已知圆内,作出一个其两腰通过圆内两个已知点的等腰三角形.第42题由共轭半径作椭圆An Ellipse from Conjugate R adii已知两个共轭半径的大小和位置,作椭圆.第43题在平行四边形内作椭圆An Ellipse in a Parallelog ram,在规定的平行四边形内作一内切椭圆,它与该平行四边形切于一边界点.第44题由四条切线作抛物线A Parabola from Four Tang ents已知抛物线的四条切线,作抛物线.第45题由四点作抛物线A Parabola from Four Points.过四个已知点作抛物线.第46题由四点作双曲线A Hyperbola from Four Points.已知直角(等轴)双曲线上四点,作出这条双曲线.第47题范·施古登轨迹题Van Schooten's Locus Probl em平面上的固定三角形的两个顶点沿平面上一个角的两个边滑动,第三个顶点的轨迹是什么?第48题卡丹旋轮问题Cardan's Spur Wheel Problem.一个圆盘沿着半径为其两倍的另一个圆盘的内缘滚动时,这个圆盘上标定的一点所描出的轨迹是什么?第49题牛顿椭圆问题Newton's Ellipse Problem.确定内切于一个已知(凸)四边形的所有椭圆的中心的轨迹.第50题彭赛列-布里昂匈双曲线问题The Poncelet-Brianc hon Hyperbola Problem确定内接于直角(等边)双曲线的所有三角形的顶垂线交点的轨迹.第51题作为包络的抛物线A Parabola as Envelope从角的顶点,在角的一条边上连续n次截取任意线段e,在另一条边上连续n次截取线段f,并将线段的端点注以数字,从顶点开始,分别为0,1,2,…,n和n,n-1,…,2,1,0.求证具有相同数字的点的连线的包络为一条抛物线.第52题星形线The Astroid直线上两个标定的点沿着两条固定的互相垂直的轴滑动,求这条直线的包络.第53题斯坦纳的三点内摆线Steiner's Three-pointed Hy pocycloid确定一个三角形的华莱士(Wallace)线的包络.第54题一个四边形的最接近圆的外接椭圆The Most Nearl y Circular Ellipse Circumscribing a Quadrilateral一个已知四边形的所有外接椭圆中,哪一个与圆的偏差最小?第55题圆锥曲线的曲率The Curvature of Conic Sectio ns确定一个圆锥曲线的曲率.第56题阿基米德对抛物线面积的推算Archimedes' Squar ing of a Parabola确定包含在抛物线内的面积.第57题推算双曲线的面积Squaring a Hyperbola确定双曲线被截得的部分所含的面积.第58题求抛物线的长Rectification of a Parabola确定抛物线弧的长度.第59题笛沙格同调定理(同调三角形定理)Desargues' H omology Theorem (Theorem of Homologous Triangles)如果两个三角形的对应顶点连线通过一点,则这两个三角形的对应边交点位于一条直线上.反之,如果两个三角形的对应边交点位于一条直线上,则这两个三角形的对应顶点连线通过一点.第60题斯坦纳的二重元素作图法Steiner's Double Eleme nt Construction由三对对应元素所给定的重迭射影形,作出它的二重元素.第61题帕斯卡六边形定理Pascal's Hexagon Theorem求证内接于圆锥曲线的六边形中,三双对边的交点在一直线上.第62题布里昂匈六线形定理Brianchon's Hexagram The orem求证外切于圆锥曲线的六线形中,三条对顶线通过一点.第63题笛沙格对合定理Desargues' Involution Theore m一条直线与一个完全四点形*的三双对边的交点与外接于该四点形的圆锥曲线构成一个对合的四个点偶. 一个点与一个完全四线形*的三双对顶点的连线和从该点向内切于该四线形的圆锥曲线所引的切线构成一个对合的四个射线偶.*一个完全四点形(四线形)实际上含有四点(线)1,2,3,4和它们的六条连线交点23,14,31,24,12,34;其中23与14、31与24、12与34称为对边(对顶点).第64题由五个元素得到的圆锥曲线A Conic Section fro m Five Elements求作一个圆锥曲线,它的五个元素——点和切线——是已知的.第65题一条圆锥曲线和一条直线A Conic Section and a Straight Line一条已知直线与一条具有五个已知元素——点和切线——的圆锥曲线相交,求作它们的交点.第66题一条圆锥曲线和一定点A Conic Section and a P oint已知一点及一条具有五个已知元素——点和切线——的圆锥曲线,作出从该点列到该曲线的切线.第67题斯坦纳的用平面分割空间Steiner's Division of S pace by Planesn个平面最多可将整个空间分割成多少份?第68题欧拉四面体问题Euler's Tetrahedron Problem以六条棱表示四面体的体积.第69题偏斜直线之间的最短距离The Shortest DistanceBetween Skew Lines计算两条已知偏斜直线之间的角和距离.第70题四面体的外接球The Sphere Circumscribing a Tetrahedron确定一个已知所有六条棱的四面体的外接球的半径.第71题五种正则体The Five Regular Solids将一个球面分成全等的球面正多边形.第72题正方形作为四边形的一个映象The Square as an Image of a Quadrilateral证明每个四边形都可以看作是一个正方形的透视映象.第73题波尔凯-许瓦尔兹定理The Pohlke-Schwartz The orem一个平面上不全在同一条直线上的四个任意点,可认为是与一个已知四面体相似的四面体的各隅角的斜映射.第74题高斯轴测法基本定理Gauss' Fundamental Theor em of Axonometry正轴测法的高斯基本定理:如果在一个三面角的正投影中,把映象平面作为复平面,三面角顶点的投影作为零点,边的各端点的投影作为平面的复数,那么这些数的平方和等于零.第75题希帕查斯球极平面射影Hipparchus' Stereographi c Projection试举出一种把地球上的圆转换为地图上圆的保形地图射影法.第76题麦卡托投影The Mercator Projection画一个保形地理地图,其坐标方格是由直角方格组成的.第77题航海斜驶线问题The Problem of the Loxodrom e确定地球表面两点间斜驶线的经度.第78题海上船位置的确定Determining the Position of a Ship at Sea利用天文经线推算法确定船在海上的位置.第79题高斯双高度问题Gauss' Two-Altitude Problem根据已知两星球的高度以确定时间及位置.第80题高斯三高度问题Gauss' Three-Altitude Problem从在已知***球获得同高度瞬间的时间间隔,确定观察瞬间,观察点的纬度及星球的高度.第81题刻卜勒方程The Kepler Equation根据行星的平均近点角,计算偏心及真近点角.第82题星落Star Setting对给定地点和日期,计算一已知星落的时间和方位角.第83题日晷问题The Problem of the Sundial制作一个日晷.第84题日影曲线The Shadow Curve当直杆置于纬度φ的地点及该日太阳的赤纬有δ值时,确定在一天过程中由杆的一点投影所描绘的曲线.第85题日食和月食Solar and Lunar Eclipses如果对于充分接近日食时间的两个瞬间太阳和月亮的赤经、赤纬以及其半径均为已知,确定日食的开始和结束,以及太阳表面被隐蔽部分的最大值.第86题恒星及会合运转周期Sidereal and Synodic Revo lution Periods确定已知恒星运转周期的两共面旋转射线的会合运转周期.第87题行星的顺向和逆向运动Progressive and Retrogr ade Motion of Planets行星什么时候从顺向转为逆向运动(或反过来,从逆向转为顺向运动)?第88题兰伯特慧星问题Lambert's Comet Prolem借助焦半径及连接弧端点的弦,来表示慧星描绘抛物线轨道的一段弧所需的时间.第89题与欧拉数有关的斯坦纳问题Steiner's Problem Co ncerning the Euler Number如果x为正变数,x取何值时,x的x次方根为最大?第90题法格乃诺关于高的基点的问题Fagnano's Altitude Base Point Problem在已知锐角三角形中,作周长最小的内接三角形.第91题费马对托里拆利提出的问题Fermat's Problem forTorricelli试求一点,使它到已知三角形的三个顶点距离之和为最小.第92题逆风变换航向Tacking Under a Headwind帆船如何能顶着北风以最快的速度向正北航行?第93题蜂巢(雷阿乌姆尔问题)The Honeybee Cell (Pr oblem by Reaumur)试采用由三个全等的菱形作成的顶盖来封闭一个正六棱柱,使所得的这一个立体有预定的容积,而其表面积为最小.第94题雷奇奥莫塔努斯的极大值问题Regiomontanus' Ma ximum Problem在地球表面的什么部位,一根垂直的悬杆呈现最长?(即在什么部位,可见角为最大?)第95题金星的最大亮度The Maximum Brightness of V enus在什么位置金星有最大亮度?第96题地球轨道内的慧星A Comet Inside the Earth's Orbit慧星在地球的轨道内最多能停留多少天?第97题最短晨昏蒙影问题The Problem of the Shortest Twilight在已知纬度的地方,一年之中的哪一天晨昏蒙影最短?第98题斯坦纳的椭圆问题Steiner's Ellipse Problem在所有能外接(内切)于一个已知三角形的椭圆中,哪一个椭圆有最小(最大)的面积?第99题斯坦纳的圆问题Steiner's Circle Problem在所有等周的(即有相等周长的)平面图形中,圆有最大的面积.反之:在有相等面积的所有平面图形中,圆有最小的周长.第100题斯坦纳的球问题Steiner's Sphere Problem在表面积相等的所有立体中,球具有最大体积.在体积相等的所有立体中,球具有最小的表面。
Distributionally robust joint chance constraints with second-order moment information
Math.Program.,Ser.ADOI10.1007/s10107-011-0494-7FULL LENGTH PAPERDistributionally robust joint chance constraintswith second-order moment informationSteve Zymler·Daniel Kuhn·BerçRustemReceived:20August2010/Accepted:26August2011©Springer and Mathematical Optimization Society2011Abstract We develop tractable semidefinite programming based approximations for distributionally robust individual and joint chance constraints,assuming that only thefirst-and second-order moments as well as the support of the uncertain parameters are given.It is known that robust chance constraints can be conservatively approxi-mated by Worst-Case Conditional Value-at-Risk(CVaR)constraints.Wefirst prove that this approximation is exact for robust individual chance constraints with concave or(not necessarily concave)quadratic constraint functions,and we demonstrate that the Worst-Case CVaR can be computed efficiently for these classes of constraint func-tions.Next,we study the Worst-Case CVaR approximation for joint chance constraints. This approximation affords intuitive dual interpretations and is provably tighter than two popular benchmark approximations.The tightness depends on a set of scaling parameters,which can be tuned via a sequential convex optimization algorithm.We show that the approximation becomes essentially exact when the scaling parameters are chosen optimally and that the Worst-Case CVaR can be evaluated efficiently if the scaling parameters are kept constant.We evaluate our joint chance constraint approx-imation in the context of a dynamic water reservoir control problem and numerically demonstrate its superiority over the two benchmark approximations. Mathematics Subject Classification(2010)90C15·90C221IntroductionA large class of decision problems in engineering andfinance can be formulated as chance constrained programs of the formS.Zymler(B)·D.Kuhn·B.RustemDepartment of Computing,Imperial College London,180Queen’s Gate,London SW72AZ,UKe-mail:sz02@S.Zymler et al.minimize x ∈R n c T x subject to Q a i (˜ξ)T x ≤b i (˜ξ)∀i =1,...,m ≥1−(1)x ∈X ,where x ∈R n is the decision vector,X ⊆R n is a convex closed set that can be rep-resented by semidefinite constraints,and c ∈R n is a cost vector.Without much loss of generality,we assume that c is deterministic.The chance constraint in (1)requires a set of m uncertainty-affected inequalities to be jointly satisfied with a probability of at least 1− ,where ∈(0,1)is a desired safety factor specified by the modeler.The uncertain constraint coefficients a i (˜ξ)∈R n and b i (˜ξ)∈R ,i =1,...,m ,depend affinely on a random vector ˜ξ∈R k ,whose distribution Q is assumed to be known.We thus havea i (˜ξ)=a 0i +kj =1a j i ˜ξj and b i (˜ξ)=b 0i +k j =1b j i ˜ξj .For ease of notation we introduce auxiliary functions y j i :R n →R ,which are defined throughy j i (x )=(a j i )T x −b j i ,i =1,...,n ,j =0,...,k .These functions enable us to rewrite the chance constraint in problem (1)asQ y 0i (x )+y i (x )T ˜ξ≤0∀i =1,...,m ≥1− ,(2)where y i (x )=[y 1i (x ),...,y k i (x )]T is affine in x for i =1,...,m .By convention,(2)is referred to as an individual or joint chance constraint if m =1or m >1,respec-tively.Chance constrained programs were first discussed by Charnes et al.[8],Miller and Wagner [18]and Prékopa [23].Although they have been studied for a long time,they have not found wide application in practice due to the following reasons.Firstly,computing the optimal solution of a chance constrained program is noto-riously difficult.In fact,even checking the feasibility of a fixed decision x requires the computation of a multi-dimensional integral,which becomes increasingly difficult as the dimension k of the random vector ˜ξincreases.Furthermore,even though the inequalities in the chance constraint (2)are biaffine in x and ˜ξ,the feasible set of problem (1)is typically nonconvex and sometimes even disconnected.Secondly,in order to evaluate the chance constraint (2),full and accurate informa-tion about the probability distribution Q of the random vector ˜ξis required.However,in many practical situations Q must be estimated from historical data and is therefore itself uncertain.Typically,one has only partial information about Q ,e.g.about its moments or its support.Replacing the unknown distribution Q in (1)by an estimate ˆQ corrupted by measurement errors may lead to over-optimistic solutions which often fail to satisfy the chance constraint under the true distribution Q .Distributionally robust joint chance constraintsIn a few special cases chance constraints can be reformulated as tractable convex constraints.For example,it is known that if the random vector˜ξfollows a Gauss-ian distribution and ≤0.5,then an individual chance constraint can be equivalently expressed as a single second-order cone constraint.In this case,the chance constrained problem becomes a tractable second-order cone program(SOCP),which can be solved in polynomial time,see Alizadeh and Goldfarb[1].More generally,Calafiore and El Ghaoui[6]have shown that for ≤0.5individual chance constraints can be con-verted to second-order cone constraints whenever the random vector˜ξis governed by a radial distribution.Tractability results for joint chance constraints are even more scarce.In a seminal paper,Prékopa[23]has shown that joint chance constraints are convex when only the right-hand side coefficients b i(˜ξ)are uncertain and follow a log-concave distribution.However,under generic distributions,chance constrained programs are computationally intractable.Indeed,Shapiro and Nemirovski[20]point out that computing the probability of a weighted sum of uniformly distributed variables being nonpositive is already N P-hard.Recently,Calafiore and Campi[5]as well as Luedtke and Ahmed[17]have pro-posed to replace the chance constraint(2)by a pointwise constraint that must hold at afinite number of sample points drawn randomly from the distribution Q.A similar approach was suggested by Erdoˇg an and Iyengar[12].The advantage of this Monte Carlo approach is that no structural assumptions about Q are needed and that the resulting approximate problem is convex.Calafiore and Campi[5]showed that one requires O(n/ )samples to guarantee that a solution of the approximate problem is feasible in the original chance constrained program.However,this implies that it may be computationally prohibitive to solve large problems or to solve problems for which a small violation probability is required.A natural way to immunize the chance constraint(2)against uncertainty in the prob-ability distribution is to adopt a distributionally robust approach.To this end,let P denote the set of all probability distributions on R k that are consistent with the known properties of Q,such as itsfirst and second moments and/or its support.Consider now the following ambiguous or distributionally robust chance constraint.inf P∈P Py0i(x)+y i(x)T˜ξ≤0∀i=1,...,m≥1− (3)It is easily verified that whenever x satisfies(3)and Q∈P,then x also satisfies the chance constraint(2)under the true probability distribution Q.Replacing the chance constraint(2)with its distributionally robust counterpart(3)yields the following dis-tributionally robust chance constrained programminimizex∈R nc T xsubject to infP∈P Py0i(x)+y i(x)T˜ξ≤0∀i=1,...,m≥1−x∈X,(4)which constitutes a conservative approximation for problem(1)in the sense that it has the same objective function but a smaller feasible set.S.Zymler et al.A common method to simplify the distributionally robust joint chance constraint(3),which looks even less tractable than(2),is to decompose it into m individualchance constraints by using Bonferroni’s inequality.Indeed,by ensuring that the totalsum of violation probabilities of the individual chance constraints does not exceed ,the feasibility of the joint chance constraint is guaranteed.Nemirovski and Shapiro[20]propose to divide the overall violation probability equally among the m indi-vidual chance constraints.However,the Bonferroni inequality is not necessarily tight,and the corresponding decomposition could therefore be over-conservative.In fact,forpositively correlated constraint functions,the quality of the approximation is knownto decrease as m increases[9].Consequently,the Bonferroni method may result ina poor approximation for problems with joint chance constraints that involve manyinequalities.A recent attempt to improve on the Bonferroni approximation is due to Chen et al.[9].Theyfirst elaborate a convex conservative approximation for a joint chance con-straint in terms of a Worst-Case Conditional Value-at-Risk(CVaR)constraint.Then,they rely on a classical inequality in order statistics to determine a tractable conserva-tive approximation for the Worst-Case CVaR and show that the resulting approximationfor the joint chance constraint necessarily outperforms the Bonferroni approximation.An attractive feature of this method is that the arising approximate constraints aresecond-order conic representable.However,the employed probabilistic inequality isnot necessarily tight,which may again render the approximation over-conservative.The principal aim of this paper is to develop new tools and models for approximatingrobust individual and joint chance constraints under the assumption that only thefirst-and second-order moments as well as the support of the random vector˜ξare known.We embrace the modern approach to approximate robust chance constraints by Worst-CaseCVaR constraints,but in contrast to the state-of-the-art methods described above,wefind exact semidefinite programming(SDP)reformulations of the Worst-Case CVaRwhich do not rely on potentially loose probabilistic inequalities.These reformulationsare facilitated by the theory of moment problems and by conic duality arguments.Weprove that the CVaR approximation is in fact exact for individual chance constraintswhose constraint functions are either concave or(possibly nonconcave)quadratic inξand for joint chance constraints whose constraint functions depend linearly onξ.Wealso demonstrate that robust individual chance constraints have manifestly tractableSDP representations in most cases in which the CVaR approximation is exact.The main contributions of this paper can be summarized as follows:(1)In Sect.2we review and extend existing approximations for distributionallyrobust individual chance constraints and prove that a robust individual chanceconstraint is equivalent to a tractable Worst-Case CVaR constraint if theunderlying constraint function is either concave or(possibly nonconcave)qua-dratic inξ.We also demonstrate that this equivalence can fail to hold even if theconstraint function is convex and piecewise linear inξ.(2)In Sect.3we develop a new tractable CVaR approximation for robust joint chanceconstraints and prove that this approximation consistently outperforms the state-of-the-art methods described above.We show that the approximation qualityis controlled by a set of scaling parameters and that the CVaR approximationDistributionally robust joint chance constraintsbecomes essentially exact if the scaling parameters are chosen optimally.We also present an intuitive dual interpretation for the CVaR approximation in this case.(3)In Sect.4we analyze the performance of the new joint chance constraint approx-imation when applied to a dynamic water reservoir control problem.Notation We use lower-case bold face letters to denote vectors and upper-case bold face letters to denote matrices.The space of symmetric matrices of dimension n is denoted by S n.For any two matrices X,Y∈S n,we let X,Y =Tr(XY)be the trace scalar product,while the relation X Y(X Y)implies that X−Y is positive semidefinite(positive definite).Random variables are always represented by symbols with tildes,while their realizations are denoted by the same symbols without tildes. For x∈R,we define x+=max{x,0}.2Distributionally robust individual chance constraintsIt is known that robust individual chance constraints can be conservatively approxi-mated by Worst-Case CVaR constraints.In this section,wefirst show how the theory of moment problems can be used to reformulate these Worst-Case CVaR constraints in terms of tractable semidefinite constraints.Subsequently,we prove that the Worst-Case CVaR constraints are in fact equivalent to the underlying robust chance constraints for a large class of constraint functions.Distributional assumptions In the remainder of this paper we letμ∈R k be the mean vector and ∈S k be the covariance matrix of the random vector˜ξunder the true distribution Q.Thus,we implicitly assume that Q hasfinite second-order moments. Without loss of generality we also assume that 0.Furthermore,we let P denote the set of all probability distributions on R k that have the samefirst-and second-order moments as Q.For notational simplicity,we let=+μμTμμT1be the second-order moment matrix of˜ξ.2.1The Worst-Case CVaR approximationFor m=1,(3)reduces to a distributionally robust individual chance constraintinf P∈P Py0(x)+y(x)T˜ξ≤0≥1− ,(5)whose feasible set is denoted byS.Zymler et al.X ICC=x∈R n:infP∈PPy0(x)+y(x)T˜ξ≤0≥1−.In the remainder of this section we will demonstrate that X ICC has a manifestly trac-table representation in terms of Linear Matrix Inequalities(LMIs).To this end,we first recall the definition of CVaR due to Rockafellar and Uryasev[24].For a given measurable loss function L:R k→R,probability distribution P on R k,and tolerance ∈(0,1),the CVaR at level with respect to P is defined asP-CVaR (L(˜ξ))=infβ∈Rβ+1E P(L(˜ξ)−β)+,(6)where E P(·)denotes expectation with respect to P.CVaR essentially evaluates the conditional expectation of loss above the(1− )-quantile of the loss distribution.It can be shown that CVaR represents a convex functional of the random variable L(˜ξ).CVaR can be used to construct convex approximations for chance constraints. Indeed,it is well known thatPL(˜ξ)≤P-CVaR (L(˜ξ))≥1−for any measurable loss function L,see,e.g.,Ben-Tal et al.[3,Sect.4.3.3].Thus, P-CVaR (L(˜ξ))≤0is sufficient to imply P(L(˜ξ)≤0)≥1− .As this implication holds for any probability distribution and loss function,we conclude thatsup P∈P P-CVaRy0(x)+y(x)T˜ξ≤0 ⇒infP∈PPy0(x)+y(x)T˜ξ≤0≥1− .(7)Thus,the Worst-Case CVaR constraint on the left hand side constitutes a conservative approximation for the distributionally robust chance constraint on the right hand side of(7).The above discussion motivates us to define the feasible setZ ICC=x∈R n:supP∈PP-CVaRy0(x)+y(x)T˜ξ≤0,(8)and the implication(7)gives rise to the following elementary result.Proposition2.1The feasible set Z ICC constitutes a conservative approximation for X ICC,that is,Z ICC⊆X ICC.We will now show that Z ICC has a tractable representation in terms of LMIs. Theorem21The feasible set Z ICC can be written asZ ICC=⎧⎪⎪⎨⎪⎪⎩x∈Rn:∃(β,M)∈R×S k+1,M 0,β+1 ,M ≤0,M−012y(x)12y(x)T y0(x)−β⎫⎪⎪⎬⎪⎪⎭.Distributionally robust joint chance constraintsProof By using(6),the Worst-Case CVaR in(8)can be expressed assup P∈P P-CVaRy0(x)+y(x)T˜ξ=supP∈P infβ∈Rβ+1E P(y0(x)+y(x)T˜ξ−β)+=infβ∈Rβ+1supP∈PE P(y0(x)+y(x)T˜ξ−β)+,(9)where the interchange of the maximization and minimization operations is justified by a stochastic saddle point theorem due to Shapiro and Kleywegt[26],see also Delage and Ye[11]or Natarajan et al.[19].We now show that the Worst-Case CVaR(9)of somefixed decision x∈R n can be computed by solving a tractable SDP.To this end, wefirst derive an SDP reformulation of the worst-case expectation problemsup P∈P E P(y0(x)+y(x)T˜ξ−β)+,which can be identified as the subordinate maximization problem in(9).Lemma A.1 in the Appendix enables us to reformulate this worst-case expectation problem as infM∈S k+1,M s.t.M 0,ξT1MξT1T≥y0(x)+y(x)Tξ−β∀ξ∈R k.(10)Note that the semi-infinite constraint in(10)can be written as the following LMI.ξ1 TM−012y(x)12y(x)T y0(x)−βξ1≥0∀ξ∈R k⇐⇒M−012y(x)12y(x)T y0(x)−βThis in turn allows us to reformulate the worst-case expectation problem asinfM∈S k+1,Ms.t.M 0,M−012y(x)12y(x)T y0(x)−β0.(11)S.Zymler et al. By replacing the subordinate worst-case expectation problem in(9)by(11),we obtainsup P∈P P-CVaRy0(x)+y(x)T˜ξ=infβ+1 ,Ms.t.M∈S k+1,β∈RM 0,M−012y(x)12y(x)T y0(x)−β0,(12)and thus the claim follows.2.2Exactness of the Worst-Case CVaR approximationSo far we have shown that the feasible set Z ICC defined in terms of a Worst-Case CVaRconstraint constitutes a tractable conservative approximation for X ICC.We now dem-onstrate that this approximation is in fact exact,that is,we show that the implication(7)is in fact an equivalence.Wefirst recall the nonlinear Farkas Lemma as well as the S-lemma,which are crucial ingredients for the proof of this result.We refer to Pólik and Terlaky[22]for a derivation and an in-depth survey of the S-lemma as well as areview of the Farkas Lemma.Lemma2.2(Farkas Lemma)Let f0,...,f p:R k→R be convex functions,and assume that there exists a strictly feasible point¯ξwith f i(¯ξ)<0,i=1,...,p.Then, f0(ξ)≥0for allξwith f i(ξ)≤0,i=1,...,p,if and only if there exist constants τi≥0such thatf0(ξ)+pi=1τi f i(ξ)≥0∀ξ∈R k.Lemma2.2(S-lemma)Let f i(ξ)=ξT A iξwith A i∈S n be quadratic functions of ξ∈R n for i=0,...,p.Then,f0(ξ)≥0for allξwith f i(ξ)≤0,i=1,...,p,if there exist constantsτi≥0such thatA0+pi=1τi A i 0.For p=1,the converse implication holds if there exists a strictly feasible point¯ξwith f1(¯ξ)<0.Theorem2.2Let L:R k→R be a continuous loss function that is either(i)concave inξ,or(ii)(possibly nonconcave)quadratic inξ.Then,the following equivalence holds.sup P∈P P-CVaRL(˜ξ)≤0⇐⇒infP∈PPL(˜ξ)≤0≥1− (13)Distributionally robust joint chance constraintsProof Consider the Worst-Case Value-at-Risk of the loss function L ,which is defined asWC-VaR (L (˜ξ))=inf γ∈R γ:inf P ∈PP L (˜ξ)≤γ ≥1− .(14)By definition,the WC-VaR is indeed equal to the (1− )-quantile of L (˜ξ)evaluated under some worst-case distribution in P .We first show that the following equivalenceholds.inf P ∈PP L (˜ξ)≤0 ≥1− ⇐⇒WC-VaR L (˜ξ) ≤0(15)Indeed,if the left hand side of (15)is satisfied,then γ=0is feasible in (14),which implies that WC-VaR (L (˜ξ))≤0.To see that the converse implication holds as well,we note that for any fixed P ∈P ,the mapping γ→P (L (˜ξ)≤γ)is upper semi-continuous,see [21].Thus,the related mapping γ→inf P ∈P P (L (˜ξ)≤γ)is also upper semi-continuous.If WC-VaR (L (˜ξ))≤0,there exists a sequence {γn }n ∈N that converges to zero and is feasible in (14),which impliesinf P ∈P PL (˜ξ)≤0 ≥lim sup n →∞inf P ∈PP L (˜ξ)≤γn ≥1− .Thus,(15)follows.To prove the postulated equivalence (13),it is now sufficient to show thatsup P ∈PP -CVaR L (˜ξ) =WC-VaR L (˜ξ) .Note that (14)can be rewritten asWC-VaR (L (˜ξ))=inf γ∈R γ:sup P ∈P P L (˜ξ)>γ ≤ .(16)We proceed by simplifying the subordinate worst-case probability problem sup P ∈PP (L (˜ξ)>γ),which,by Lemma A.2in the Appendix,can be expressed as inf M ∈S k +1 ,M :M 0, ξT 1 M ξT 1 T ≥1∀ξ:γ−L (ξ)<0 .(17)We will now argue that for all but one value of γproblem (17)is equivalent toinf ,Ms .t .M ∈S k +1,τ∈R ,M 0,τ≥0 ξT 1 M ξT 1 T −1+τ(γ−L (ξ))≥0∀ξ∈R k .(18)S.Zymler et al.For ease of exposition,we define h =inf ξ∈R k γ−L (ξ).The equivalence of (17)and (18)is proved case by case.Assume first that h <0.Then,the strict inequal-ity in the parameter range of the semi-infinite constraint in (17)can be replaced by a weak inequality without affecting its optimal value.The equivalence then follows from the Farkas Lemma (when L (ξ)is concave in ξ)or from the S -lemma (when L (ξ)is quadratic in ξ).Assume next that h >0.Then,the semi-infinite constraint in(17)becomes redundant and,since 0,the optimal solution of (17)is given by M =0with a corresponding optimal value of 0.The optimal value of problem (18)is also equal to 0.Indeed,by choosing τ=1/h ,the semi-infinite constraint in (18)is satisfied for any M 0.Finally,note that (17)and (18)may be different for h =0.Since (17)and (18)are equivalent for all but one value of γand since their optimal values are nonincreasing in γ,we can express WC-VaR (L (˜ξ))in (16)as WC-VaR (L (˜ξ))=inf γs .t .M ∈S k +1,τ∈R ,γ∈R ,M ≤ ,M 0,τ≥0 ξT 1 M ξT 1 T −1+τ(γ−L (ξ))≥0∀ξ∈R k .(19)It can easily be shown that ,M ≥1for any feasible solution of (19)with vanishing τ-component.However,since <1,this is in conflict with the constraint ,M ≤ .We thus conclude that no feasible point can have a vanishing τ-component.This allows us to divide the semi-infinite constraint in problem (19)by τ.Subsequently we per-form variable substitutions in which we replace τby 1/τand M by M /τ.This yields the following reformulation of problem (19).WC-VaR (L (˜ξ))=inf γs .t .M ∈S k +1,τ∈R ,γ∈R 1 ,M ≤τ,M 0,τ≥0 ξT 1 M ξT 1 T −τ+γ−L (ξ)≥0∀ξ∈R kNote that,since 0and M 0,we have 1 ,M ≥0.This allows us to remove the redundant nonnegativity constraint on τ.We now introduce a new decision variable β=γ−τ,which allows us to eliminate γ.WC-VaR (L (˜ξ))=inf β+τs .t .M ∈S k +1,τ∈R ,β∈R 1 ,M ≤τ,M 0 ξT 1 M ξT 1 T +β−L (ξ)≥0∀ξ∈R kNote that at optimality τ=1 ,M ,which finally allows us to express WC-VaR (L (˜ξ))asWC-VaR (L (˜ξ))=inf β+1,M s .t .M ∈S k +1,β∈R ,M 0ξT 1 M ξT 1 T+β−L (ξ)≥0∀ξ∈R k .(20)Recall now that by Lemma A.1we have sup P ∈PP -CVaRL (˜ξ)=inf β∈Rβ+1 sup P ∈P E P (L (˜ξ)−β)+ =inf β+1,Ms .t .M ∈S k +1,β∈R ,M 0ξT 1 M ξT 1 T+β−L (ξ)≥0∀ξ∈R k ,which is clearly equivalent to (20).This observation completes the proof.Corollary 2.1The following equivalence holdssup P ∈PP -CVaRy 0(x )+y (x )T ˜ξ≤0⇐⇒inf P ∈PPy 0(x )+y (x )T ˜ξ≤0≥1− ,which implies that Z ICC =X ICC .Proof The claim follows immediately from Theorem 2.2by observing that L (ξ)=y 0(x )+y (x )T ξis linear (and therefore concave)in ξ.In the following example we demonstrate that the equivalence (13)can fail to holdeven if the loss function L is convex and piecewise linear in ξ.Example 2.1Let ˜ξbe a scalar random variable with mean μ=0and standard devi-ation σ=1.Moreover,let P be the set of all probability distributions on R con-sistent with the given mean and standard deviation.Consider now the loss function L (ξ)=max {ξ−1,4ξ−4},and note that L is strictly increasing and convex in ξ.In particular,L is neither concave nor quadratic and thus falls outside the scope of Theorem 2.2.We now show that for this particular L the Worst-Case CVaR constraintsup P ∈P P -CVaR 12(L (˜ξ))≤0is violated even though the distributionally robust indi-vidual chance constraint inf P ∈P P (L (˜ξ)≤0)≥1/2is satisfied.To this end,we note that the Chebychev inequality P (˜ξ−μ≥κσ)≤1/(1+κ2)for κ=1implies sup P ∈P P˜ξ≥1 ≤12⇐⇒sup P ∈PP L (˜ξ)≥L (1)=0 ≤12 ⇒sup P ∈PP L (˜ξ)>0 ≤12⇐⇒inf P ∈PP L (˜ξ)≤0 ≥12,where the first equivalence follows from the monotonicity of L .Assume now thatthe true distribution Q of ˜ξis discrete and defined through Q (˜ξ=−2)=1/8,Q (˜ξ=0)=3/4,and Q (˜ξ=2)=1/8.It is easy to verify that Q ∈P and that Q -CVaR 12(L (˜ξ))=0.25.Thus,sup P ∈P P -CVaR 12(L (˜ξ))≥0.25>0.We therefore conclude that the Worst-Case CVaR constraint is not equivalent to the robust chance constraint.2.3Tractability of the Worst-Case CVaR approximationWe have already seen that Worst-Case CVaR constraints are equivalent to distribution-ally robust chance constraints when the loss function is continuous and either concave or quadratic in ξ.We now prove that the Worst-Case CVaR can also be computed efficiently for these classes of loss functions.Theorem 2.3Assume that L :R k →R is either(i)concave piecewise affine in ξwith a finite number of pieces or (ii)(possibly nonconcave )quadratic in ξ.Then,sup P ∈P P -CVaR (L (˜ξ))can be computed efficiently as the optimal value of a tractable SDP .Proof Assume that (i)holds and that L (˜ξ)=min i =1,...,l {a i +b T i ˜ξ}for some a i ∈Rand b i ∈R k ,i =1,...,l .Then,the Worst-Case CVaR is representable asinfβ∈Rβ+1sup P ∈PE Pmin i =1,...,l{a i +b T i ˜ξ}−β +.(21)By Lemma A.1,the subordinate worst-case expectation problem in (21)can be rewrit-ten asinfM ∈S k +1,M s .t .M 0,ξT 1 M ξT 1 T≥min i =1,...,l{a i +b T i ξ}−β∀ξ∈R k .(22)Noting thatmin i =1,...,l{a i +b T i ξ}=minλ∈l i =1λi (a i +b T i ξ),where ={λ∈R l : l i =1λi =1,λ≥0}denotes the probability simplex in R l ,we can use techniques developed in [4,Theorem 2.1]to reexpress the semi-infinite constraint in (22)asξT 1 M ξT1 T −min λ∈li =1λi (a i +b T i ξ)+β≥0∀ξ∈R k⇐⇒min ξ∈R kmaxλ∈ξT 1 M ξT 1 T −li =1λi (a i +b T i ξ)+β≥0⇐⇒max λ∈ min ξ∈R kξT 1 M ξT1 T −l i =1λi (a i +b T i ξ)+β≥0⇐⇒minξ∈R kξT 1 M ξT1 T −li =1λi (a i +b T i ξ)+β≥0,λ∈⇐⇒M −l i =1λi2b il i =1λi2b Ti l i =1λi a i −β 0,λ∈ .The second equivalence in the above expression follows from the classical saddlepoint theorem.Thus,the Worst-Case CVaR (21)can be rewritten as the optimal value of the following tractable SDP.inf β+1 ,Ms .t .β∈R ,M ∈S k +1,λ∈R lM 0,M − 0l i =1λi 2b il i =1λi 2b T i l i =1λi a i −β0,λ∈ (23)Assume now that (ii)holds and that L (ξ)=ξT Q ξ+q T ξ+q 0for some Q ∈S k ,q ∈R k ,and q 0∈R .In this case we havesup P ∈P P -CVaR (L (˜ξ))=inf β∈R β+1 sup P ∈PE P ˜ξT Q ˜ξ+˜ξT q +q 0−β + .(24)As usual,we first find an SDP reformulation of the subordinate worst-case expectation problem in (24).By Lemma A.1,this problem can be rewritten asinfM ∈S k +1,Ms .t .M 0, ξT 1 M ξT 1 T≥ξT Q ξ+ξT q +q 0−β∀ξ∈R k .(25)Note that the semi-infinite constraint in (25)is equivalent to ξ1 TM − Q 12q 12qTq 0−βξ1≥0∀ξ∈R k ⇐⇒M − Q 12q 12qT q 0−β0,which enables us to rewrite the Worst-Case CVaR (24)as the optimal value ofinf β+1 ,Ms .t .M ∈S k +1,β∈RM 0,M − Q12q 12qTq 0−β0,which is indeed a tractable SDP.Remark If the loss function is concave but not piecewise affine,the Worst-Case CVaRcan sometimes still be evaluated efficiently,though not by solving an explicit SDP.Indeed,the Worst-Case CVaR can be computed in polynomial time with an ellipsoid method if L (ξ)is concave and if,for any ξ∈R k ,one can evaluate both L (ξ)as well as a super-gradient ∇ξL (ξ)in polynomial time.This is an immediate conse-quence of a result on the computation of worst-case expectations by Delage and Ye [11,Proposition 2].3Distributionally robust joint chance constraintsWe define the feasible set X JCC of the distributionally robust joint chance constraint (3)asXJCC = x ∈R n :inf P ∈PPy 0i (x )+y i (x )T ˜ξ≤0∀i =1,...,m ≥1− .The aim of this section is to investigate the structure of X JCC and to elaborate tractable conservative approximations.We first review two existing approximations and discuss their benefits and shortcomings.3.1The Bonferroni approximationA popular approximation for X JCC is based on Bonferroni’s inequality.Note that the robust joint chance constraint (3)is equivalent toinf P ∈PPm i =1y 0i (x )+y i (x )T ˜ξ≤0≥1−⇐⇒sup P ∈PPm i =1y 0i (x )+y i (x )T ˜ξ>0 ≤ .Furthermore,Bonferroni’s inequality implies thatPm i =1y 0i (x )+y i (x )T ˜ξ>0≤mi =1P y 0i (x )+y i (x )T ˜ξ>0 ∀P ∈P .。
2025届广东深圳罗湖外国语学校高三第三次模拟考试英语试卷含解析
2025届广东深圳罗湖外国语学校高三第三次模拟考试英语试卷考生须知:1.全卷分选择题和非选择题两部分,全部在答题纸上作答。
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第一部分(共20小题,每小题1.5分,满分30分)1._____ at the differences between her culture and theirs, Annie wanted to return home.A.Confusing B.ConfusedC.Having confused D.To confuse2.I shook hands and ________ greetings with the manager, who I impressed a lot.A.conveyed B.swapped C.exchanged D.switched3.Don’t worry. The ha rd work that you do now _____ later in life.A.will be repaid B.was being repaidC.has been repaid D.was repaid4.His advice made me happy, but ____others angry.A.making B.to make C./ D.make5.Some pre-school children go to a day care center, __________ they learn simple games and songs.A.then B.there C.while D.where6.Rent usually ________ up in the summer, when college graduates are moving out of their dormitories and seeking for new places to move in.A.will go B.goesC.has gone D.went7.Mary became ______ homesick and critical of the United States, so she fled from her home in West Bloomfield to her hometown in Austria.A.completely B.sincerelyC.approximately D.increasingly8.It was not until she got home____Jennifer realized she had lost her keys.A.when B.thatC.where D.before9.—Tom, do you enjoy your present job?—________. I just do it for a living.A.Of course B.Not reallyC.Not likely D.That’s all right10.The 90’s people seem to have enjoyed the great benefits ________ about by the great level of cultural andeconomic development.A.brought B.bringingC.to be brought D.having brought11.If you sleep less than seven hours, you are three times more to catch a cold.A.possible B.certainly C.probable D.likely12.---How’s your tour around the North Lake? Is it beautiful?---It ________ be, but it is now heavily polluted.A.will B.would C.should D.must13.________ an increase in foreign legal conflicts,China is expected to see the number continue to rise.A.To witness B.Being witnessedC.Witnessed D.Having witnessed14.Is this your cell phone, Tony? I ________ it when I was cleaning the classroom.A.came across B.dealt withC.looked after D.held on to15.I’m tired out.I stayed up the whole night, ______ for my midterm math exam.A.studying B.to study C.to be studying D.studied16.It’s nearly four years since I worked in that firm. I ________ a band with other fellows.A.operated B.had been operatingC.was operating D.am operating17.—Let’s go and have dinner this evening.—_____. Have you come out first in the exam?A.Thanks a lot. B.Why not?C.What for? D.Yes, I’d like to.18.The recently released film Kong:Skull Island successfully ________ the audience to the adventure with Dolby 3-D technology.A.transports B.adjustsC.transforms D.relates19.World Food Day is held each year to underline the progress that ________ against hunger and that still needs to be made.A.is made B.was madeC.has been made D.will be made20.---Kingsman: The Secret Service is a spy action comedy film. Wants to come with me?---I’d love to, but my best friend is getting married, and I won’t _______ it for anything.A.overlook B.trade C.miss D.forget第二部分阅读理解(满分40分)阅读下列短文,从每题所给的A、B、C、D四个选项中,选出最佳选项。
数学专业英语词汇(C)
数学专业英语词汇(C)c function c类函数c manifold c廖c mapping c类映射ca set 上解析集calculability 可计算性calculable mapping 可计算映射calculable relation 可计算关系calculate 计算calculating automaton 计算自动机calculating circuit 计算电路calculating element 计算单元calculating machine 计算机calculating punch 穿孔计算机calculating register 计算寄存器calculating unit 计算装置calculation 计算calculation of areas 面积计算calculator 计算机calculus 演算calculus of approximations 近似计算calculus of classes 类演算calculus of errors 误差论calculus of finite differences 差分法calculus of probability 概率calculus of residues 残数计算calculus of variations 变分法calibration 校准canal 管道canal surface 管道曲面cancel 消去cancellation 消去cancellation law 消去律cancellation property 消去性质cancelling of significant figures 有效数字消去canonical basis 典范基canonical coordinates 标准坐标canonical correlation coefficient 典型相关系数canonical decomposition 标准分解canonical distribution 典型分布canonical ensemble 正则总体canonical equation 典型方程canonical equation of motion 标准运动方程canonical expression 典范式canonical factorization 典范因子分解canonical flabby resolution 典型松弛分解canonical form 标准型canonical function 标准函数canonical fundamental system 标准基本系统canonical homomorphism 标准同态canonical hyperbolic system 典型双曲线系canonical image 标准象canonical mapping 标准映射canonical representation 典型表示canonical sequence 标准序列canonical solution 标准解canonical system of differential equations 标准微分方程组canonical variable 典型变量canonical variational equations 标准变分方程canonical variational problem 标准变分问题cantor curve 康托尔曲线cantor discontinum 康托尔密断统cantorian set theory 经典集论cap 交cap product 卡积capacity 容量card 卡片card punch 卡片穿孔机card reader 卡片读数器cardinal 知的cardinal number 基数cardinal product 基数积cardioid 心脏线carrier 支柱carry 进位carry signal 进位信号cartan decomposition 嘉当分解cartan formula 嘉当公式cartan subalgebra 嘉当子代数cartan subgroup 嘉当子群cartesian coordinate system 笛卡儿坐标系cartesian coordinates 笛卡尔座标cartesian equation 笛卡儿方程cartesian folium 笛卡儿叶形线cartesian product 笛卡儿积cartesian space 笛卡儿空间cartography 制图学cascaded carry 逐位进位casimir operator 卡巫尔算子cassini oval 卡吾卵形线casting out 舍去casting out nines 舍九法catastrophe theory 突变理论categorical judgment 范畴判断categorical proposition 范畴判断categorical syllogism 直言三段论categorical theory 范畴论categoricity 范畴性category 范畴category of groups 群范畴category of modules 模的范畴category of sets 集的范畴category of topological spaces 拓扑空间的范畴catenary 悬链线catenary curve 悬链线catenoid 悬链曲面cauchy condensation test 柯微项收敛检验法cauchy condition for convergence 柯握敛条件cauchy criterion 柯握敛判别准则cauchy distribution 柯沃布cauchy filter 柯嗡子cauchy inequality 柯位等式cauchy integral 柯锡分cauchy integral formula 柯锡分公式cauchy kernel 柯嗡cauchy kovalevskaya theorem 柯慰仆吡蟹蛩箍ǘɡ眵cauchy mean value formula 广义均值定理cauchy net 柯硒cauchy principal value 柯蔚cauchy problem 柯问题cauchy process 柯锡程cauchy residue theorem 残数定理cauchy sequence 柯悟列causal relation 因果关系causality 因果律cause 原因cavity 空腔cavity coefficient 空胴系数cayley number 凯莱数cayley sextic 凯莱六次线cayley transform 凯莱变换ccr algebra ccr代数celestial body 天体celestial coordinates 天体坐标celestial mechanics 天体力学cell 胞腔cell complex 多面复形cellular approximation 胞腔逼近cellular automaton 细胞自动机cellular cohomology 胞腔上同调cellular cohomology group 胞腔上同岛cellular decomposition 胞腔剖分cellular homotopy 胞腔式同伦cellular map 胞腔映射cellular subcomplex 胞腔子复形center 中心center of a circle 圆心center of curvature 曲率中心center of expansion 展开中心center of force 力心center of gravity 重心center of gyration 旋转中心center of inversion 反演中心center of mass 质心center of pressure 压力中心center of principal curvature 助率中心center of projection 射影中心center of symmetry 对称中心centered process 中心化过程centered system of sets 中心集系centi 厘centigram 厘克centimetre 厘米central angle 圆心角central confidence interval 中心置信区间central conic 有心圆锥曲线central derivative 中心导数central difference 中心差分central difference operator 中心差分算子central divided difference 中心均差central element 中心元central extension 中心扩张central extension field 中心扩张域central limit theorem 中心极限定理central line 中线central moment 中心矩central point 中心点central processing unit 中央处理器central projection 中心射影central quadric 有心二次曲面central series 中心群列central symmetric vector field 中心对称向量场central symmetry 中心对称centralizer 中心化子centre 中心centre of a circle 圆心centre of gyration 旋转中心centre of projection 射影中心centre of similarity 相似中心centre of similitude 相似中心centrifugal force 离心力centripetal acceleration 向心加速度centroid 形心certain event 必然事件certainty 必然cesaro mean 纬洛平均cesaro method of summation 纬洛总求法chain 链chain complex 链复形chain condition 链条件chain equivalence 链等价chain equivalent 链等价的chain group 链群chain homotopic 链同伦的chain homotopy 链同伦chain index 链指数chain map 链变换chain of prime ideals 素理想链chain of syzygies 合冲链chain rule 链式法则chain transformation 链变换chainette 悬链线chamber complex 箱盒复形chance 偶然性;偶然的chance event 随机事件chance move 随机步chance quantity 随机量chance variable 机会变量change 变化change of metrics 度量的变换change of the base 基的变换change of the variable 变量的更换channel 信道channel width 信道宽度character 符号character group 特贞群character space 特贞空间characteriatic system 特寨characteristic 特征characteristic boundary value problem 特者值问题characteristic class 示性类characteristic cone 特斩characteristic conoid 特沾体characteristic curve 特怔线characteristic derivation 特阵导characteristic determinant 特招列式characteristic differential equation 特闸分方程characteristic direction 特战向characteristic equation 特战程characteristic exponent 特崭数characteristic function 特寨数characteristic functional 特蘸函characteristic group 特蘸characteristic index 特崭标characteristic initial value problem 特挣值问题characteristic linear system 特者性系统characteristic manifold 特瘴characteristic matrix 特肇阵characteristic number 特正characteristic of a logarithm 对数的首数characteristic parameter 特瘴数characteristic polynomial 特锗项式characteristic pontrjagin number 庞德里雅金特正characteristic root 特争characteristic ruled surface 特毡纹曲面characteristic series 特招characteristic set 特寨characteristic state 特宅characteristic strip 特狰characteristic subgroup 特沼群characteristic surface 特怔面characteristic value 矩阵的特盏characteristic vector 特镇量charge 电荷chart 图chebyshev function 切比雪夫函数chebyshev inequality 切比雪夫不等式chebyshev polynomial 切比雪夫多项式check 校验check digit 检验位check routine 检验程序check sum 检查和chevalley group 歇互莱群chi square distribution 分布chi squared test 检验chi squared test of goodness of fit 拟合优度检验choice function 选择函数chord 弦chord line 弦chord of contact 切弦chord of curvature 曲率弦chordal distance 弦距离christoffel symbol 克里斯托弗尔符号chromatic number 色数chromatic polynomial 色多项式cipher 数字circle 圆circle diagram 圆图circle method 圆法circle of contact 切圆circle of convergence 收敛圆circle of curvature 曲率圆circle of inversion 反演圆circle problem 圆内格点问题circuit free graph 环道自由图circuit rank 圈数circulant 循环行列式circulant matrix 轮换矩阵circular 圆的circular arc 圆弧circular cone 圆锥circular correlation 循环相关circular cylinder 圆柱circular disk 圆盘circular domain 圆形域circular frequency 角频率circular functions 圆函数circular helix 圆柱螺旋线circular measure 弧度circular motion 圆运动circular neighborhood 圆邻域circular orbit 圆轨道circular pendulum 圆摆circular permutation 循环排列circular ring 圆环circular section 圆截面circular sector 圆扇形circular segment 圆弓形circular slit domain 圆形裂纹域circular symmetry 圆对称circular transformation 圆变换circulation 循环circulation index 环粮数circulation of vector field 向量场的循环circulatory integral 围道积分circumcenter 外心circumcentre 外心circumcircle 外接圆circumcone 外切圆锥circumference 圆周circumscribe 外接circumscribed circle 外接圆circumscribed figure 外切形circumscribed polygon 外切多边形circumscribed quadrilateral 外切四边形circumscribed triangle 外切三角形circumsphere 外接球cissoid 蔓叶类曲线cissoidal curve 蔓叶类曲线cissoidal function 蔓叶类函数clairaut equation 克莱罗方程class 类class bound 组界class field 类域class field tower 类域塔class frequency 组频率class function 类函数class interval 组距class mean 组平均class number 类数class of conjugate elements 共轭元素类classical groups 典型群classical lie algebras 典型李代数classical mechanics 经典力学classical sentential calculus 经典语句演算classical set theory 经典集论classical statistical mechanics 经典统计力学classical theory of probability 经典概率论classification 分类classification statistic 分类统计classification theorem 分类定理classify 分类classifying map 分类映射classifying space 分类空间clear 擦去clifford group 克里福特群clifford number 克里福特数clockwise 顺时针的clockwise direction 顺时针方向clockwise rotation 顺时针旋转clopen set 闭开集closable linear operator 可闭线性算子closable operator 可闭算子closed ball 闭球closed circuit 闭合电路closed complex 闭复形closed convex curve 卵形线closed convex hull 闭凸包closed cover 闭覆盖closed curve 闭曲线closed disk 闭圆盘closed domain 闭域closed equivalence relation 闭等价关系closed extension 闭扩张closed filter 闭滤子closed form 闭型closed formula 闭公式closed geodesic 闭测地线closed graph 闭图closed graph theorem 闭图定理closed group 闭群closed half plane 闭半平面closed half space 闭半空间closed hull 闭包closed interval 闭区间closed kernel 闭核closed linear manifold 闭线性廖closed loop system 闭圈系closed manifold 闭廖closed map 闭映射closed neighborhood 闭邻域closed number plane 闭实数平面closed path 闭路closed range theorem 闭值域定理closed region 闭域closed riemann surface 闭黎曼面closed set 闭集closed shell 闭壳层closed simplex 闭单形closed solid sphere 闭实心球closed sphere 闭球closed star 闭星形closed subgroup 闭子群closed subroutine 闭型子程序closed surface 闭曲面closed symmetric extension 闭对称扩张closed system 闭系统closed term 闭项closeness 附近closure 闭包closure operation 闭包运算closure operator 闭包算子closure property 闭包性质clothoid 回旋曲线cluster point 聚点cluster sampling 分组抽样cluster set 聚值集coadjoint functor 余伴随函子coalgebra 上代数coalition 联合coanalytic set 上解析集coarser partition 较粗划分coaxial circles 共轴圆cobase 共基cobordant manifolds 配边廖cobordism 配边cobordism class 配边类cobordism group 配边群cobordism ring 配边环coboundary 上边缘coboundary homomorphism 上边缘同态coboundary operator 上边缘算子cocategory 上范畴cochain 上链cochain complex 上链复形cochain homotopy 上链同伦cochain map 上链映射cocircuit 上环道cocommutative 上交换的cocomplete category 上完全范畴cocycle 上闭键code 代吗coded decimal notation 二进制编的十进制记数法codenumerable set 余可数集coder 编器codiagonal morphism 余对角射codifferential 上微分codimension 余维数coding 编码coding theorem 编码定理coding theory 编码理论codomain 上域coefficient 系数coefficient domain 系数域coefficient function 系数函数coefficient functional 系数泛函coefficient group 系数群coefficient of alienation 不相关系数coefficient of association 相伴系数coefficient of covariation 共变系数coefficient of cubical expansion 体积膨胀系数coefficient of determination 可决系数coefficient of diffusion 扩散系数coefficient of excess 超出系数coefficient of friction 摩擦系数coefficient of nondetermination 不可决系数coefficient of rank correlation 等级相关系数coefficient of regression 回归系数coefficient of the expansion 展开系数coefficient of thermal expansion 热膨胀系数coefficient of variation 变差系数coefficient of viscosity 粘性系数coefficient problem 系数问题coefficient ring 系数环coercive operator 强制算子cofactor 代数余子式cofiber 上纤维cofibering 上纤维化cofibration 上纤维化cofilter 余滤子cofinal set 共尾集cofinal subset 共尾子集cofinality 共尾性cofinite subset 上有限子集cofunction 余函数cogenerator 上生成元cogredient automorphism 内自同构coherence 凝聚coherence condition 凝聚条件coherent module 凝聚摸coherent ring 凝聚环coherent set 凝聚集coherent sheaf 凝聚层coherent stack 凝聚层coherent topology 凝聚拓扑coherently oriented simplex 协同定向单形cohomological dimension 上同惮数cohomological invariant 上同祷变量cohomology 上同调cohomology algebra 上同碟数cohomology class 上同掂cohomology functor 上同弹子cohomology group 上同岛cohomology group with coefficients g 有系数g的上同岛cohomology module 上同担cohomology operation 上同邓算cohomology ring 上同捣cohomology sequence 上同凋列cohomology spectral sequence 上同底序列cohomology theory 上同帝cohomotopy 上同伦cohomotopy group 上同伦群coideal 上理想coimage 余象coincidence 一致coincidence number 叠合数coincidence point 叠合点coincident 重合的coinduced topology 余导出拓扑cokernel 上核collect 收集collectionwise normal space 成集体正规空间collective 集体collinear diagram 列线图collinear points 共线点collinear vectors 共线向量collinearity 共线性collineation 直射变换collineation group 直射群collineatory transformation 直射变换collocation method 配置法collocation of boundary 边界配置collocation point 配置点colocally small category 上局部小范畴cologarithm 余对数colorable 可着色的column 列column finite matrix 列有限矩阵column matrix 列阵column rank 列秩column space 列空间column vector 列向量combination 组合combination principle 结合原理combination with repetitions 有复组合combination without repetition 无复组合combinatorial analysis 组合分析combinatorial closure 组合闭包combinatorial dimension 组合维数combinatorial geometry 组合几何学combinatorial manifold 组合廖combinatorial method 组合方法combinatorial optimization problem 组合最优化问题combinatorial path 组合道路combinatorial problem 组合最优化问题combinatorial sphere 组合球面combinatorial sum 组合和combinatorial theory of probabilities 概率组合理论combinatorial topology 组合拓朴学combinatorially equivalent complex 组合等价复形combinatories 组合分析combinatory logic 组合逻辑combinatory topology 组合拓朴学combined matrix 组合矩阵comma 逗点command 命令commensurability 可通约性commensurable 可通约的commensurable quantities 可公度量common denominator 公分母common difference 公差common divisor 公约数common factor 公因子common factor theory 公因子论common fraction 普通分数common logarithm 常用对数common measure 公测度common multiple 公倍元common perpendicular 公有垂线common point 公共点common ratio 公比common tangent of two circles 二圆公切线communality 公因子方差communication channel 通讯通道commutant 换位commutation law 交换律commutation relation 交换关系commutative 可换的commutative diagram 交换图表commutative group 交换群commutative groupoid 阿贝耳广群commutative law 交换律commutative lie ring 交换李环commutative ordinal numbers 交换序数commutative ring 交换环commutativity 交换性commutator 换位子commutator group 换位子群commute 交换compact 紧的compact convergence 紧收敛compact group 紧群compact open topology 紧收敛拓扑compact operator 紧算子compact set 紧集compact space 紧空间compact subgroup 紧子群compact support 紧支柱compactification 紧化compactification theorem 紧化定理compactness 紧性compactness theorem 紧性定理compactum 紧统comparability of cardinals 基数的可比较性comparable curve 可比曲线comparable function 可比的函数comparable topology 可比拓扑comparable uniformity 可比一致性comparison function 比较函数comparison method 比较法comparison series 比较用级数comparison test 比较检验comparison theorem 比较定理compass 两脚规compatibile condition 相容性条件compatibility 一致性compatibility condition 相容性条件compatible system of algebraic equations 相容代数方程组compatible topology 相容拓扑学compensate 补偿compensating method 补偿法compensation 补偿compensation of error 误差的补偿compiler 编译程序compiling routine 编译程序complanar line 共面线complele induction 数学归纳法complement 补集complement of an angle 余角complementary 补的complementary angle 余角complementary degree 余次数complementary divisor 余因子complementary event 余事件complementary function 余函数complementary graph 余图complementary ideal 余理想complementary laws 补余律complementary module 补模complementary modulus 补模数complementary set 补集complementary space 补空间complementary submodules 补子模complementary subset 余子集complementary subspace 补子空间complemented lattice 有补格complete abelian variety 完备阿贝耳簇complete accumulation point 完全聚点complete axiom system 完备公理系统complete category 完全范畴complete class 完备类complete continuity 完全连续性complete disjunction 完全析取complete elliptic integral 完全椭圆积分complete field 完全域complete field of sets 集的完全域complete graph 完全图complete group 完全群complete group variety 完备群簇complete homomorphism 完全同态complete induction 数学归纳法complete integral 完全积分complete intersection 完全交叉complete lattice 完全格complete linear system 完备线性系统complete local ring 完全局部环complete measure 完全测度complete measure space 完备测度空间complete metric space 完备度量空间complete normality axiom 完全正规性公理complete ordered field 全序域complete orthogonal sequence 完全正交序列complete orthogonal set 完全正交系complete orthogonal system 完全正交系complete orthonormal sequence 完备标准正交序列complete orthonormal system 完备标准正交系complete probability space 完全概率空间complete quadrangle 完全四点形complete quadrilateral 完全四边形complete reducibility theorem 完全可约性定理complete regularity separation axiom 完全正则性分离公理complete reinhardt domain 完全赖因哈耳特域complete set 完全集complete solution 完全积分complete space 完备空间complete subcategory 完全子范畴complete system 完备系complete system of functions 函数完备系complete system of fundamental sequences 完全基本序列系complete system of invariants 完全的不变量系complete tensor product 完全张量积completed shell 闭壳层completely additive 完全加性的completely additive family of sets 完全加性集族completely additive measure 完全加性测度completely compact set 完全紧集completely continuous function 完全连续函数completely continuous linear operator 完全连续线性算子completely continuous mapping 全连续映射completely continuous operator 全连续映射completely distributive lattice 完全分配格completely homologous maps 完全同党射completely independent system of axioms 完全独立公理系统completely integrable 完全可积的completely integrable system 完全可积组completely integrally closed 完全整闭的completely mixed game 完全混合对策completely monotone 完全单的completely monotonic function 完全单弹数completely monotonic sequence 完全单凋列completely multiplicative 完全积性的completely multiplicative function 完全积性函数completely primary ring 完全准素环completely reducible 完全可约的completely reducible group 完全可约群completely regular filter 完全正则滤子completely regular space 完全正则空间completely regular topology 完全正则拓扑completely separated sets 完全可离集completely specified automaton 完全自动机completely splitted prime ideal 完全分裂素理想completely transitive group 全可迁群completeness 完全性completeness theorem 完全性定理completion 完备化complex 复形complex analytic fiber bundle 复解析纤维丛complex analytic manifold 复解析廖complex analytic structure 复解析结构complex cone 线丛的锥面complex conjugate 复共轭的complex conjugate matrix 复共轭阵complex curve 复曲线complex curvelinear integral 复曲线积分complex domain 复域complex experiment 析因实验complex field 复数域complex flnction 复值函数complex fraction 繁分数complex group 辛群complex line 复线complex line bundle 复线丛complex manifold 复廖complex multiplication 复数乘法complex number 复数complex number plane 复数平面complex plane with cut 有割的复平面complex quantity 复量complex root 复根complex series 复级数complex sphere 复球面complex surface 线丛的曲面complex unit 单位复数complex valued function 复值函数complex variable 复变量complex vector bundle 复向量丛complex velocity potential 复速度位势complexity 复杂性complication 复杂化component 分量component of variance 方差的分量componentwise convergence 分量方式收敛composable 组成的compose 组成composite 合成composite divisor 合成除数composite function 合成函数composite functor 合成函子composite group 合成群composite hypothesis 复合假设composite number 合成数composite probability 复合概率composition 合成composition algebra 合成代数composition factor 合成因子composition homomorphism 合成同态composition of vector subspaces 向量子空间的合成composition operator 合成算子composition series 合成列compound determinant 复合行列式compound event 复合事件compound function 合成函数compound number 合成数compound probability 合成概率compound proportion 复比例compound rule 复合规则computable function 可计算函数computation 计算computational error 计算误差computational formula 计算公式computational mistake 计算误差compute 计算computer 计算机computing center 计算中心computing element 计算单元computing machine 计算机computing time 计算时间comultiplication 上乘法concave 凹的concave angle 凹角concave convex game 凹凸对策concave curve 凹曲线concave function 凹函数concave polygon 凹多边形concavity 凹性concavo convex 凹凸的concentration 集中;浓度concentration ellipse 同心椭圆concentric circles 同心圆concept 概念conchoid 蚌线conchoidal 蚌线的conclusion 结论concomitant variable 相伴变量concrete number 名数concurrent form 共点形式concurrent planes 共点面concyclic points 共圆点condensation of singularities 奇点的凝聚condensation point 凝聚点condensation principle 凝聚原理condition equation 条件方程condition for continuity 连续性条件condition number 条件数condition of connectedness 连通性条件condition of positivity 正值性条件conditional convergence 条件收敛conditional definition 条件定义conditional density 条件性密度conditional distribution 条件分布conditional entropy 条件熵conditional equation 条件方程conditional event 条件性事件conditional gradient method 条件梯度法conditional inequality 条件不等式conditional instability 条件不稳定conditional instruction 条件指令conditional jump 条件转移conditional mathematical expectation 条件数学期望conditional probability 条件概率conditional probability measure 条件概率测度conditional proposition 条件命题conditional sentence 条件命题conditional stability 条件稳定性conditional transfer of control 条件转移conditionally compact set 条件紧集conditionally complete 条件完备的conditionally convergent 条件收敛的conditionally convergent series 条件收敛级数conditionally well posed problems 条件适定的问题conditioned observation 条件观测conditioning number 条件数conditions of similarity 相似条件conduction 传导conductivity 传导率conductor 导体;前导子conductor ramification theorem 前导子分歧定理cone 锥cone of a complex 复形锥面cone of a simplex 单形锥面confidence belt 置信带confidence coefficient 置信系数confidence ellipse 置信椭圆confidence ellipsoid 置信椭面confidence interval 置信区间confidence level 置信水平confidence limit 置信界限confidence region 置信区域configuration 布局configuration space 构形空间confinal 共尾的confinality 共尾性confirmation 证实confluent divided difference 合六差confluent hypergeometric equation 合镣超几何微分方程confluent hypergeometric function 合连几何函数confluent hypergeometric series 合连几何级数confluent interpolation polynomial 汇合内插多项式confocal conic sections 共焦二次曲线confocal conics 共焦二次曲线confocal quadrics 共焦二次曲面conformable matrices 可相乘阵conformal 保角的conformal curvature tensor 保形曲率张量conformal differential geometry 保形微分几何学conformal geometry 保形几何conformal mapping 保角素示conformal projection 保形射影conformal representation 保角素示conformal transformation 保角映射conformally connected manifold 保形连通廖conformally geodesic lines 保形测地线confounding 混杂confrontation 比较confusion 混乱congruence 同余式congruence group 同余群congruence method 同余法congruence of lines 线汇congruence relation 同余关系congruence subgroup 同余子群congruence zeta function 同余函数congruent 同余的congruent mapping 合同映射congruent number 同余数congruent transformation 合同映射conic 圆锥曲线conic function 圆锥函数conic section 圆锥曲线conical helix 圆锥螺旋线conical surface 锥面conics 圆锥曲线论conjugate 共轭的conjugate axis 共轭轴conjugate class 共轭类conjugate complex 共轭复形conjugate complex number 共轭复数conjugate convex function 共轭凸函数conjugate curve 共轭曲线conjugate curve of the second order 共轭二次曲线conjugate diameter 共轭直径conjugate direction 共轭方向conjugate dyad 共轭并向量conjugate element 共轭元素conjugate exponent 共轭指数conjugate field 共轭域conjugate foci 共轭焦点conjugate function 共轭函数conjugate gradient method 共轭梯度法conjugate hyperbola 共轭双曲线conjugate latin square 共轭拉丁平conjugate line 共轭直线conjugate number 共轭数conjugate operator 共轭算子conjugate points 共轭点conjugate quaternion 共轭四元数conjugate root 共轭根conjugate ruled surface 共轭直纹曲面conjugate series 共轭级数conjugate space 共轭空间conjugate transformation 共轭变换conjugate vector 共轭向量conjugation map 共轭映射conjugation operator 共轭算子conjunction 合取conjunctive normal form 合取范式connected 连通的connected asymptotic paths 连通渐近路线connected automaton 连通自动机connected category 连通范畴connected chain 连通链connected complex 连通复形connected component 连通分支connected curve 连通曲线connected domain 连通域connected graph 连通图connected group 连通群connected sequence of functors 函子的连通序列connected set 连通集connected space 连通空间connected sum 连通和connectedness 连通性connecting homomorphism 连通同态connecting morphism 连通同态connecting path 连接道路connection 联络connection component 连通分量connectivity 连通性connex 连通conoid 劈锥曲面conormal 余法线conormal image 余法线象conrol chart technique 控制图法consequence 后承consequent 后项conservation law 守恒律conservation of angular momentum 角动量守恒conservation of energy 能量守恒conservation of mass 质量守恒conservation of momentum 动量守恒conservative extension 守恒扩张conservative field of force 保守力场conservative force 保守力conservative measurable transformation 守恒可测变换conservative vector field 守恒向量场consistency 相容性consistency conditions 相容条件consistency of equations 方程组的相容性consistency problem 相容性问题consistencyproof 相容性的证明consistent axiom system 相容性公理系consistent equations 相容方程组consistent estimator 相容估计consistent system of equations 相容方程组consistent test 相容检验constancy of sign 符号恒性constant 常数constant coefficient 常系数constant field 常数域constant function 常值函数constant mapping 常值映射constant of integration 积分常数constant of proportionality 比例系数constant of structure 构造常数constant pressure chart 等压面图constant pressure surface 等压面constant sheaf 常数层constant sum game 常和对策constant term 常数项constant value 定值constituent 组分constitutional diagram 组分图constrained game 约束对策constrained maximization 约束最大化constrained minimization 约束最小化constrained optimization 约束最优化constraint 约束construct 准constructibility 可构成性constructible 可构成的constructible map 可构成映射constructible set 可构成集construction 构成construction problem 准题constructive dilemma 构造二难推论constructive existence proof 可构造存在证明constructive mathematics 可构造数学constructive ordinal number 可构造序数consumer's risk 用户风险contact 接触contact angle 接触角contact point 接触点contact surface 接触面contact transformation 切变换content 含量context sensitive grammar 上下文有关文法contiguity 接触contiguous confluent hypergeometric function 连接合连几何函数contiguous hypergeometric function 连接超几何函数contiguous map 连接映射contingency 随机性contingency table 列contingent 偶然事故continuability 可延拓性continuation method 连续法continued equality 连等式continued fraction 连分数continued fraction expansion 连分式展开式continued proportion 连比例continuity 连续性continuity axiom 连续性公理continuity condition 连续性条件continuity equation 连续方程continuity in the mean 均方连续性continuity interval 连续区间continuity method 连续法continuity of function 函数的连续性continuity on both sides 双边连续性continuity on the left 左连续性continuity on the right 右连续性continuity principle 连续性原理continuity theorem 连续性定理continuous 连续的continuous analyzer 连续分析器continuous approximation 连续近似continuous curve 连续曲线continuous differentiability 连续可微性continuous distribution 连续分布continuous distribution function 连续分布函数continuous dynamical system 连续动力系统continuous function 连续函数continuous function in the mean 均方连续函数continuous game 连续对策continuous geometry 连续几何continuous group 拓扑群continuous homology 连续同调continuous homology group 连续同岛continuous image 连续象continuous in x 依x连续的continuous limit 连续极限continuous map 连续映射continuous on the left 左方连续的continuous operator 连续算子continuous ordered set 连续有序集continuous part 连续部分continuous random process 连续随机过程continuous random variable 连续随机变量continuous ruin problem 连续破产问题。
考研数学中柯西中值定理的应用
考研数学中柯西中值定理的应用The Cauchy Mean Value Theorem is a fundamental concept in the field of mathematics, especially in the study of calculus. It states that if a function is continuous on a closed interval and differentiable on the open interval, then there exists at least one point in the interval where the derivative of the function is equal to the average rate of change of the function over the interval. This theorem is widely used in various branches of mathematics, including optimization, physics, and engineering.柯西中值定理是数学领域的一个基本概念,特别在微积分的研究中。
它指出,如果一个函数在一个闭区间上连续,并且在一个开区间上可微分,那么在这个区间内至少存在一个点,这个点的导数等于函数在该区间上的平均变化率。
这个定理在数学的各个分支中被广泛应用,包括优化、物理学和工程学。
One of the key applications of the Cauchy Mean Value Theorem is in the field of optimization. When trying to find the maximum or minimum values of a function, the theorem can be used to show the existence of critical points where the derivative of the function is zero or undefined. By identifying these points, mathematicians cananalyze the behavior of the function and determine its extreme values.柯西中值定理的一个关键应用领域是在优化领域。
柯西积分定理与柯西积分公式的由来及其应用
柯西积分定理与柯西积分公式的由来及其应⽤( 2012 届)本科毕业论⽂(设计)题⽬:柯西积分定理与柯西积分公式的由来及其应⽤学院:教师教育学院专业:数学与应⽤数学(师范)班级:数学082学号:姓名:指导教师:完成⽇期:教务处制诚信声明我声明,所呈交的论⽂(设计)是本⼈在⽼师指导下进⾏的研究⼯作及取得的研究成果。
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论⽂(设计)作者签名:签名⽇期:年⽉⽇柯西积分定理与柯西积分公式的由来及其应⽤王莉莉(嘉兴学院数学与信息⼯程学院)摘要:复变函数是综合性⼤学或师院类院校理⼯专业的必修课,是实变函数微积分的推⼴和发展.其中柯西积分定理和柯西积分公式是复变函数理论的基础,是研究复变函数理论的关键.它的核⼼内容是柯西积分定理,即解析函数沿围线的积分值为零.本⽂研究了柯西积分定理和柯西积分公式的相关概念、证明、推⼴及在代数基本定理证明、实积分计算中的应⽤,论述了柯西积分定理与复变函数的积分有着密切的联系,利⽤柯西积分定理很容易导出著名的柯西积分公式,还对留数定理作了简要介绍,利⽤留数定理可以分别得到复变函数中的柯西积分定理、柯西积分公式和⾼阶导数公式.关键词:复变函数;柯西积分定理;柯西积分公式;留数定理Cauchy Integral Theorem and Cauchy Integral Formulas ofthe Origin and its ApplicationWanglili(College of Mathematics and Information Engineering , Jiaxing University)Abstract:Complex-variable function is a comprehensive university or institute of technology of normal colleges and universities professional required courses. It is real veriables function of the promotion and development of calculus. One cauchy integral theorem and cauchy integral formula is a complex function theory foundation. It is the key of sresearching complex function theory. One of its important contents is the cauchy integral theorem, which says that the integral along a contour of an analytic function is zero. This paper studies the cauchy integral theorem and cauchy integral formula related concepts and prove, promotion and in algebra fundamental theorem of integral proof, in the calculation of the application. It discusses the closely related of the cauchy integral theorem and cauchy complex functions. The famous cauchy integral formula can follows easily from the cauchy integral theorem. Also residue theorem are briefly introduced. Use of residue theorem can get the complex functions respectively cauchy integral theorem and cauchy integral formulas and high derivatives formula.Key words:Complex-variable function;cauchy integral theorem;cauchy integral formula;residue theorem⽬录1 绪论 (1)1.1 研究背景 (1)1.1.1 复变函数概况 (1)1.1.2 复积分的定义 (2)1.1.3 柯西积分定理的引⼊ (3)1.2 本⽂的研究⼯作 (4)1.3 本⽂的未来⼯作 (4)2 柯西积分定理 (5)2.1 柯西积分定理 (5)2.2 柯西积分定理的证明 (5)2.3 柯西积分定理的推⼴ (6)2.4 柯西积分定理的应⽤ (9)3 柯西积分公式 (12)3.1 柯西积分公式 (12)3.2 柯西积分公式的证明 (12)3.3 柯西积分公式的推⼴ (13)3.4 柯西积分公式的应⽤ (14)4 复变函数积分之间的关系 (18)4.1 柯西积分定理与柯西积分公式的关系 (18)4.2 复变函数积分与留数定理的关系 (19)参考⽂献 (22)1 绪论1.1 研究背景在18世纪后半叶到19世纪初,开始了复函数的偏导数与积分性质的探索.复分析真正作为现代分析的⼀个研究领域是在19世纪建⽴起来的,主要奠基⼈:柯西、黎曼和魏尔斯特拉斯.柯西建⽴了复变函数的微分和积分理论.1814年、1825年的论⽂《关于积分限为虚数的定积分的报告》建⽴了柯西积分定理,1826年提出留数概念,1831年获得柯西积分公式,1846年发现积分与路径⽆关定理[3].1.1.1 复变函数概况复数的概念起源于求⽅程的根,在⼆次、三次代数⽅程的求根中就出现了负数开平⽅的情况.在很长时间⾥,⼈们对这类数不能理解.但随着数学的发展,这类数的重要性就⽇益显a ,其中i是虚数单位.以复数作为⾃变量的函数就叫做复现出来.复数的⼀般形式是:bi变函数,⽽与之相关的理论就是复变函数论.解析函数是复变函数中⼀类具有解析性质的函数,复变函数论主要就是研究复数域上的解析函数,因此通常也称复变函数论为解析函数论.复变函数论的全⾯发展是在⼗九世纪,就像微积分的直接扩展统治了⼗⼋世纪的数学那样,复变函数这个新的分⽀统治了⼗九世纪的数学.当时的数学家公认复变函数论是最丰饶的数学分⽀,并且称为这个世纪的数学享受,也有⼈称赞它是抽象科学中最和谐的理论之⼀.复变函数中的许多概念、理论和⽅法是实变函数在复数领域内的推⼴和发展,因⽽它们之间有着许多的相似之处.但是,复变函数⼜有与实变函数不同之点,它是数学分析在研究领域的扩展.在我们学习中,要勤于思考,善于⽐较,既要注意共同点,更要弄清不同点.这样,才能抓住本质,融会贯通.复变函数论主要包括单值解析函数理论、黎曼曲⾯理论、⼏何函数论、留数理论、⼴义解析函数等⽅⾯的内容.如果当函数的变量取某⼀定值的时候,函数就有⼀个唯⼀确定的值,那么这个函数解就叫做单值解析函数,多项式就是这样的函数.复变函数研究多值函数,黎曼曲⾯理论是研究多值函数的主要⼯具.由许多层⾯安放在⼀起⽽构成的⼀种曲⾯叫做黎曼曲⾯.利⽤这种曲⾯,可以使多值函数的单值枝和⽀点概念在⼏何上有⾮常直观的表⽰和说明.对于某⼀个多值函数,如果能作出它的黎曼曲⾯,那么,函数在黎曼曲⾯上就变成单值函数.黎曼曲⾯理论是复变函数论和⼏何间的⼀座桥梁,能够使我们把⽐较深奥的函数的解析性质和⼏何性质联系起来.近来,关于黎曼曲⾯的研究还对另⼀门数学分⽀拓扑学产⽣了⽐较⼤的影响,逐渐地趋向于讨论它的拓扑性质.复变函数论中⽤⼏何⽅法来说明、解决问题的内容,⼀般叫做⼏何函数论,复变函数可以通过共形映像理论为它的性质提供⼏何说明.导数处处不是零的解析函数所实现的映像都都是共形映像,共形映像也叫做保⾓变换.共形映像在流体⼒学、空⽓动⼒学、弹性理论、静电场理论等⽅⾯都得到了⼴泛的应⽤.留数理论是复变函数论中⼀个重要的理论.留数也叫做残数,它的定义⽐较复杂.应⽤留数理论对于复变函数积分的计算⽐起线积分计算⽅便.计算实变函数定积分,可以化为复变函数沿闭回路曲线的积分后,再⽤留数基本定理化为被积分函数在闭合回路曲线内部孤⽴奇点上求留数的计算,当奇点是极点的时候,计算更加简洁.把单值解析函数的⼀些条件适当地改变和补充,以满⾜实际研究⼯作的需要,这种经过改变的解析函数叫做⼴义解析函数.⼴义解析函数所代表的⼏何图形的变化叫做拟保⾓变换。
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Cauchy’s Theorem and Edge Lengths of ConvexPolyhedraTherese Biedl,Anna Lubiw,and Michael SpriggsUniversity of Waterloo,Waterloo,ON,N2L3G1,Canada,{alubiw}{biedl}{mjspriggs}@Abstract.In this paper we explore,from an algorithmic point of view,the extent to which the facial angles and combinatorial structure of aconvex polyhedron determine the polyhedron—in particular the edgelengths and dihedral angles of the polyhedron.Cauchy’s rigidity theo-rem of1813states that the dihedral angles are uniquely determined.Finding them is a significant algorithmic problem which we express asa spherical graph drawing problem.Our main result is that the edgelengths,although not uniquely determined,can be found via linear pro-gramming.We make use of significant mathematics on convex polyhedraby Stoker,Van Heijenoort,Gale,and Shepherd.1IntroductionCauchy proved that convex polyhedra are rigid in the sense that if the faces were metal plates,and the edges were hinges,noflexing would be possible.Although most presentations(e.g.see[6,1])don’t point this out,Cauchy actually proved a stronger result:that the dihedral angles of a convex polyhedron are completely determined by the facial angles and the combinatorial structure(the list of faces, edges,vertices,and their containments).In other words,Cauchy’s proof makes no use of the edge lengths.See[26]or[3]for presentations where this is explicit.In this paper we examine the relationships among these four attributes of convex polyhedra:the facial angles and combinatorial structure,which we con-sider as givens;and the dihedral angles and the edge lengths,which we consider as unknowns.Dihedral angles are uniquely determined,by Cauchy’s Theorem; edge lengths are not,as the family of boxes demonstrates.This paper addresses the question:Are there efficient algorithms tofind dihedral angles/edge lengths for given facial angles and combinatorial structure?Our main result is an algorithm for the case of edge lengths(see Section4). We give a linear system expressing the edge lengths in terms of facial angles and combinatorial structure.Correctness depends on a new characterization(in Section3)of the edge lengths,facial angles,and dihedral angles of convex poly-hedra.This is related to recent work on“local”or“easily checkable”conditions for convex polyhedra[17,10,20].It is a major open question to devise an efficient algorithm tofind the dihedral angles corresponding to given facial angles and combinatorial structure—i.e.todevise an algorithm for Cauchy’s theorem.It is usually assumed that edge lengths are given as well.Such an algorithm can be used tofind the unique polyhedron formed by“folding up”a surface satisfying Alexandrov’s conditions[3].(See[9] for further explanation.)In1998Sabitov([21],or see the sketch in[9])gave a finite algorithm for Cauchy’s theorem.His algorithm uses the edge lengths heav-ily and crucially,and involves trying out all roots of the“volume polynomial”. The algorithm takes an exponential number of steps,where solving a high-degree polynomial is counted as one step.Recently Bobenko and Izmestiev([5],see also [19])gave an algorithm for the more general Alexandrov’s problem that,although it is not polynomial time,is effective in practice and has been implemented.As noted,both these algorithms assume edge lengths are given—an assump-tion that Cauchy did not make.Our workfills in this gap:it is possible to compute edge lengths from facial angles and combinatorial structure and then proceed with these algorithms.The present work falls under the general topic of reconstructing polyhedra. For other results and open problems in this area see[14,8,15].We assume standard definitions about convex polyhedra and graphs,see e.g.[6].By the“combinatorial structure”of a convex polyhedron we mean the list of faces,edges,and vertices and their containments.Equivalently,the com-binatorial structure is a3-connected planar graph,from which we can uniquely determine a combinatorial embedding,i.e.a cyclic list of the edges around each vertex that can be used to draw the graph in the plane without edge crossings. 2The Spherical DualIn this section we describe the spherical dual of a convex polyhedron,which we will use in the next section for our characterization of the edge lengths,facial angles,and dihedral angles of convex polyhedra.In a1968paper Stoker[26]gave some generalizations of Cauchy’s rigidity theorem.He pointed out explicitly that Cauchy’s proof does not use edge lengths, and transformed Cauchy’s problem in a way that abolishes edge lengths.This transformation is known as the spherical dual or“Gauss map”(see,e.g.[2]).Given a convex polyhedron P,map it to the unit sphere as follows.Translate the sphere so that the origin is an interior point.Consider any point p on the unit sphere as a vector.Because the origin is inside the polyhedron,this vector p is the outward normal to a unique supporting planeπp of the bel the point p on the sphere according to the vertex/edge/face of the polyhedron that lies in the planeπp.Thus each face f of P,having a single supporting plane,maps to a single point s(f)on the sphere.Each edge e of P has a one-dimensional space of supporting planes and maps to a geodesic arc s(e);if f and g are the two faces on either side of e,s(e)is the shorter arc of the great circle though s(f)and s(g).Each vertex v of P maps to a convex spherical polygon bounded by the arcs corresponding to the edges incident to v.See Figure1.Let G be the skeleton graph of the polyhedron P.Mapping P to the sphere produces an embedded graph s(G)with vertices{s(f):f a face of P},and edgesFig.1.The Gauss map and the correspondence of facial angles,β=π−α.{s(e):e an edge of P}and the cyclic order of edges around vertices induced by the order of edges around faces in G.Clearly s(G)is the dual graph of G.We now consider what the Gauss map does to facial and dihedral angles.Let e and e′be two incident edges of a face f of P.Letαbe the facial angle between them.Letβbe the angle between s(e)and s(e′)at the point s(f).Then,as Stoker[26]shows,βandαare supplementary angles,i.e.β=π−α.Let f and g be two faces of P joined at edge e.Letγbe the dihedral angle between f and g,and letδbe the length of the arc s(e)(measured in radians as an angle from the origin).Thenγandδare supplementary angles[26].In our situation,we know the embedded graph G and the facial angles. Applying the Gauss map,we know the embedded graph s(G)and its facial angles.Dihedral angles of the original map to edge lengths in the spherical dual,and Cauchy’s theorem says that these edge lengths are unique.Under this transformation the algorithmic form of Cauchy’s theorem becomes:Given an embedded3-connected planar graph and an angle between each consecutive pair of edges incident on a vertex,find a drawing of the graph on the sphere with non-crossing geodesic arcs for the edges,and with the specified angles.Supplements of arc lengths in the drawing provide the dihedral angles for the original problem.No efficient algorithm is known for this problem,but it is connected to quite a body of work in graph drawing.The problem of drawing a graph in the plane with specified angles wasfirst considered by Vijayan[27]and later proved NP-hard by Garg[12].Drawing on the sphere might be harder,but all our angles are convex, which should be easier.See also[4]and[23]for the case of triangulated graphs. Spherical drawing of triangulated graphs has been addressed in the graphics community in the context of spherical parameterization,see in particular[24].A closely related problem is to efficiently represent a3-connected planar graph as the skeleton graph of a convex polyhedron[7].3Conditions for Existence of a Convex PolyhedronIn this section we give conditions on the edge lengths,facial angles,and dihedral angles that are necessary and sufficient for the existence of a convex polyhedron. In some sense this is solved by the“local”or“easily checkable”conditions for convex polyhedra[17,10,20](see below for more details);however,our goal is to give conditions that separate the role of edge lengths and dihedral angles. Theorem1.A3-connected planar graph(with its unique combinatorial embed-ding)and given edge lengths and convex facial and dihedral angles are those ofa convex polyhedron iff(1)the edges around every face form a simple convex polygon(2)in the spherical dual,the arcs of the edges around every face form a simpleconvex spherical polygonWe will prove Theorem1using a1952result of Van Heijenoort[13]on locally convex manifolds.Wefirst discuss algorithmic ramifications for computing edge lengths and/or dihedral angles.Note that Condition(1)depends on facial angles and edge lengths;Condition(2)depends on facial angles and dihedral angles—recall that dihedral angles correspond to arc lengths in the spherical dual.We were unable to use the conditions to help usfind dihedral angles,but we can use them tofind edge lengths.We separate Condition(1)into a part(1a)depending only on facial angles,and a part(1b)depending on both facial angles and edge lengths and expressible via linear inequalities.Facial angles determine edge di-rections.More precisely,if we choose a unit vector in the plane for the direction of one edge of face f,then the facial angles determine unit direction vectors d(e)∈R2for each edge e as we go around f from the initial edge.Condition (1b)is that the sum of these unit vectors times the appropriate edge lengths is the zero vector,i.e.that the sequence of edges closes up to form a polygon.What are the conditions on facial angles?It is not sufficient that every facial angle be convex,i.e.in the interval(0,π):the polygon in Figure2,from[17], has only convex angles,but is not a simple convex polygon,nor would any other choice of edge lengths make it so.To guarantee a simple convex polygon,we impose Condition(1a):that the facial angles around a face of k edges sum to π(k−2).We therefore arrive at the following conditions:(1a)for each face f of k edges,π(k−2)= {α:αa facial angle of f}. (1b)for each face f, e∈f l(e)d(e)=(0,0)where l(e)is the length of edge e and d(e)is its direction,relative to some initial choice for one edge.Lemma1.Condition(1)is equivalent to Conditions(1a)and(1b).Fig.2.Convex angles do not always make a simple polygon(left),or a simple polyhe-dron(right).Proof.The main part of this is proved by Vijayan[27].The proof is easy;we outline it for completeness.Clearly(1)implies(1a)and(1b).For the other direction,(1b)implies that we have a sequence of line segments that closes up to form a cycle.We prove by induction on k,the number of segments,that a simple convex polygon is formed.This is obvious for k=3,and easy for k=4. Consider k>4.If there are two consecutive angles with sum greater thanπwe can eliminate the edge between them by extending the two neighbouring edges, and apply induction.If all pairs of consecutive angles have sum at mostπthen 2 α≤kπ.Applying condition(1a),2π(k−2)≤πk,so2k−4≤k,so k≤4.Translated to the sphere,Condition(2)seems symmetric with Condition(1) except that it involves arc lengths(corresponding to dihedral angles)in place of edge lengths.It seems tantalizing to express Condition(2)using subconditions analogous to those above,and thus obtain an algorithm tofind dihedral angles.Condition(1b)—that following the sequence of edges around a face“closes up”the polygon—can be transferred to the spherical situation,though it is computationally more difficult for the following reason.In the plane the edges around a face provide successive translations,so we get a linear system for the edge lengths;however,on the sphere the edges around a face provide successive rotations,so we get a non-linear system.This is not the main difficulty.In the plane,the remaining condition(1a)did not depend on edge lengths,but on the sphere it does,as we now show.Recall that condition(1a)precluded a polygon “wrapping around”more than once as in Figure2(left).The same issue arises on the sphere.As described by Mehlhorn et al.[17],the example of Figure2can be extended to three dimensions by adding two vertices,one above the plane and one below,with triangular faces joining each of these vertices to each edge of the polygon.Figure2(right)shows the new upper vertex.The resulting object is combinatorially a bipyramid with a7-sided base;each face is a triangle;and each facial angle and each dihedral angle is in the range(0,π).In the spherical dual the face corresponding to the upper vertex is a spherical polygon that wraps around twice and intersects itself.In the plane,condition(1a)excluded such“wrapping around”by requiring that the sum of facial angles beπ(k−2)for any face of k edges.On the sphere no condition on facial angles alone will suffice:we give an example(prior to the Gauss map)of two spherical polygons with the same facial angles,exactly one of which is simple.Consider the example of Figure2with the upper vertex far away from the plane of the rest of the Figure,and with many acute triangles incident to it.With these same acute angles we can instead make the dihedral angles larger and connect to a simple polygon—see Figure3.Fig.3.The same facial angles at a vertex can form a simple or non-simple cone In the remainder of this section we give a proof of Theorem1using the fol-lowing result of Van Heijenoort.The terms used in the theorem are defined just below.Our situation is more specialized in that we have a piece-wise linear man-ifold,which,as we shall see,makes the topological conditions straightforward. Theorem2.[13]If a2-dimensional manifold M is(i)mapped into R3by a locally topological mapping f(ii)locally convex under f(iii)absolutely convex at a point(iv)complete under fthen f(M)is the boundary of a3-dimensional convex set.Van Heijendoort defines the manifold M to be complete if“every bounded infinite subset of M has an accumulation point in M”.“Bounded”in this case means that the distances are bounded,using the metric induced by the mapping of M into R3.M is locally convex under f if every point p of M has a neighbour-hood N s.t.f(N)lies on the boundary of a convex body K.Absolute convexity means that,in addition,there is a support plane of K at f(p)that contains no other point of K.Proof(of Theorem1).The forward direction is clear.For the other direction,as-sume conditions(1)and(2)hold.We need to prove Van Heijenoort’s conditions. The embedded3-connected planar graph drawn on the surface of a sphere pro-vides a manifold.We begin by assigning vertex coordinates.Arbitrarily choose coordinates for one vertex v and directions for two consecutive edges incident with that vertex,forming the correct facial angle for face f between them.The plane of face f is now determined.So are the coordinates of the vertices around face f.From these,and the dihedral angles,we get the planes of the faces adje-cent to face f.Continuing in this way,we obtain coordinates for all the vertices as we expand outward from the initial choices.We claim that these coordinates are well-defined—i.e.that they are independent of the order in which we expand outward.Two paths to a vertex provide a cycle,so it suffices to show that every cycle closes up.Conditions(1)and(2)give this for facial cycles in the graph and its dual,and any other cycle is a sum of facial cycles,which gives the result.This gives us a mapping of the vertices to points,and the edges to line segments in R3.By condition(1)every face of the graph is mapped to a simple planar convex polygon in R3.We thus have a piece-wise linear mapping of a manifold into R3,and conditions(i)and(iv)of Van Heijenoort’s theorem follow.We turn to conditions(ii)and(iii).Our Condition(2)ensures local convexity at every vertex.Local convexity at an interior point of an edge follows from the fact that no dihedral angle is larger thanπ.Local convexity at an interior point of a face is obvious.Thus condition(ii)holds.Finally,only an unbounded object can be locally convex at every point but not absolutely convex anywhere,giving condition(iii).Thus by Van Heijenoort’s Theorem we have the boundary of a piece-wise linear3-dimensional convex set—i.e.a convex polyhedron.3.1Background:Local Conditions for ConvexityAlthough we found Van Heijenoort’s conditions most useful,there is more recent, more algorithmic work on conditions for a polyhdron to be convex.In this section we briefly describe such work by Mehlhorn et al.[17],Devillers et al.[10],and Rybnikov[20].The conditions of Mehlhorn et al.involve checking if a ray from a point that lies on the“inside”of the plane through every face intersects only one face.The conditions of Devillers et al.are that all dihedral angles be convex and that the projection of the seam to the x-y plane be a convex polygon.The seam consists,roughly speaking,of the edges that are extreme with respect to some plane perpendicular to the x-y plane.The idea of specializing Van Heijenoort’s conditions to piece-wise linear mani-folds is due to Rybnikov.In3-dimensions it is clear that it suffices to check local convexity at vertices.Rybnikov’s result[20],which he proves using Van Hei-jenoort’s higher dimensional extension[13],is that to check convexity of piece-wise linear hypersurfaces in n dimensions,it suffices to check local convexity at the(n−3)-dimensional faces.Rybnikov gives a convexity-testing algorithm;the main step is to transform the local convexity test at an(n−3)-dimensional face to a convexity test for a[possibly self-intersecting]polygon,for which he gives a straight-forward algorithm(Devillers et al.[10]also give an algorithm for this.)4Determining Edge LengthsIn this section we consider the following problem:given the combinatorial struc-ture of a convex polyhedron and given the facial angles,find edge lengths for the polyhedron.The edge lengths are not unique,even discounting scaling.For example,a cube can be stretched along any of its three axes.Non-uniqueness is discussed in section4.4.It turns out to be equivalent to“indecomposability”,a notion introduced by Gale[11],and studied by Shephard[25],Meyer[18],and McMullen[16]among others.We will make use of the conditions for the existence of a convex polyhedron from the previous section,which were expressed in terms of facial angles,dihedral angles,and edge lengths.Recall that the only condition involving edge lengths was Condition(1b);we will express that condition in terms of linear inequalities.In section4.2we consider the version of the problem where the dihedral angles are known,and we apply duality to give a characterization of when a polyhedron exists with given facial and dihedral angles.4.1An LP FormulationLet V,E and F be the vertices,edges and faces of the graph,respectively. For each face f,choose one edge e0and choose a unit-length direction vector d f(e0)∈R2for it.Based on this choice,the facial angles determine unit direction vectors d f(e)for all the edges e in clockwise order around the face f.Note that an edge is in two faces,and may be assigned totally different edge direction vectors in those two faces.The question of whether there exist edge lengths satisfying condition(1b)is equivalent to feasibility of the following linear system in variablesλ(e),e∈E.∀e∈Eλ(e)>0∀f∈F e∈fλ(e)d f(e)=(0,0)(3) Theorem3.Suppose a convex polyhedron exists with given facial angles and combinatorial structure.Then its edge lengths satisfy(3)and any solution to(3) gives edge lengths of such a polyhedron.The problem offinding edge lengths is thus solvable via linear programming algorithms[22].Note that we need an algebraic model of computing to go from facial angles to d(e).Linear programming,however,is only solvable in polyno-mial time in the bit complexity model,so we cannot claim a polynomial time algorithm tofind edge lengths.Still,the simplex method should be practical. Note also that solving the linear system says nothing about whether the input facial angles and combinatorial structure are those of a convex polyhedron.4.2With Dihedral AnglesThe above method computes direction vectors for edges within the plane of each face.If we have dihedral angles,we can compute true3-D direction vectors for edges.We make an initial choice of coordinates for one vertex,and direction vectors for two edges consecutively incident at the vertex,ensuring that the angle between the two vectors matches the required facial angle.Based on these initial choices,we can compute direction vectors for all edges in3-D.For edge e=(u,v)∈E,let d(e)∈R3be the direction vector of the edge from u to v. Note that we(arbitrarily)choose an order(u,v)or(v,u)to do this.For face f∈F,distinguish cw(f),the edges of face f whose vector d(e)is directed clockwise around f,and ccw(f),the edges of face f whose vector is directed counter-clockwise around f.The linear system becomes:∀e∈Eλ(e)>0λ(e)d(e)=(0,0,0)(4)∀f∈F e∈cw(f)λ(e)d(e)−e∈ccw(f)Theorem4.There exists a convex polyhedron with given face and dihedral an-gles and given combinatorial structure iffconditions(1a)and(2)hold,and the linear system(4)is feasible.Our purpose in this section is to give duality conditions for feasibility of (4),but we mentionfirst that it is possible to test conditions(1a)and(2)in polynomial time—see the work referenced in section3.1.Duality theory gives a characterization of when the linear system(4)is fea-sible.The linear system has the form Ax=b,x>0.By Stiemke’s Transposition Theorem(see Schrijver[22,p.95]),there is a solution x ifffor any y,yA≥0im-plies yA=0.Translating into our situation,we have a dual variableν(f)∈R3 for each face f∈F.For edge e=(u,v)let f r(e)be the face to the right of e and let f l(e)be the face to the left of e.The dual linear system is:∀e∈E d(e)·(ν(f r(e))−ν(f l(e)))≥0(5)A change of variables gives more intuitive conditions.For each edge e let ν(e)=ν(f r(e)−ν(f l(e)).Formula(5)becomes d(e)·ν(e)≥0.We can recover theν(f)vectors from theν(e)vectors so long as the sum of theν(e)’s is0around any dual cycle.Let F be the faces of the dual graph.We obtain:Theorem5.Given an embedded3-connected planar graph with specified facial and dihedral angles s.t.conditions(1a)and(2)hold,either there exists a corre-sponding convex polyhedron OR there are vectorsν(e)∈R3,e∈E s.t.∀e∈E d(e)·ν(e)≥0(6)ν(e)=0(7)∀f∈Fe∈with strict inequality in(6)for at least one edge e.Furthermore,NOT BOTH the polyhedron and the vectors can exist.Proof.Straightforward:If there is no convex polyhedron then there are vectors ν(f)∈R3,f∈F s.t.(5)holds and with strict inequality for at least one edge e. Performing a change of variables as described above,gives vectorsν(e)∈R3,e∈E s.t.(6)and(7)hold,and with strict inequality in(6)for at least one edge.Conversely,if vectorsν(e)∈R3,e∈E exist s.t.(6)and(7)hold,and with strict inequality in(6)for at least one edge,then define vectorsν(f)∈R3for each f∈F as follows.Begin by choosing one f0∈F and settingν(f0)=(0,0,0). Then use the formulaν(e)=ν(f r(e)−ν(f l(e))to defineν:F→R3.Note that νis well-defined by(7).From(6)we obtain(5),so there is no convex polyhedron satisfying the requirements.4.3ExampleRecall that in Section3we gave conditions(1a),(1b)and(2)for the existence of a convex polyhedron with specified combinatorial structure,edge lengths,and facial and dihedral angles.That section contained an example to show that the “convexity”condition(1a)was necessary.In this section we show that condition (1b)is necessary by giving an example where Conditions(1a)and(2)hold but the linear system(3)is not feasible.The construction starts with an octahedron,which has facial angles ofπ3=60◦and dihedral angles of cos−1(−13)≈109.47◦.Split one vertex and add a newedge e as shown in Figure4.The four new facial angles are23π=120◦.All otherfacial and dihedral angles stay the same.Consistent edge direction vectors exist, and all convexity conditions are satisfied.The linear system(3)is not feasible: in order for edge e to have positive length while maintaining the specified angles, the square visible in Figure4as the silhouette of the octahedron must become a rectangle—but this destroys the bottom half of the octahedron.Fig.4.An octahedron(left)and the addition of one new edge(right)making an example where angle convexity conditions hold,but no feasible edge lengths exist.4.4Relation to Decomposability of PolyhedraThe current Section4has been about the existence of a convex polyhedron with specified combinatorial structure and facial and dihedral angles.There is a considerable body of work on the related uniqueness question:given a convex polyhedron,can we preserve all facial and dihedral angles but alter edge lengths (other than by scaling).In this subsection we briefly summarize this work.For polytopes P and Q,Gale[11]defined Q≤P if for every direction u, the extreme set of Q in direction u has dimension less than or equal to the dimension of the extreme set of P in direction u.In particular,this means that any face of Q has a corresponding face of P with the same normal;however,the combinatorial structure may be different in that a face of P may have shrunk to an edge or vertex of Q,and an edge of P may have shrunk to a vertex.Thus this concept seems atfirst glance to be more general than the uniqueness of edge-lengths question mentioned above.But in fact the notions are equivalent.Gale[11]defined a convex polyhedron P to be decomposable if P can be expressed as a Minkowski sum,P=R+S where neither R nor S is homothetic to(i.e.a scaled translated version of)P.Shephard[25]proved that a convex polyhedron P is decomposable iffthere is a convex polyhedron Q≤P that is not homothetic to P.In fact he proved a stronger thing,that such a Q can be used in a decomposition of P.We will use Shephard’s result to relate uniqueness of edge lengths to the relation≤.Lemma2.For convex polyhedron P,the following are equivalent:(i)P is decomposable(ii)there is a convex polyhedron Q≤P that is not homothetic to P(iii)there is a convex polyhedron R with the same combinatorial structure as P and the same facial and dihedral angles,but with different non-zero edge lengths(not just re-scaled)Proof.Equivalence of(i)and(ii)is Shephard’s result.Clearly,(iii)implies(ii). 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