Surfaces in 4-Manifolds
基底和膜层-基底系统的赝布儒斯特角计算(英文)
基底和膜层-基底系统的赝布儒斯特角计算(英文)刘华松;姜玉刚;王利栓;姜承慧;季一勤【期刊名称】《光子学报》【年(卷),期】2013(0)7【摘要】对基底和膜层-基底系统的赝布儒斯特角进行了数值计算.结果显示:当基底的消光系数小于0.01时,基底的赝布儒斯特角主要是由折射率决定;当基底的消光系数大于0.1时,基底的赝布儒斯特角不仅与折射率有关,而且还与消光系数有关,随着消光系数发生后周期性变化.研究表明:单层膜-基底系统的赝布儒斯特角主要由膜层的物理厚度、折射率、基底的光学常量所决定;在HfO2-硅和HfO2-融石英基底系统中,赝布儒斯特角随着入射光波长和膜层厚度的变化呈现准周期性规律变化,可能是由入射光在膜层的干涉效应引起的.【总页数】6页(P817-822)【关键词】光学常量;折射率;消光系数;膜层-基底系统;赝布儒斯特角【作者】刘华松;姜玉刚;王利栓;姜承慧;季一勤【作者单位】天津津航技术物理研究所天津市薄膜光学重点实验室,天津300192;同济大学物理系先进微结构材料教育部重点实验室,上海200092;哈尔滨工业大学光电子技术研究所可调谐激光技术国家级重点实验室,哈尔滨150080【正文语种】中文【中图分类】O484【相关文献】1.以介孔TiO2膜为过渡层在玻璃基底上制备Cu3(BTC)2连续膜 [J], 李力成;钱祺;王磊;仇龙云;王昊翊;张所瀛;杨祝红;李小保;赵学娟2.前列腺癌发生发展中基底细胞层和基底膜的改变 [J], 杨敏;刘爱军;韦立新;郭爱桃;宋欣;陈薇3.镍改性层增强铜基底沉积金刚石膜的形核(英文) [J], 刘学璋;魏秋平;翟豪;余志明;4.硅基底上生长金刚石层细晶粒的研究(英文) [J], 何敬晖;玄真武;刘尔凯5.在n型硅基底上二次注入硼离子金刚石膜的p-n结效应(英文) [J], 孙秀平;冯克成;李超;张红霞;费允杰因版权原因,仅展示原文概要,查看原文内容请购买。
表面等离子体共振技术在生物分子识别中的应用
表面等离子体共振技术在生物分子识别中的应用表面等离子体共振技术(surface plasmon resonance,SPR)是一种先进的分子识别技术,它通过监测生物分子与表面共振器件之间的化学反应,实现对生物分子行为的研究和分析。
1. SPR技术的原理及应用SPR技术是一种基于生物物理学的新兴技术,在分子生物学、蛋白质研究、药物筛选等领域具有广泛的应用。
其原理是利用共振器件表面的金属薄膜(一般是金或银)振荡的一种表面等离子体波,在化学反应发生时会引起这种波的共振峰位移,进而测定样品中的生物分子浓度、亲和力等参数。
SPR技术可用于分析生物反应、药物作用和生物分子相互作用等生物性质,如测定蛋白质的亲和力、酶的活性、低分子药物与蛋白质的结合和特异性等。
同时,SPR技术还可用于药物筛选、疾病诊断、疫苗开发和纳米技术等领域。
2. SPR技术在生物分子识别中的应用2.1 蛋白质-蛋白质间的相互作用蛋白质相互作用对细胞的生命活动起着重要作用。
利用SPR技术可以研究蛋白质的互补性和特异性作用,进而了解蛋白质的功能和相互作用机理。
研究表明,SPR技术可用于测定蛋白质亲和力和稳态化常数的测定,并准确地分析蛋白质间的相互作用。
2.2 蛋白质-核酸相互作用蛋白质和核酸的相互作用在生物学研究中也是重要的研究内容。
利用SPR技术可以研究DNA或RNA与蛋白质的相互作用,如DNA序列和蛋白质结合及稳定化常数等,进而了解生物分子之间的相互作用和分子机理。
2.3 蛋白质-低分子小分子相互作用利用SPR技术可以研究蛋白质和低分子小分子(如药物、脂质等)相互作用,进一步了解化合物的结合性能和稳态化常数,从而可达到高效和精确的药物开发和筛选。
3. SPR技术的优势和不足SPR技术具有灵敏度高、实时性好、复现性稳定、分析量小等特点,优于传统的生物分析方法。
同时,由于该技术不需要特殊的标记物,可以避免标记物对分子本身的影响,因此是得到广泛应用的分子分析方法之一。
英文高等数学教材
英文高等数学教材Mathematics is a universal language, and its importance cannot be overstated. It serves as the foundation for countless scientific and technological advancements, making it an essential subject for students in higher education, especially those pursuing degrees in science, engineering, and related fields. As such, a well-designed and comprehensive English-language textbook for advanced mathematics is crucial to assist students in mastering the subject.I. IntroductionThe introduction of the English-language advanced mathematics textbook should provide a brief overview of the subject, emphasizing its significance and relevance to various academic disciplines. It should also highlight the intended audience, specifically upper-level undergraduate and graduate students, who already possess a solid mathematical foundation.II. Chapter Divisions and TopicsThe textbook should be divided into coherent chapters, each covering a specific topic within advanced mathematics. The organization of these chapters should be logical, allowing students to progress from fundamental concepts to more complex theories seamlessly. Some possible chapter divisions and topics could include:1. Calculus and Analysis- Limits and Continuity- Derivatives and Applications- Integration and Techniques of Integration- Differential Equations2. Linear Algebra- Matrices and Vectors- Linear Transformations- Eigenvalues and Eigenvectors- Orthogonality and Inner Product Spaces3. Differential Geometry- Curves and Surfaces- Manifolds and Tensors- Riemannian Geometry- Geodesics and CurvatureIII. Pedagogical ApproachTo assist students in comprehending complex mathematical concepts, the textbook should employ various pedagogical approaches. These can include:1. Clear Explanations: Each chapter should provide clear, concise explanations of key theoretical concepts, supplemented with illustrative examples.2. Step-by-Step Solutions: Worked-out examples should be provided, guiding students through the problem-solving process, highlighting key steps and reasoning.3. Practice Problems: A collection of practice problems should be included at the end of each chapter to allow students to consolidate their understanding of the material.4. Supplementary Resources: Additional resources, such as online tutorials, interactive simulations, and video lectures, should be made available to enhance the learning experience.IV. Visual Aids and DiagramsVisual aids, such as graphs, diagrams, and illustrations, play a crucial role in visualizing abstract mathematical concepts. Including well-designed visual representations throughout the textbook can significantly aid students' understanding and comprehension.V. Real-Life ApplicationsThe textbook should incorporate real-life applications of advanced mathematics where possible. By demonstrating the practical relevance of mathematical theories, students can develop a deeper appreciation for the subject and its potential for solving real-world problems.VI. Exercises and AssessmentsApart from practice problems at the end of each chapter, the textbook should include comprehensive exercises and assessments to challengestudents' understanding and encourage critical thinking. These exercises can range from computational problems to proof-based questions.VII. ConclusionA well-crafted English-language advanced mathematics textbook can greatly enhance students' learning experience in higher education. By providing clear explanations, utilizing visual aids, and incorporating real-life applications, such a textbook can assist students in mastering the subject and preparing them for professional careers requiring advanced mathematical skills.Note: This is a fictional article and does not follow the exact structure or content of an actual advanced mathematics textbook.。
斯普林格数学研究生教材丛书
《斯普林格数学研究生教材丛书》(Graduate Texts in Mathematics)GTM001《Introduction to Axiomatic Set Theory》Gaisi Takeuti, Wilson M.Zaring GTM002《Measure and Category》John C.Oxtoby(测度和范畴)(2ed.)GTM003《Topological Vector Spaces》H.H.Schaefer, M.P.Wolff(2ed.)GTM004《A Course in Homological Algebra》P.J.Hilton, U.Stammbach(2ed.)(同调代数教程)GTM005《Categories for the Working Mathematician》Saunders Mac Lane(2ed.)GTM006《Projective Planes》Daniel R.Hughes, Fred C.Piper(投射平面)GTM007《A Course in Arithmetic》Jean-Pierre Serre(数论教程)GTM008《Axiomatic set theory》Gaisi Takeuti, Wilson M.Zaring(2ed.)GTM009《Introduction to Lie Algebras and Representation Theory》James E.Humphreys(李代数和表示论导论)GTM010《A Course in Simple-Homotopy Theory》M.M CohenGTM011《Functions of One Complex VariableⅠ》John B.ConwayGTM012《Advanced Mathematical Analysis》Richard BealsGTM013《Rings and Categories of Modules》Frank W.Anderson, Kent R.Fuller(环和模的范畴)(2ed.)GTM014《Stable Mappings and Their Singularities》Martin Golubitsky, Victor Guillemin (稳定映射及其奇点)GTM015《Lectures in Functional Analysis and Operator Theory》Sterling K.Berberian GTM016《The Structure of Fields》David J.Winter(域结构)GTM017《Random Processes》Murray RosenblattGTM018《Measure Theory》Paul R.Halmos(测度论)GTM019《A Hilbert Space Problem Book》Paul R.Halmos(希尔伯特问题集)GTM020《Fibre Bundles》Dale Husemoller(纤维丛)GTM021《Linear Algebraic Groups》James E.Humphreys(线性代数群)GTM022《An Algebraic Introduction to Mathematical Logic》Donald W.Barnes, John M.MackGTM023《Linear Algebra》Werner H.Greub(线性代数)GTM024《Geometric Functional Analysis and Its Applications》Paul R.HolmesGTM025《Real and Abstract Analysis》Edwin Hewitt, Karl StrombergGTM026《Algebraic Theories》Ernest G.ManesGTM027《General Topology》John L.Kelley(一般拓扑学)GTM028《Commutative Algebra》VolumeⅠOscar Zariski, Pierre Samuel(交换代数)GTM029《Commutative Algebra》VolumeⅡOscar Zariski, Pierre Samuel(交换代数)GTM030《Lectures in Abstract AlgebraⅠ.Basic Concepts》Nathan Jacobson(抽象代数讲义Ⅰ基本概念分册)GTM031《Lectures in Abstract AlgebraⅡ.Linear Algabra》Nathan.Jacobson(抽象代数讲义Ⅱ线性代数分册)GTM032《Lectures in Abstract AlgebraⅢ.Theory of Fields and Galois Theory》Nathan.Jacobson(抽象代数讲义Ⅲ域和伽罗瓦理论)GTM033《Differential Topology》Morris W.Hirsch(微分拓扑)GTM034《Principles of Random Walk》Frank Spitzer(2ed.)(随机游动原理)GTM035《Several Complex Variables and Banach Algebras》Herbert Alexander, John Wermer(多复变和Banach代数)GTM036《Linear Topological Spaces》John L.Kelley, Isaac Namioka(线性拓扑空间)GTM037《Mathematical Logic》J.Donald Monk(数理逻辑)GTM038《Several Complex Variables》H.Grauert, K.FritzsheGTM039《An Invitation to C*-Algebras》William Arveson(C*-代数引论)GTM040《Denumerable Markov Chains》John G.Kemeny, urie Snell, Anthony W.KnappGTM041《Modular Functions and Dirichlet Series in Number Theory》Tom M.Apostol (数论中的模函数和Dirichlet序列)GTM042《Linear Representations of Finite Groups》Jean-Pierre Serre(有限群的线性表示)GTM043《Rings of Continuous Functions》Leonard Gillman, Meyer JerisonGTM044《Elementary Algebraic Geometry》Keith KendigGTM045《Probability TheoryⅠ》M.Loève(概率论Ⅰ)(4ed.)GTM046《Probability TheoryⅡ》M.Loève(概率论Ⅱ)(4ed.)GTM047《Geometric Topology in Dimensions 2 and 3》Edwin E.MoiseGTM048《General Relativity for Mathematicians》Rainer.K.Sachs, H.Wu伍鸿熙(为数学家写的广义相对论)GTM049《Linear Geometry》K.W.Gruenberg, A.J.Weir(2ed.)GTM050《Fermat's Last Theorem》Harold M.EdwardsGTM051《A Course in Differential Geometry》Wilhelm Klingenberg(微分几何教程)GTM052《Algebraic Geometry》Robin Hartshorne(代数几何)GTM053《A Course in Mathematical Logic for Mathematicians》Yu.I.Manin(2ed.)GTM054《Combinatorics with Emphasis on the Theory of Graphs》Jack E.Graver, Mark E.WatkinsGTM055《Introduction to Operator TheoryⅠ》Arlen Brown, Carl PearcyGTM056《Algebraic Topology:An Introduction》W.S.MasseyGTM057《Introduction to Knot Theory》Richard.H.Crowell, Ralph.H.FoxGTM058《p-adic Numbers, p-adic Analysis, and Zeta-Functions》Neal Koblitz(p-adic 数、p-adic分析和Z函数)GTM059《Cyclotomic Fields》Serge LangGTM060《Mathematical Methods of Classical Mechanics》V.I.Arnold(经典力学的数学方法)(2ed.)GTM061《Elements of Homotopy Theory》George W.Whitehead(同论论基础)GTM062《Fundamentals of the Theory of Groups》M.I.Kargapolov, Ju.I.Merzljakov GTM063《Modern Graph Theory》Béla BollobásGTM064《Fourier Series:A Modern Introduction》VolumeⅠ(2ed.)R.E.Edwards(傅里叶级数)GTM065《Differential Analysis on Complex Manifolds》Raymond O.Wells, Jr.(3ed.)GTM066《Introduction to Affine Group Schemes》William C.Waterhouse(仿射群概型引论)GTM067《Local Fields》Jean-Pierre Serre(局部域)GTM069《Cyclotomic FieldsⅠandⅡ》Serge LangGTM070《Singular Homology Theory》William S.MasseyGTM071《Riemann Surfaces》Herschel M.Farkas, Irwin Kra(黎曼曲面)GTM072《Classical Topology and Combinatorial Group Theory》John Stillwell(经典拓扑和组合群论)GTM073《Algebra》Thomas W.Hungerford(代数)GTM074《Multiplicative Number Theory》Harold Davenport(乘法数论)(3ed.)GTM075《Basic Theory of Algebraic Groups and Lie Algebras》G.P.HochschildGTM076《Algebraic Geometry:An Introduction to Birational Geometry of Algebraic Varieties》Shigeru IitakaGTM077《Lectures on the Theory of Algebraic Numbers》Erich HeckeGTM078《A Course in Universal Algebra》Stanley Burris, H.P.Sankappanavar(泛代数教程)GTM079《An Introduction to Ergodic Theory》Peter Walters(遍历性理论引论)GTM080《A Course in_the Theory of Groups》Derek J.S.RobinsonGTM081《Lectures on Riemann Surfaces》Otto ForsterGTM082《Differential Forms in Algebraic Topology》Raoul Bott, Loring W.Tu(代数拓扑中的微分形式)GTM083《Introduction to Cyclotomic Fields》Lawrence C.Washington(割圆域引论)GTM084《A Classical Introduction to Modern Number Theory》Kenneth Ireland, Michael Rosen(现代数论经典引论)GTM085《Fourier Series A Modern Introduction》Volume 1(2ed.)R.E.Edwards GTM086《Introduction to Coding Theory》J.H.van Lint(3ed .)GTM087《Cohomology of Groups》Kenneth S.Brown(上同调群)GTM088《Associative Algebras》Richard S.PierceGTM089《Introduction to Algebraic and Abelian Functions》Serge Lang(代数和交换函数引论)GTM090《An Introduction to Convex Polytopes》Ame BrondstedGTM091《The Geometry of Discrete Groups》Alan F.BeardonGTM092《Sequences and Series in BanachSpaces》Joseph DiestelGTM093《Modern Geometry-Methods and Applications》(PartⅠ.The of geometry Surfaces Transformation Groups and Fields)B.A.Dubrovin, A.T.Fomenko, S.P.Novikov (现代几何学方法和应用)GTM094《Foundations of Differentiable Manifolds and Lie Groups》Frank W.Warner(可微流形和李群基础)GTM095《Probability》A.N.Shiryaev(2ed.)GTM096《A Course in Functional Analysis》John B.Conway(泛函分析教程)GTM097《Introduction to Elliptic Curves and Modular Forms》Neal Koblitz(椭圆曲线和模形式引论)GTM098《Representations of Compact Lie Groups》Theodor Breöcker, Tammo tom DieckGTM099《Finite Reflection Groups》L.C.Grove, C.T.Benson(2ed.)GTM100《Harmonic Analysis on Semigroups》Christensen Berg, Jens Peter Reus Christensen, Paul ResselGTM101《Galois Theory》Harold M.Edwards(伽罗瓦理论)GTM102《Lie Groups, Lie Algebras, and Their Representation》V.S.Varadarajan(李群、李代数及其表示)GTM103《Complex Analysis》Serge LangGTM104《Modern Geometry-Methods and Applications》(PartⅡ.Geometry and Topology of Manifolds)B.A.Dubrovin, A.T.Fomenko, S.P.Novikov(现代几何学方法和应用)GTM105《SL₂ (R)》Serge Lang(SL₂ (R)群)GTM106《The Arithmetic of Elliptic Curves》Joseph H.Silverman(椭圆曲线的算术理论)GTM107《Applications of Lie Groups to Differential Equations》Peter J.Olver(李群在微分方程中的应用)GTM108《Holomorphic Functions and Integral Representations in Several Complex Variables》R.Michael RangeGTM109《Univalent Functions and Teichmueller Spaces》Lehto OlliGTM110《Algebraic Number Theory》Serge Lang(代数数论)GTM111《Elliptic Curves》Dale Husemoeller(椭圆曲线)GTM112《Elliptic Functions》Serge Lang(椭圆函数)GTM113《Brownian Motion and Stochastic Calculus》Ioannis Karatzas, Steven E.Shreve (布朗运动和随机计算)GTM114《A Course in Number Theory and Cryptography》Neal Koblitz(数论和密码学教程)GTM115《Differential Geometry:Manifolds, Curves, and Surfaces》M.Berger, B.Gostiaux GTM116《Measure and Integral》Volume1 John L.Kelley, T.P.SrinivasanGTM117《Algebraic Groups and Class Fields》Jean-Pierre Serre(代数群和类域)GTM118《Analysis Now》Gert K.Pedersen(现代分析)GTM119《An introduction to Algebraic Topology》Jossph J.Rotman(代数拓扑导论)GTM120《Weakly Differentiable Functions》William P.Ziemer(弱可微函数)GTM121《Cyclotomic Fields》Serge LangGTM122《Theory of Complex Functions》Reinhold RemmertGTM123《Numbers》H.-D.Ebbinghaus, H.Hermes, F.Hirzebruch, M.Koecher, K.Mainzer, J.Neukirch, A.Prestel, R.Remmert(2ed.)GTM124《Modern Geometry-Methods and Applications》(PartⅢ.Introduction to Homology Theory)B.A.Dubrovin, A.T.Fomenko, S.P.Novikov(现代几何学方法和应用)GTM125《Complex Variables:An introduction》Garlos A.Berenstein, Roger Gay GTM126《Linear Algebraic Groups》Armand Borel(线性代数群)GTM127《A Basic Course in Algebraic Topology》William S.Massey(代数拓扑基础教程)GTM128《Partial Differential Equations》Jeffrey RauchGTM129《Representation Theory:A First Course》William Fulton, Joe HarrisGTM130《Tensor Geometry》C.T.J.Dodson, T.Poston(张量几何)GTM131《A First Course in Noncommutative Rings》m(非交换环初级教程)GTM132《Iteration of Rational Functions:Complex Analytic Dynamical Systems》AlanF.Beardon(有理函数的迭代:复解析动力系统)GTM133《Algebraic Geometry:A First Course》Joe Harris(代数几何)GTM134《Coding and Information Theory》Steven RomanGTM135《Advanced Linear Algebra》Steven RomanGTM136《Algebra:An Approach via Module Theory》William A.Adkins, Steven H.WeintraubGTM137《Harmonic Function Theory》Sheldon Axler, Paul Bourdon, Wade Ramey(调和函数理论)GTM138《A Course in Computational Algebraic Number Theory》Henri Cohen(计算代数数论教程)GTM139《Topology and Geometry》Glen E.BredonGTM140《Optima and Equilibria:An Introduction to Nonlinear Analysis》Jean-Pierre AubinGTM141《A Computational Approach to Commutative Algebra》Gröbner Bases, Thomas Becker, Volker Weispfenning, Heinz KredelGTM142《Real and Functional Analysis》Serge Lang(3ed.)GTM143《Measure Theory》J.L.DoobGTM144《Noncommutative Algebra》Benson Farb, R.Keith DennisGTM145《Homology Theory:An Introduction to Algebraic Topology》James W.Vick(同调论:代数拓扑简介)GTM146《Computability:A Mathematical Sketchbook》Douglas S.BridgesGTM147《Algebraic K-Theory and Its Applications》Jonathan Rosenberg(代数K理论及其应用)GTM148《An Introduction to the Theory of Groups》Joseph J.Rotman(群论入门)GTM149《Foundations of Hyperbolic Manifolds》John G.Ratcliffe(双曲流形基础)GTM150《Commutative Algebra with a view toward Algebraic Geometry》David EisenbudGTM151《Advanced Topics in the Arithmetic of Elliptic Curves》Joseph H.Silverman(椭圆曲线的算术高级选题)GTM152《Lectures on Polytopes》Günter M.ZieglerGTM153《Algebraic Topology:A First Course》William Fulton(代数拓扑)GTM154《An introduction to Analysis》Arlen Brown, Carl PearcyGTM155《Quantum Groups》Christian Kassel(量子群)GTM156《Classical Descriptive Set Theory》Alexander S.KechrisGTM157《Integration and Probability》Paul MalliavinGTM158《Field theory》Steven Roman(2ed.)GTM159《Functions of One Complex Variable VolⅡ》John B.ConwayGTM160《Differential and Riemannian Manifolds》Serge Lang(微分流形和黎曼流形)GTM161《Polynomials and Polynomial Inequalities》Peter Borwein, Tamás Erdélyi(多项式和多项式不等式)GTM162《Groups and Representations》J.L.Alperin, Rowen B.Bell(群及其表示)GTM163《Permutation Groups》John D.Dixon, Brian Mortime rGTM164《Additive Number Theory:The Classical Bases》Melvyn B.NathansonGTM165《Additive Number Theory:Inverse Problems and the Geometry of Sumsets》Melvyn B.NathansonGTM166《Differential Geometry:Cartan's Generalization of Klein's Erlangen Program》R.W.SharpeGTM167《Field and Galois Theory》Patrick MorandiGTM168《Combinatorial Convexity and Algebraic Geometry》Günter Ewald(组合凸面体和代数几何)GTM169《Matrix Analysis》Rajendra BhatiaGTM170《Sheaf Theory》Glen E.Bredon(2ed.)GTM171《Riemannian Geometry》Peter Petersen(黎曼几何)GTM172《Classical Topics in Complex Function Theory》Reinhold RemmertGTM173《Graph Theory》Reinhard Diestel(图论)(3ed.)GTM174《Foundations of Real and Abstract Analysis》Douglas S.Bridges(实分析和抽象分析基础)GTM175《An Introduction to Knot Theory》W.B.Raymond LickorishGTM176《Riemannian Manifolds:An Introduction to Curvature》John M.LeeGTM177《Analytic Number Theory》Donald J.Newman(解析数论)GTM178《Nonsmooth Analysis and Control Theory》F.H.clarke, Yu.S.Ledyaev, R.J.Stern, P.R.Wolenski(非光滑分析和控制论)GTM179《Banach Algebra Techniques in Operator Theory》Ronald G.Douglas(2ed.)GTM180《A Course on Borel Sets》S.M.Srivastava(Borel 集教程)GTM181《Numerical Analysis》Rainer KressGTM182《Ordinary Differential Equations》Wolfgang WalterGTM183《An introduction to Banach Spaces》Robert E.MegginsonGTM184《Modern Graph Theory》Béla Bollobás(现代图论)GTM185《Using Algebraic Geomety》David A.Cox, John Little, Donal O’Shea(应用代数几何)GTM186《Fourier Analysis on Number Fields》Dinakar Ramakrishnan, Robert J.Valenza GTM187《Moduli of Curves》Joe Harris, Ian Morrison(曲线模)GTM188《Lectures on the Hyperreals:An Introduction to Nonstandard Analysis》Robert GoldblattGTM189《Lectures on Modules and Rings》m(模和环讲义)GTM190《Problems in Algebraic Number Theory》M.Ram Murty, Jody Esmonde(代数数论中的问题)GTM191《Fundamentals of Differential Geometry》Serge Lang(微分几何基础)GTM192《Elements of Functional Analysis》Francis Hirsch, Gilles LacombeGTM193《Advanced Topics in Computational Number Theory》Henri CohenGTM194《One-Parameter Semigroups for Linear Evolution Equations》Klaus-Jochen Engel, Rainer Nagel(线性发展方程的单参数半群)GTM195《Elementary Methods in Number Theory》Melvyn B.Nathanson(数论中的基本方法)GTM196《Basic Homological Algebra》M.Scott OsborneGTM197《The Geometry of Schemes》David Eisenbud, Joe HarrisGTM198《A Course in p-adic Analysis》Alain M.RobertGTM199《Theory of Bergman Spaces》Hakan Hedenmalm, Boris Korenblum, Kehe Zhu(Bergman空间理论)GTM200《An Introduction to Riemann-Finsler Geometry》D.Bao, S.-S.Chern, Z.Shen GTM201《Diophantine Geometry An Introduction》Marc Hindry, Joseph H.Silverman GTM202《Introduction to Topological Manifolds》John M.LeeGTM203《The Symmetric Group》Bruce E.SaganGTM204《Galois Theory》Jean-Pierre EscofierGTM205《Rational Homotopy Theory》Yves Félix, Stephen Halperin, Jean-Claude Thomas(有理同伦论)GTM206《Problems in Analytic Number Theory》M.Ram MurtyGTM207《Algebraic Graph Theory》Chris Godsil, Gordon Royle(代数图论)GTM208《Analysis for Applied Mathematics》Ward CheneyGTM209《A Short Course on Spectral Theory》William Arveson(谱理论简明教程)GTM210《Number Theory in Function Fields》Michael RosenGTM211《Algebra》Serge Lang(代数)GTM212《Lectures on Discrete Geometry》Jiri Matousek(离散几何讲义)GTM213《From Holomorphic Functions to Complex Manifolds》Klaus Fritzsche, Hans Grauert(从正则函数到复流形)GTM214《Partial Differential Equations》Jüergen Jost(偏微分方程)GTM215《Algebraic Functions and Projective Curves》David M.Goldschmidt(代数函数和投影曲线)GTM216《Matrices:Theory and Applications》Denis Serre(矩阵:理论及应用)GTM217《Model Theory An Introduction》David Marker(模型论引论)GTM218《Introduction to Smooth Manifolds》John M.Lee(光滑流形引论)GTM219《The Arithmetic of Hyperbolic 3-Manifolds》Colin Maclachlan, Alan W.Reid GTM220《Smooth Manifolds and Observables》Jet Nestruev(光滑流形和直观)GTM221《Convex Polytopes》Branko GrüenbaumGTM222《Lie Groups, Lie Algebras, and Representations》Brian C.Hall(李群、李代数和表示)GTM223《Fourier Analysis and its Applications》Anders Vretblad(傅立叶分析及其应用)GTM224《Metric Structures in Differential Geometry》Gerard Walschap(微分几何中的度量结构)GTM225《Lie Groups》Daniel Bump(李群)GTM226《Spaces of Holomorphic Functions in the Unit Ball》Kehe Zhu(单位球内的全纯函数空间)GTM227《Combinatorial Commutative Algebra》Ezra Miller, Bernd Sturmfels(组合交换代数)GTM228《A First Course in Modular Forms》Fred Diamond, Jerry Shurman(模形式初级教程)GTM229《The Geometry of Syzygies》David Eisenbud(合冲几何)GTM230《An Introduction to Markov Processes》Daniel W.Stroock(马尔可夫过程引论)GTM231《Combinatorics of Coxeter Groups》Anders Bjröner, Francesco Brenti(Coxeter 群的组合学)GTM232《An Introduction to Number Theory》Graham Everest, Thomas Ward(数论入门)GTM233《Topics in Banach Space Theory》Fenando Albiac, Nigel J.Kalton(Banach空间理论选题)GTM234《Analysis and Probability:Wavelets, Signals, Fractals》Palle E.T.Jorgensen(分析与概率)GTM235《Compact Lie Groups》Mark R.Sepanski(紧致李群)GTM236《Bounded Analytic Functions》John B.Garnett(有界解析函数)GTM237《An Introduction to Operators on the Hardy-Hilbert Space》Rubén A.Martínez-Avendano, Peter Rosenthal(哈代-希尔伯特空间算子引论)GTM238《A Course in Enumeration》Martin Aigner(枚举教程)GTM239《Number Theory:VolumeⅠTools and Diophantine Equations》Henri Cohen GTM240《Number Theory:VolumeⅡAnalytic and Modern Tools》Henri Cohen GTM241《The Arithmetic of Dynamical Systems》Joseph H.SilvermanGTM242《Abstract Algebra》Pierre Antoine Grillet(抽象代数)GTM243《Topological Methods in Group Theory》Ross GeogheganGTM244《Graph Theory》J.A.Bondy, U.S.R.MurtyGTM245《Complex Analysis:In the Spirit of Lipman Bers》Jane P.Gilman, Irwin Kra, Rubi E.RodriguezGTM246《A Course in Commutative Banach Algebras》Eberhard KaniuthGTM247《Braid Groups》Christian Kassel, Vladimir TuraevGTM248《Buildings Theory and Applications》Peter Abramenko, Kenneth S.Brown GTM249《Classical Fourier Analysis》Loukas Grafakos(经典傅里叶分析)GTM250《Modern Fourier Analysis》Loukas Grafakos(现代傅里叶分析)GTM251《The Finite Simple Groups》Robert A.WilsonGTM252《Distributions and Operators》Gerd GrubbGTM253《Elementary Functional Analysis》Barbara D.MacCluerGTM254《Algebraic Function Fields and Codes》Henning StichtenothGTM255《Symmetry Representations and Invariants》Roe Goodman, Nolan R.Wallach GTM256《A Course in Commutative Algebra》Kemper GregorGTM257《Deformation Theory》Robin HartshorneGTM258《Foundation of Optimization》Osman GülerGTM259《Ergodic Theory:with a view towards Number Theory》Manfred Einsiedler, Thomas WardGTM260《Monomial Ideals》Jurgen Herzog, Takayuki HibiGTM261《Probability and Stochastics》Erhan CinlarGTM262《Essentials of Integration Theory for Analysis》Daniel W.StroockGTM263《Analysis on Fock Spaces》Kehe ZhuGTM264《Functional Analysis, Calculus of Variations and Optimal Control》Francis ClarkeGTM265《Unbounded Self-adjoint Operatorson Hilbert Space》Konrad Schmüdgen GTM266《Calculus Without Derivatives》Jean-Paul PenotGTM267《Quantum Theory for Mathematicians》Brian C.HallGTM268《Geometric Analysis of the Bergman Kernel and Metric》Steven G.Krantz GTM269《Locally Convex Spaces》M.Scott Osborne。
综述Representation learning a review and new perspectives
explanatory factors for the observed input. A good representation is also one that is useful as input to a supervised predictor. Among the various ways of learning representations, this paper focuses on deep learning methods: those that are formed by the composition of multiple non-linear transformations, with the goal of yielding more abstract – and ultimately more useful – representations. Here we survey this rapidly developing area with special emphasis on recent progress. We consider some of the fundamental questions that have been driving research in this area. Specifically, what makes one representation better than another? Given an example, how should we compute its representation, i.e. perform feature extraction? Also, what are appropriate objectives for learning good representations?
Simrit
Plug & SealFast-fit plug Connections for Housings, Pipe Ends and AssembliesMake the most of Simrit’s service package and give yourself a real competitive edge:Constant innovations Uniquely wide range of productsStrong product brands Unique materials expertise A wide range of value added servicesVibration ControlSpecial Sealing Products: Bellows, Diaphragms,Elastomer Composite Parts and Precision MouldingsLederer Liquid Silicone ProductsISC O-RingIntegral AccumulatorMerkel Hydraulics / PneumaticsSimmerring ®Simrit ®, Your Global Technology Specialist for Seals and Vibration ControlThis way we secure competitive advantages for you based on experience all around the world:Simrit has a presence through-out Europe, America and Asia,either directly or through its affiliated companies NOK (Japan) or Freudenberg-NOK (USA). The transfer of know-ledge between these markets is incorporated directly into the Simrit service package. With our many Simrit Service Centres and Simrit distribution Partners, we serve and supply more than 100,000 customers worldwide. Our Simrit Partners ensure rapid availability from stock. This means spare parts quickly arrive when and where they are needed. There is aSimrit Partner near you as well.Simrit, Your Global Technology Specialist for Seals and Vibration Control offers you a complete service pack-age. A unique range of products and services guarantees you numer-ous advantages over the competition.Simrit acts as a partner togeneral industry. Its position as a market leader is achieved through continuous research,development and manufacture.We have the world’s widest ran-ge of seals and vibration con-trol products, and can offer you solutions based on the demands of state-of-the-art-technology,solutions which set standards.Simrit offers a complete package of products and services, including leading brands such as Simmerring ®, Merkel,Integral Accumulator, Meillor andISC O-Ring.23Overview of Plug & SealSimple to replacePlug & Seal plug connections offer a wide range of benefits and help to do away with inadequate substitution solutions. This includes:■cast-iron pipe with turned grooves■machined aluminium pipe with two fitted O-Rings (Fig. 2)■hose with hose-clips ■gasket or O-Ring seal.Fig. 2: Machined aluminium pipeSelection of materialsRubber coatings and shock absorption are available with modern elastomer materials –for a range of different physical requirements. You are also free to choose the base material of the pipe section: steel, alumini-um or plastic. Thanks to the flexible range of materials the plug connections can be used in virtually all sectors of fluids and gas transport.Simrit has brought about a marked improvement in the connection of two housings for the trans-port of media. With Plug & Seal plug connections safety shortcomings in terms of tightness or high fitting costs with alterna-tive competitor solutions can be avoided.Simple designPlug & Seal plug connections are designed as pipe sections rubber-coated on the outside with sealing beads and shock absorbers. They are used to create a leakfree connection between two housings or units –to ensure the safe transport of media such as oils, water or air. Beside standard-design Plug & Seal Simrit also offers individual product solutions which are tailored to specific customer requirements.Shock absorberBase part■Steel■Aluminium ■PlasticSealing beadsElastomer coating■FKM ■ACM ■VMQ■EPDM ■HNBR ■AEM■NBROverview of benefitsPlug & Seal plug connections from Simrit■create a reliable sealincluding with high pressures ■give simple, secure and low-cost fitting■ensure acoustic and mechanical decoupling ■minimise maintenance costs due to a greatly improved service life■compensate for misalignment and permit greater tolerances on installation■reduce logistics costs■combine several functions in a single component■offer clear benefits through lower total cost.Examples of applications for special purposes There is an enormousrange of possibleapplications for Plug &Seal plug connectionsfrom Simrit. They offeran optimum solutionin many branches ofindustry.Wide range of applicationsPlug & Seal plug connections are used in areas such as the following:■in water and oil circuits or in air routing systems of internal combustion engines■in ancillary engine compo-nents such as superchargers, turbochargers or intake manifolds■in automatic/manual transmission systems■in valve and pipework systems■in heating and air-conditio-ning systems of installations and buildings.Plug & Seal in engines and ancillary components In turbo diesel engines the turbocharger needs a reliable supply of charge air. Here the use of Plug & Seal between the air supply and the charge air pipe guarantees a secure leak-free connection. The elastomer component of the Plug & Seal plug connection is madeof FKM and is temperature-resistant to 220°C.With this application it is above all compensation of the offset that makes Plug & Seal so advantageous.In addition, with modern diesel engines it is possible to comply with tighter limit values of future exhaust emissions standards thanks to exhaust gas recircula-tion systems (EGR). The use of Plug & Seal as a connection pipe in an EGR system results in reliable sealing and acoustic decoupling. Here aggressive media and temperatures up to 180°C make extremely high demands on Plug & Seal. For this reason materials such FKMand stainless steel are used.45Plug & Seal in trans-mission systemsIn transmission systems of vehicles and machines a conti-nuous oil circuit is necessary.Plug & Seal plug connections can be used here to ensure a reliable oil supply also going beyond the limits of various transmission components. The elastomer component of the Plug & Seal plug connection is made of HNBR and is tempera-ture-resistant to 150°C. With this application the key benefits of Plug & Seal are extremely secure fitting and reliable life-long sealing.Plug & Seal in heating systemsIf water is to pass through radiators, the individual fins need to be connected to form a circuit by means of a manifold.Plug & Seal fulfils this function safely and reliably. The elasto-mer component of the Plug &Seal plug connection is made of EPDM and is temperature-resistant to 140°C. A plastic pipe is used as the base part.For this application it is particu-larly advantageous that Plug &Seal makes the fitting of radia-tors simpler, safer and moreefficient.7Fig. 1: O-Ring solutionTechnical BenefitsReduced requirements on plane parallelismIn practice sealing problems often crop up when connecting housings with uneven surfaces that are not plane-parallel.Plug & Seal offers an appro-priate solution here. Unlike O-Ring-solutions the seal re-quires no direct contact to the housing surfaces; plane parallelism is not essential either (Fig. 1).Plug & Seal thus provides for greater tolerances, reducing the cost of housing manufacture (Fig. 2).The Simrit brand product Plug & Seal wins over customers with technical benefits such as high pressure resistance including with complex applications.Acoustic and mechanical decouplingThe statutory provisions for the reduction of noise levels for machines and vehicles become more stringent every year.Particularly when dynamic units or housings are to be connec-ted, the transmission of noise and vibrations is a major pro-blem. With Plug & Seal these effects are eliminated by the plug connections themselves.The elastomer shock absorbers perform acoustic and mechani-cal decoupling for Plug & Seal.Shock absorberFig. 59Clear benefits in a direct cost comparisonThe following example of a cost comparison (see table) demon-strates the savings potential available. The Plug & Seal element listed performs additio-nal functions besides leakfree media routing. Special dust lips protect the actual sealing lip from soiling, thus ensuring a long service life (Fig.1).There are also economical benefits to Plug & Seal:Simple, secure and low-cost fittingPlug & Seal-components can be installed quickly and at low cost. The plug connections fix themselves in position automati-cally on installation. In addi-tion, several Plug & Seal units can be fitted in a single opera-tion. Automatic fitting is also possible.Low logistical costsCompared with many substitu-Long service lifeIn long-term applications Plug &Seal-solutions last much longer than O-Ring-connections. In comparison their life is 10 to 50% greater. Positive effect: reduced maintenance costs in terms of work time and the materials required. In addition,there is a major reduction in the costs of complaints for failures occurring in the field.Lower manufacturing Example of a cost comparison between Plug & Seal and an O-Ring-solution10Plug & Seal Standard VariantsTo give a cost effective solution for Plug & Seal with low piece numbers,there is a standard programme without additional tool costs.Product varietyEven the standard programme can offer the right sealing solution for a whole range of applications thanks to its wide variety.The standard-Plug & Seal plug connections basically consist of a base part in steel and a seal made of the following elasto-mer materials (see also table on next page):■EPDM ■FKM■on request: AEM, ACM,NBR, HNBR, VMQThe standard dimensions of Plug & Seal cover a wide range of operating conditions (see table below):■15 to 40 mm diameter of locating bore■20 to 60 mm connection-lengthPlug & Seal standard dimensionsNo tool costsThere is a major cost advan-tage for the Plug & Seal stan-dard variants particularly with a low annual requirement. As in the case of all standard pro-ducts from Simrit, tool costs are no longer incurred, something that would otherwise have an adverse effect on total costs.Wall thickness of base part (b):1.0 mm (Plug & Seal for locating bore 15, 20, 25 mm)1.5 mm (Plug & Seal for locating bore 30, 40 mm)Delivery times for the individual dimensions are available on demand as the standard programme is currently in development (status 01/05). To ensure full functioning the specifications regarding the quality of the housing should be observed (see next page).*Minimum compression of 15%**Recommended values,depending on elastomer base material: steel (bonderised)11Wall thickness of base part (b):1.0 mm (Plug & Seal for locating bore 15, 20, 25 mm)1.5 mm (Plug & Seal for locating bore 30, 40 mm)Selection of diverse materials and specifications for installationElastomers for a wide range of applicationsFor the selection and design of Plug & Seal a whole range of elastomers and base parts is offered (incl. steel, plastic, aluminium). The table shown below lists the elastomer mate-rials available for the seals as well as the possible appli-cations.Plug & Sealmaterials and operating conditions for elastomer seal:*Standard materialsIf Plug & Seal is to offer a secure leakfree connection in practice, a number of outline conditions need to be fulfilled. This includes selection of the right elastomer for the appli-cation and the proper preparation of the housing.Specifications for quality of housing■surface roughness Rstatic pressures: R max <16µm,pulsating pressures: R max <6µm ■tolerance ISO H8■recommended insertion angle:chamfer of min. 20°,chamfer length (a) approx. 2 mm,edges burr-free and rounded ■depth of housing (t1):>7 mm■max. axial offset as agreedProduct InformationSpecial Sealing Products30 G B 055 3.0 0205 B r . A B THeadquarters Europe Freudenberg Simrit KG69465 Weinheim, GermanyPhone:+49 (0) 1805-746748Fax:+49 (0) 1803-746748e-mail:info @simrit.de Simrit, Your Global Technology Specialist for Seals and Vibration ControlVibration ControlSpecial Sealing Products: Bellows, Diaphragms,Elastomer Composite Parts and Precision MouldingsLederer Liquid Silicone ProductsISC O-RingIntegral AccumulatorMerkel Hydraulics / PneumaticsSimmerring ®Seals for high pressure/structure-borne sound insulation Compensation for misalignment/offset in housing Simple low-cost fittinge.g.Your BenefitsSimrit ServicesY our BenefitsPlug & Seal: Fast-fit plug Connections for Housings, Pipe Ends and AssembliesUnique materials expertiseSpecialised technological expertise All from one sourceTechnological edge Constant innovationsUniquely wide range of products Strong product brands Longer unit service lifeCompetitive advantages, efficiency and lower costsA wide range of value added services。
manifold-based method
manifold-based method
manifold-based方法是一类机器学习方法,其核心思想是:
高维数据实际上处于一个低维的manifold(流形)结构上,这个低维流形折叠、弯曲在高维空间内。
manifold-based方法试图学习和保留这个低维流形的结构。
比如著名的Isomap算法,它通过维持高维数据两点之间的流形距离来降维。
相比传统的线性降维方法如PCA,manifold-based方法的优点是可以保留非线性流形结构,更好地反映真实数据的内在低维分布。
典型的manifold-based方法还包括LLE(局部线性嵌入)、LE(拉普拉斯特征映射)等,它们虽然技术细节不同,但都遵循这个核心思路。
综上,manifold-based方法是一类非线性降维技术,通过假设数据分布在低维流形上,试图学习和保留数据的流形结构,比传统线性降维方法更好地反映数据的内在特征。
一次性使用工艺组件-ASMEBPE-2023新增内容解读
一次性使用工艺组件|ASMEBPE—2023新增内容解读加添了一次性使用部件和组件的要求,分为三个章节,分别是第七章一次性使用设计、第八章一次性使用工艺组件和第九章一次性使用的制造、组装和安装。
本文连续介绍第八章一次性使用工艺组件。
一次性使用工艺组件1.蒸汽直通和蒸汽直通连接器2.无菌连接器2.1制造商责任制造商应:(a)进行微生物侵入试验,以确认连接后无菌液路不会受到损害(b)定义连接器是干连接器还是湿连接器(1)干燥意味着液体不能进入连接器。
使用前,必需使用夹钳或其他合适的技术将液体与连接器隔离。
(2)湿意味着连接器中可以有液体进行连接。
(c)供给产品规格,包括但不限于以下内容:(1)温度额定值(2)压力额定值(3)灭菌方法的兼容性(例如,伽马灭菌,高压灭菌)(4)产品流路清洁度(微粒、内毒素、生物负载)(5)流速(d)定义连接器两半部分的性别(1)独。
特的阳半部分和阴半部分(2)没有性别,每一半都是一样的(e)定义连接是设计用于一次性连接还是多个连接(1)设计用于一次性连接的连接器应具有不可逆的锁定机制,除非其专门设计用于无菌断开。
(2)设计用于多重连接和断开的连接器应具有规定的最大连接数。
(f)供给装配说明,以确保正确连接2.2 全部者/用户责任全部者/用户应(a)依据全部适用过程和灭菌条件的服务要求,审查制造商的质量标准(b)确保由经过适当培训的操作员依照合格程序进行连接,以保持系统完整性3.柔性生物工艺容器(袋)3.1材料多层膜通常用于制造一次性袋。
制造商应确定袋的全部薄膜和连接层的构造材料。
对于预期用于过程接触的袋,制造商应识别全部材料(例如,重要材料、粘结层和添加剂),这些材料可能会掺杂袋内产品。
3.2确认制造商应供给一次性袋的工作温度和压力限值。
制造商应规定适当的灭菌方法,包括暴露范围、灭菌后有效期和其他限制。
制造商应供给处理和安全使用程序,包括悬挂限制、填充限制和二次密封建议。
Parker Hannifin 安全放流阀安装指南说明书
OperationPrior to installing safety relief valves the included safety bulletins must be read and understood.ENGLISHESPAÑOL InstallationSafety relief valves should not be discharged prior to installation. Do not install safety relief valves prior to pressure testing a system. If safety relief valves have been installed prior to a system pressure test, remove them. In the event there is a discharge prior or during installation the valve will need to be replaced or recertified.Do not attempt to change the pressure setting of the safety relief valves in the field.When installing a safety relief valve it must be in the vertical upright position and must follow the ANSI/ASHRAE 15 installation requirements for refrigeration systems.ServicePer IIAR, Bulletin 110, safety relief valves are to be replaced or tested and recertified every 5 years. After a discharge safety relief valves must then be replaced or recertified. Liquid safety relief valves do not have to be replaced after a discharge if the release is into the system, but the 5 year recertification or replacement policy still applies.Valves are required to be marked with the date of original manufacture, tagged with the date of manufacture and projected service/replacement date. Service can be performed at certified valve repair shops (VR). Refrigerating Specialties does not service or recertify valves in-house, but will provide repair kits to certified VR shops.A preventative maintenance schedule should be established for visual inspections and leaks. Vent lines shall be inspected to ensure they are clear and properly protected against ingress of moisture, which could freeze.H Safety Relief Valve FlangesThe R/S division of Parker Hannifin supplies flange bolt torque values that can be found in our Safety Procedures Bulletin. These values are offered as a reference, not a requirement, for installation and maintenance of product utilizing flanged connections supplied by the R/S Division.Proper alignment of the mating gasket flange surfaces and tightening bolts in a “crisscross” pattern to insure even gasket forces is accepted practice ofexperienced refrigeration technicians. In most cases, the use of a torque wrench is not required. We strongly recommend that all personal working on valves within a refrigeration system be properly trained to do so.For proper flange gasket sealing, care must be taken when threading or welding to assure flanges are parallel to each other and perpendicular to the pipe. Gaskets should be lightly oiled and all bolts must be tightened evenly.See bulletin 70-01, 71-00, 72-00, 72-10, 73-00 and 74-00 for information on the H, SR, SRH, CSR/CSRH, manifolds, and SRLQ valves.Safety Relief Valve Installation InformationFigure 1: CSR, CSRH & M1 SeriesFigure 2: SR, SRH, SR1R & M1 SeriesFigure 3: H, M2, M3 & M4 SeriesRefrigerantsSuitable for ammonia and halocarbonrefrigerantsTemperature Range-40ºC to 150ºC (-40ºF to 300ºF)Maximum Rated Pressure (MRP)27.6 barg (400 psig)Vapor Safety Relief Valves / ManifoldsConnection Types Female Pipe Threads (FPT)Material Valve Body - Ductile Iron Manifold Body - Ductile Iron Internal Components - Stainless Steel, PTFE O-Rings - Neoprene Gasket - Gylon 3504Bolts - Steel Grade 5, Zinc Plated Pipe Stubs - Schedule 80 Steel Figure 4: SRLQ SeriesRefrigerantsSuitable for ammonia and halocarbonrefrigerantsTemperature Range-29ºC to 94ºC (-20ºF to 200ºF)Maximum Rated Pressure (MRP)28 barg (400 psig)Liquid Safety Relief ValvesConnection Types Female Pipe Threads (FPT)Material Valve Body - Ductile Iron Internal Components - Stainless Steel, PTFE O-Rings - Neoprene Operación Antes de instalar las válvulas de seguridad se deben leer y entender los boletines de rmación de instalación de válvulas de seguridad Figura 1: Series CSR, CSRH & M1Figura 2: Series SR, SRH, SR1R & M1Figura 3: Series H, M2, M3 & M4Refrigerantes Adecuado para amoníaco y refrigerantes halocarbonos Rango de Temperatura -40ºC to 150ºC (-40ºF to 300ºF)Presión Máxima de Trabajo (MRP)27.6 barg (400 psig)Válvulas de Seguridad de Vapor / Válvulas de 3 Vías Tipo de Conexiónes Roscables: Female Pipe Threads (FPT)Material Curepo del la Válvula - Acero Dúctil Curepo del la Válvula de 3 Vías - Acero Dúctil Componentes Internos - Acero Inoxidable, PTFE Sellos - Neopreno Empaques - Gylon 3504Tornillos - Acero Grado 5, Zincado Terminación de Tubería - Acero, Cédula 80Válvulas de Seguridad de Líquido Figura 1: Series SRLQ Refrigerantes Adecuado para amoníaco y refrigerantes halocarbonos Rango de Temperatura -29ºC to 94ºC (-20ºF to 200ºF)Presión Máxima de Trabajo (MRP)28 barg (400 psig)Tipo de Conexiónes Roscables: Female Pipe Threads (FPT)Material Curepo del la Válvula - Acero Dúctil Compnentes Internos - Acero Inoxidable, PTFE Sellos - Neopreno Instalación Las válvulas de seguridad no deben ser desfogadas antes de la instalación. No instale válvulas de seguridad antes de la prueba de presión del sistema. Sí las válvulas de seguridad han sido instaladas antes de la prueba de presión del sistema, retírelas. En el caso de que haya un desfogue antes o durante la instalación de la válvula, esta deberá ser reemplazada o recertificada.No intente cambiar la presión de ajuste de las válvulas de seguridad en campo.Cuando se esté instalando una válvula de seguridad, esta debe estar en posición recta, vertical y debe seguir los requisitos de instalación ANSI / ASHRAE 15 para sistemas de refrigeración.Servicio Para el IIAR, en el Boletín 110, las válvulas de seguridad deben ser reemplazadas o evaluadas y certificadas cada 5 años. Después de un desfogue, las válvulas de seguridad deben de ser reemplazadas o recertificadas. Las válvulas de seguridad de líquido no tienen que ser reemplazadas después de un desfogue si la descarga es dentro del sistema, pero la política de recertificación o reemplazo cada 5 años continúa aplicás válvulas requieren estar marcadas con la fecha de fabricación original y se etiquetan con la fecha de fabricación y el plan de servicio/fecha de reemplazo. El servicio puede realizarse en talleres certificados en reparación de válvulas (RV). Especialidades en Refrigeración no repara o recertifica las válvulas en fábrica, pero puede proporcionar kits de reparación a talleres certificados (RV).Se recomienda establecer un programa de mantenimiento preventivo para inspecciones visuales e identificación de fugas. Las líneas de venteo deberán ser inspeccionadas para asegurar que estén limpias y adecuadamente protegidas contra infiltraciones de humedad, la cual podría congelarse.Bridas para Válvulas de Seguridad H La división R/S de Parker Hannifin proporciona valores de torque para los pernos de las bridas, disponibles en nuestro Boletín de Procedimientos de Seguridad. Estos valores se presentan como una referencia, no como un requisito para la instalación y el mantenimiento de los productos que utilizan conexión con bridas suministrados por la División de R/S.Verificar la alineación apropiada de la superficie de las juntas de las bridas de acoplamiento y los pernos de apriete de forma “entrecruzada” para asegurar inclusoel forzar las juntas, es una práctica aceptada para experimentados técnicos en refrigeración. En la mayoría de los casos, el uso de una llave de torsión no es nece-sario. Recomendamos que todo el personal que trabajan con válvulas dentro de un sistema de refrigeración debe estar adecuadamente entrenado para hacerlo.Para el sellado adecuado de la junta de la brida, se debe tener cuidado cuando se esté roscando o soldando para asegurar que las bridas son paralelas entre sí y perpendiculares a la tubería. Las juntas deben estar engrasadas ligeramente y todos los pernos se deben apretar de manera uniforme.Ver boletín 70-01, 71-00, 72-00, 72-10, 00 73 y 74-00 para información sobre las válvulas H, SR, SRH, CSR/CSRH, manifold y SRLQ中文安全阀安装说明安装安全阀在安装前不得被泄放压力。
数学专业英语第八讲附数学课程英文表达ppt
• 代数几何: 1、Harris,Algebraic Geometry: a first course:代数几何得入门教材; 2、Algebraic Geometry Robin Hartshorne :经典得代数几何教材,难度很高; 3、Basic Algebraic Geometry 1&2 2nd ed、 I、R、Shafarevich、:非常好得代数几 何入门教材; 4、Principles of Algebraic Geometry by giffiths/harris:全面、经典得代数几何参考 书,偏复代数几何; 5、mutative Algebra with a view toward Algebraic Geometry by Eisenbud:高级得 代数几何、交换代数得参考书,最新得交换代数全面参考; 6、The Geometry of Schemes by Eisenbud:很好得研究生代数几何入门教材; 7、The Red Book of Varieties and Schemes by Mumford:标准得研究生代数几何入 门教材; 8、Algebraic Geometry I : plex Projective Varieties by David Mumford:复代数几 何得经典。
数学专业英语第八讲附数学课程英文表达
• 数学类
• 第一学年 几何与拓扑: 1、James R、 Munkres, Topology
• 2、Basic Topology by Armstrong 3、Kelley, General Topology:
• 4、Willard, General Topology:一般拓扑学 5、Topology and geometry:
• 代数拓扑: 1、Algebraic Topology, A、 Hatcher:最新得研究生代数拓扑标准教材; 2、Spaniers “Algebraic Topology”:经典得代数拓扑参考书; 3、Differential forms in algebraic topology, by Raoul Bott and Loring W、 Tu:研究生代数拓扑标准教材; 4、Massey, A basic course in Algebraic topology:经典得研究生代数拓扑教材
ComplexGeometry
Complex GeometryA Conference in Honor ofDomingo Toledo’s60th BirthdayUniversity of UtahMarch24and25,2006AbstractsDaniel Allcock:A monstrous proposalA series of coincidences suggests an appearance of the monster simple group in the deck group of a branched cover of a particular arithmetic quotient of complex hyperbolic13-space,possibly with a moduli-space interpretation.Jim Carlson:New Hodge theory for cubic threefoldsThe moduli space of smooth cubic threefolds,like that of cubic surfaces,has a complex hyperbolic structure.That is,it can be realized as the quotient of the unit ball in a complex Euclidean space,minus a set of totally geodesic complex hyperplanes,modulo an arithmetic group.We discuss this construction and a natural partial compactification of it which is isomorphic to the ball modulo the group.Geometrically,the components added are(a)nodal cubics(b)the secant variety of a rational normal curve of degree four with a set of twelve points marked on it.The identification with a ball quotient involves two pieces of Hodge theory.First is the cyclic cover trick,which goes back to Picard and which was exploited by Deligne and Mostow in their study of moduli of points on the projective line and their relation to ball quotients.Second is a way of relating certain complex Hodge structures of weight four on a fourfold to other complex Hodge structures of weight one on an algebraic curve.(Joint work with Domingo Toledo and Daniel Allcock).Bill Goldman:Toledo’s invariant of surface group representations (tentative abstract)First,a historical account of early work of the author and of Toledo’s Math Scandinavica harmonic maps paper and how it led to the local rigidity of surface1groups in U(1,1)in U(n,1).This then led to Toledo’s global rigidity on surface group representations in U(n,1).I will also discuss connections with my work with Millson on higher dimensional local rigidity,which led into Corlette’s thesis on global rigidity.I may also try to survey some of the work in complex hyperbolic geometry(Parker,Falbel, Gusevskii)on the Toledo invariant and(maybe if time allows)work of Bradlow/Garcia-Prada/Gothen/Mundet/Xia on Higgs bundles.Luis Hern´a ndez:Almost-hermitian structures of minimal energyLet(M,g)be a compact Riemannian manifold and J an orthogonal almost-complex struc-ture on M.The energy of J is defined asE(J)=∇ω,Mwhereωis the K¨a hler form associated to J and g.Reminiscent of what happens in Yang-Mills theory,we show this energy decomposes into pieces according to a certain U n-representation(exactly two pieces when dim M=4), and a certain linear combination of such pieces(the difference of the two,in dimension4) turns out to be,not a topological invariant as in Yang-Mills theory,but a multiple of the total scalar curvature(and thus depending only on g)when the metric g happens to be conformallyflat(of ASD in dimension4).We’ll use this to give examples of minimal energy J,e.g.the almost-complex J given by Cayley multiplication on the round S6,the usual hermitian structure on S3×S1,etc.Misha Kapovich:Generalized triangle inequalities and their applications Abstract.Everybody knows how to construct triangles in the Euclidean plane given their side-lengths which satisfy the familiar triangle inequalities.In this talk I will explain how to generalize this in the setting of nonpositively curved symmetric spaces and buildings,where the real-valued distance function is replaced by an appropriate vector-valued function.If the time permits I will explain the relation of this problem to the geometric invariant theory and theoretical computer science.J´a nos Koll´a r:Holonomy groups of stable vector bundlesAbstract:We define the notion of holonomy group for a stable vector bundle F on a variety in terms of the Narasimhan–Seshadri unitary representation of its restriction to curves.Next we relate the holonomy group to the minimal structure group and to the decomposition of tensor powers of F.Finally we illustrate the principle that either the2holonomy is large or there is a clear geometric reason why it should be small.(Joint work with Balaji.)Bruno Klingler:On the Andre-Oort conjectureAbstract:The Andre-Oort conjecture describes the geometry of collection of special points on Shimura varieties:any irreducible component of the Zariski closure of a set of special points on a Shimura variety is conjectured to be a subvariety of Hodge type.I will explain a proof of this conjecture under the Generalized Riemann Hypothesis(joint work with Andrei Yafaev).Yum-Tong Siu:Multiplier ideal sheaves and thefinite generation of canon-ical ringstbaDennis Sullivan:Operations in the string spaces of a smooth manifold and compactified spaces of Riemann surfacesThere are canonical minimal energy area preservingflows on Riemann surfaces with input punctures where thefluid enters at given rates and output punctures where theflow exits at given rates.Theseflows are pictorially easy to analyze as the surface developes nodes. There are also versions on surfaces with boundary...The combinatorics of the orbits touching rest points of theflows leads to two discussions.Thefirst is a cell decomposition of the open moduli space of Riemann surfaces(discussed first by Giddings and Wolpert in a physics oriented paper and independently by C.F. Bodigheimer in a more precise mathematical treatment).The open moduli space cell discussion extends naturally to the nodal compactification of moduli space using the above mentioned pictures.The second discussion makes use of the combinatorics,in particular how theflow moves, splits and reconnects the orthogonal one manifolds to theflow,and regularized transversal-ity in families of poly curves in a manifold to construct operations in the algebraic topology of the free loop space as well as in that of path spaces with boundary conditions.The reg-ularization is a technical device which diffuses the objects acted upon using a measure on afinite dimensional space of diffeomorphisms constructed from a coordinate cover.3Anna Weinhard:Why you should maximize the Toledo invariantThe Toledo invariant associates a real number to every homomorphism of the fundamental group of a(closed)Riemann surface into a semisimple Lie group of Hermitian type.The Toledo invariant is locally constant and bounded.Homomorphisms which realize the max-imal possible value of the Toledo invariant were studied around15years ago by Goldman, Toledo and Hernandez.They showed that in many cases homomorphisms with maximal Toledo invariant have nice geometric properties.I will present recent work with Burger and Iozzi on homomorphisms of fundamental groups of(not necessarily closed)Riemann surfaces with maximal Toledo invariants extending their results.Our approach owes a lot to Toledo’s treatment of the problem when the Lie group of Hermitian type is the isometry group of a complex hyperbolic space.4。
四种木纤维表面接触角和表面自由能的比较
四种木纤维表面接触角和表面自由能的比较刘如;张智林【摘要】通过毛细管上升法测定了四种木纤维的表面接触角,并依据Washburn方程和Owens-Wendt法,对四种木纤维的表面自由能及其极性和非极性分量进行计算.结果表明,四种木纤维的表面自由能排序依次为:南方松>杉木>橡胶木>青杨.青杨和橡胶木体现分子非极性的色散力分量分别为5.19和6.59 mJ/m2,说明青杨和橡胶木表现出较强的极性.南方松和杉木的色散力分量分别为42.30和31.54mJ/m2,表现出较强的非极性.【期刊名称】《陕西林业科技》【年(卷),期】2016(000)003【总页数】4页(P20-23)【关键词】木纤维;接触角;表面自由能;极性;非极性【作者】刘如;张智林【作者单位】中国林业科学研究院木材工业研究所,北京海淀100091;陕西建森实业有限公司,西安710016【正文语种】中文【中图分类】TU366.3以天然植物纤维为原材料制备木质复合材料是近年来的研究热点[1-3]。
相比人工纤维,天然植物纤维具有可再生、可降解、来源广泛、密度低、强重比高以及价格较低廉等优点,因此,将其制备成为木质复合材料可以提高复合材料的附加值,使其应用于建筑、家具、园林、室内地板、装饰墙体等各个领域[4-6]。
常见的天然植物纤维包括木纤维、竹纤维、麻纤维、棉花纤维、秸秆纤维等,其中木纤维是制备木质复合材料最常用的一种天然植物纤维[7]。
由于各种木纤维之间的化学组分和微观结构存在着很大的差异,因此,在制备木质复合材料时会对木质复合材料的性能产生很大的影响[8]。
表面自由能是固体表面最基本的特性之一,它体现了固体表面的极性与非极性情况,与固体润湿性和粘结性等性能密切相关[9]。
因此,本研究采用毛细管上升法测定了四种市场上常见木纤维的接触角,包括两种针叶材木纤维(南方松与杉木)与两种阔叶材木纤维(青杨与橡胶木)。
依据Washburn方程和Owens-Wendt-Kaelble 法,对四种木纤维的表面自由能及其极性和非极性分量进行计算,旨在为研究和制备高性能的天然植物纤维复合材料提供基础的理论数据。
J. reine angew. Math. 549 (2002), 47—77 Journal für die reine und angewandte Mathematik (
J.reine angew.Math.549(2002),47—77Journal fu¨r die reine undangewandte Mathematik(Walter de GruyterBerlinÁNew York2002Discrete constant mean curvature surfaces andtheir indexBy Konrad Polthier at Berlin and Wayne Rossman at KobeAbstract.We define triangulated piecewise linear constant mean curvature surfaces using a variational characterization.These surfaces are critical for area amongst continuous piecewise linear variations which preserve the boundary conditions,the simplicial structures, and(in the nonminimal case)the volume to one side of the surfaces.We thenfind explicit formulas for complete examples,such as discrete minimal catenoids and helicoids.We use these discrete surfaces to study the index of unstable minimal surfaces,by nu-merically evaluating the spectra of their Jacobi operators.Our numerical estimates confirm known results on the index of some smooth minimal surfaces,and provide additional in-formation regarding their area-reducing variations.The approach here deviates from other numerical investigations in that we add geometric interpretation to the discrete surfaces.1.IntroductionSmooth submanifolds,and surfaces in particular,with constant mean curvature(cmc) have a long history of study,and modern work in thisfield relies heavily on geometric and analytic machinery which has evolved over hundreds of years.However,nonsmooth sur-faces are also natural mathematical objects,even though there is less machinery available for studying them.For example,consider M.Gromov’s approach of doing geometry using only a set with a measure and a measurable distance function[9].Here we consider piecewise linear triangulated surfaces—we call them‘‘discrete surfaces’’—which have been brought more to the forefront of geometrical research by com-puter graphics.We define cmc for discrete surfaces in R3so that they are critical for volume-preserving variations,just as smooth cmc surfaces are.Discrete cmc surfaces have both in-teresting di¤erences from and similarities with smooth ones.For example,they are di¤erent in that smooth minimal graphs in R3over a bounded domain are stable,whereas discrete minimal graphs can be highly unstable.We will explore properties like this in section2.In section3we will see some ways in which these two types of surfaces are similar. We will see that:a discrete catenoid has an explicit description in terms of the hyperboliccosine function,just as the smooth catenoid has;and a discrete helicoid can be described with the hyperbolic sine function,just as a conformally parametrized smooth helicoid is;and there are discrete Delaunay surfaces which have translational periodicities,just as smooth Delaunay surfaces have.Pinkall and Polthier [17]used Dirichlet energy and a numerical minimization proce-dure to find discrete minimal surfaces.In this work,we rather have the goal to describe dis-crete minimal surfaces as explicitly as possible,and thus we are limited to the more funda-mental examples,for example the discrete minimal catenoid and helicoid.We note that these explicit descriptions will be useful test candidates when implementing a procedure that we describe in the next paragraphs.Discrete surfaces have finite dimensional spaces of admissible variations,therefore the study of linear di¤erential operators on the variation spaces reduces to the linear algebra of matrices.This advantage over smooth surfaces with their infinite dimensional variation spaces makes linear operators easier to handle in the discrete case.This suggests that a useful procedure for studying the spectra of the linear Jacobi operator in the second variation formula of smooth cmc surfaces is to consider the corre-sponding spectra of discrete cmc approximating surfaces.Although similar to the finite ele-ment method in numerical analysis,here the finite element approximations will have geo-metric and variational meaning in their own right.As an example,consider how one finds the index of a smooth minimal surface,that is the number of negative points in the spectrum.The standard approach is to replace the metric of the surface with the metric obtained by pulling back the spherical metric via the Gauss map.This approach can yield the index:for example,the indexes of a complete catenoid and a complete Enneper surface are 1([7]),the index of a complete Jorge-Meeks n -noid is 2n À3([12],[11])and the index of a complete genus k Costa-Ho¤man-Meeks surface is 2k þ3for every k e 37([14],[13]).However,this approach does not yield the eigenvalues and eigenfunctions on compact portions of the original minimal surfaces,as the metric has been changed.It would be interesting to know the eigenfunctions associated to negative eigenvalues since these represent the directions of variations that reduce area.The above procedure of approximating by discrete surfaces can provide this information.In sections 5and 6we establish some tools for studying the spectrum of discrete cmc surfaces.Then we test the above procedure on two standard cases—a (minimal)rectangle,and a portion of a smooth minimal catenoid bounded by two circles.In these two cases we know the spectra of the smooth surfaces (section 4),and we know the discrete minimal sur-faces as well (section 3),so we can check that the above procedure produces good approx-imations for the eigenvalues and smooth eigenfunctions (section 7),which indeed must be the case,by the theory of the finite element method [4],[8].With these successful tests,we go on to consider cases where we do not a priori know what the smooth eigenfunctions should be,such as the Jorge-Meeks 3-noid and the genus 1Costa surface (section 7).The above procedure can also be implemented using discrete approximating surfaces which are found only numerically and not explicitly,such as surfaces found by the method in [17].And in fact,we use the method in [17]to find approximating surfaces for the 3-noid and Enneper surface and Costa surface.Polthier and Rossman,Curvature surfaces48We note also that Ken Brakke’s surface evolver software [3]is an e‰cient tool for numerical index calculations using the same discrete ansatz.Our main emphasis here is to provide explicit formulations for the discrete Jacobi operator and other geometric proper-ties of discrete surfaces.Many of the discrete minimal and cmc surfaces introduced here are available as in-teractive models at EG-Models [19].2.Discrete minimal and cmc surfacesWe start with a variational characterization of discrete minimal and discrete cmc sur-faces.This characterization will allow us to construct explicit examples of unstable discrete cmc surfaces.Note that merely finding minima for area with respect to a volume constraint would not su‰ce for this as that would produce only stable examples.We will later use these discrete cmc surfaces for our numerical spectra computations.The following definitions for discrete surfaces and their variations work equally well in any ambient space R n but for simplicity we restrict to R 3.Definition 2.1.A discrete surface in R 3is a triangular mesh T which has the topology of an abstract 2-dimensional simplicial surface K combined with a geometric C 0realization in R 3that is piecewise linear on each simplex.The geometric realization j K j is determined by a set of vertices V ¼f p 1;...;p m g H R 3.T can be identified with the pair ðK ;V Þ.The simplicial complex K represents the connectivity of the mesh.The 0,1,and 2dimensional simplices of K represent the vertices,edges,and triangles of the discrete surface.Let T ¼ðp ;q ;r Þdenote an oriented triangle of T with vertices p ;q ;r A V .Let pq denote an edge of T with endpoints p ;q A V .For p A V ,let star ðp Þdenote the triangles of T that contain p as a vertex.For an edge pq ,let star ðpq Þdenote the (at most two)triangles of T that contain the edge pq .Definition 2.2.Let V ¼f p 1;...;p m g be the set of vertices of a discrete surface T .A variation T ðt Þof T is defined as a C 2variation of the vertices p iFigure 1.At each vertex p the gradient of discrete area is the sum of the p 2-rotated edge vectors J ðr Àq Þ,as in Equation(1).p i ðt Þ:½0;e Þ!R 3so that p i ð0Þ¼p i E i ¼1;...;m :The straightness of the edges and the flatness of the triangles are preserved as the vertices move.In the smooth situation,the variation at interior points is typically restricted to nor-mal variation,since the tangential part of the variation only performs a reparametrization of the surface.However,on discrete surfaces there is an ambiguity in the choice of normal vectors at the vertices,so we allow arbitrary variations.But we will later see (section 7)that our experimental results can accurately estimate normal variations of a smooth surface when the discrete surface is a close approximation to the smooth surface.In the following we derive the evolution equations for some basic entities under sur-face variations.The area of a discrete surface isarea ðT Þ:¼PT A T area T ;where area T denotes the Euclidean area of the triangle T as a subset of R 3.Let T ðt Þbe a variation of a discrete surface T .At each vertex p of T ,the gradient of area is‘p area T ¼12P T ¼ðp ;q ;r ÞA star pJ ðr Àq Þ;ð1Þwhere J is rotation of angle p 2in the plane of each oriented triangle T .The first derivative of the surface area is then given by the chain ruled dt area T ¼P p A Vh p 0;‘p area T i :ð2ÞThe volume of an oriented surface T is the oriented volume enclosed by the cone of the surface over the origin in R 3vol T :¼16P T ¼ðp ;q ;r ÞA T h p ;q Âr i ¼13P T ¼ðp ;q ;r ÞA Th ~N ;p i Áarea T ;where p is any of the three vertices of the triangle T and~N¼ðq Àp ÞÂðr Àp Þ=jðq Àp ÞÂðr Àp Þj is the oriented normal of T .It follows thatPolthier and Rossman,Curvature surfaces50‘p vol T¼PT¼ðp;q;rÞA star p qÂr=6ð3Þandd dt vol T¼Pp A Vh p0;‘p vol T i:ð4ÞRemark2.1.Note also that‘p vol T¼PT¼ðp;q;rÞA star p À2Áarea TÁ~NþpÂðrÀqÞÁ=6.Furthermore,if p is an interior vertex,then the boundary of star p is closed and PT A star ppÂðrÀqÞ¼0.Hence the qÂr in Equation(3)can be replaced with2Áarea TÁ~N whenever p is an interior vertex.In the smooth case,a minimal surface is critical with respect to area for any variation thatfixes the boundary,and a cmc surface is critical with respect to area for any variation that preserves volume andfixes the boundary.We wish to define discrete cmc surfaces so that they have the same variational properties for the same types of variations.So we will consider variations TðtÞof T thatfix the boundary q T and that additionally preserve volume in the nonminimal case,which we call permissible variations.The condition that makes a discrete surface area-critical for any permissible variation is expressed in the fol-lowing definition.Definition2.3.A discrete surface has constant mean curvature(cmc)if there exists a constant H so that‘p area¼H‘p vol for all interior vertices p.If H¼0then it is minimal.This definition for discrete minimality has been used in[17].In contrast,our definition of discrete cmc surfaces di¤ers from[15],where cmc surfaces are characterized algorithm-ically using discrete minimal surfaces in S3and a conjugation pare also [2]for a definition via discrete integrable systems which lacks variational properties.Remark2.2.If T is a discrete minimal surface that contains a simply-connected dis-crete subsurface T0that lies in a plane,then it follows easily from Equation(1)that the dis-crete minimality of T is independent of the choice of triangulation of the trace of T0.2.0.1.Notation from th e th eoryoffinite elements.Consider a vector-valued functionv pj A R3defined on the n interior vertices V int¼f p1;...;p n g of T.We may extend thisfunction to the boundary vertices of T as well,by assuming v p¼~0A R3for each boundaryvertex p.The vectors v pj are the variation vectorfield of any boundary-fixing variation ofthe formp jðtÞ¼p jþtÁv pj þOðt2Þ;ð5Þthat is,p0jð0Þ¼v pj.We define the vector~v A R3n by~v t¼ðv t p1;...;v tp nÞ:ð6ÞThe variation vectorfield~v can be naturally extended to a piece-wise linear continuous R3-valued function v on T,with v in the following vector space:Polthier and Rossman,Curvature surfaces51Definition2.4.On a discrete surface T we define the space of piecewise linear functionsS h:¼f v:T!R3j v A C0ðTÞ;v is linear on each T A T and v j q T¼0g: This space is named S h,as in the theory offinite elements.Note that any compo-nent function of any function v A S h has bounded Sobolev H1norm.For each triangle T¼ðp;q;rÞin T and each v A S h,v j T ¼v p c pþv q c qþv r c r;ð7Þwhere c p:T!R is the head function on T which is1at p and is0at all other vertices ofT and extends linearly to all of T in the unique way.The functions c pj form a basis(withscalars in R3)for the3n-dimensional space S h.2.0.2.Non-uniqueness of discrete minimal disks.Uniqueness of a bounded mini-mal surface with a given boundary ensures that it is stable.For smooth minimal surfaces, uniqueness can sometimes be decided using the maximum principle of elliptic equations, which ensures that the minimal surface is contained in the convex hull of its boundary, and,if the boundary has a1-1projection to a convex planar curve,then it is unique for that boundary and is a minimal graph.The maximum principle also shows that any mini-mal graph is unique even when the projection of its boundary is not convex.More gener-ally,stability still holds when the surface merely has a Gauss map image contained in a hemisphere,as shown in[1](although their proof employs tools other than the maximum principle).However,such statements do not hold for discrete minimal surfaces.Consider the surface shown in the left-hand side of Figure2,whose height function has a local maxi-mum at an interior vertex.This example does not lie in the convex hull of its boundary and thereby disproves the general existence of a discrete version of the maximum principle.Also, the three surfaces on the right-hand side in Figure3are all minimal graphs over an annular domain with the same boundary contours and the same simplicial structure,and yet they are not the same surfaces,hence graphs with given simplicial structure are not unique.And the left-hand surface in Figure3is a surface whose Gauss map is contained in a hemisphere but which is unstable(this surface is not a graph)—another example of this property is the first annular surface in Figure3,which is also unstable.(We define stability of discrete cmc surfaces in section5.)The influence of the discretization on nonuniqueness,like as in the annular examples of Figure3,can also be observed in a more trivial way for a discrete minimal graph over a simply connected convex domain.The two surfaces on the right-hand side of Figure2have the same trace,i.e.they are identical as geometric surfaces,but they are di¤erent as discrete surfaces.Interior vertices may be freely added and moved inside the middle planar square without a¤ecting minimality(see Remark2.2).In contrast to existence of these counterexamples we believe that some properties of smooth minimal surfaces remain true in the discrete setting.We say that a discrete surface is a disk if it is homeomorphic to a simply connected domain.Conjecture2.1.Let T H R3be a discrete minimal disk whose boundary projects in-jectively to a convex planar polygonal curve,then T is a graph over that plane.The authors were able to prove this conjecture with the extra assumption that all the triangles of the surface are acute,using the fact that the maximum principle(a height function cannot attain a strict interior maximum)actually does hold when all triangles are acute.One can ask if a discrete minimal surface T with given simplicial structure and boundary is unique if it has a1-1perpendicular or central projection to a convex polygonal domain in a plane.The placement of the vertices need not be unique,as we saw in Remark 2.2,however,one can consider if there is uniqueness in the sense that the trace of T in R3is unique:Conjecture2.2.Let G H R3be a polygonal curve that eitherðAÞ:projects injec-tively to a convex planar polygonal curve,orðBÞ:has a1-1central projection from a point p A R3to a convex planar polygonal curve.Let K be a given abstract simplicial disk,and let g:q K!G be a given piecewise linear map.If T is a discrete minimal surface that is a geometric realization of K so that the map q K!q T equals g,then the trace of T in R3is uniquely determined.Furthermore,T is a graph in the caseðAÞ,and T is contained in the cone of G over p in the caseðBÞ.We have the following weaker form of Conjecture2.2,which follows from Corollary5.1of section5in the case that there is only one interior vertex:Conjecture 2.3.If a discrete minimal surface is a graph over a convex polygonal do-main ,then it is stable .3.Explicit discrete surfacesHere we describe explicit discrete catenoids and helicoids,which seem to be the first explicitly known nontrivial complete discrete minimal surfaces (with minimality defined variationally).3.1.Discrete minimal catenoids.To derive an explicit formula for embedded com-plete discrete minimal catenoids,we choose the vertices to lie on congruent planar polygo-nal meridians,with the meridians placed so that the traces of the surfaces will have dihedral symmetry.We will find that the vertices of a discrete meridian lie equally spaced on a smooth hyperbolic cosine curve.Furthermore,these discrete catenoids will converge uniformly in compact regions to the smooth catenoid as the mesh is made finer.We begin with a lemma that prepares the construction of the vertical meridian of the discrete minimal catenoid,by successively adding one horizontal ring after another starting from an initial ring.Since our construction will lead to pairwise coplanar triangles,the star of each individual vertex can be made to consist of four triangles (see Remark 2.2).We now derive an explicit representation of the position of a vertex surrounded by four such triangles in terms of the other four vertex positions.The center vertex is assumed to be coplanar with each of the two pairs of two opposite vertices,with those two planes becoming the plane of the vertical meridian and the horizontal plane containing a dihedrally symmetric polygonal ring (consisting of edges of the surface).See Figure 4.Lemma 3.1.Suppose we have four vertices p ¼ðd ;0;e Þ,q 1¼ðd cos y ;Àd sin y ;e Þ,q 2¼ða ;0;b Þ,and q 3¼ðd cos y ;d sin y ;e Þ,for given real numbers a ,b ,d ,e ,and angle y so that b 3e .Then there exists a choice of real numbers x and y and a fifth vertex q 4¼ðx ;0;y Þso that the discrete surface formed by the four triangles ðp ;q 1;q 2Þ,ðp ;q 2;q 3Þ,ðp ;q 3;q 4Þ,and ðp ;q 4;q 1Þis minimal ,i.e.‘p area ðstar p Þ¼0;if and only if2ad >ðe Àb Þ21þcos y:Figure 4.The construction in Lemma 3.1and a discrete minimal catenoid.Polthier and Rossman,Curvature surfaces54Furthermore,when x and y exist,they are unique and must be of the formx¼2ð1þcos yÞd3þðaþ2dÞðeÀbÞ2 2adð1þcos yÞÀðeÀbÞ2;y¼2eÀb:Proof.First we note that the assumption b3e is necessary.If b¼e,then one may choose y¼b,and then there is a free1-parameter family of choices of x,leading to a trivial planar surface.For simplicity we apply a vertical translation and a homothety about the origin of R3 to normalize d¼1,e¼0,and by doing a reflection if necesary,we may assume b<0.Let c¼cos y and s¼sin y.We derive conditions for the coordinate components of‘p area to vanish.The second component vanishes by symmetry of star ing the definitionsc1:¼ðaÀ1Þs2Àb2ð1ÀcÞffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2b2ð1ÀcÞþðaÀ1Þ2s2q;c2:¼abþbffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2b2ð1ÀcÞþðaÀ1Þ2s2q;thefirst(resp.third)component of‘p area vanishes ifc1¼y2ð1ÀcÞÀðxÀ1Þs2ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2y2ð1ÀcÞþðxÀ1Þ2s2q;resp:c2¼ÀðxÀ1ÞyÀ2yffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2y2ð1ÀcÞþðxÀ1Þ2s2q:ð8ÞDividing one of these equations by the other we obtainxÀ1¼c2yð1ÀcÞþ2c1c2sÀc1yy;ð9Þso x is determined by y.It now remains to determine if one canfind y so that c2s2Àc1y30.If xÀ1is chosen as in equation(9),then thefirst minimality condition of equation(8)holds if and only if the second one holds as well.So we only need to insert this value for xÀ1into thefirst minimality condition and check for solutions y.When c130, wefind that the condition becomes1¼c2s2Àc1yj c2s2Àc1y jyj y jÀð1ÀcÞy2À2s2ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2ð1ÀcÞc22s4þ4c21s2þÀ2ð1ÀcÞc21þs2ð1ÀcÞ2c22Áy2 q:SinceÀð1ÀcÞy2À2s2<0,note that this equation can hold only if c2s2Àc1y and y have opposite signs,so the equation becomes1¼ð1ÀcÞy2þ2s2ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2ð1ÀcÞc22s4þ4c21s2þÀ2ð1ÀcÞc21þs2ð1ÀcÞ2c22Áy2q;Polthier and Rossman,Curvature surfaces55which simplifies to1¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffið1ÀcÞy2þ2s2 pffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffið1ÀcÞc22s2þ2c21 q:This implies y2is uniquely determined.Inserting the valuey¼G b;onefinds that the above equation holds.When y¼b<0,wefind that c2s2Àc1y<0, which is impossible.When y¼Àb>0,wefind that c2s2Àc1y<0if and only if 2að1þcÞ>b2.And when y¼Àb and2að1þcÞ>b2,we have the minimality condition whenx¼2þ2cþab2þ2b2 2aþ2acÀb:Inverting the transformation we did at the beginning of this proof brings us back to the general case where d and e are not necessarily1and0,and the equations for x and y be-come as stated in the lemma.When c1¼0,we haveðaÀ1Þð1þcÞ¼b2andðxÀ1Þð1þcÞ¼y2,so,in particular, we have a>1and therefore2að1þcÞ>b2.The right-hand side of equation(8)implies y¼Àb and x¼a.Again,inverting the transformation from the beginning of this proof, we have that x and y must be of the form in the lemma for the case c1¼0as well.rThe next lemma provides a necessary and su‰cient condition for when two points lie on a scaled cosh curve,a condition that is identical to that of the previous lemma.That these conditions are the same is crucial to the proof of the upcoming theorem.Lemma3.2.Given two pointsða;bÞandðd;eÞin R2with b3e,and an angle y with j y j<p,there exists an r so that these two points lie on some vertical translate of the modified cosh curvegðtÞ¼0@r cosh teÀbarccosh1þ1rðeÀbÞ21þcos y!"#;t1A;t A R;if and only if2ad>ðeÀbÞ2 1þcos y.Proof.Define^d¼eÀb1þcos y.Without loss of generality,we may assume0<a e dand e>0,and henceÀe e b<e.If the pointsða;bÞandðd;eÞboth lie on the curve gðtÞ, thenarccosh1þ^d2r2!¼arccoshdrÀsignðbÞÁarccoshar;Polthier and Rossman,Curvature surfaces 56where signðbÞ¼1if b f0and signðbÞ¼À1if b<0.Note that if b¼0,then a must equalr(and so arccosh a r¼0).This equation is solvable(for either value of signðbÞ)if and only ifd r þffiffiffiffiffiffiffiffiffiffiffiffiffiffid2r2À1r!arþffiffiffiffiffiffiffiffiffiffiffiffiffia2r2À1r!¼1þ^d2r2þ^drffiffiffiffiffiffiffiffiffiffiffiffiffi2þ^d2r2swhen b e0,ord r þffiffiffiffiffiffiffiffiffiffiffiffiffiffid2rÀ1 sa r þffiffiffiffiffiffiffiffiffiffiffiffiffia2rÀ1s¼1þ^d2rþ^drffiffiffiffiffiffiffiffiffiffiffiffiffi2þ^d2rswhen b f0,for some r Að0;a .The right-hand side of these two equations has the follow-ing properties:(1)It is a nonincreasing function of r Að0;a .(2)It attains somefinite positive value at r¼a.(3)It is greater than the function2^d2=r2.(4)It approaches2^d2=r2asymptotically as r!0.The left-hand sides of these two equations have the following properties:(1)They attain the samefinite positive value at r¼a.(2)Thefirst one is a nonincreasing function of r Að0;a .(3)The second one is a nondecreasing function of r Að0;a .(4)The second one attains the value d=a at r¼0.(5)Thefirst one is less than the function4ad=r2.(6)Thefirst one approaches4ad=r2asymptotically as r!0.It follows from these properties that one of the two equations above has a solution for some r if and only if2ad>^d2.This completes the proof.rWe now derive an explicit formula for discrete minimal catenoids,by specifying the vertices along a planar polygonal meridian.Then the traces of the surfaces will have dihe-dral symmetry of order k f3.The surfaces are tessellated by planar isosceles trapezoids like a Z2grid,and each trapezoid can be triangulated into two triangles by choosing a di-Polthier and Rossman,Curvature surfaces57agonal of the trapeziod as the interior edge.Either diagonal can be chosen,as this does not a¤ect the minimality of the catenoid,by Remark 2.2.The discrete catenoid has two surprising features.First,the vertices of a meridian lie on a scaled smooth cosh curve (just as the profile curve of smooth catenoids lies on the cosh curve),and there is no a priori reason to have expected this.Secondly,the vertical spacing of the vertices along the meridians is constant.Theorem 3.1.There exists a four-parameter family of embedded and complete discrete minimal catenoids C ¼C ðy ;d ;r ;z 0Þwith dihedral rotational symmetry and planar meridians .If we assume that the dihedral symmetry axis is the z-axis and that a meridian lies in the xz-plane ,then ,up to vertical translation ,the catenoid is completely described by the following properties :(1)The dihedral angle is y ¼2p k,k A N ,k f 3.(2)The vertices of the meridian in the xz-plane interpolate the smooth cosh curvex ðz Þ¼r cosh 1raz ;witha ¼r d arccosh 1þ1r 2d 21þcos y!;where the parameter r >0is the waist radius of the interpolated cosh curve ,and d >0is the constant vertical distance between adjacent vertices of the meridian .(3)For any given arbitrary initial value z 0A R ,the profile curve has vertices of the form ðx j ;0;z j Þwithz j ¼z 0þj d ;x j ¼x ðz j Þ;where x ðz Þis the meridian in item 2above .(4)The planar trapezoids of the catenoid may be triangulated independently of each other (by Remark 2.2).Proof.By Lemma 3.1,if we have three consecutive vertices ðx n À1;z n À1Þ,ðx n ;z n Þ,and ðx n þ1;z n þ1Þalong the meridian in the xz -plane,they satisfy the recursion formulax n þ1¼ðx n À1þ2x n Þ^d 2þ2x 3n 2x n x n À1À^d 2;z n þ1¼z n þd ;ð10Þwhere d ¼z n Àz n À1and ^d¼d =ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi1þcos y p .As seen in Lemma 3.1,the vertical distance be-Polthier and Rossman,Curvature surfaces58。
带旋转自由度的四边形平板壳单元
边界上 的参数 F在 节点 i 为 - 1, 在节点 j 为 + 1, 取值范围为 - 1 [ F[ 1; l ij 是 ij 边的长度 . 1. 3 切线刚度推导 推导采用的是 U. L. 列式 . 几何方程为 9u 9x 9v 9y 9u 9v + 9y 9x 9H x 9x
y 9H 9y
a ( 4 , 5) = [ N 9 ( F ) - N 5( F ) ] sinA cos A a ( 4 , 9) = N 7 ( F ) cos A a ( 4 , 10) = N 6 ( F ) sin A+ N 10 ( F ) cos A a ( 4 , 11) = [ N 10 ( F ) - N 6( F ) ] sin A cos A a ( 5 , 1) = N 8 ( F ) sinA a ( 5 , 2) = [ N 9 ( F ) - N 5( F ) ] sinA cos A a ( 5 , 3) = N 5 ( F ) cos2 A+ N 9 ( F ) sin2 A a ( 5 , 9) = N 7 ( F ) sinA a ( 5 , 10) = [ N 10 ( F ) - N 6( F ) ] sin A cos A a ( 5 , 11) = N 6 ( F ) cos2 A+ N 10 ( F ) sin2 A a ( 6 , 1) = N 7 ( F ) sinA a ( 6 , 2) = - N 7 ( F ) cos A a ( 6 , 6) = N 9 ( F ) a ( 6, 7) = N 8 ( F ) sinA a ( 6 , 8) = - N 8 ( F ) cos A a ( 6 , 12) = N 10 ( F ) a 中未给出的值为 0. N 1 ( F ) ~ N 10 ( F )为
庞加莱猜想难题poincare
THE POINCAR´E CONJECTUREJOHN MILNOR1.IntroductionThe topology of two-dimensional manifolds or surfaces was well understood in the19th century.In fact there is a simple list of all possible smooth compact orientable surfaces.Any such surface has a well-defined genus g≥0,which can be described intuitively as the number of holes;and two such surfaces can be put into a smooth one-to-one correspondence with each other if and only if they have the same genus.1The corresponding question in higher dimensions is much moreFigure1.Sketches of smooth surfaces of genus0,1,and2.difficult.Henri Poincar´e was perhaps thefirst to try to make a similar study of three-dimensional manifolds.The most basic example of such a manifold is the three-dimensional unit sphere,that is,the locus of all points(x,y,z,w)in four-dimensional Euclidean space which have distance exactly1from the origin: x2+y2+z2+w2=1.He noted that a distinguishing feature of the two-dimensional sphere is that every simple closed curve in the sphere can be deformed continuously to a point without leaving the sphere.In1904,he asked a corresponding question in dimension3.In more modern language,it can be phrased as follows:2 Question.If a compact three-dimensional manifold M3has the property that every simple closed curve within the manifold can be deformed continuously to a point, does it follow that M3is homeomorphic to the sphere S3?He commented,with considerable foresight,“Mais cette question nous entraˆıne-rait trop loin”.Since then,the hypothesis that every simply connected closed 3-manifold is homeomorphic to the3-sphere has been known as the Poincar´e Con-jecture.It has inspired topologists ever since,and attempts to prove it have led to many advances in our understanding of the topology of manifolds.1For definitions and other background material,see,for example,[21]or[29],as well as[48].2See[36,pages498and370].To Poincar´e,manifolds were always smooth or polyhedral,so that his term“homeomorphism”referred to a smooth or piecewise linear homeomorphism.12JOHN MILNOR2.Early MisstepsFrom thefirst,the apparently simple nature of this statement has led mathe-maticians to overreach.Four years earlier,in1900,Poincar´e himself had been the first to err,stating a false theorem that can be phrased as follows.False Theorem.Every compact polyhedral manifold with the homology of an n-dimensional sphere is actually homeomorphic to the n-dimensional sphere.But his1904paper provided a beautiful counterexample to this claim,based on the concept of fundamental group,which he had introduced earlier(see[36, pp.189–192and193–288]).This example can be described geometrically as fol-lows.Consider all possible regular icosahedra inscribed in the two-dimensional unit sphere.In order to specify one particular icosahedron in this family,we must provide three parameters.For example,two parameters are needed to specify a single vertex on the sphere,and then another parameter to specify the direction to a neighboring vertex.Thus each such icosahedron can be considered as a single “point”in the three-dimensional manifold M3consisting of all such icosahedra.3 This manifold meets Poincar´e’s preliminary criterion:By the methods of homology theory,it cannot be distinguished from the three-dimensional sphere.However,he could prove that it is not a sphere by constructing a simple closed curve that cannot be deformed to a point within M3.The construction is not difficult:Choose some representative icosahedron and consider its images under rotation about one vertex through angles0≤θ≤2π/5.This defines a simple closed curve in M3that cannot be deformed to a point.Figure2.The Whitehead linkThe next important false theorem was by Henry Whitehead in1934[52].As part of a purported proof of the Poincar´e Conjecture,he claimed the sharper state-ment that every open three-dimensional manifold that is contractible(that can be continuously deformed to a point)is homeomorphic to Euclidean space.Following in Poincar´e’s footsteps,he then substantially increased our understanding of the topology of manifolds by discovering a counterexample to his own theorem.His counterexample can be briefly described as follows.Start with two disjoint solidtori T0and T1in the3-sphere that are embedded as shown in Figure2,so that each one individually is unknotted,but so that the two are linked together withlinking number zero.Since T1is unknotted,its complement T1=S3 interior( T1)3In more technical language,this M3can be defined as the coset space SO(3)/I60where SO(3) is the group of all rotations of Euclidean3-space and where I60is the subgroup consisting of the60 rotations that carry a standard icosahedron to itself.The fundamental groupπ1(M3),consisting of all homotopy classes of loops from a point to itself within M3,is a perfect group of order120.THE POINCAR ´E CONJECTURE 3is another unknotted solid torus that contains T 0.Choose a homeomorphism h of the 3-sphere that maps T 0onto this larger solid torus T 1.Then we can inductively construct solid toriT 0⊂T 1⊂T 2⊂···in S 3by setting T j +1=h (T j ).The union M 3= T j of this increasing sequence isthe required Whitehead counterexample,a contractible manifold that is not home-omorphic to Euclidean space.To see that π1(M 3)=0,note that every closed loop in T 0can be shrunk to a point (after perhaps crossing through itself)within the larger solid torus T 1.But every closed loop in M 3must be contained in some T j ,and hence can be shrunk to a point within T j +1⊂M 3.On the other hand,M 3is not homeomorphic to Euclidean 3-space since,if K ⊂M 3is any compact subset large enough to contain T 0,one can prove that the difference set M 3 K is not simply connected.Since this time,many false proofs of the Poincar´e Conjecture have been proposed,some of them relying on errors that are rather subtle and difficult to detect.For a delightful presentation of some of the pitfalls of three-dimensional topology,see [4].3.Higher DimensionsThe late 1950s and early 1960s saw an avalanche of progress with the discovery that higher-dimensional manifolds are actually easier to work with than three-dimensional ones.One reason for this is the following:The fundamental group plays an important role in all dimensions even when it is trivial,and relations between generators of the fundamental group correspond to two-dimensional disks,mapped into the manifold.In dimension 5or greater,such disks can be put into general position so that they are disjoint from each other,with no self-intersections,but in dimension 3or 4it may not be possible to avoid intersections,leading to serious difficulties.Stephen Smale announced a proof of the Poincar´e Conjecture in high dimensions in 1960[41].He was quickly followed by John Stallings,who used a completely different method [43],and by Andrew Wallace,who had been working along lines quite similar to those of Smale [51].Let me first describe the Stallings result,which has a weaker hypothesis and easier proof,but also a weaker conclusion.He assumed that the dimension is seven or more,but Christopher Zeeman later extended his argument to dimensions 5and 6[54].Stallings–Zeeman Theorem.If M n is a finite simplicial complex of dimension n ≥5that has the homotopy type 4of the sphere S n and is locally piecewise linearly homeomorphic to the Euclidean space R n ,then M n is homeomorphic to S n under a homeomorphism that is piecewise linear except at a single point.In other words,the complement M n (point )is piecewise linearly homeomorphic to R n .The method of proof consists of pushing all of the difficulties offtoward a single point;hence there can be no control near that point.4In order to check that a manifold M n has the same homotopy type as the sphere S n ,we must check not only that it is simply connected,π1(M n )=0,but also that it has the same homology as the sphere.The example of the product S 2×S 2shows that it is not enough to assume that π1(M n )=0when n >3.4JOHN MILNORThe Smale proof,and the closely related proof given shortly afterward by Wal-lace,depended rather on differentiable methods,building a manifold up inductively, starting with an n-dimensional ball,by successively adding handles.Here a k-handle can be added to a manifold M n with boundary byfirst attaching a k-dimensional cell,using an attaching homeomorphism from the(k−1)-dimensional boundary sphere into the boundary of M n,and then thickening and smoothing corners so as to obtain a larger manifold with boundary.The proof is carried out by rearranging and canceling such handles.(Compare the presentation in[24].)Figure3.A three-dimensional ball with a1-handle attachedSmale Theorem.If M n is a differentiable homotopy sphere of dimension n≥5, then M n is homeomorphic to S n.In fact,M n is diffeomorphic to a manifold obtained by gluing together the boundaries of two closed n-balls under a suitable diffeomorphism.This was also proved by Wallace,at least for n≥6.(It should be noted that thefive-dimensional case is particularly difficult.)The much more difficult four-dimensional case had to wait twenty years,for the work of Michael Freedman[8].Here the differentiable methods used by Smale and Wallace and the piecewise linear methods used by Stallings and Zeeman do not work at all.Freedman used wildly non-differentiable methods,not only to prove the four-dimensional Poincar´e Conjecture for topological manifolds,but also to give a complete classification of all closed simply connected topological4-manifolds.The integral cohomology group H2of such a manifold is free abelian.Freedman needed just two invariants:The cup productβ:H2⊗H2→H4∼=Z is a symmetric bilinear form with determinant±1,while the Kirby–Siebenmann invariantκis an integer mod2that vanishes if and only if the product manifold M4×R can be given a differentiable structure.Freedman Theorem.Two closed simply connected4-manifolds are homeomor-phic if and only if they have the same bilinear formβand the same Kirby–Sieben-mann invariantκ.Anyβcan be realized by such a manifold.Ifβ(x⊗x)is odd for some x∈H2,then either value ofκcan be realized also.However,ifβ(x⊗x) is always even,thenκis determined byβ,being congruent to one eighth of the signature ofβ.THE POINCAR´E CONJECTURE5 In particular,if M4is a homotopy sphere,then H2=0andκ=0,so M4 is homeomorphic to S4.It should be noted that the piecewise linear or differen-tiable theories in dimension4are much more difficult.It is not known whether every smooth homotopy4-sphere is diffeomorphic to S4;it is not known which4-manifolds withκ=0actually possess differentiable structures;and it is not known when this structure is essentially unique.The major results on these questions are due to Simon Donaldson[7].As one indication of the complications,Freedman showed,using Donaldson’s work,that R4admits uncountably many inequivalent differentiable structures.(Compare[12].)In dimension3,the discrepancies between topological,piecewise linear,and dif-ferentiable theories disappear(see[18],[28],and[26]).However,difficulties with the fundamental group become severe.4.The Thurston Geometrization ConjectureIn the two-dimensional case,each smooth compact surface can be given a beauti-ful geometrical structure,as a round sphere in the genus zero case,as aflat torus in the genus1case,and as a surface of constant negative curvature when the genus is2 or more.A far-reaching conjecture by William Thurston in1983claims that some-thing similar is true in dimension3[46].This conjecture asserts that every compact orientable three-dimensional manifold can be cut up along2-spheres and tori so as to decompose into essentially unique pieces,each of which has a simple geometri-cal structure.There are eight possible three-dimensional geometries in Thurston’s program.Six of these are now well understood,5and there has been a great deal of progress with the geometry of constant negative curvature.6The eighth geometry, however,corresponding to constant positive curvature,remains largely untouched. For this geometry,we have the following extension of the Poincar´e Conjecture. Thurston Elliptization Conjecture.Every closed3-manifold withfinite funda-mental group has a metric of constant positive curvature and hence is homeomorphic to a quotient S3/Γ,whereΓ⊂SO(4)is afinite group of rotations that acts freely on S3.The Poincar´e Conjecture corresponds to the special case where the groupΓ∼=π1(M3)is trivial.The possible subgroupsΓ⊂SO(4)were classified long ago by [19](compare[23]),but this conjecture remains wide open.5.Approaches through Differential Geometryand Differential Equations7In recent years there have been several attacks on the geometrization problem (and hence on the Poincar´e Conjecture)based on a study of the geometry of the infinite dimensional space consisting of all Riemannian metrics on a given smooth three-dimensional manifold.5See,for example,[13],[3],[38,39,40],[49],[9],and[6].6See[44],[27],[47],[22],and[30].The pioneering papers by[14]and[50]provided the basis for much of this work.7Added in20046JOHN MILNORBy definition,the length of a path γon a Riemannian manifold is computed,in terms of the metric tensor g ij ,as the integral γds = γ g ij dx i dx j .From the first and second derivatives of this metric tensor,one can compute the Ricci curvature tensor R ij ,and the scalar curvature R .(As an example,for the flat Euclidean space one gets R ij =R =0,while for a round three-dimensional sphere of radius r ,one gets Ricci curvature R ij =2g ij /r 2and scalar curvature R =6/r 2.)One approach by Michael Anderson,based on ideas of Hidehiko Yamabe [53],studies the total scalar curvature M 3R dV as a functional on the space of all smooth unit volume Riemannian metrics.The critical points of this functional are the metrics of constant curvature (see [1]).A different approach,initiated by Richard Hamilton studies the Ricci flow [15,16,17],that is,the solutions to the differential equationdg ij dt=−2R ij .In other words,the metric is required to change with time so that distances de-crease in directions of positive curvature.This is essentially a parabolic differential equationa and behaves much like the heat equation studied by physicists:If we heat one end of a cold rod,then the heat will gradually flow throughout the rod until it attains an even temperature.Similarly,a naive hope for 3-manifolds with finite fundamental group might have been that,under the Ricci flow,positive curvature would tend to spread out until,in the limit (after rescaling to constant size),the manifold would attain constant curvature.If we start with a 3-manifold of posi-tive Ricci curvature,Hamilton was able to carry out this program and construct a metric of constant curvature,thus solving a very special case of the Elliptization Conjecture.However,in the general case,there are very serious difficulties,since this flow may tend toward singularities.8I want to thank many mathematicians who helped me with this report.May 2000,revised June 2004References[1]M.T.Anderson,Scalar curvature,metric degenerations and the static vacuum Einstein equa-tions on 3-manifolds ,Geom.Funct.Anal.9(1999),855–963and 11(2001)273–381.See also:Scalar curvature and the existence of geometric structures on 3-manifolds ,J.reine angew.Math.553(2002),125–182and 563(2003),115–195.[2]M.T.Anderson,Geometrization of 3-manifolds via the Ricci flow ,Notices AMS 51(2004),184–193.[3]L.Auslander and F.E.A.Johnson,On a conjecture of C.T.C.Wall ,J.Lond.Math.Soc.14(1976),331–332.[4]R.H.Bing,Some aspects of the topology of 3-manifolds related to the Poincar´e conjecture ,in Lectures on Modern Mathematics II (T.L.Saaty,ed.),Wiley,New York,1964.[5]J.Birman,Poincar´e ’s conjecture and the homeotopy group of a closed,orientable 2-manifold ,J.Austral.Math.Soc.17(1974),214–221.8Grisha Perelman,in St.Petersburg,has posted three preprints on which go a long way toward resolving these difficulties,and in fact claim to prove the full geometrization conjecture[32,33,34].These preprints have generated a great deal of interest.(Compare [2]and [25],as well as the website /research/ricciflow/perelman.html organized by B.Kleiner and J.Lott.)However,full details have not appeared.THE POINCAR´E CONJECTURE7 [6] A.Casson and D.Jungreis,Convergence groups and Seifertfibered3-manifolds,Invent.Math.118(1994),441–456.[7]S.K.Donaldson,Self-dual connections and the topology of smooth4-manifolds,Bull.Amer.Math.Soc.8(1983),81–83.[8]M.H.Freedman,The topology of four-dimensional manifolds,J.Diff.Geom.17(1982),357–453.[9] D.Gabai,Convergence groups are Fuchsian groups,Ann.Math.136(1992),447–510.[10] D.Gabai,Valentin Poenaru’s program for the Poincar´e conjecture,in Geometry,topology,&physics,Conf.Proc.Lecture Notes Geom.Topology,VI,Internat.Press,Cambridge,MA, 1995,139–166.[11] D.Gillman and D.Rolfsen,The Zeeman conjecture for standard spines is equivalent to thePoincar´e conjecture,Topology22(1983),315–323.[12]R.Gompf,An exotic menagerie,J.Differential Geom.37(1993)199–223.[13] C.Gordon and W.Heil,Cyclic normal subgroups of fundamental groups of3-manifolds,Topology14(1975),305–309.[14]W.Haken,¨Uber das Hom¨o omorphieproblem der3-Mannigfaltigkeiten I,Math.Z.80(1962),89–120.[15]R.S.Hamilton,Three-manifolds with positive Ricci curvature,J.Differential Geom.17(1982),255–306.[16]R.S.Hamilton,The formation of singularities in the Ricciflow,in Surveys in differentialgeometry,Vol.II(Cambridge,MA,1993),Internat.Press,Cambridge,MA,1995,7–136. [17]R.S.Hamilton,Non-singular solutions of the Ricciflow on three-manifolds Comm.Anal.Geom.7(1999),695–729.[18]M.Hirsch,Obstruction theories for smoothing manifolds and maps,Bull.Amer.Math.Soc.69(1963),352-356.[19]H.Hopf,Zum Clifford–Kleinschen Raumproblem,Math.Ann.95(1925-26)313-319.[20]W.Jakobsche,The Bing-Borsuk conjecture is stronger than the Poincar´e conjecture,Fund.Math.106(1980),127–134.[21]W.S.Massey,Algebraic Topology:An Introduction,Harcourt Brace,New York,1967;Springer,New York1977;or A Basic Course in Algebraic Topology,Springer,New York, 1991.[22] C.McMullen,Riemann surfaces and geometrization of3-manifolds,Bull.Amer.Math.Soc.27(1992),207–216.[23]nor,Groups which act on S n withoutfixed points,Amer.J.Math.79(1957),623–630.[24]nor(with L.Siebenmann and J.Sondow),Lectures on the h-Cobordism Theorem,Princeton Math.Notes,Princeton University Press,Princeton,1965.[25]nor,Towards the Poincar´e conjecture and the classification of3-manifolds,NoticesAMS50(2003),1226–1233.[26] E.E.Moise,Geometric Topology in Dimensions2and3,Springer,New York,1977.[27]J.Morgan,On Thurston’s uniformization theorem for three-dimensional manifolds,in TheSmith Conjecture(H.Bass and J.Morgan,eds.),Pure and Appl.Math.112,Academic Press, New York,1984,37–125.[28]J.Munkres,Obstructions to the smoothing of piecewise-differentiable homeomorphisms,Ann.Math.72(1960),521–554.[29]J.Munkres,Topology:A First Course,Prentice–Hall,Englewood Cliffs,NJ,1975.[30]J.-P.Otal,The hyperbolization theorem forfibered3-manifolds,translated from the1996French original by Leslie D.Kay,SMF/AMS Texts and Monographs7,American Mathemat-ical Society,Providence,RI;Soci´e t´e Mathatique de France,Paris,2001.[31] C.Papakyriakopoulos,A reduction of the Poincar´e conjecture to group theoretic conjectures,Ann.Math.77(1963),250–305.[32]G.Perelman,The entropy formula for the Ricciflow and its geometric applications,arXiv:math.DG/0211159v1,11Nov2002.[33]G.Perelman,Ricciflow with surgery on three-manifolds,arXiv:math.DG/0303109,10Mar2003.[34]G.Perelman,Finite extinction time for the solutions to the Ricciflow on certain three-manifolds,arXiv:math.DG/0307245,17Jul2003.8JOHN MILNOR[35]V.Po´e naru,A program for the Poincar´e conjecture and some of its ramifications,in Topicsin low-dimensional topology(University Park,PA,1996),World Sci.Publishing,River Edge, NJ,1999,65–88.[36]H.Poincar´e,Œuvres,Tome VI,Gauthier–Villars,Paris,1953.[37] C.Rourke,Algorithms to disprove the Poincar´e conjecture,Turkish J.Math.21(1997),99–110.[38]P.Scott,A new proof of the annulus and torus theorems,Amer.J.Math.102(1980),241–277.[39]P.Scott,There are no fake Seifertfibre spaces with infiniteπ1,Ann.Math.117(1983),35–70.[40]P.Scott,The geometries of3-manifolds,Bull.Lond.Math.Soc.15(1983),401–487.[41]S.Smale,Generalized Poincar´e’s conjecture in dimensions greater than four,Ann.Math.74(1961),391–406.(See also:Bull.Amer.Math.Soc.66(1960),373–375.)[42]S.Smale,The story of the higher dimensional Poincar´e conjecture(What actually happenedon the beaches of Rio),Math.Intelligencer12,no.2(1990),44–51.[43]J.Stallings,Polyhedral homotopy spheres,Bull.Amer.Math.Soc.66(1960),485–488.[44] D.Sullivan,Travaux de Thurston sur les groupes quasi-fuchsiens et sur les vari´e t´e s hyper-boliques de dimension3fibr´e es sur le cercle,S´e m.Bourbaki554,Lecture Notes Math.842, Springer,New York,1981.[45]T.L.Thickstun,Open acyclic3-manifolds,a loop theorem and the Poincar´e conjecture,Bull.Amer.Math.Soc.(N.S.)4(1981),192–194.[46]W.P.Thurston,Three dimensional manifolds,Kleinian groups and hyperbolic geometry,inThe Mathematical heritage of Henri Poincar´e,Proc.Symp.Pure Math.39(1983),Part1.(Also in Bull.Amer.Math.Soc.6(1982),357–381.)[47]W.P.Thurston,Hyperbolic structures on3-manifolds,I,deformation of acyclic manifolds,Ann.Math.124(1986),203–246[48]W.P.Thurston,Three-Dimensional Geometry and Topology,Vol.1,ed.by Silvio Levy,Princeton Mathematical Series35,Princeton University Press,Princeton,1997.[49]P.Tukia,Homeomorphic conjugates of Fuchsian groups,J.Reine Angew.Math.391(1988),1–54.[50] F.Waldhausen,On irreducible3-manifolds which are sufficiently large,Ann.Math.87(1968),56–88.[51] A.Wallace,Modifications and cobounding manifolds,II,J.Math.Mech10(1961),773–809.[52]J.H.C.Whitehead,Mathematical Works,Volume II,Pergamon Press,New York,1962.(Seepages21-50.)[53]H.Yamabe,On a deformation of Riemannian structures on compact manifolds,Osaka Math.J.12(1960),21–37.[54] E.C.Zeeman,The Poincar´e conjecture for n≥5,in Topology of3-Manifolds and RelatedTopics Prentice–Hall,Englewood Cliffs,NJ,1962,198–204.(See also Bull.Amer.Math.Soc.67(1961),270.)(Note:For a representative collection of attacks on the Poincar´e Conjecture,see [31],[5],[20],[45],[11],[10],[37],and[35].)。
MOTORVAC 技术公司 SteerClean 1000 电动助力系统服务系统 操作手册说明书
MOTORVAC TECHNOLOGIES INC. SteerClean 1000 Power Steering Service SystemOperator ManualTableContentsofIntroduction (3)Overview (4)System Features and Functions......................................................................................................1-1 Control Panel Features and Functions.........................................................................................1-2 Left View.......................................................................................................................................1-3 RightView…………………………………………………………………………………………………...............................................................................................................................................1-4 Safety Information.............................................................................................................................2-1 Before You Begin..............................................................................................................................3-1 First Time Operation.....................................................................................................................3-1 Service Procedure.............................................................................................................................4-1 Selling the SteerClean Service........................................................................................................5-1 Troubleshooting and Additional Help.............................................................................................6-1 Appendix A - Maintenance...............................................................................................................A-1 Maintenance Procedures..............................................................................................................A-1 Cleaning the Unit’s Filter Screen………………………………………………………………………....................................................A-1 Maintenance Record.....................................................................................................................A-3 Appendix B - System Accessories..................................................................................................B-1 Adapter Kits………………………………………………………………………………………..……..B-1Appendix C - Parts............................................................................................................................C-1 Service Parts ...............................................................................................................................C-1 OrderingParts……………………………………………………………………………………………...............C-1IntroductionCongratulations on your selection of the MotorVac STEERCLEAN Service System. By choosing this product, you are acquiring the most technologically advanced method available for power steering service and fluid exchange.The STEERCLEAN System is a self-contained system; designed to service virtually all power steering systems. Once the unit is connected, it can be used to exchange all the old power steering fluid with new, while flushing and conditioning the fluid at the same time.With the engine idling, simply follow the simple instructions on the control panel. The STEERCLEAN Service System is designed to be fast, easy, and highly profitable. How profitable is up to you! Every car or truck that comes into your shop with over 30,000 miles is a potential customer. This service is also recommended every two years. But the key to profit is to sell the service, so we have included a detailed sales procedure at the end of this manual.It is recommended that a vehicle’s power steering system be serviced every 30,000 miles or every two years (Or according to the vehicle owner’s manual) to obtain the highest lubricant protection, to reduce friction and wear from internal components, and thus increase the efficiency and life span of the power steering system to it’s maximum.Please study this Operators Manual to become thoroughly familiar with the STEERCLEAN Power Steering Service System.IMPORTANTUse of other chemicals during this process may cause operational failure of the STEERCLEAN System and voids the manufacturer’s warranty.See warranty card for details.OverviewThis manual contains all the information you need to use the STEERCLEAN System. Please make sure all technicians using the unit read this manual and have it within easy reach whenever the unit is being used.The following is a quick reference to the information in this manual:System Features and FunctionsThis chapter describes the STEERCLEAN Service System’s Switches, Lights andConnections.Safety InformationAdhere to the safety guidelines in this chapter at all times!Before You BeginFollow the instructions in this chapter before using the unit for the first time.Service ProcedureThis chapter contains step-by-step setup and service procedure for using the unit to flush the vehicle’s power steering system fluid completely.Frequently Asked QuestionsHelpful information to common questions.Troubleshooting and Additional HelpTurn to this chapter in the unlikely event you have problems with your STEERCLEANSystem or need additional help.Appendices - Maintenance, Accessories, and PartsThe appendices contain routine maintenance procedures for the STEERCLEAN System,such as cleaning the filter screen, lists of available accessories, replacement parts.System Features and FunctionsThe front of the MotorVac SteerClean 1000 cabinet showing the control panel, Clean fluid tank, & service hoses.Control Panel Features and FunctionsA. Start Button Press the Start button to begin the service, (or continue theservice if paused).B. POWER light Illuminates when power cord is hooked up to 12V. source.C. Service light Illuminates when start switch is in “RUN” and pumps are on.D. Circuit Breaker 15 Amp circuit breaker.E. OperatingInstructions Basic Operating Instructions.A. Waste Tank Captures waste fluid.B. Service Hose Fluid hose for clean and dirty fluid transfer.C. Mini-Wand Inserts into Power Steering Fluid Reservoir.Right ViewA. Clean Fluid tank Holds the cleaner and new fluid.B. Power CordPower cord for hooking up to 12 V. BatteryBSafety Information and Precautions/!\ DANGERVehicle exhaust gases contain Carbon Monoxide, which is a colorless and odorless lethal gas.Only run engines in well-ventilated areas and avoid breathing exhaust gases.Extended breathing of exhaust gases will cause serious injury or death./!\ WARNINGExhaust gases, moving parts, hot surfaces are present during and after the vehicle’s engine is running. This list is by no means complete. Always pay close attention to the job at hand and obey all safety procedures. Read and understand the operator’s manual before using the STEERCLEAN Service system.When using petroleum products always refer to the MSDS sheets and manufacturer’s instructions for the proper procedure to handle emergency medical treatment, cleanup, handling, and storage requirements.Improper use of the STEERCLEAN Service System can cause injury.Spilled service fluid on an engine can ignite.Avoid exposure to flames, sparks, hot engine parts, and other ignition sources.Always keep fully charge fire extinguisher nearby. The extinguisher should have a class B rating and be suitable for gasoline, chemical, and electrical fires.Cleanup any oil spills immediately.Dispose of contaminated cleanup material according to governing environmental laws.Never look directly into the air induction plenum or carburetor throat when the engine is operating.Explosion or flame or exposure to flammable liquid and vapors can cause injury.Flammable liquid (service fluid) can splash out of reservoir when filling. Steering Fluid temperatures can reach in excess of 350°F, which can cause serious injury to the human body.Always keep Reservoir Cap secure except when filling reservoir.Explosion or flame can cause injury.Power steering systems may maintain residual pressure in connection lines to and from pump even after the engine has been turned off.Wear safety goggles.Wear chemical resistant gloves when connecting or disconnecting fitting and adapters.Do not swallow or ingest any chemicals.Use with adequate ventilation. Avoid breathing vapors.Improper use of service fluid can cause injury.Over exposure can have harmful effect on eyes, skin, respiratory system and possible unconsciousness and asphyxiation.Improperly blocked vehicles can move.Set the parking brake and chock the wheels.Moving vehicles can cause injury.Moving engine parts.The engine cooling fan will cycle on and off depending on the coolant temperature and could operate without the engine running.Wear safety goggles.Always keep objects, clothing, and hands away from the cooling fans and engine parts.Moving engine parts can cause injury.Hot surfaces are present during and after running the engine.Do not contact hot surfaces such as, manifolds, pipes, mufflers, catalytic converters, or radiators and hoses.Hot surfaces can cause injury.Catalytic converters become extremely hot.Do not park a converter-equipped vehicle over dry grass, leaves, paper, or any other flammable material.Do not touch a catalytic converter until the engine has been off for at least 45 minutes.Catalytic converters can cause burns.Cracked fan blade can become airborne.Examine fan blades for cracks. If found, do not service the vehicle.Flying objects can cause injury.Batteries produce explosive gases and can explode, resulting in injury.Wear safety goggles when working on or near batteries.Use in a well-ventilated area.Keep sparks and flames away from the battery and never lay tools, equipment, or other conductive objects on the battery.When is connecting to the battery, make sure the unit’s power switch is off. Connect the positive lead of the unit to the positive lead battery first; connect the negative lead of the unit to a solid ground point as far from the battery as possible.Keep battery acid away from skin or eyes. In case of eye contact, flush with clean water for 15 minutes and get medical attention.Always use a fender cover when working under the hood, to protect vehicles finish.Rinse any spills with water immediately.Before You BeginFirst Time OperationNOTEThis unit has been tested with Power Steering Fluid, and is readyfor service after receiving inspection of the unit. Operate in above50 degrees Fahrenheit area. Remember to send in your warrantycard.NOTECheck the output/return hoses, battery connections,and all external components for damage.Beginning the Service……Performing a Standard Fluid Exchange:1. Connect the power cord to 12 V. battery.(red+ black-).2. Pour the power steering “flush” fluid into the clean fluid tank.3. Verify that the cap is installed on the waste fluid tank.4. Start the vehicles engine.5. Insert the service hose “wand” into the vehicles power steering fluid reservoir.(fill level is controlled by the position of the short hose of the wand).6. Turn the service switch to “run” position.7. When the clean tank is emptly, turn the service switch to “off”.8. Turn the vehicles steering wheel fully right and left 3 times.9. Turn off vehicle.10. Pour Conditioner into “new” fluid tank and fill the tank with steering fluidrecommended for vehicle. (Do not exceed 2000 ml level on tank).11. Check level in waste tank to verify that there is enough ‘empty’ space to receivethe amount of fluid in clean tank. If necessary, empty waste tank and replace capbefore continuing.12. Repeat steps 4 thru 9.13. Check fluid level in vehicles reservoir, top off if necessary.14. Empty waste fluid tankThe Sale: Since the MotorVac SteerClean Power Steering Fluid Exchange Service System is new, virtually every car or truck with at least 30,000 miles is a potential candidate for this service. You can sell the service based on fluid condition or mileage. To sell based on fluid condition, place a drop of the customer’s power steering fluid on a clean rag or piece of paper, and then place a drop of new fluid next to it. Show this to the customer. Explain that the old fluid is burnt, dirty, and contaminated. It is no longer able to provide the lubrication and protection needed. Over time, the fluid will damage power steering components, leading to failure. To sell based on mileage, you’re on solid ground by recommending the service as regular maintenance. Some auto manufactures are recommending the power steering fluid be replaced every 30,000 miles. Just as automatic transmissions require regular fluid replacement, so do power steering fluids.The Six Most Common Objections:1 – “I’ve never heard of servicing the power steering system.”Your reply: Until recently, there was never a practical cost effective way to replace power steering fluid. With the MotorVac SteerClean System, you actually introduce a cleaning agent first (p.n.400-0160 flush), and then flush the system completely with MotorVac’s(p.n. 400-0154 conditioner) and Power Steering Fluid. In under ten minutes, your power steering system protected with the necessary conditioners and lubricants.2 – “I can’t afford it.”Your reply: With the high cost of labor and parts especially for a power steering rack or power steering pump, how can you not afford it? We can offer you a special price today to close the deal.3 – “The cars not worth it.”4 – “It’s a lease car, why spend the money?”Your reply: (Treat both 3 & 4 the same) Servicing your car’s power steering system isn’t about the car; it’s about your safety, and the safety of your family. Consider how a power steering failure could impact your life.5 – “ I’m getting rid of the car soon.”Your reply: To get the most out of your sale, show the buyer that you have done everything possible to keep the car in good running condition, including servicing the power steering system.6 – “ Why doesn’t my owners manual say anything about it?” Your reply: Some major auto manufacturers are recommending servicing the power steering. Others will probably follow soon. We recommend the MotorVac SteerClean Service to keep your cars power steering system like new!Follow up: Always answer any questions as truthfully as possible, and then always come back to the sales question: Can we take care of that for you now?Once his objectives have been satisfied, you have good chance of selling the service.Troubleshooting and Additional HelpRefer to the list below in the unlikely event that you have problems with your SteerClean Power Steering Service System.Problem:Solution:1. Unit does not power-up. -Inspect power cord for breaks-Reset Circuit Breaker2. vacuum or fill pump inop. -check wiring or switch.3. Slow flow -check service filterADDITIONAL HELPPlease verify that items above have been reviewed before callingfor additional assistance.In the unlikely event that problems persist with the unit callTechnical Support, have your model and serial numbers availablebefore you call. Remember to send in your warranty card.In the U.S. Canada:localyour(800)Contact841-8810(714) 558-4822 MotorVac distirbutorAppendix A - MaintenanceMaintenance ProceduresThe following maintenance procedures should be performed on a routine basis:1. Carefully clean the exterior with a soft cloth to keep the cabinet looking new.2. Check all hoses and wires for cuts or frays.3. Clean the unit’s filter screen after every 100 services or6 months, which ever comes first. See the next section for procedure.Cleaning The Unit’s Filter1. Remove the back panel.2. Place suitable catch tray under filter assembly.3. Filter is the Plastic ‘dome’ located in the hose from the tank.4. Hold the bottom half of the filter while rotating the other half of the filtercounter-clockwise until the four lock tabs clear. (Press & turn like a radiator cap) Then separate the two pieces by lifting by pulling apart.5. Use a fine pick or bent pin to pull screen away from the filter housing. Cleanscreen.6. Assemble in reverse order. NOTE: Use caution not to pinch o’ring onreassembly7. Enter initials, date, and a check mark in the appropriate boxes of theMaintenance Record at the end of the chapter.Maintenance RecordUse the following table to keep a record of maintenance performed on the unit.Initial/Date DRAIN WASTETANK9CLEANEDFILTER9CLEAN EXT.CABINET9CHECK HOSESAND WIRES9OTHER9/ / / / / / / / / / / / / / / / / /IIII /Standard Adapters080-2607Appendix C – PartsService Parts for the SteerClean Power Steering Service System. Please refer to the part numbers below when ordering parts for this unit.Part #Description010-0027 Wheel (8 x 1.75)010-0026 Hub cap (Black Plastic)040-0604 Cap Nut (½” ID – Push 0n)040-0507 Axle Bushing (Black Nylon)010-5500 Axle, Rear Wheels (½” x 20.875 lg.)010-5004 Hosebracket020-8043 Harness, External Power050-1000 Screen filter- inline, ½ MPT. Pp.050-3013 Check valve (1psi), (disposal hose)200-4063 Output/Return Service hose assembly / Clear Braided080-6009 Hose Clamp, 3/8”( Crimp Style, Steel )080-6016 Hose Clamp, 1/4”( Crimp Style, Steel )200-4064 Disposal hose assemblyManual200-8917 Operators010-5627 Mini-Wand (Standard)ORDERING PARTSParts for the unit may be ordered by calling CustomerService, have your model and serial numbers available:inside U.S.A. Canada:(800) 841-8810 Contact your local(714) 558-4822 MotorVac distributor。
楔形空间中圆弧形沉积对平面SH波的散射解析解
楔形空间中圆弧形沉积对平面SH波的散射解析解刘中宪;梁建文【摘要】为揭示楔形空间中沉积谷地对地震动的显著影响,基于大圆弧假定,利用Fourier-Bessel波函数展开,采用一种新方法求解了楔形空间中圆弧形沉积对平面SH波的散射问题.首先利用2个大圆弧面模拟地表面,以方便构造地表面引起的散射波场.然后由连续性边界条件建立方程并求解得出该问题的解析解,通过同现有结果的对比,验证该方法的计算精度,进而进行详细的参数分析.计算结果表明,楔形空间中沉积附近地表位移反应特征依赖于波入射角、入射波频率、楔形夹角及沉积内外的材料特性,位移放大效应比半空间情况更为显著,因而需适当提高此类场地上建筑物的抗震设防标准.【期刊名称】《天津大学学报》【年(卷),期】2010(000)007【总页数】10页(P573-582)【关键词】楔形空间;沉积谷地;平面SH波;散射;解析解【作者】刘中宪;梁建文【作者单位】天津大学建筑工程学院,天津300072;天津大学建筑工程学院,天津300072【正文语种】中文【中图分类】TU352.1多次的地震观测以及理论研究均表明沉积谷地或盆地对地震动具有显著的影响.自20世纪 70年代以来,国内外多位学者对相关问题进行了研究分析.求解方法主要有解析法[1-6]和数值法[7-11].解析法主要是波函数展开法,数值法则包括域内离散型的有限差分法、有限元法和边界离散型的边界元法、离散波数法和波源法等.值得指出的是,上述研究一般是基于半空间假定.而在我国重庆、青岛、大连等地有大量建筑座落在山坡、山顶或者近海高岸上.此类地形宏观上一般可简化为楔形或阶梯场地.该地形中沉积谷地对地震动的影响一方面源于沉积对地震波的散射,另一方面还源于特殊地形本身对地震动的放大作用.这同半空间情况有着本质的不同,在问题的处理上也更为复杂.迄今为止,国内外有关楔形空间局部场地反应问题的研究成果较少.基于 MacDonald对电磁波的研究成果,Sanchez-Sesma[12]首先研究了 SH波在楔形空间中的衍射.而后Lee等[13-14]给出了楔形空间中圆弧形峡谷和沉积对平面 SH波的散射解答.Dermendjian等[15-16]采用矩量法研究了楔形空间中任意形状凹陷地形和刚性基础对 SH波的散射.史文谱等[17-18]则采用复变函数法分别求解了楔形空间中(直角情况)固定圆形夹杂和圆孔对SH波的散射.综上,目前的研究多以SH波的散射为对象,对于P、SV 波入射情况则研究很少(严格满足楔形空间边界条件的散射波函数难以精确构造).Lee的方法[14]同样仅适用于SH波入射情况,且求解中散射体圆心须位于楔形顶点处.为此,笔者借鉴文献[3]的思路,采用2个大圆弧面分别模拟楔形空间的2个表面,对楔形空间中局部场地反应问题给出了一种有效的求解方法.该方法避免了楔形空间中散射波构造上的困难,使得散射波函数易于表达且边界条件容易处理,因而适用于楔形空间中任意波型输入情况,且散射体位置比较灵活.笔者以 SH波入射为例,给出了问题求解的思路和过程,并进行了方法验证和数值分析.1 模型及方法如图1所示,一圆弧形沉积位于楔形空间顶部附近.设楔形空间斜面与水平面夹角为vπ,圆弧半径为a.为方便推导,假定圆心位于楔形空间顶点O处.为方便地利用边界条件和构造散射波场,由两半径非常大的圆弧面Ⅰ和Ⅱ来分别模拟楔形空间的水平面和倾斜面,圆弧半径均取为d,圆心分别位于 1O、2O处.假设沉积内外介质均为弹性、均匀和各向同性,剪切模量和密度分别为vμ、vρ和sμ、sρ,下标v代表沉积介质,s代表沉积外介质.vβ、sβ为相应剪切波速.为方便问题求解,在这里设定了 3套极坐标系:O-θ,1O-1θ和2O-2θ.图1 楔形空间中沉积谷地计算模型Fig.1 Computational model for the alluvial valley in wedge-shaped space设楔形空间内入射波为 w ( i),比拟光的几何传播路线(射线理论).由于楔形空间的特殊性,楔形空间内会存在二次反射波,即一个平面上的反射波在另一平面上的再次反射.设波在水平面上的初次反射波为,该反射波在倾斜面上的二次反射设为;同理,设倾斜面上的初次反射波为,该反射波在水表面上的二次反射设为.由简单的几何推导,二次反射波的存在范围不难确定.楔形空间中总位移波场 (t)w 在极坐标系r-O-θ中满足波动方程1.1 波场分析坐标O-θ下,各入射、反射波函数可以表示为式中:sk为沉积外楔形空间内横波波数,ss/kωβ=;vk为沉积内横波波数,vv/kωβ=.时间因子exp(i)tω−已略去.坐标 1 1-O θ下,沉积内外大圆弧面Ⅰ上散射波可以分别表示为坐标 2 2-O θ下,沉积内外大圆弧面Ⅱ上散射波可以分别表示为沉积内外圆弧界面上散射波为以上各式中Jm(kr)和 H (m1 )(kr)分别表示第一类 Bessel和第一类Hankel函数.综上,沉积内外总波场可分别表示为式中 (r)w 为楔形空间中几种反射波的组合.1.2 模型求解问题的边界条件包括楔形空间表面零应力沉积内表面表面零应力以及圆弧交界面上位移及应力连续条件为利用位移和应力连续性条件(17),需采用Graf加法公式进行坐标转换,将各散射波系数转化到 -Oθ坐标下.限于篇幅,具体步骤从略.利用恒等变换则入射反射波可以统一用级数形式表示为由连续性边界条件最终可以推得出同理为利用边界条件(15)和(16),需将总波场分别转换到O1-θ1和O2-θ2下,从而得到另两组方程.最后问题归结为求解一无穷项数线性方程组,保证边界条件满足一定精度,通过项数截断可以求得未知散射波系数.将各散射波系数带入,可求得沉积内外各区域内总波场表达式、,继而得出楔形空间表面位移幅值.2 精度检验通过边界条件的满足程度和与现有结果的对比,检验本文方法的精度.首先引入无量纲频率η.它定义为圆弧沉积的直径与入射波波长之比,计算式为由于楔形空间表面由大圆弧面近似模拟,大圆弧面上零应力条件经验算容易满足.为验算圆弧交界面上位移和应力连续性条件满足程度,定义位移差值和应力差值分别为图2给出了90°楔形空间情况下,Δw和Δτ随项数增大的收敛趋势,无量纲频率η=2.0、3.0.横轴坐标表示和水平边界的夹角(由φ表示).容易看出,Δw 和Δτ随着计算截断项数的增大,收敛速度较快,最终能达到10-5量级,表明位移和应力连续性条件能得到较好的满足.图2 沉积交界面连续性条件检验Fig.2 Verification of the continuous boundary on the valley interface图 3给出了120°楔形空间情况,SH波不同角度入射下,本文方法所得沉积附近地表位移幅值同文献[14]所给结果的对比.沉积内外材料密度比= 1 .5,剪切模量比 = 6 ,无量纲频率η= 3 .0.容易看出 2种方法所得结果整体上吻合良好,但局部反应略微有一定差异.这是由于对本文模型而言,为使大圆弧面能足够精确地模拟地表面,大圆弧半径需远远大于散射体尺寸,但这同时会引起数值计算上的误差:半径过大会使得 Graf坐标转化中特殊函数截断项数增大,最终使得线性方程组求解困难.因而大圆弧面并不能完全真实地模拟地表散射,使得本文结果有一定误差.本文计算当中大圆弧半径取值:d=100a.图3 本文结果与文献[14]结果的比较Fig.3 Comparison between results in this study and those of reference [14]3 算例分析在精度检验基础上,分别对楔形空间中软沉积(见图 4~图 7)和硬沉积(见图 8~图11)对平面 SH波的散射进行了求解分析.3.1 软沉积情况图4 90°楔形空间中软沉积场地位移幅值Fig.4 Surface displacement amplitude ar ound the soft alluvial valley in 90°wedge-shaped space图5 120°楔形空间中软沉积场地位移幅值Fig.5 Surface displacement amplitude around the soft alluvial valley in 120°wedge-shaped space图6 150°楔形空间中软沉积场地位移幅值Fig.6 Surface displacement amplitude around the soft alluvial va lley in 150°wedge-shaped space图7 180°楔形空间中软沉积场地位移幅值Fig.7 Surface displacement amplitude around the soft alluvial valley in 180° wedge-shaped space图8 90°楔形空间中硬沉积场地位移幅值Fig.8 Surface displacement amplitude around the hard alluvial valley in 90°wedge-shaped space图9 120 °楔形空间中硬沉积场地位移幅值Fig.9 Surface displacement amplitude around the hard alluvial valley in 120°wedge-shaped space图10 150°楔形空间中硬沉积场地位移幅值Fig.10 Surface displacement amplitude around the hard alluvial valley in 150°wedge-shaped space图11 180°楔形空间中硬沉积场地位移幅值Fig.11 Surface displacementamplitude around the hard alluvial valley in 180°wedge-shaped space图4 ~图 7分别给出了90°、120°、150°和180°楔形空间中,在不同角度(α=0、π/6、π/3和π/2)及不同频率(η=0.5、1.0和2.0)SH波入射下,沉积附近地表位移幅值.α表示入射波方向与竖直线的夹角.沉积内外介质剪切模量比μv/μs=1/6,密度比ρv /ρs=2/3.图中横坐标为地表面上各点与楔形顶点的距离同沉积半径的比值,横轴上的负值对应楔形水平面上点,而正值对应楔形倾斜面上点;纵轴对应位移幅值w( t) .需要指出的是,180°楔形空间(半空间)情况的结果与文献[1]吻合很好,表明本文方法可以退化为半空间情况,这从另一方面验证了方法精度.3.2 硬沉积情况图 8~图 11分别给出了90°、120°、150°和180°楔形空间中硬沉积场地位移幅值.设沉积内外材料特性比值:剪切模量比为μv/μs=6,密度比ρv /ρs=3/2.入射波频率η取 0.5、1.0和 2.0,计算了不同入射角度下的地表位移幅值.通过对上述结果的总体分析,可以得出下述结论.(1)楔形空间中沉积谷地反应特征依赖于4个因素,即楔形空间夹角vπ、波入射角α、无量纲频率η以及沉积内外弹性介质的剪切模量比和密度比.(2)随着楔形空间夹角的减小,位移空间分布同半空间情况的差异逐渐增大,且即便对于较小斜度的楔形空间(ν=5/6),位移反应幅值和分布特征仍然有很大不同.从整体上看,位移放大效应要比半空间情况更为显著,这是由于在楔形空间中存在波的多次反射叠加作用.因此,对于斜坡和阶梯地形中的局部场地反应问题,需考虑特殊地形和地质不均匀性的复合影响,而不能简单地按半空间情况处理.(3)随着入射波角度变化,散射波能量的空间分布发生改变,而位移峰值一般出现在SH波沿一边掠入射情况;无量纲频率η反映了沉积直径同入射波长的比值关系,该参数直接决定了位移的空间振荡频度,并且对位移幅值具有关键影响.当该值在1.5~2.5之间,即沉积半径和波长相当时,散射作用比较显著.(4)楔形空间中软沉积场地位移放大作用十分明显.这是由于楔形空间中沉积内散射波具有更强的相干作用,波动能量由此产生汇聚效应,沉积范围之内场地反应比较剧烈.计算表明,对较软介质情况,局部地表位移幅值能放大10倍以上.(5)硬沉积场地位移反应特征同软沉积情况有明显差异.硬沉积对波的吸收作用较小(计算得出沉积内散射波系数较小),而波向楔形空间中的散射作用增强,故沉积内部位移幅值反而会有所降低,沉积外部地表位移(一般是朝向入射波的一侧)则显示出明显的位移放大作用.如图 8所示,沉积附近地表位移峰值接近 7.0,达到无沉积情况位移幅值的 2.3倍;随着地表点位和沉积距离的增大,位移放大效应逐渐减弱.4 结语本文对楔形空间中圆弧形沉积对弹性波的散射问题进行了方法上的探索和深入的研究,给出了一种新的解析求解技术.通过边界条件验算及同现有结果的比较验证了方法精度,为楔形空间中 P、SV波的散射求解奠定了基础.数值结果分析表明:楔形空间中沉积对弹性波的散射同半空间情况具有本质的不同,需综合考虑地形和地质不均匀性对地震动的复合影响;楔形夹角、无量纲频率、波入射角和沉积内外介质特性是影响地表反应特征的几个主要因素;平面波入射下,同半空间情况相比,由于波的多次散射叠加,楔形空间中沉积附近场地反应放大效应更为显著.因此为安全考虑,对地震多发区的高岸或斜坡地带,需更细致地评估局部场地对地震动的影响,进而更科学合理地提高当地建筑物的抗震设防标准.需要指出的是,本文以位于楔形空间顶部的圆弧形沉积为例,进行了推导计算和参数分析.当散射体(圆弧形)位于楔形空间其他位置时,两大圆弧面的坐标系和边界条件不变,另外需以散射体的圆心为中心建立一个坐标系,进而利用零应力或连续性边界条件,并结合 Graf变换公式,分别将不同的散射波场统一在同一个坐标系下表达,建立方程求解得到散射波系数.求解思路和过程与本文情况无本质区别.【相关文献】[1] Trifunac M D. Surface motion of a semi-cylindrical alluvial valley for incident plane SH waves[J]. Bulletin of Seismological Society of America,197l,61(6):1755-l770.[2] Wong H L,Trifunac M D. Surface motion of a semielliptical alluvial valley for incident plane SH waves[J].Bulletin of Seismological Society of America,1974,64(5):1389-1408.[3] Todorovska M,lee V W. Surface motion of shallow circular alluvial valleys for incident plane SH waves:Analytical solution[J]. Soil Dynamics and Earthquake Engineering,1991,10(4):192-200.[4] Yuan Xiaoming,Liao Zhenpeng. Scattering of plane SH waves by a cylindrical alluvial valley of circular-arc cross-section[J]. Earthquake Engineering and Structural Dynamics,1995,24(10):1303-1313.[5]梁建文,张郁山,顾晓鲁. 圆弧形层状沉积河谷场地在平面 SH波入射下动力响应分析[J]. 岩土工程学报,2000,22(4):396-401.Liang Jianwen,Zhang Yushan,Gu Xiaolu. Surface motion of circular-arc layered alluvial valleys for incident plane SH waves[J]. Chinese Journal of Geotechnical Engineering,2000,22(4):396-401(in Chinese).[6]李伟华,赵成刚. 具有饱和土沉积层的充水河谷对平面波的散射[J]. 地球物理学报,2006,49(1):212-224.Li Weihua,Zhao Chenggang. Scattering of plane waves by circular arc alluvial valleys with saturated soil deposits and water[J]. Chinese Journal of Geophysics,2006,49(1):212-224(in Chinese).[7] Boore D M,Larner K L,Aki K. Comparison of two independent methods for the solution of wave scattering problems:response of a sedimentary basin to incident SH waves[J]. Journal of Geophysical Research,1971,76(2): 558-569.[8] Dravinski M. Scattering of plane harmonic SH wave by dipping layers or arbitrary shape [J]. Bulletin of Seismological Society of America,1983,73(5):1303-1319.[9]杜修力,熊建国,关慧敏. 平面SH 波散射问题的边界积分方程分析法[J]. 地震学报,1992,15(3):331-338.Du Xiuli,Xiong Jianguo,Guan Huimin. The boundary integration equation methods in scattering of plane SH waves[J]. Acta Seismologica Sinica,1992,15(3):331-338(inChinese).[10] Sanchez-Sesma F J,Ramos-Martinez J,Campillo M. An indirect boundary element method applied to simulate the seismic response of alluvial valleys for incident P,S and Rayleigh waves[J]. Earthquake Engineering and Structural Dynamics,1993,22(4):279-295.[11]廖振鹏. 工程波动理论导论[M]. 2版.北京:科学出版社,2002.Liao Zhenpeng. Introduction to Wave Motion Theories in Engineering[M]. 2nd ed. Beijing:Science Press,2002(in Chinese).[12] Sanchez-Sesma F J. Diffraction of elastic SH-waves by wedges[J]. Bull Seismological Soc of Am,1985,75(5):1435-1446.[13] Lee V W,Sherif R I. Diffraction around circular canyon in elastic wedge space[J]. Journal of Engineering Mechanics,1996,122(6):539-544.[14] Lee V W, Sherif R I. Diffraction around a circular alluvial valley in an elasticwedge-shaped medium due to plane SH-waves[J]. European Earthquake Engineering,1996,10(3):21-28.[15] Dermendjian N,Lee V W,Liang Jianwen. Anti-plane deformation around arbitrary-shaped canyons in wedgeshape half space:Moment-method solutions[J]. Earthquake Engineering and Engineering Vibration,2003,2(2):281-287.[16] Dermendjian N,Lee V W,Moment solutions of antiplane(SH)wave diffraction around arbitrary-shaped rigid foundations on a wedge-shape half space[J]. ISET Journal of Earthquake Technology,2003,40(2):161-172.[17]史文谱,刘殿魁,禇京莲,等. 二维直角平面内固定圆形夹杂对稳态入射反平面剪切波的散射[J]. 爆炸与冲击,2007,27(1):57-62.Shi Wenpu,Liu Diankui,Chu Jinglian,et al. Scattering of fixed cirucular inclusion inright-angled plane to steady incident planar shearing horizontal wave[J]. Explosion and Shock Waves,2007,27(1):57-62(in Chinese).[18]史文谱,刘殿魁,宋永涛,等. 直角平面内圆孔对稳态SH 波的散射[J]. 应用数学和力学,2006,27(12):1417-1423.Shi Wenpu,Liu Diankui,Song Yongtao,et al. Scattering of circular cavity in right-angular planar space to steady SH-wave[J]. Applied Mathematics and Mechanics,2006,27(12):1417-1423(in Chinese).。
FREEZEPRO 冰冻保护系统说明书
123FREEZEPRO ® FROST PROTECTION SYSTEMS:TABLE OF CONTENTS4The Energy ProblemThe difficult truth about energy consumption ... and the solutionFreezePro ® Frost Protection SystemsSimple and quick insulation for your pipe runs and valve fittingsHow to MeasureMeasuring FreezePro ® productsHow to InstallInstalling FreezePro ® productsFreezePro ® AccessoriesFreezePro ® product line accessories6.13.161.26.13.161.24The Hard Reality and a Difficult Truth:When the winter chill sets in,companies lose profits, productivity and valuable equipment due to freezing temperatures. 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(U.S. Environmental Protection Agency, ENERGY STAR Homes. Calculations performed by B. McNary, October 2006.)DID YOU KNOW …There are two corrective maintenance types – planned (proactive) and unplanned (reactive) maintenance. Unplanned, breakdown maintenance costs are 3-9 times more expensive than planned maintenance costs.*Take a look at our “Cost Comparison Breakdown” example in the table below to see how much you cansave with just one FreezePro ® Frost Protection Systems Insulation Jacket.67FACILITATE TEMPERATURE CONTROL OF A PROCESSPREVENT OR REDUCE DAMAGE TO EQUIPMENT™FREEZEPRO ® FROST PROTECTION SYSTEMS:FreezePro ® Frost Protection Systems deliver a barrier of uniform, directional heat where it is needed most - to tanks, pipelines, drums, buckets, IBC totes, and other temperature sensitive equipment. The advanced, all-in-one design of FreezePro ® eliminates the need for multipleproduct purchases and simplifies the entire implementation process while saving time and money. The end result is an efficient heating solution with the most cost-effective method for minimizing damage caused by harsh or freezing temperatures.»FreezePro ® Frost Protection Systems are used to PROTECT KEY COMPONENTS FROM FREEZING and help prevent costly damage from occurring.»FreezePro ® Frost Protection Systems create a SAFER WORKING ENVIRONMENT for your employees and increase equipment lifespan by protecting key components from extreme temperatures.»FreezePro ® Frost Protection Systems are made with STANDARD, READILYAVAILABLE, OFF-THE-SHELF COMPONENTS that can be easily configured for almost any application requirement.»FreezePro ® Frost Protection Systems are COMPLIANT WITH OSHA SAFE-TOUCH STANDARDS for exposed surfaces (if there is a potential for injury). »FreezePro ® Frost Protection Systems deliver an INCREASED CONTROL OF PROCESS TEMPERATURES to enhance production capacity by maintaining temperatures and minimizing heat loss to keep equipment running at optimal temperatures.»FreezePro ® Frost Protection Systems ALL-IN-ONE DESIGN SIMPLIFIES THE OVERALL SYSTEM CONFIGURATION REQUIREMENTS and eliminates the need for additional/expensive add-ons.FREEZEPRO ® FROST PROTECTION SYSTEMS ARE USED TO PERFORM ONE OR MORE OF THE FOLLOWING FUNCTIONS:9FREEZEPRO ® WRAP:FREEZEPRO ® TOTE TANK:FREEZEPRO ® FROST PROTECTION SYSTEMS:FreezePro ®Valve & Wrap Insulation Jackets are constructed in three layers:•The primary inner layer (hot face) is made of Gray / Grey Silicone -65°F (-54°C) to 500°F (260°C).• The middle layer is made of IceRock -40°F (-40°C) to 1000°F (538°C).• The primary inner layer (hot face) is made of Gray / Grey Silicone -65°F (-54°C) to 500°F (260°C).10FREEZEPRO ® V ALVE:FreezePro ® Valve Insulation Jackets are designed to fit closely with tight joints on complex shapes, such as valve fittings, strainers, T and Y joints, and the like.Applications:• Manual Valves:• Stopper-type closure — globe, needle • Vertical slide — gate• Rotary type — ball, plug, butterfly • Flexible body — diaphragm • Check Valves:• Lift check• Swing check (single and double plate)• Tilting disc • Diaphragm • Other:• Bonnet valves • Control valves• Bronze screw valves • T-Fitting • Knife valves • Y strainers• Industrial HVAC equipment • Fittings • Pumps• Sight glasses • Manifolds• Filters & regulators • DesuperheatersFREEZEPRO ® DRUM:FreezePro ® Drum Insulation Jackets are designed to ensure temperature stability for temperature-sensitive products during the transport, handling, and storage of chemicals, fluids, and bulk materials.Applications:• 55-gallon barrels • 55-gallon drums• 55-gallon steel drums • Composite containers • 1-gallon buckets • 5-gallon buckets •10-gallon bucketsSIMPLICITY BREEDS USABILITYU S E R -F O C U S E D D E S I G N 11*OPTIONALFREEZEPRO ®INSULATION LIDS SOLD SEPARATELY12Selecting the right size FreezePro ® Wrap for your equipment is a lot easier than you might think. All you need is a tape measure, and you are ready to go!Click Here For Video Tutorial: How to Measure FreezePro ® Wrap1. Measure for either the (1) CIRCUMFERENCE OR (2) DIAMETER:2. Measure for the DESIRED WIDTH:ORWARNING:13FPW 3012.ORFPW 3012.CIRCUMFERENCEDIAMETER6in(152mm)12in(305mm)18in(457mm)24in(610mm)0in - 6in(0mm-152mm)0in-2in (0mm-51mm)FPW 1206FPW 1212FPW 1218FPW 12246in-13in(152mm-330mm)2in-4in (51mm-102mm)FPW 1806FPW 1812FPW 1818FPW 182413in-19in (330mm-483mm)4in-6in (102mm-152mm)FPW 2406FPW 2412FPW 2418FPW 242419in-25in (483mm-635mm)6in-8in(152mm-203mm)FPW 3006FPW 3012FPW 3018FPW 302425in-31in (635mm-787mm)8in-10in(203mm-254mm)FPW 3606FPW 3612FPW 3618FPW 362431in-38in (787mm-965mm)10in-12in (254mm-305mm)FPW 4206FPW 4212FPW 4218FPW 422438in-44in (965mm-1118mm)12in-14in (305mm-356mm)FPW 4806FPW 4812FPW 4818FPW 482444in-53in(1118mm-1346mm)14in-17in(356mm-432mm)FPW 6006FPW 6012FPW 6018FPW 6024WIDTHyou need is a tape measure, and you are ready to go!Click Here For Video Tutorial: How to Measure FreezePro ® Tote1. Measure for the CIRCUMFERENCE:2. 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Measure for the HEIGHT:WARNING:19FPD 7834.*OPTIONAL CIRCUMFERENCE15in(381mm)34in(864mm)0in-35in(0mm-889mm)FPD 4515N/A36in-72in(914mm-1829mm)N/A FPD 7834HEIGHTSUGGESTED LID SIZES FOR FREEZEPRO ® DRUM INSULATION JACKETS FREEZEPRO ® DRUM PART #’SFREEZEPRO ® DRUM LID PART #’SFPD4515FPDL15FPD7834FPDL24HOW TO INSTALL FREEZEPRO ® V ALVE & WRAP:Click Here For Video Tutorial: How to Install FreezePro ® Valve & Wrap(DO NOT OVER TIGHTEN)power socket; OR (Optional)(attached to the FreezePro HOW TO INSTALL FREEZEPRO ® TOTE & DRUM:Click Here For Video Tutorial: How to Install FreezePro ® Tote & Drum(DO NOT OVER TIGHTEN)(DO NOT OVER TIGHTEN)(Optional)(DO NOT OVER TIGHTEN)2223¾” S.S. SHARP POINT HOG RINGS¾” S.S. SHARP POINT HOG RING is ideal for industrial applications where fastening or tie-downs are desired. 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Our .051” diameter safety wire is thick, reliable, and ideal for use with our safety wirepliers for enhanced installation.Part # SSLW304ETC SINGLE STAGE CONTROLLER -NEMA TYPE 4XETC SINGLE STAGE CONTROL- NEMA TYPE 4X is a microprocessor based temperature controller suitable for switching 120Volts at up to 16Amps for heating or cooling applications making it suitable for a wide range of applications. This is a great universal controller for any application where switching 120Volts or temperatures outside that of a normal home thermostat are required. The sensor with an 8’ foot cable and instructions are included with the unit.Part # HE-C-01PTFE HEAT TRACE CABLEPTFE SELF-REGULATING HEAT TRACE CABLE products are designed to supply a specified amount of heat at any point along their length in direct response to local temperature variations. 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a rXiv:d g-ga/9759v129May1997SURF ACES IN 4-MANIFOLDSRONALD FINTUSHEL AND RONALD J.STERN Abstract.In this paper we introduce a technique,called rim surgery ,which can change a smooth embedding of an orientable surface Σof positive genus and nonnegative self-intersection in a smooth 4-manifold X while leaving the topological embedding unchanged.This is accomplished by replacing the tubular neighborhood of a particular nullhomologous torus in X with S 1×E (K ),where E (K )is the exterior of a knot K ⊂S 3.The smooth change can be detected easily for certain pairs (X,Σ)called SW-pairs .For example,(X,Σ)is an SW-pair if Σis a symplectically and primitively embedded surface with positive genus and nonnegative self-intersection in a simply connected symplectic 4-manifold X .We prove the following theorem:Theorem.Consider any SW-pair (X,Σ).For each knot K ⊂S 3there is a surface ΣK ⊂X such that the pairs (X,ΣK )and (X,Σ)are homeomorphic.However,if K 1and K 2are two knots for which there is a diffeomorphism of pairs (X,ΣK 1)→(X,ΣK 2),then their Alexander polynomials are equal:∆K 1(t )=∆K 2(t ).1.Introduction We say that a surface Σis primitively embedded in a simply connected smooth 4-manifold X if Σis smoothly embedded with π1(X \Σ)=0.In particular,by Alexander duality,Σmust represent a primitive homology class [Σ]∈H 2(X ;Z ).In general,any smoothly embedded (connected)surface S in a simply connected smooth 4-manifold X with [S ]=0has the property that the surface Σwhich represents the homology class [S ]−[E ]in X #CP 2is primitively embedded (since the surface Σtransversally intersects the sphere E inone point).Given a primitively embedded positive genus surface Σin X ,in the first part of this paper we shall construct for each knot K in S 3a smoothly embedded surface ΣK in X which is Σ-compatible ;i.e.[Σ]=[ΣK ]and there is a homeomorphism (X,Σ)→(X,ΣK ).This construction will have two properties.The first is that (X,Σunknot )=(X,Σ).The main result of this paper is the second property:under suitable hypotheses on the pair (X,Σ),if K 1and K 2are two knots in S 3and if there is a diffeomorphism (X,ΣK 1)→(X,ΣK 2),then K 1and K 2have the same symmetric Alexander polynomial,i.e.∆K 1(t )=∆K 2(t ).As a special case we show:2RONALD FINTUSHEL AND RONALD J.STERNTheorem1.1.Let X be a simply connected symplectic4-manifold andΣa symplectically and primitively embedded surface with positive genus and nonnegative self-intersection.IfK1and K2are knots in S3and if there is a diffeomorphism of pairs(X,ΣK1)→(X,ΣK2),then∆K1(t)=∆K2(t).Furthermore,if∆K(t)=1,thenΣK is not smoothly ambientisotopic to a symplectic submanifold of X.For example,Theorem1.1applies to the K3surface whereΣis a generic ellipticfiber. It also applies to surfaces of the form S−E in CP2#CP2consider the surface Σn=Σ− n j=1E j(resp.Σn,K=ΣK− n j=1E j)obtained fromΣ(resp.ΣK)by tubing together with the exceptional spheres E j,j=1,...,n,of the copies ofSURF ACES IN4-MANIFOLDS3 Theorem1.2.Consider any SW-pair(X,Σ).If K1and K2are two knots in S3and ifthere is a diffeomorphism of pairs(X,ΣK1)→(X,ΣK2),then∆K1(t)=∆K2(t).Finally,in§6we complete the proof of Theorem1.1by showing that in the case thatΣis sympletically embedded in X and∆K(t)=1,thenΣK is not smoothly ambient isotopic to a symplectic submanifold of X.We conclude this introduction with two conjectures.Thefirst conjecture is that,underthe hypothesis of Theorem1.2,there is a diffeomorphism(X,ΣK1)→(X,ΣK2)if and onlyif the knots K1and K2are isotopic.In particular,this conjecture would imply that the study of the equivalence clases ofΣ-compatible surfaces under diffeomorphism is at least as complicated as classical knot theory.The second conjecture is afiniteness conjecture: given a symplectic4-manifold X and a symplectic submanifoldΣ,we conjecture that there are onlyfinitely many distinct smooth isotopy classes of symplectic submanifoldsΣ′which are topologically isotopic toΣ.2.The construction ofΣKLet X be a smooth4-manifold which contains a smoothly embedded surfaceΣwith genus g>0.Then there is a diffeomorphismh:Σ→T2#···#T2=(T2\D2)∪(T2\(D2∐D2))∪···∪(T2\D2).Let C⊂Σbe a curve whose image under h is the curve S1×{pt}⊂T2\D2=(S1×S1)\D2 in thefirst T2\D2summand of h(Σ).Keep in mind that,since there are many such diffeomorphisms h,there are many such curves C.Given a knot K in S3we shall give two different constructions of a surfaceΣK,C.Thefirst is an explicit construction,while the second shows how to obtainΣK,C by what we call a rim surgery,a surgical operation on a particular homologically trivial torus in a neighborhood ofΣ.It is this second construction that will allow us to compute appropriate invariants to distinguish the surfacesΣK,C.2.1.An explicit description ofΣK,C.Viewing S1as the union of two arcs A1and A2, we haveT2\D2=(S1×S1)\D2=((A1∪A2)×(A1∪A2))\(A1×A1)=(A2×S1)∪(A1×A2)with h(C)=A2×{pt}∪A1×{pt}.Now the normal bundle ofΣin X when restricted to T2\D2⊂Σis trivial,hence it is diffeomorphic to((A2×S1)∪(A1×A2))×D2=((A2×D2)×S1)∪((A1×D2)×A2)). Furthermore,under this diffeomorphism,the inclusion(T2\D2)×{0}⊂(T2\D2)×D24RONALD FINTUSHEL AND RONALD J.STERNbecomes(A2×{0})×S1)∪((A1×{0})×A2)⊂((A2×D2)×S1)∪((A1×D2)×A2).Now tie a knot K in the arc(A2×{0})⊂(A2×D2)to obtain a knotted arc A K and to obtain a new punctured torusT K\D2=(A K×S1)∪((A1×{0})×A2)⊂((A2×D2)×S1)∪((A1×D2)×A2)with∂(T K\D2)=∂(T\D2).Then letΣK,C=(T K\D2)∪(T2\(D2∐D2))∪···∪(T2\D2)⊂N(Σ)⊂X.2.2.A description ofΣK,C via rim surgery.Keeping the notation above,wefirst recall how,via a3-manifold surgery,we can tie a knot K in the arc(A2×{0})⊂(A2×D2).In short,we just remove a small tubular neighborhood in A2×D2of a pushed-in copyγof the meridional circle{0}×S1⊂A2×D2and sew in the exterior of the knot K in S3so that the meridian of K is identified withγ.This has the effect of tying a knot in the arc A2×{0}⊂A2×D2.More specifically,consider the standard embedding of the solid torus A=(A1∪A2)×D2=S1×D2in S3with complementary solid torus B=D2×S1with core C′={0}×S1⊂D2×S1.In A\C=(S1×D2)\C=S1×S1×(0,1]=(A1∪A2)×S1×(0,1], consider the circleγ={t}×S1×{1SURF ACES IN4-MANIFOLDS5 Proof.In S3=A∪B,the above operation replaces a tubular neighborhood of the unknot γ⊂A⊂S3with the exterior E(K)of the knot K in S3.Thus there is a diffeomorphism h:E(K)∪D→A∪B=S3sending the core circle of D to the knot K.Now C′⊂B⊂E(K)∪D is unknotted,since in D,the curve C′is isotopic toγ′,which bounds a disk.Thus S K,which is the complement of a tubular neighborhood of C′,is an unknotted solid torus in S3=E(K)∪D.Furthermore,as we have noted above,C is isotopic to the core of D;so C⊂S K is the knot K.Thus there is a diffeomorphism h:S K→S1×D2 which is the identity on the boundary.After an isotopy rel boundary we can arrange that h(G)=G.To obtainΣK,C we cross everything with S1;i.e.remove the neighborhood N(γ)×S1⊂(A2×D2)×S1⊂N(Σ)of the(nullhomologous)torusγ×S1⊂(A2×D2)×S1⊂N(Σ)and sew in E(K)×S1as above on the E(K)factor and the identity on the S1factor.We refer to this as a rim surgery onΣ.Notice that this construction does not change the ambient manifold X.Except where it is absolutely necessary to keep track of the curve C,we shall suppress it from our notation and abbreviateΣK,C asΣK.2.3.The complement ofΣK.From the construction,it is clear that if the complement ofΣin X is simply connected,then so is the complement ofΣK in X,since the meridian of the knot(which is identified with the boundary of the normalfiber toΣ)normally generates the fundamental group of the exterior of K.Now there is a map f:E(K)→B∼=D2×S1 which induces isomorphisms on homology and restricts to a homeomorphism∂E(K)→∂B taking the class of a meridian to[{pt}×S1]and the class of a longitude to[∂D2×{pt}].The map f×id S1on E(K)×S1extends via the identity to a homotopy equivalence X\N(ΣK)→X\N(Σ)which restricts to a homeomorphism∂N(ΣK)→∂N(Σ).Then topological surgery [F,B]guarantees the existence of a homeomorphism h:(X,Σ)→(X,ΣK).Ifπ1(X\Σ)=0,it is not clear when X\ΣK is homeomorphic(or even homotopy equivalent)to X\ΣK.We avoid such issues in this paper and only deal with the case where π1(X\Σ)=0.However,as already noted;the surfaceΣ−E in X#CP2is primitively embedded;so there is a homeomorphism h:(X#CP2,ΣK−E).In summary:Theorem2.2.Let X be a simply connected smooth4-manifold with a primitively embedded surfaceΣ.Then for each knot K in S3,the above construction produces aΣ-compatible surfaceΣK.3.The standard pair(Y g,S g)Let g>0.In this section we shall construct a simply connected smooth4-manifold Y g and a primitive embedding of S g,the surface of genus g,in Y g such that the torus used in6RONALD FINTUSHEL AND RONALD J.STERNthe previous section to construct the S g-compatible embedding(S g)K=S g,K is contained in a cusp neighborhood.To this end,consider the(2,2g+1)-torus knot T(2,2g+1).It is afibered knot whose fiber is a punctured genus g surface and whose monodromy t′is periodic of order4g+2.If we attach a2-handle to∂B4along T(2,2g+1)with framing0,we obtain a manifold C(g) whichfibers over the2-disk with genericfiber a Riemann surface S g of genus g and whose monodromy map t,induced from t′,is a periodic holomorphic map t:S g→S g of order 4g+2.The singularfiber is the topologically(non-locallyflatly)embedded sphere obtained from the cone in B4on the torus knot T(2,2g+1)union the core of the2-handle.Now consider thefibration over the punctured2-sphere obtained from gluing together4g+2such neighborhoods C(g)along a neighborhood of afiber in the boundary of C(g).This is a complex surface,and the monodromy is trivial around a loop which contains in its interior the images of all the singularfibers.Thus we may compactify this manifold to obtain a complex surface Y g which is holomorphicallyfibered over S2.For example,Y1is the rational elliptic surface CP2#92}×∂D2).The curveτis one of the generatingcircles for H1(S g;Z)with a dual circleσ.The curveγspans a−1-disk contained inΛ.The curveτdegenerates to a point on the singularfiber in C(g).Thus we see both required vanishing cycles.4.SW-pairsRecall that the Seiberg-Witten invariant SW X of a smooth closed oriented4-manifold X with b+>1is an integer valued function which is defined on the set of spin c structures over X,(cf.[W]).In case H1(X;Z)has no2-torsion,there is a natural identification of the spin c structures of X with the characteristic elements of H2(X;Z).In this case we view the Seiberg-Witten invariant asSW X:{k∈H2(X,Z)|k≡w2(T X)(mod2))}→Z.SURF ACES IN4-MANIFOLDS7 The Seiberg-Witten invariant SW X is a smooth invariant whose sign depends on an orien-tation of H0(X;R)⊗det H2+(X;R)⊗det H1(X;R).If SW X(β)=0,then we callβa basic class of X.It is a fundamental fact that the set of basic classes isfinite.Ifβis a basic class,then so is−βwithSW X(−β)=(−1)(e+sign)(X)/4SW X(β)where e(X)is the Euler number and sign(X)is the signature of X.As in[FS]we need to view the Seiberg-Witten invariant as a Laurent polynomial.To do this,let{±β1,...,±βn}be the set of nonzero basic classes for X.We my then view the Seiberg-Witten invariant of X as the‘symmetric’Laurent polynomialSW X=b0+nj=1b j(t j+(−1)(e+sign)(X)/4t−1j)where b0=SW X(0),b j=SW X(βj)and t j=exp(βj).Now letΣbe genus g>0primitively embedded surface in the simply connected4-manifold X.If the self-intersection ofΣis n≥0,then in X n=X#nCP2in X n.Note thatthefiber sum X n#Σn=S g Y g of X n and Y g along the surfacesΣn and S g has b+>1.AnSW-pair is such a pair(X,Σ)which satisfies the property that the Seiberg-Witten invariant SW Xn#Σn=S g Y g=0.As we have pointed out earlier,there are several curves C that can be used to construct the surfacesΣK,C,and there are potentially several differentfiber sums that can be performedin the construction of X n#Σn=S g Y g.We pin down our choice of C by declaring it to bethe image of the curveσfrom§3under the diffeomorphism used in the construction ofthefiber sum.A simple Mayer-Vietoris argument shows that in X n#Σn=S g Y g the rim torus(equivalentlyγ×τ)becomes homologically essential and is contained in a cusp neighborhood. Thus our results from[FS]apply.5.SW-pairs and the Alexander polynomialWe are now in a position to prove our main theorem:Theorem1.2.Consider any SW-pair(X,Σ).If K1and K2are two knots in S3and ifthere is a diffeomorphism of pairs(X,ΣK1)→(X,ΣK2),then∆K1(t)=∆K2(t).Proof.With notation as above,we have a diffeomorphism(X n,Σn,K1)→(X n,Σn,K2).Thenthere is a diffeomorphismZ1=X n#Σn,K1=S g Y g→Z2=X n#Σn,K2=S gY g.8RONALD FINTUSHEL AND RONALD J.STERNIt follows from [FS]that SW Z i =SW X n #Σn =S g Y g ·∆K i (t )for t =exp(2[T ]),where Tdenotes the rim torus.Since (X,Σ)is a SW-pair,and since [T ]=0in H 2(Z i ;Z )we must have ∆K 1(t )=∆K 2(t ).6.Rim surgery on symplectically embedded surfacesWe conclude with a proof of our claim of the introduction.Theorem 1.1.Let X be a simply connected symplectic 4-manifold and Σa symplectically and primitively embedded surface with positive genus and nonnegative self-intersection.If K 1and K 2are knots in S 3and if there is a diffeomorphism of pairs (X,ΣK 1)→(X,ΣK 2),then ∆K 1(t )=∆K 2(t ).Furthermore,if ∆K (t )=1,then ΣK is not smoothly ambient isotopic to a symplectic submanifold of X .Proof.Since Σand S g are symplectic submanifolds of X and Y g ,the fiber sum X n #Σn =S g Y g is also a symplectic manifold [G].Thus SW X n #Σn =S g Y g =0[T1];so (X,Σ)forms an SW-pair.This proves the first statement of the theorem.Next,suppose that ΣK is smoothly ambient isotopic to a symplectic submanifold Σ′of X .This isotopy carries the rim torus T to a rim torus T ′of Σ′.We haveSW X n #Σ′n=S g Y g =SW X n #Σn,K =S g Y g =SW X n #Σn =S g Y g ·∆K (t )(1)with t =exp(2[T ′])when this expression is viewed as SW X n #Σ′n =S g Y g .As above,[T ′]=0in H 2(X n #Σ′n =S g Y g;Z ).Symplectic forms ωX on X n (with respect to which Σ′n is symplectic)and ωY on Y ginduce a symplectic form ωon the symplectic fiber sum X n #Σ′n =S g Y gwhich agrees with ωX and ωY away from the region where the manifolds are glued together.In particular,since T ′is nullhomologous in X n ,we have ω,T ′ = ωX ,T ′ =0.Now (1)implies thatthe basic classes of X n #Σ′n =S g Y gare exactly the classes b +2mT ′where b is a basic class of X n #Σn =S g Y g and t m has a nonzero coefficient in ∆K (t ).Thus the basic classes ofX n #Σ′n =S g Y gcan be grouped into collections C b ={b +2mT ′},and if ∆K (t )=1then each C b contains more than one basic class.Note,however,that ω,b +2mT ′ = ω,b .Now Taubes has shown [T2]that the canonical class κof a symplectic manifold with b +>1is the basic class which is characterized by the condition ω,κ > ω,b ′ for any other basic class b ′.But this is impossible for X n #Σn =S g Y g since each C b contains more than one class.References[B]S.Boyer,Simply-connected 4-manifolds with a given boundary ,Trans.Amer.Math.Soc.,298,(1986),331–357.[FS]R.Fintushel and R.Stern,Knots,links,and 4-manifolds ,1996preprint.[F]M.Freedman,The topology of four–dimensional manifolds ,J.Diff.Geo.17(1982),357–432.[Fu]T.Fuller,Generalized Nuclei ,UCI Preprint 1997.[G]R.Gompf,A new construction of symplectic manifolds ,Ann.Math.142(1995),527–595.SURF ACES IN4-MANIFOLDS9 [T1] C.Taubes,The Seiberg-Witten invariants and symplectic forms,Math.Res.Letters1(1994),809–822. [T2] C.Taubes,More constraints on symplectic manifolds from Seiberg-Witten invariants,Math.Res.Let-ters2(1995),9–14.[W] E.Witten,Monopoles and four-manifolds,Math.Res.Letters1(1994),769–796.Department of Mathematics,Michigan State UniversityEast Lansing,Michigan48824E-mail address:ronfint@Department of Mathematics,University of CaliforniaIrvine,California92697E-mail address:rstern@。