Hermitian operators and convex functions

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协同(r,(h,m))-凸函数的Hermite-Hadamard型积分不等式

协同(r,(h,m))-凸函数的Hermite-Hadamard型积分不等式

则称 f 为 I 上的 (h, m) -凸函数。
M. P. Gill 等人在文[4]中引进了“r-凸函数”的等价形式
定义 2:设 I ⊆ 为区间,实数 r ∈ ,函数 f : I → =+ (0, +∞) ,若对任意的点 x, y ∈ I 和任意的 λ ∈[0,1] ,有
( )
f

x
( a, c )
+
f
(b,c) +
f
(a, d
)+
f
(b, d ) ,
其中 L (u, v) 为对数平均,且
= Ψ f (∆)
1 4
L
(
f
( a, c ) ,
f
(b, c ))
+
L
(
f
(a,
d
),
f
(b, d
))
+
L
(
f
(a,
c),
f
(a,
d
))
+
L
(
f
(b,
c),
f
(b,
d
) ) .
定理 1 [பைடு நூலகம்] 设函数 f : [a,b] ⊆ → + 为对数凸函数,且 a < b ,则
b
1 −
a
b
∫a
f
(
x)
dx

L
(
f
(a),
f
(b)),
其中 L (u, v) 为对数平均数。
定理 2 [4] 设一元函数 f : [a,b] ⊆ → + 为 r-凸函数,且 a < b , r ∈ ,若 f ∈ L1 ([a, b]) ,则

代数英语

代数英语

(0,2) 插值||(0,2) interpolation0#||zero-sharp; 读作零井或零开。

0+||zero-dagger; 读作零正。

1-因子||1-factor3-流形||3-manifold; 又称“三维流形”。

AIC准则||AIC criterion, Akaike information criterionAp 权||Ap-weightA稳定性||A-stability, absolute stabilityA最优设计||A-optimal designBCH 码||BCH code, Bose-Chaudhuri-Hocquenghem codeBIC准则||BIC criterion, Bayesian modification of the AICBMOA函数||analytic function of bounded mean oscillation; 全称“有界平均振动解析函数”。

BMO鞅||BMO martingaleBSD猜想||Birch and Swinnerton-Dyer conjecture; 全称“伯奇与斯温纳顿-戴尔猜想”。

B样条||B-splineC*代数||C*-algebra; 读作“C星代数”。

C0 类函数||function of class C0; 又称“连续函数类”。

CA T准则||CAT criterion, criterion for autoregressiveCM域||CM fieldCN 群||CN-groupCW 复形的同调||homology of CW complexCW复形||CW complexCW复形的同伦群||homotopy group of CW complexesCW剖分||CW decompositionCn 类函数||function of class Cn; 又称“n次连续可微函数类”。

Cp统计量||Cp-statisticC。

物理学专业英语

物理学专业英语

华中师范大学物理学院物理学专业英语仅供内部学习参考!2014一、课程的任务和教学目的通过学习《物理学专业英语》,学生将掌握物理学领域使用频率较高的专业词汇和表达方法,进而具备基本的阅读理解物理学专业文献的能力。

通过分析《物理学专业英语》课程教材中的范文,学生还将从英语角度理解物理学中个学科的研究内容和主要思想,提高学生的专业英语能力和了解物理学研究前沿的能力。

培养专业英语阅读能力,了解科技英语的特点,提高专业外语的阅读质量和阅读速度;掌握一定量的本专业英文词汇,基本达到能够独立完成一般性本专业外文资料的阅读;达到一定的笔译水平。

要求译文通顺、准确和专业化。

要求译文通顺、准确和专业化。

二、课程内容课程内容包括以下章节:物理学、经典力学、热力学、电磁学、光学、原子物理、统计力学、量子力学和狭义相对论三、基本要求1.充分利用课内时间保证充足的阅读量(约1200~1500词/学时),要求正确理解原文。

2.泛读适量课外相关英文读物,要求基本理解原文主要内容。

3.掌握基本专业词汇(不少于200词)。

4.应具有流利阅读、翻译及赏析专业英语文献,并能简单地进行写作的能力。

四、参考书目录1 Physics 物理学 (1)Introduction to physics (1)Classical and modern physics (2)Research fields (4)V ocabulary (7)2 Classical mechanics 经典力学 (10)Introduction (10)Description of classical mechanics (10)Momentum and collisions (14)Angular momentum (15)V ocabulary (16)3 Thermodynamics 热力学 (18)Introduction (18)Laws of thermodynamics (21)System models (22)Thermodynamic processes (27)Scope of thermodynamics (29)V ocabulary (30)4 Electromagnetism 电磁学 (33)Introduction (33)Electrostatics (33)Magnetostatics (35)Electromagnetic induction (40)V ocabulary (43)5 Optics 光学 (45)Introduction (45)Geometrical optics (45)Physical optics (47)Polarization (50)V ocabulary (51)6 Atomic physics 原子物理 (52)Introduction (52)Electronic configuration (52)Excitation and ionization (56)V ocabulary (59)7 Statistical mechanics 统计力学 (60)Overview (60)Fundamentals (60)Statistical ensembles (63)V ocabulary (65)8 Quantum mechanics 量子力学 (67)Introduction (67)Mathematical formulations (68)Quantization (71)Wave-particle duality (72)Quantum entanglement (75)V ocabulary (77)9 Special relativity 狭义相对论 (79)Introduction (79)Relativity of simultaneity (80)Lorentz transformations (80)Time dilation and length contraction (81)Mass-energy equivalence (82)Relativistic energy-momentum relation (86)V ocabulary (89)正文标记说明:蓝色Arial字体(例如energy):已知的专业词汇蓝色Arial字体加下划线(例如electromagnetism):新学的专业词汇黑色Times New Roman字体加下划线(例如postulate):新学的普通词汇1 Physics 物理学1 Physics 物理学Introduction to physicsPhysics is a part of natural philosophy and a natural science that involves the study of matter and its motion through space and time, along with related concepts such as energy and force. More broadly, it is the general analysis of nature, conducted in order to understand how the universe behaves.Physics is one of the oldest academic disciplines, perhaps the oldest through its inclusion of astronomy. Over the last two millennia, physics was a part of natural philosophy along with chemistry, certain branches of mathematics, and biology, but during the Scientific Revolution in the 17th century, the natural sciences emerged as unique research programs in their own right. Physics intersects with many interdisciplinary areas of research, such as biophysics and quantum chemistry,and the boundaries of physics are not rigidly defined. New ideas in physics often explain the fundamental mechanisms of other sciences, while opening new avenues of research in areas such as mathematics and philosophy.Physics also makes significant contributions through advances in new technologies that arise from theoretical breakthroughs. For example, advances in the understanding of electromagnetism or nuclear physics led directly to the development of new products which have dramatically transformed modern-day society, such as television, computers, domestic appliances, and nuclear weapons; advances in thermodynamics led to the development of industrialization; and advances in mechanics inspired the development of calculus.Core theoriesThough physics deals with a wide variety of systems, certain theories are used by all physicists. Each of these theories were experimentally tested numerous times and found correct as an approximation of nature (within a certain domain of validity).For instance, the theory of classical mechanics accurately describes the motion of objects, provided they are much larger than atoms and moving at much less than the speed of light. These theories continue to be areas of active research, and a remarkable aspect of classical mechanics known as chaos was discovered in the 20th century, three centuries after the original formulation of classical mechanics by Isaac Newton (1642–1727) 【艾萨克·牛顿】.University PhysicsThese central theories are important tools for research into more specialized topics, and any physicist, regardless of his or her specialization, is expected to be literate in them. These include classical mechanics, quantum mechanics, thermodynamics and statistical mechanics, electromagnetism, and special relativity.Classical and modern physicsClassical mechanicsClassical physics includes the traditional branches and topics that were recognized and well-developed before the beginning of the 20th century—classical mechanics, acoustics, optics, thermodynamics, and electromagnetism.Classical mechanics is concerned with bodies acted on by forces and bodies in motion and may be divided into statics (study of the forces on a body or bodies at rest), kinematics (study of motion without regard to its causes), and dynamics (study of motion and the forces that affect it); mechanics may also be divided into solid mechanics and fluid mechanics (known together as continuum mechanics), the latter including such branches as hydrostatics, hydrodynamics, aerodynamics, and pneumatics.Acoustics is the study of how sound is produced, controlled, transmitted and received. Important modern branches of acoustics include ultrasonics, the study of sound waves of very high frequency beyond the range of human hearing; bioacoustics the physics of animal calls and hearing, and electroacoustics, the manipulation of audible sound waves using electronics.Optics, the study of light, is concerned not only with visible light but also with infrared and ultraviolet radiation, which exhibit all of the phenomena of visible light except visibility, e.g., reflection, refraction, interference, diffraction, dispersion, and polarization of light.Heat is a form of energy, the internal energy possessed by the particles of which a substance is composed; thermodynamics deals with the relationships between heat and other forms of energy.Electricity and magnetism have been studied as a single branch of physics since the intimate connection between them was discovered in the early 19th century; an electric current gives rise to a magnetic field and a changing magnetic field induces an electric current. Electrostatics deals with electric charges at rest, electrodynamics with moving charges, and magnetostatics with magnetic poles at rest.Modern PhysicsClassical physics is generally concerned with matter and energy on the normal scale of1 Physics 物理学observation, while much of modern physics is concerned with the behavior of matter and energy under extreme conditions or on the very large or very small scale.For example, atomic and nuclear physics studies matter on the smallest scale at which chemical elements can be identified.The physics of elementary particles is on an even smaller scale, as it is concerned with the most basic units of matter; this branch of physics is also known as high-energy physics because of the extremely high energies necessary to produce many types of particles in large particle accelerators. On this scale, ordinary, commonsense notions of space, time, matter, and energy are no longer valid.The two chief theories of modern physics present a different picture of the concepts of space, time, and matter from that presented by classical physics.Quantum theory is concerned with the discrete, rather than continuous, nature of many phenomena at the atomic and subatomic level, and with the complementary aspects of particles and waves in the description of such phenomena.The theory of relativity is concerned with the description of phenomena that take place in a frame of reference that is in motion with respect to an observer; the special theory of relativity is concerned with relative uniform motion in a straight line and the general theory of relativity with accelerated motion and its connection with gravitation.Both quantum theory and the theory of relativity find applications in all areas of modern physics.Difference between classical and modern physicsWhile physics aims to discover universal laws, its theories lie in explicit domains of applicability. Loosely speaking, the laws of classical physics accurately describe systems whose important length scales are greater than the atomic scale and whose motions are much slower than the speed of light. Outside of this domain, observations do not match their predictions.Albert Einstein【阿尔伯特·爱因斯坦】contributed the framework of special relativity, which replaced notions of absolute time and space with space-time and allowed an accurate description of systems whose components have speeds approaching the speed of light.Max Planck【普朗克】, Erwin Schrödinger【薛定谔】, and others introduced quantum mechanics, a probabilistic notion of particles and interactions that allowed an accurate description of atomic and subatomic scales.Later, quantum field theory unified quantum mechanics and special relativity.General relativity allowed for a dynamical, curved space-time, with which highly massiveUniversity Physicssystems and the large-scale structure of the universe can be well-described. General relativity has not yet been unified with the other fundamental descriptions; several candidate theories of quantum gravity are being developed.Research fieldsContemporary research in physics can be broadly divided into condensed matter physics; atomic, molecular, and optical physics; particle physics; astrophysics; geophysics and biophysics. Some physics departments also support research in Physics education.Since the 20th century, the individual fields of physics have become increasingly specialized, and today most physicists work in a single field for their entire careers. "Universalists" such as Albert Einstein (1879–1955) and Lev Landau (1908–1968)【列夫·朗道】, who worked in multiple fields of physics, are now very rare.Condensed matter physicsCondensed matter physics is the field of physics that deals with the macroscopic physical properties of matter. In particular, it is concerned with the "condensed" phases that appear whenever the number of particles in a system is extremely large and the interactions between them are strong.The most familiar examples of condensed phases are solids and liquids, which arise from the bonding by way of the electromagnetic force between atoms. More exotic condensed phases include the super-fluid and the Bose–Einstein condensate found in certain atomic systems at very low temperature, the superconducting phase exhibited by conduction electrons in certain materials,and the ferromagnetic and antiferromagnetic phases of spins on atomic lattices.Condensed matter physics is by far the largest field of contemporary physics.Historically, condensed matter physics grew out of solid-state physics, which is now considered one of its main subfields. The term condensed matter physics was apparently coined by Philip Anderson when he renamed his research group—previously solid-state theory—in 1967. In 1978, the Division of Solid State Physics of the American Physical Society was renamed as the Division of Condensed Matter Physics.Condensed matter physics has a large overlap with chemistry, materials science, nanotechnology and engineering.Atomic, molecular and optical physicsAtomic, molecular, and optical physics (AMO) is the study of matter–matter and light–matter interactions on the scale of single atoms and molecules.1 Physics 物理学The three areas are grouped together because of their interrelationships, the similarity of methods used, and the commonality of the energy scales that are relevant. All three areas include both classical, semi-classical and quantum treatments; they can treat their subject from a microscopic view (in contrast to a macroscopic view).Atomic physics studies the electron shells of atoms. Current research focuses on activities in quantum control, cooling and trapping of atoms and ions, low-temperature collision dynamics and the effects of electron correlation on structure and dynamics. Atomic physics is influenced by the nucleus (see, e.g., hyperfine splitting), but intra-nuclear phenomena such as fission and fusion are considered part of high-energy physics.Molecular physics focuses on multi-atomic structures and their internal and external interactions with matter and light.Optical physics is distinct from optics in that it tends to focus not on the control of classical light fields by macroscopic objects, but on the fundamental properties of optical fields and their interactions with matter in the microscopic realm.High-energy physics (particle physics) and nuclear physicsParticle physics is the study of the elementary constituents of matter and energy, and the interactions between them.In addition, particle physicists design and develop the high energy accelerators,detectors, and computer programs necessary for this research. The field is also called "high-energy physics" because many elementary particles do not occur naturally, but are created only during high-energy collisions of other particles.Currently, the interactions of elementary particles and fields are described by the Standard Model.●The model accounts for the 12 known particles of matter (quarks and leptons) thatinteract via the strong, weak, and electromagnetic fundamental forces.●Dynamics are described in terms of matter particles exchanging gauge bosons (gluons,W and Z bosons, and photons, respectively).●The Standard Model also predicts a particle known as the Higgs boson. In July 2012CERN, the European laboratory for particle physics, announced the detection of a particle consistent with the Higgs boson.Nuclear Physics is the field of physics that studies the constituents and interactions of atomic nuclei. The most commonly known applications of nuclear physics are nuclear power generation and nuclear weapons technology, but the research has provided application in many fields, including those in nuclear medicine and magnetic resonance imaging, ion implantation in materials engineering, and radiocarbon dating in geology and archaeology.University PhysicsAstrophysics and Physical CosmologyAstrophysics and astronomy are the application of the theories and methods of physics to the study of stellar structure, stellar evolution, the origin of the solar system, and related problems of cosmology. Because astrophysics is a broad subject, astrophysicists typically apply many disciplines of physics, including mechanics, electromagnetism, statistical mechanics, thermodynamics, quantum mechanics, relativity, nuclear and particle physics, and atomic and molecular physics.The discovery by Karl Jansky in 1931 that radio signals were emitted by celestial bodies initiated the science of radio astronomy. Most recently, the frontiers of astronomy have been expanded by space exploration. Perturbations and interference from the earth's atmosphere make space-based observations necessary for infrared, ultraviolet, gamma-ray, and X-ray astronomy.Physical cosmology is the study of the formation and evolution of the universe on its largest scales. Albert Einstein's theory of relativity plays a central role in all modern cosmological theories. In the early 20th century, Hubble's discovery that the universe was expanding, as shown by the Hubble diagram, prompted rival explanations known as the steady state universe and the Big Bang.The Big Bang was confirmed by the success of Big Bang nucleo-synthesis and the discovery of the cosmic microwave background in 1964. The Big Bang model rests on two theoretical pillars: Albert Einstein's general relativity and the cosmological principle (On a sufficiently large scale, the properties of the Universe are the same for all observers). Cosmologists have recently established the ΛCDM model (the standard model of Big Bang cosmology) of the evolution of the universe, which includes cosmic inflation, dark energy and dark matter.Current research frontiersIn condensed matter physics, an important unsolved theoretical problem is that of high-temperature superconductivity. Many condensed matter experiments are aiming to fabricate workable spintronics and quantum computers.In particle physics, the first pieces of experimental evidence for physics beyond the Standard Model have begun to appear. Foremost among these are indications that neutrinos have non-zero mass. These experimental results appear to have solved the long-standing solar neutrino problem, and the physics of massive neutrinos remains an area of active theoretical and experimental research. Particle accelerators have begun probing energy scales in the TeV range, in which experimentalists are hoping to find evidence for the super-symmetric particles, after discovery of the Higgs boson.Theoretical attempts to unify quantum mechanics and general relativity into a single theory1 Physics 物理学of quantum gravity, a program ongoing for over half a century, have not yet been decisively resolved. The current leading candidates are M-theory, superstring theory and loop quantum gravity.Many astronomical and cosmological phenomena have yet to be satisfactorily explained, including the existence of ultra-high energy cosmic rays, the baryon asymmetry, the acceleration of the universe and the anomalous rotation rates of galaxies.Although much progress has been made in high-energy, quantum, and astronomical physics, many everyday phenomena involving complexity, chaos, or turbulence are still poorly understood. Complex problems that seem like they could be solved by a clever application of dynamics and mechanics remain unsolved; examples include the formation of sand-piles, nodes in trickling water, the shape of water droplets, mechanisms of surface tension catastrophes, and self-sorting in shaken heterogeneous collections.These complex phenomena have received growing attention since the 1970s for several reasons, including the availability of modern mathematical methods and computers, which enabled complex systems to be modeled in new ways. Complex physics has become part of increasingly interdisciplinary research, as exemplified by the study of turbulence in aerodynamics and the observation of pattern formation in biological systems.Vocabulary★natural science 自然科学academic disciplines 学科astronomy 天文学in their own right 凭他们本身的实力intersects相交,交叉interdisciplinary交叉学科的,跨学科的★quantum 量子的theoretical breakthroughs 理论突破★electromagnetism 电磁学dramatically显著地★thermodynamics热力学★calculus微积分validity★classical mechanics 经典力学chaos 混沌literate 学者★quantum mechanics量子力学★thermodynamics and statistical mechanics热力学与统计物理★special relativity狭义相对论is concerned with 关注,讨论,考虑acoustics 声学★optics 光学statics静力学at rest 静息kinematics运动学★dynamics动力学ultrasonics超声学manipulation 操作,处理,使用University Physicsinfrared红外ultraviolet紫外radiation辐射reflection 反射refraction 折射★interference 干涉★diffraction 衍射dispersion散射★polarization 极化,偏振internal energy 内能Electricity电性Magnetism 磁性intimate 亲密的induces 诱导,感应scale尺度★elementary particles基本粒子★high-energy physics 高能物理particle accelerators 粒子加速器valid 有效的,正当的★discrete离散的continuous 连续的complementary 互补的★frame of reference 参照系★the special theory of relativity 狭义相对论★general theory of relativity 广义相对论gravitation 重力,万有引力explicit 详细的,清楚的★quantum field theory 量子场论★condensed matter physics凝聚态物理astrophysics天体物理geophysics地球物理Universalist博学多才者★Macroscopic宏观Exotic奇异的★Superconducting 超导Ferromagnetic铁磁质Antiferromagnetic 反铁磁质★Spin自旋Lattice 晶格,点阵,网格★Society社会,学会★microscopic微观的hyperfine splitting超精细分裂fission分裂,裂变fusion熔合,聚变constituents成分,组分accelerators加速器detectors 检测器★quarks夸克lepton 轻子gauge bosons规范玻色子gluons胶子★Higgs boson希格斯玻色子CERN欧洲核子研究中心★Magnetic Resonance Imaging磁共振成像,核磁共振ion implantation 离子注入radiocarbon dating放射性碳年代测定法geology地质学archaeology考古学stellar 恒星cosmology宇宙论celestial bodies 天体Hubble diagram 哈勃图Rival竞争的★Big Bang大爆炸nucleo-synthesis核聚合,核合成pillar支柱cosmological principle宇宙学原理ΛCDM modelΛ-冷暗物质模型cosmic inflation宇宙膨胀1 Physics 物理学fabricate制造,建造spintronics自旋电子元件,自旋电子学★neutrinos 中微子superstring 超弦baryon重子turbulence湍流,扰动,骚动catastrophes突变,灾变,灾难heterogeneous collections异质性集合pattern formation模式形成University Physics2 Classical mechanics 经典力学IntroductionIn physics, classical mechanics is one of the two major sub-fields of mechanics, which is concerned with the set of physical laws describing the motion of bodies under the action of a system of forces. The study of the motion of bodies is an ancient one, making classical mechanics one of the oldest and largest subjects in science, engineering and technology.Classical mechanics describes the motion of macroscopic objects, from projectiles to parts of machinery, as well as astronomical objects, such as spacecraft, planets, stars, and galaxies. Besides this, many specializations within the subject deal with gases, liquids, solids, and other specific sub-topics.Classical mechanics provides extremely accurate results as long as the domain of study is restricted to large objects and the speeds involved do not approach the speed of light. When the objects being dealt with become sufficiently small, it becomes necessary to introduce the other major sub-field of mechanics, quantum mechanics, which reconciles the macroscopic laws of physics with the atomic nature of matter and handles the wave–particle duality of atoms and molecules. In the case of high velocity objects approaching the speed of light, classical mechanics is enhanced by special relativity. General relativity unifies special relativity with Newton's law of universal gravitation, allowing physicists to handle gravitation at a deeper level.The initial stage in the development of classical mechanics is often referred to as Newtonian mechanics, and is associated with the physical concepts employed by and the mathematical methods invented by Newton himself, in parallel with Leibniz【莱布尼兹】, and others.Later, more abstract and general methods were developed, leading to reformulations of classical mechanics known as Lagrangian mechanics and Hamiltonian mechanics. These advances were largely made in the 18th and 19th centuries, and they extend substantially beyond Newton's work, particularly through their use of analytical mechanics. Ultimately, the mathematics developed for these were central to the creation of quantum mechanics.Description of classical mechanicsThe following introduces the basic concepts of classical mechanics. For simplicity, it often2 Classical mechanics 经典力学models real-world objects as point particles, objects with negligible size. The motion of a point particle is characterized by a small number of parameters: its position, mass, and the forces applied to it.In reality, the kind of objects that classical mechanics can describe always have a non-zero size. (The physics of very small particles, such as the electron, is more accurately described by quantum mechanics). Objects with non-zero size have more complicated behavior than hypothetical point particles, because of the additional degrees of freedom—for example, a baseball can spin while it is moving. However, the results for point particles can be used to study such objects by treating them as composite objects, made up of a large number of interacting point particles. The center of mass of a composite object behaves like a point particle.Classical mechanics uses common-sense notions of how matter and forces exist and interact. It assumes that matter and energy have definite, knowable attributes such as where an object is in space and its speed. It also assumes that objects may be directly influenced only by their immediate surroundings, known as the principle of locality.In quantum mechanics objects may have unknowable position or velocity, or instantaneously interact with other objects at a distance.Position and its derivativesThe position of a point particle is defined with respect to an arbitrary fixed reference point, O, in space, usually accompanied by a coordinate system, with the reference point located at the origin of the coordinate system. It is defined as the vector r from O to the particle.In general, the point particle need not be stationary relative to O, so r is a function of t, the time elapsed since an arbitrary initial time.In pre-Einstein relativity (known as Galilean relativity), time is considered an absolute, i.e., the time interval between any given pair of events is the same for all observers. In addition to relying on absolute time, classical mechanics assumes Euclidean geometry for the structure of space.Velocity and speedThe velocity, or the rate of change of position with time, is defined as the derivative of the position with respect to time. In classical mechanics, velocities are directly additive and subtractive as vector quantities; they must be dealt with using vector analysis.When both objects are moving in the same direction, the difference can be given in terms of speed only by ignoring direction.University PhysicsAccelerationThe acceleration , or rate of change of velocity, is the derivative of the velocity with respect to time (the second derivative of the position with respect to time).Acceleration can arise from a change with time of the magnitude of the velocity or of the direction of the velocity or both . If only the magnitude v of the velocity decreases, this is sometimes referred to as deceleration , but generally any change in the velocity with time, including deceleration, is simply referred to as acceleration.Inertial frames of referenceWhile the position and velocity and acceleration of a particle can be referred to any observer in any state of motion, classical mechanics assumes the existence of a special family of reference frames in terms of which the mechanical laws of nature take a comparatively simple form. These special reference frames are called inertial frames .An inertial frame is such that when an object without any force interactions (an idealized situation) is viewed from it, it appears either to be at rest or in a state of uniform motion in a straight line. This is the fundamental definition of an inertial frame. They are characterized by the requirement that all forces entering the observer's physical laws originate in identifiable sources (charges, gravitational bodies, and so forth).A non-inertial reference frame is one accelerating with respect to an inertial one, and in such a non-inertial frame a particle is subject to acceleration by fictitious forces that enter the equations of motion solely as a result of its accelerated motion, and do not originate in identifiable sources. These fictitious forces are in addition to the real forces recognized in an inertial frame.A key concept of inertial frames is the method for identifying them. For practical purposes, reference frames that are un-accelerated with respect to the distant stars are regarded as good approximations to inertial frames.Forces; Newton's second lawNewton was the first to mathematically express the relationship between force and momentum . Some physicists interpret Newton's second law of motion as a definition of force and mass, while others consider it a fundamental postulate, a law of nature. Either interpretation has the same mathematical consequences, historically known as "Newton's Second Law":a m t v m t p F ===d )(d d dThe quantity m v is called the (canonical ) momentum . The net force on a particle is thus equal to rate of change of momentum of the particle with time.So long as the force acting on a particle is known, Newton's second law is sufficient to。

泛函微分方程-泛函微分方程

泛函微分方程-泛函微分方程

泛函微分方程是指除了理想的情形以外,任何具有反馈的动力系统总是存在滞后现象;用传统的常微分方程去描述物理系统只是一种近似,而且是有条件的,这就需要考虑带有各种滞后量的微分方程,诸如微分差分方程,各种具有复杂偏差变元的微分方程,有滞后量的积分微分方程,等等。

泛函微分方程是这一类方程的概括和抽象。

最早的泛函微分方程来自1750年L.欧拉提出的几何问题:求一曲线使之与其渐缩线相似。

这种曲线便满足一个特殊的泛函微分方程,此后不断从各个学科中提出这类问题。

到20世纪40年代为止,主要是研究微分差分方程的解析解。

50年代开始探讨稳定性理论,1959年H.H.克拉索夫斯基在函数空间之间建立解映射,从而确立了滞后型泛函微分方程。

70年代初,J.黑尔与A.克鲁兹分离出一类广泛的中立型方程。

1978年赫尔与加藤敏夫共同奠立了具有无穷滞后的泛函微分方程。

以后又有对其他类型的中立型泛函微分方程的研究。

给定实数r≥0,区间【-r,0】到n维实(或复)线性空间R n的连续映射全体记为C(【-r,0】,R n),简记为C,C中元素φ的范数取为则C 为巴拿赫空间且具有一致收敛拓扑。

若t0∈R,A≥0,且x∈C(【t0-r,t0+A】,R n),则对任何t∈【t0,t0+A】,记x t(θ)=x(t+θ)(-r ≤θ≤0),显然x t∈C。

若D吇R×C,给定映射ƒ:D→R n,则(1)叫做D上的滞后型泛函微分方程,记为RFDE(ƒ)。

(1)中为右导数。

若存在t0∈R,A >0 使得,(t,x t)∈D,且当)时x(t)满足(1),则称x(t)为(1)之解。

若t0∈R ,φ∈C 给定,且x(t;t0,φ)为(1)之解。

则当时称x为过 (t0,φ)的解。

由此可以建立两种解映射:及。

而且一般地说解空间是无穷维的。

当r=0时(1)退化为常微分方程,解映射为,解空间是有限维的。

二者截然不同,通常解的存在惟一性,稳定性,周期解的存在性都不等价。

A New Approach for Filtering Nonlinear Systems

A New Approach for Filtering Nonlinear Systems

computational overhead as the number of calculations demanded for the generation of the Jacobian and the predictions of state estimate and covariance are large. In this paper we describe a new approach to generalising the Kalman filter to systems with nonlinear state transition and observation models. In Section 2 we describe the basic filtering problem and the notation used in this paper. In Section 3 we describe the new filter. The fourth section presents a summary of the theoretical analysis of the performance of the new filter against that of the EKF. In Section 5 we demonstrate the new filter in a highly nonlinear application and we conclude with a discussion of the implications of this new filter1
Tቤተ መጻሕፍቲ ባይዱ
= = =
δij Q(i), δij R(i), 0, ∀i, j.
(3) (4) (5)

ROHM Solution Simulator用户指南说明书

ROHM Solution Simulator用户指南说明书

User’s Guide ROHM Solution SimulatorAutomotive High Precision & Input/Output Rail-to-Rail CMOS Operational Amplifiers (Dual Op-Amps) TLR2377YFVM-C –Non-inverting Amplifier (Sine Wave Input) – Transient Response sim This circuit simulates the transient response to sine wave input with non-inverting amplifier configured Op-Amps. You can observe the output voltage and how faithfully the sine wave input voltage is reproduced. You can customize the parameters of the components shown in blue, such as VSOURCE, or peripheral components, and simulate the non-inverting amplifier with the desired operating condition.You can simulate the circuit in the published application note: Operational amplifier, Comparator (Tutorial). [JP] [EN] [CN] [KR] General CautionsCaution 1: The values from the simulation results are not guaranteed. Please use these results as a guide for your design.Caution 2: These model characteristics are specifically at Ta=25°C. Thus, the simulation result with temperature variances may significantly differ from the result with the one done at actual application board (actual measurement).Caution 3: Please refer to the Application note of Op-Amps for details of the technical information.Caution 4: The characteristics may change depending on the actual board design and ROHM strongly recommend to double check those characteristics with actual board where the chips will be mounted on.1 Simulation SchematicFigure 1. Simulation Schematic2 How to simulateThe simulation settings, such as parameter sweep or convergence options,are configurable from the ‘Simulation Settings’ shown in Figure 2, and Table1 shows the default setup of the simulation.In case of simulation convergence issue, you can change advancedoptions to solve. The temperature is set to 27 °C in the default statement in‘Manual Options’. You can modify it.Figure 2. Simulation Settings and execution Table 1.Simulation settings default setupParameters Default NoteSimulation Type Time-Domain Do not change Simulation TypeEnd Time 300 µs -Advanced options Balanced - Time Resolution Enhancement Convergence Assist-Manual Options .temp 27 - SimulationSettingsSimulate3Simulation ConditionsTable 2. List of the simulation condition parametersInstanceNameType ParametersDefaultValue Variable Range Units Min Max VSOURCE Voltage Source Frequency 10k 10 10M Hz Peak_voltage 0.5 0 5.5V Initial_phase0 free ° DC_offset2.5 0 5.5V DF0.0 fixed 1/s AC_magnitude 0.0 fixed V AC_phase 0.0 fixed ° VDD Voltage SourceFor Op-AmpVoltage_level5 2.5(Note1) 5.5(Note1)V AC_magnitude0.0 fixed V AC_phase 0.0 fixed ° VREF Voltage Source Voltage_level2.5 VSS VDDV AC_magnitude0.0 fixed V AC_phase0.0fixed°(Note 1) Set it to the guaranteed operating range of the Op-Amps.3.1 VSOURCE parameter setupFigure 3 shows how the VSOURCE parameters correspond to the VIN stimulus waveform.Figure 3. VSOURCE parameters and its waveform4 Op-Amp modelTable 3 shows the model pin function implemented. Note that the Op-Amp model is the behavior model for its input/output characteristics, and no protection circuits or the functions not related to the purpose are not implemented.Table 3. Op-Amp model pins used for the simulationPin Name Description+INNon-inverting input -INInverting input VDDPositive power supply VSSNegative power supply / Ground OUTOutputInitial_phaseDC_offsetPeak_voltage1/FrequencyVOVIN5 Peripheral Components5.1 Bill of MaterialTable 4 shows the list of components used in the simulation schematic. Each of the capacitors has the parameters of equivalent circuit shown below. The default values of equivalent components are set to zero except for the ESR ofC. You can modify the values of each component.Table 4. List of capacitors used in the simulation circuitType Instance Name Default Value Variable RangeUnits Min MaxResistor R2_1 10k 1k 1M ΩR2_2 10k 1k 1M ΩRL2 10k 1k 1M, NC ΩCapacitor C2_1 10 10 100 pF CL2 10 free, NC pF5.2 Capacitor Equivalent Circuits(a) Property editor (b) Equivalent circuitFigure 4. Capacitor property editor and equivalent circuitThe default value of ESR is 0.01 Ω.(Note 2) These parameters can take any positive value or zero in simulation but it does not guarantee the operation of the IC in any condition. Refer to the datasheet to determine adequate value of parameters.6 Recommended Products6.1 Op-AmpTLR2377YFVM-C : Automotive High Precision & Input/Output Rail-to-Rail CMOS Operational Amplifier (DualOp-Amp). [JP] [EN] [CN] [KR] [TW] [DE]TLR377YG-C : Automotive High Precision & Input/Output Rail-to-Rail CMOS Operational Amplifier. [JP] [EN] [CN] [KR] [TW] [DE]LMR1802G-LB : Low Noise, Low Input Offset Voltage CMOS Operational Amplifier. [JP] [EN] [CN] [KR] [TW] [DE] Technical Articles and Tools can be found in the Design Resources on the product web page.NoticeROHM Customer Support System/contact/Thank you for your accessing to ROHM product informations.More detail product informations and catalogs are available, please contact us.N o t e sThe information contained herein is subject to change without notice.Before you use our Products, please contact our sales representative and verify the latest specifica-tions :Although ROHM is continuously working to improve product reliability and quality, semicon-ductors can break down and malfunction due to various factors.Therefore, in order to prevent personal injury or fire arising from failure, please take safety measures such as complying with the derating characteristics, implementing redundant and fire prevention designs, and utilizing backups and fail-safe procedures. ROHM shall have no responsibility for any damages arising out of the use of our Poducts beyond the rating specified by ROHM.Examples of application circuits, circuit constants and any other information contained herein areprovided only to illustrate the standard usage and operations of the Products. The peripheral conditions must be taken into account when designing circuits for mass production.The technical information specified herein is intended only to show the typical functions of andexamples of application circuits for the Products. ROHM does not grant you, explicitly or implicitly, any license to use or exercise intellectual property or other rights held by ROHM or any other parties. ROHM shall have no responsibility whatsoever for any dispute arising out of the use of such technical information.The Products specified in this document are not designed to be radiation tolerant.For use of our Products in applications requiring a high degree of reliability (as exemplifiedbelow), please contact and consult with a ROHM representative : transportation equipment (i.e. cars, ships, trains), primary communication equipment, traffic lights, fire/crime prevention, safety equipment, medical systems, servers, solar cells, and power transmission systems.Do not use our Products in applications requiring extremely high reliability, such as aerospaceequipment, nuclear power control systems, and submarine repeaters.ROHM shall have no responsibility for any damages or injury arising from non-compliance withthe recommended usage conditions and specifications contained herein.ROHM has used reasonable care to ensur e the accuracy of the information contained in thisdocument. However, ROHM does not warrants that such information is error-free, and ROHM shall have no responsibility for any damages arising from any inaccuracy or misprint of such information.Please use the Products in accordance with any applicable environmental laws and regulations,such as the RoHS Directive. For more details, including RoHS compatibility, please contact a ROHM sales office. ROHM shall have no responsibility for any damages or losses resulting non-compliance with any applicable laws or regulations.W hen providing our Products and technologies contained in this document to other countries,you must abide by the procedures and provisions stipulated in all applicable export laws and regulations, including without limitation the US Export Administration Regulations and the Foreign Exchange and Foreign Trade Act.This document, in part or in whole, may not be reprinted or reproduced without prior consent ofROHM.1) 2)3)4)5)6)7)8)9)10)11)12)13)。

《2024年无穷维Hamilton算子的拟谱》范文

《2024年无穷维Hamilton算子的拟谱》范文

《无穷维Hamilton算子的拟谱》篇一摘要:本文旨在探讨无穷维Hamilton算子的拟谱问题。

首先,我们将介绍Hamilton算子的基本概念及其在物理和数学领域的重要性。

随后,我们将阐述拟谱方法的基本原理和在处理无穷维系统中的优势。

最后,我们将详细描述我们的研究方法和结果,以及这些结果对无穷维系统理论和相关领域研究的潜在贡献。

一、引言Hamilton算子是一种广泛应用于量子力学、光学、电磁学等领域的数学工具。

在处理具有无穷维度的系统时,Hamilton算子的谱问题变得尤为重要。

然而,由于无穷维系统的复杂性,直接求解其谱往往面临巨大挑战。

因此,寻求有效的拟谱方法成为研究的关键。

二、Hamilton算子的基本概念Hamilton算子是一种描述系统动力学的算子,具有特定的形式和性质。

在量子力学中,它描述了粒子的能量和动量关系。

在光学和电磁学中,它用于描述光场或电磁场的演化。

由于系统的复杂性,Hamilton算子往往具有无穷维度,使得其谱的求解变得困难。

三、拟谱方法的基本原理及优势拟谱方法是一种用于处理无穷维系统的数学方法。

它通过将系统在一定的近似空间中进行展开,将原本复杂的无穷维问题转化为有限维问题进行处理。

这种方法在处理具有复杂相互作用的系统时具有显著优势,能够有效地降低问题的复杂度。

四、无穷维Hamilton算子的拟谱研究针对无穷维Hamilton算子的拟谱问题,我们采用了一种基于拟谱方法的解决方案。

首先,我们选择了一个合适的近似空间,将Hamilton算子在这个空间中进行展开。

然后,我们利用数值方法求解展开后的有限维问题,得到Hamilton算子的近似谱。

最后,我们通过分析近似谱的性质,了解原系统的动力学特性。

五、研究方法与结果我们采用了一种基于多项式展开的拟谱方法。

首先,我们选择了一组合适的多项式基函数作为近似空间的基底。

然后,我们将Hamilton算子在这组基底上进行展开,得到一个有限维的矩阵表示。

量子化学课程习题及标准答案

量子化学课程习题及标准答案

量子化学习题及标准答案Chapter 011. A certain one-particle,one-dimensional system has/2bmx ibt e ae --=ψ,where a and b are constants and m is theparticle ’s mass. Find thepotential-energy function V for thissystem. (Hint : Use the time-dependentSchrodinger equation.)Solution :As (x,t) is known, we canderive the corresponding derivatives. ⎪⎪⎩⎪⎪⎨⎧ψ+ψ-=∂ψ∂ψ-=∂ψ∂⇒=ψ--222222/42),(),(),(2 x m b bm xt x ib t t x e ae t x bmx ibtAccording to time-dependentSchroedinger equation,substituting into the derivatives, weget222),(mx b t x V =2. At a certain instant of time, aone-particle, one-dimensional systemhas bx xe b /||2/13)/2(-=ψ, where b = 3.000 nm. If ameasurement of x is made at this time inthe system, find the probability thatthe result (a) lies between 0.9000 nm and0.9001 nm (treat this interval asinfinitesimal); (b) lies between 0 and2 nm (use the table of integrals, ifnecessary). (c) For what value of x isthe probability density a minimum?(There is no need to use calculus toanswer this.) (d) Verify that ψ isnormalized. 222(,)(,)2x t x t V i t m x∂ψ∂ψ=-+∂∂Solution :a) The probability of findingan particle in a space between x and x+dx is given by6/223210*29.32--==ψ=dx e x b dx P b x b) 0753.02910*20/223==⎰--dx e x bP b x c) Clearly, the minimum of probabilitydensity is at x=0, where the probabilitydensity vanishes. d)4220/223/223/2232===ψ=⎰⎰⎰⎰+∞-+∞∞--+∞∞--+∞∞-dx e x b dx e x b dx e x b dx P b x b x b x3. A one-particle, one-dimensionalsystem has the state function2222/4/16/4/12)/32)((cos )/2)((sin c x c x xe c at e c at --+=ψππwhere a is a constant and c = 2.000 Å.If the particle ’s position is measuredat t = 0, estimate the probability thatthe result will lie between 2.000 Å and2.001 Å.Solution :when t=0, the wavefunction is simplified as441610*158.2)32(),(22--==ψc x xec t x πChapter 021. Consider an electron in a one-dimensional box of length2.000Åwith the left end of the box at x = 0.(a) Suppose we have one million of these systems, each in the n= 1 state, and we measure the x coordinate of the electron in each system. About how many times will the electron be found between 0.600 Åand 0.601 Å? Consider the interval to be infinitesimal. Hint: Check whether your calculator is set to degrees or radians.(b) Suppose we have a large number of these systems, each in the n =1 state, and we measure the x coordinate of the electron in each system and find the electron between 0.700 Å and 0.701 Å in 126 of the measurements. In about how many measurements will the electron be found between 1.000 Å and 1.001 Å? Solution: a) In a 1D box, the energyand wave-function of a micro-system are given by)sin(2,22222x ln l ml n E πψπ== therefore, the probability density offinding the electron between 0.600 and0.601 Å is65510*545.6)(sin 242⇒==-dx x ln l P πb) From the definition of probability,the probability of finding an electron between x and x+dx is given bydx x l n l P )(sin 22π= As the number of measurements of findingthe electron between 0.700 and 0.701 Å is known, the number of system is1(sin 22*158712158712001.0)7.02*1(sin 2212612622=⇒===πP P N2. When a particle of mass 9.1*10-28 g ina certain one-dimensional box goes from the n = 5 level to the n = 2 level, itemits a photon of frequency 6.0*1014 s -1.Find the length of the box. Solution.lml h n n ml n n E lower up lower up 36222222222110*26646.18)(2)(-=-=-=∆ π3. An electron in a stationary state of a one-dimensional box of length 0.300 nmemits a photon of frequency 5.05*1015 s -1.Find the initial and final quantum numbers for this transition. Solution:2,388)(2)(22222222222===-⇒=-=-=∆lower upper lower up lower up lower up n n n n hv ml h n n ml n n E π4. For the particle in a one-dimensional box of length l , we could have put the coordinate origin at the center of the box. Find the wave functions and energylevels for this choice of origin.Solution: The wavefunction for a particle in a one-dimernsional box can be written as)2()2()(x mE BSin x mE ACos x+=ψ If the coordinate origin is defined at the center of the box, the boundary conditions are given as2()22(0)(2()22(0)(22mE BSin l mE ACos x mE BSin l mE ACos x l x lx +⇒=-⇒==-= ψψ Combining Eq1 with Eq2, we get)4(,0)22()3(,0)22(Eq l mE BSin Eq l mE ACos ==Eq3 leads to A=0, or )22(l mE Cos =0. We willdiscuss both situations in the following section.If A=0, B must be non-zero number otherwise the wavefunction vanishes.2220)22(02mlh n E n l mE l mE Sin B π=⇒=⇒=⇒≠If A ≠08)12()21(220)22(00)22(0)22(0222mlh n E n l mE l mE Cos B l mE Sin l mE Cos A ψπ⇒+=⇒+=⇒==⇒≠⇒=⇒≠5. For an electron in a certain rectangular well with a depth of 20.0 eV, the lowest energy lies 3.00 eV above the bottom of the well. Find the width of this well. Hint : Use tanθ = sin θ/cos θ Solution : For the particle in a certainrectangular well, the E fulfill with)2sin()2()2cos()(21010l mE V E l mE E E V ---=- Substituting into the V and E, we get1010011110*64.22)7954.0(7954.022)(2)2()2()2(-----=⇒+-=⇒+-=⇒-=--==lowest l mEn l n l mE V E E E V l mE Tan l mE Cos l mE Sin ππChapter 03 1. If A ˆf (x ) = 3x 2f (x ) + 2xd f /dx , givean expression for Aˆ. Solution :Extracting f(x) from the known equationleads to the expression of Adx d x x A 23ˆ2+=2. (a) Show that (Aˆ+Bˆ)2= (Bˆ+Aˆ)2for any two operators. (b) Under what conditionsis (A ˆ+B ˆ)2 equal to A ˆ2+2A ˆB ˆ+B ˆ2?Solution:a)2222ˆ()ˆˆ)(ˆˆ(ˆˆˆˆˆˆˆˆˆˆˆ)ˆˆ)(ˆˆ()ˆˆ(B A B A BA B A A B B A B B A A B A B A B A =++=+++=+++=++=+ b)B AA B A B B A A B A ˆˆ2ˆˆˆˆˆˆˆ)ˆˆ(2222++=+++=+If and only if A and B commute, (Aˆ+Bˆ)2equals to A ˆ2+2A ˆB ˆ+B ˆ2 3. If A ˆ = d 2/dx 2 and B ˆ = x 2, find (a) A ˆB ˆx 3; (b) B ˆA ˆx 3; (c) AˆB ˆf (x ); (d)B ˆA ˆf (x )Solution:a)3522320ˆˆx x dxd x B A == b)3322236ˆˆx x dxd x x A B == c))()(4)(2)]()(2[)]([)(ˆˆ2222222x f dxd x x f dx d x x f x f dxd x x xf dx d x f x dx d x f B A ++=+==d))()()(ˆˆ222222x f dxd x x f dx d x x f A B ==4. Classify these operators as linear ornonlinear: (a) 3x 2d 2/dx 2; (b) ( )2; (c) ∫dx ; (d) exp; (e) ∑=n x 1.Solution:Linear operator is subject to the following condition.f A c cf Ag A f A g f A ˆ)(ˆˆˆ)(ˆ=+=+ a) Linearb) Nonlinear c) Linear d) Nonlinear e) Linear5. The Laplace transform operator Lˆ is defined by⎰∞-=0)()(ˆdx x f e x f L px(a) Is L ˆ linear? (b) Evaluate L ˆ(1). (c)Evaluate L ˆe ax , assuming that p >a .Solution:a) L is a linear operatorb),1)1(ˆ0>==⎰∞-p p dx e L px c)pdx e dx e e e L x a p ax px ax ===⎰⎰∞--∞-)(ˆ0)(06. We define the translation operator hTˆ by hT ˆf (x ) = f (x + h ). (a) Is hT ˆ a linear operator? (b) Evaluate(2ˆ3ˆ121+-T T )x 2.Solution:a) The translation operator is linear operator2212212121(2ˆ3ˆ)2ˆ3ˆ(x x x T x T x T T +=+-=+-7. Evaluate the commutators (a) [xˆ,xp ˆ]; (b) [x ˆ,2ˆxp ]; (c) [x ˆ,y p ˆ]; (d) [x ˆ, ),,(ˆz y x V ]; (e)[xˆ,H ˆ]; (f) [z y x ˆˆˆ, 2ˆxp ]. Solution:a)i xx x x i x x i p xx =∂∂--∂∂-=∂∂-=)ˆ1ˆ(],ˆ[]ˆ,ˆ[b)xp i p p x p x p p xx x x x x x∂∂==+=222ˆ2)ˆ]ˆ,ˆ[]ˆ,ˆ[ˆ(]ˆ,ˆ[c)0)ˆˆ(],ˆ[]ˆ,ˆ[=∂∂-∂∂-=∂∂-=yx y x i y x i p xy0ˆ),,(ˆ),,(ˆˆ)],,(ˆ,ˆ[=-=x z y x V z y x V x z y x V xe)mxT x V T x H x ==+=21,ˆ[]ˆ,ˆ[]ˆˆ,ˆ[]ˆ,ˆ[f)xz y p z y xx∂∂=ˆˆ2]ˆ,ˆˆˆ[22Chapter 041:The one-dimensional harmonic-oscillator is at its first excited state and its wavefunction is given as)21exp()()(2)(24/14/31x x x βπβψ-=please evaluate the expectation values(average values) of kinetic energy (T), potential energy (V) and the total energy.Answer: 1) First of all, check the normalization property of the wavefunction.2) Evaluate the expectationvalue of kinetic energy.3) Evaluate the expectation valueof potential energy4) Total Energy = T + V 2. The one-dimensional harmonic-oscillator Hamiltonian is2222ˆ22ˆˆxm v mp H xπ+= The raising and lowering operators forthis problem are defined as]ˆ2ˆ[)2(1ˆ2/1x ivm p m A x π+=+, ]ˆ2ˆ[)2(1ˆ2/1x ivm p m A x π-=-Show thathv H A A 21ˆˆˆ-=-+, hv HA A21ˆˆˆ+=+-, hv A A-=-+]ˆ,ˆ[ ++=A hv A H ˆ]ˆ,ˆ[, ---=A hv A Hˆ]ˆ,ˆ[ Show that +Aˆ and -A ˆ are indeed ladder operators and that the eigenvalues are spaced at intervals of hv . Since both the kinetic energy and the potential energy are nonnegative, we expect the energy eigenvalues to be nonnegative. Hence there must be a state of minimum energy. Operate on the wave function for thisstate first with -A ˆ and then with +Aˆ and show that the lowest energy eigenvalueis hv 21. Finally, conclude that hvn E )21(+=, n = 0, 1, 2, …Answer:1) Write down the definition of operatordx di px -=ˆ2) Expand the operators in full form.]2[21]2[2122ˆ222222vmxi dx di mA vmxi dx d i mA mx v dx d m H πππ--=+-=+-=-+ 3) Evaluate the correspondingcombination of operators]22][2[21ˆ4222[21]2[2]2[2[21]2[21]22[ˆ21ˆ2122]4222[21]]2[2]2[[21]2[21]2[2121ˆ2122]42[21]4222[21]]2[2]2[[21]2[21]2[21222222332222222333222222222222222222222222222222222222222222222mx v dx d m vmxi dx d i mH A v dx d i mx v dx d ix v dx d i v dxd m i m vmxi dx d i mx v vmxi dx d i dxd m m vmxi dx d i mmx v dx d m A H hv H hv mx v dx d m x m v dxd vmx dx d x vm vm dx d m vmxi dxd i vmxi vmxi dx d i dx d i m vmxi dx d i mvmxi dx d i m A A hv H hv mx v dx d m x m v vm dxd m x m v dxd vmx dx d x vm vm dx d m vmxi dxd i vmxi vmxi dx d i dx d i m vmxi dx d i mvmxi dx d i m A A πππππππππππππππππππππππππππππππππ+-+-=+---=+-++--=+-+-=+=++-=+-++-=+--+--=+---=-=-+-=+--=++---=--+---=--+-=+++--++++=+-=+-=+-=-hvA vmxi m dx d i m hv vmxi m hv dxd i m hv mxi v dx d i v m H A A H ]22121[]221[]21[]42[21ˆˆ222ππππIn the same manner, we can get---=-hvA H A A H ˆˆ 4) Substituting the above communicatorsinto the Schroeidnger equation, we getψψψψψψψψψψψψ------++++++-=-=-=+=+=+==A hv E hvA E A hvA H A A H A hv E hvA E A hvA H A A H E H)(]ˆ[ˆ)(]ˆ[ˆˆThis shows that +Aˆ and -A ˆ are indeed ladder operators and that theeigenvalues are spaced at intervals ofhv . 5) Suppose that is the eigenfunctionwith the lowest eigenvalue. ψψlowest E H =ˆAccording to the definition of A_operator, we haveψψ---=A hv E A H )(ˆ As is the eigenfunction with thelowest eigenvalue, the above equation isfulfilled if and only if 0=-ψAOperating on the wave function for thisstate first with -Aˆ and then with +A ˆ leads to ψψψψhv H hv H A A 21ˆ]21ˆ[0=⇒-==-+Therefore, the lowest energy is 1/2 hv.3,2,1,0,)(21ˆ=+=n hv n H ψψChapter 051. For the ground state of theone-dimensional harmonic oscillator,compute the standard deviations x andp x and check that the uncertaintyprinciple is obeyed.Answer:1) The ground state wavefunction of theone-dimensional harmonic oscillator isgiven by2214141)(x e ααπψ--=2) The standard deviations x and p xare defined as222x x x -=∆222)∆∆-=p(p∆)(pThe product of x and p is given by2422122 ==∙=∆∆ααp xIt shows that the uncertainty principleis obeyed.2. (a) Show that the three commutationrelations [x L ˆ,y L ˆ] = z L i ˆ , [y L ˆ,z L ˆ] = x L i ˆ , [z L ˆ,x Lˆ] = y Li ˆ are equivalent to the single relation L L Lˆˆˆ i =⨯ (b) Find [2ˆx L ,y L ˆ] Answer:1): zy x y x z x z y z y x y x x z z y x y y x z x x z y z z y y z x z z y x y z x y x z y x z y x z y x L i L L L i L L L i L L k L j L i L i k L L j L L i L L k L L L L j L L L L i L L L L i L L j L L i L L k L L j L L k L L k L j L i L k L j L i L L L k L j L i L L ===⇒++=++=-+-+-=-++--=++⨯++=⨯++=],[],[],[)(],[],[],[)()()()()(ˆˆˆ2):)()()(],[],[],[2x z z x xz z x x y x y x x y x L L L L i L L i L i L L L L L L L L L +=+=+=3. Calculate the possible angles betweenL and the z axis for l = 2.Answer:The possible angles between L and thez axis are equivalent the angles betweenL and L z . Hence, the angles are given by:Lm Cos L z ==+=θ6)12(2 ︒︒︒︒=7.144,10.114,00.90,91.65,26.35θ 4. Complete this equation:m l m l z Y m Y L 333ˆChapter 061. Explain why each of the following integrals must be zero, where the functions are hydrogenlike wave functions: (a) <2p 1|z L ˆ|3p -1>; (b) <3p 0|z L ˆ|3p 0>Answer:Both 3p -1 and 3p 0 are eigenfunctions of L z , with eigenvalues of -1 and 0, respectively. Therefore, the above integrals can be simplified asa) due to orthogonalization properties of eigenfunctions03|213ˆ21111=-=--p p p L p z b) 02. Use parity to find which of the following integrals must be zero: (a)<2s |x |2p x >; (b) <2s |x 2|2p x >; (c)<2p y |x |2p x >. The functions in these integrals are hydrogenlike wave functions.Answer:1) b) and c) must be zero.3. For a hydrogen atom in a p state, the possible outcomes of a measurement of L z are – ħ, 0, and ħ. For each of the following wave functions, give the probabilities of each of these three results: (a)z p 2ψ; (b) y p 2ψ; (c) 12p ψ. Then find <L z > for each of these three wave functions.Answer:a) 022p p z ψψ=, therefore, the probabilities are: 0%, 100%, 0% )(2111222-+=p p p x ψψψ, the probabilities are 50%, 0%, 50%.12p ψ,the probabilities are 100%, 0%, 0% b) 0,0,14. A measurement yields 21/2ħ for themagnitude of a particle’s orbital angular momentum. If L x is now measured,what are the possible outcomes?Answer:1): Since the wavefunction is the eigenfunction of L2, a measurement of the magnitude of the orbital angular momentum should be+LLL=)1⇒21 (=,The possible outcomes when measure L x are-1, 0, 1Chapter 071. Which of the following operators areHermitian: d /dx , i (d /dx ), 4d 2/dx 2,i (d 2/d x 2)?Answer :An operator in one-D space is Hermitianif⎰⎰=dx A dx A **)ˆ(ˆψψψψ a)⎰⎰⎰⎰-=-=-=∞∞-dx dx d dx dx d dx dx d dx dxd *****)(ψψψψψψψψψψ b)⎰⎰⎰⎰=-=-=∞∞-dx dx d i dx d i dx dx d i i dx dx d i ****)(ψψψψψψψψψψc)⎰⎰⎰⎰⎰=+-=-=-=∞∞-∞∞-dxdxddxddxddxdxddxddxddxddxddxdxdψψψψψψψψψψψψψ2*22****22*44 444 44This operator can be written as a product of 1D kinetic operator and a constant. Hence, it’s Hermitian.d) As the third operator is Hermitian, this operator is not Hermitian.2. If Aˆ and Bˆ are Hermitian operators, prove that their product AˆBˆ is Hermitian if and only if Aˆ and Bˆcommute. (b) If Aˆ and Bˆ are Hermitian,prove that 1/2(A ˆB ˆ+B ˆA ˆ) is Hermitian. (c)Is x px ˆˆHermitian? (d) Is 1/2(x p x ˆˆ+x p xˆˆ) Hermitian?Answer:1)If operator A and B commute , we have⎰=-⇒=-⇒=0])ˆˆˆˆ[(0ˆˆˆˆˆˆˆˆˆ*τψψd A B B AA B B A A B B A ⎰⎰⎰=⇒=-⇒τψψτψψτψψd A B d B A d A B B A ***]ˆˆ[]ˆˆ[0])ˆˆˆˆ[( Operator A and B are Hermitian, we have⎰⎰⎰==⇒τψψτψψτψψd B A d B A d A B ˆˆ)ˆ()ˆ(]ˆˆ[***Therefore, when A and B commute, thefollowing equation fulfills. Namely, ABis also Hermitian.⎰⎰=τψψτψψd B A d B A ˆˆ]ˆˆ[** 2)]ˆˆˆˆ[21)]ˆˆˆˆ(21[***⎰⎰⎰+=+τψψτψψτψψd A B d B A d A B B AOperator A and B are Hermitian, we get⎰⎰⎰⎰⎰⎰⎰+=+⇒+=+=+τψψτψψτψψτψψτψψτψψτψψd A B B A d A B B A d B A A B d B A d A B d A B d B A *******])ˆˆˆˆ(21[)ˆˆˆˆ(21])ˆˆˆˆ(21[)ˆˆ()ˆˆ([21]ˆˆˆˆ[21The above equation shows that theoperator 1/2[AB+BA] is Hermitian.c) xp x is not Hermitian since both x andpx are Hermitian and do not commute.d) YesChapter 081. Apply the variation function cr e -=φtothe hydrogen atom; choose the parameterc to minimize the variational integral,and calculate the percent error in theground-state energy.Solution :1) The requirement of the variationfunction being a well-behaved functionrequires that c must be a positivenumber.2) check the normalization of the variation function.322*)(c d d Sin dr r e d cr πϕθθτφφ==⎰⎰⎰⎰- 3) The variation integral equals to)2(214])2[(2)1(21()121(ˆ32223*32*32*3**-=-∂∂+∂∂-=-∇-=-∇-==⎰⎰⎰⎰⎰⎰--c c c dr r e rr r e c d r c c d r c d d H w cr cr τφφπφπτφφπτφφτφφ4) The minimum of the variation integral is 21101-=⇒=⇒=-=∂∂w c c c w5) The percent error in the ground stateis 0%2. If the normalized variation functionx l 2/13)/3(=φ for 0 ≤ x ≤ l is applied tothe particle-in-a-one-dimensional-boxproblem, one finds that the variationintegral equals zero, which is less thanthe true ground-state energy. What is wrong?Solution:The correct trail variation function must be subject to the same boundary condition of the given problem. For the particle in a 1D box problem, the correct wavefunction must equal to zero at x=0 and x=l. However, the trial variation function x l 2/13)/3(=φ does not fulfill these requirement. The variation integral based on this incorrect variation function does not make any sense.3. Application of the variation function 2cx e -=φ(where c is a variationparameter) to a problem with V = af (x), where a is a positive constant and f (x ) is a certain function of x , gives thevariation integral as W = c ħ2/2m+15a /64c 3. Find the minimum value of Wfor this variation function.Solution:23434123434141min 4141413272598.03)25(23)25(0)64152(m a m a w m a c dc c a m c d c w ==⇒±=⇒=+=∂∂4. In 1971 a paper was published that applied the normalized variationfunction N exp(-br 2a 02-cr /a 0) to thehydrogen atom and stated that minimization of the variation integral with respect to the parameters b and c yielded an energy 0.7% above the true ground-state energy for infinite nuclear mass. Without doing any calculations, state why this result must be wrong. Solution:From the evaluation of exercise 1, we know that the variation function exp(-cr) gives no error in the ground state of hydrogen atom. This function is a special case of the normalized variationfunction N exp(-br 2a 02-cr /a 0) when bequals to zero. Therefore, adopting the normalized variation function as a trial variation function should also have no error in the ground state energy for hydrogen atom.5. Prove that, for a system with anondegenerate ground state, 0*ˆE d H >⎰τφφ, ifφ is any normalized, well-behaved function that is not equal to the true ground-state wave function. (E 0 is thelowest-energy eigenvalue of H ˆ) Solution:As the eigenfunctions of the Hermitian operator H form a complete set, any well-behaved function which is subjectto the same boundary condition can be expanded as a linear combination of the eigenfunction of the Hermitian operator, namely,∑∞==0i i i c ψφ, where i s are eigenfunctions of Hermitian operator H, c i s are constant.The expectation valueof with respect to the Hermitian operator is0201020201020020*00**00*0*0*ˆˆ)(ˆE c E E c E c c E c E c E c c E c cH c c d c H c d H i i i i i i i i i i i i i ij j j j i i i j j i i j j j i i i ==+>+======∑∑∑∑∑∑∑⎰∑∑⎰∑∑⎰∞=∞=∞=∞=∞=∞=∞=∞=∞=∞=∞=δψψτψψτφφChapter 09, 101. For the anharmonic oscillator with Hamiltonian43222212ˆdx cx kx dx d m H +++-= , evaluate E (1) for the first excited state, taking the unperturbed system as the harmonic oscillator.Solution:The wavefunction of the first excited state of the harmonic oscillator is241312)4(x xe απαψ-=Hence, the first order correct to energy of the first excited state is given by6213422134134324131'*1415)4()4()4)(()4(ˆ222απαπαπαπαψψαααd dx e x d dx x d e x xe x d x c xe dx H x x x ==∙=∙+∙=---⎰⎰⎰⎰2. Consider the one-particle, one-dimensional system withpotential-energyV = V 0 for l x l 4341<<, V = 0 for l x 410≤≤ and l x l ≤≤43and V = ∞ elsewhere, where V 0 = 22/ml .Treat the system as a perturbed particle in a box. (a) Find the first-order energy correction for the general stationary state with quantum number n . (b) Find the first-order correction to the wave function of the stationary state with quantum number n .Solution:The wavefunction of a particle in 1D box is given by)(2)0(x ln Sin l n πψ= Take this as unperturbed wavefunction, and the perturbation H ’ is given by V. a) The first-order energy correction forn is])23[]2[(224]2[4[2)()(2)()(2ˆ00004341)0('*)0()1(πππππππππψψn Sin n Sin n V V n S n Sin l l V dx V x l n Sin x l n Sin l dx x ln VSin x l n Sin l dx H E l ln n -+=-+====⎰⎰⎰b) The first correction to the wavefunction is given by)0()0()0()0()0()1(2)0()0(222)0('(818mn m mn nm n mn n E E H n E E ml h n E ψψψψ∑∞≠-==-⇒=3. For an anharmonic oscillator with3222212ˆcx kx dx d m H ++-= , take 'ˆH as cx 3. (a) Find E (1) for the state with quantum number v .(b) Find E (2) for the state with quantumnumber v . You will need the following integral:3,'2/13)0(3)0('2/)1[(3]8/)3)(2)(1[(||++++++>=<v v v v v v v v x αδαψψ1,'2/38/)2)(1([)2/(3---++v v v v v v αδα Solution: a) As the potential of the unperturbed is a even function, the eigenfunctions of the unperturbed system are either even or odd. The perturbation is an odd function with respect to x. Hence, thefirst order energy correction is zero.b) The second order energy correction is given by)51212(8]38)2)(1(838)1(338)3)(2)(1([()2(3)21(38)3)(2)(1((''2323333332)0()0(1,2/31,2/33,32)0()0(2)0(3)0()0()0()0()0()0()0()2(++-=--++-++-+++=-+++++++=-=-=∑∑∑∞≠-++∞≠∞≠n n hvc hvn n n hv n hv n hv n n n c E E n n n n n n n c E E cx E E H H E n m mn n n n n n n n m mn m n n m m n m n nm n αααααδαδαδαψψψψψψ4. Calculate the angle that the spin vector S makes with the z axis for an electron with spin function α.Solution:For an electron, both S and S z equal to one half. The magnitude of S is74.54]31[23)1(===+=ArcCos S S S θ5. (a) Show that 12ˆP and 23ˆP do not commutewith each other. (b) Show that 12ˆPand 23ˆP commute when they are applied to antisymmetric functions. Solution:a) Set the wavefunction to be)1()3()2()2()1()3(321321φφφφφφ≠b) When the function is antisymmetric, we haveψψψψψψψ2312121223231223ˆˆ)(ˆˆˆ)(ˆˆˆP P P P P P P P =-=-==-=-=6. Which of the following functions are (a) symmetric? (b) antisymmetric?(1) )2()1()2()1(ααg f ; (2) )]2()1()2()1()[2()1(αββα-f f ;(3) )3()2()1()3()2()1(βββf f f ; (4) )(21r r a e --;(5) )]1()2()2()1()][2()1()2()1([βαβα--f g g f ; (6) )(21221r r a e r +-. Solution:(2) is antisymmetric(3), (5) and (6) are symmetricChapter 11, 131. How many electrons can be put in each of the following: (a) a shell with principal quantum number n ; (b) a subshell with quantum numbers n and l ; (c) an orbital; (d) a spin-orbital? Solution:a) 2n 2, b) 2*(2l+1), c) 2, d) 12. Give the possible values of the total-angular-momentum quantum number J that result from the addition of angular momentum with quantum numbers (a) 3/2 and 4; (b) 2, 3, and 1/2 Solution:Coupling between two angular momentums with quantum number j 1 and j 2 gives the possible quantum number J of the total angular momentum as:2121j j J j j +<<-a) The possible values are 11/2, 9/2, 7/2,5/2b) The possible values are:11/2, 9/2, 9/2, 7/2, 7/2, 5/2, 5/2, 3/2, 3/2, 1/23. Find the terms that arise from each of the following electron configurations: (a) 1s22s22p63s23p5g; (b) 1s22s22p3p3d (c) 1s22s22p24dSolution:As fully-filled sub-shells do not contribution the total orbital and spin angular momentum, we can ignore the electrons in these sub-shells while considering the atomic terms. Hence, a) The atomic terms can be:3H, 1H, 3G, 1G, 3F, 1Fb) The atomic terms can be:4G, 2G, 4F, 2F, 4D, 2D, 4P, 2P, 4S, 2S4F 2F, 4D, 2D, 4P, 2P4D, 2D, 4P, 2P, 4S, 2Sc) The atomic terms can be:。

《计算电磁学》--2010讲义

《计算电磁学》--2010讲义
《计算电磁学》讲义
赖生建 (内部资料)
物理电子学院 二零一零年一月 印刷
1
1、 前 言
一个多世纪以来,由电磁学发展起来的现代电子技术已应用在电力工程、电子工程、通 信工程、计算机技术等多学科领域。电磁理论已广泛应用于国防、工业、农业、医疗、卫生 等领域,并深人到人们的日常生活中。今天,电磁场问题的研究及其成果的广泛运用,已成 为人类社会现代化的标志之一。
电磁场理论早期主要应用在军事领域,其发展和无线电通信、雷达的发展是分不开的。 现在,电磁场理论的应用已经遍及地学、生命科学和医学、材料科学和信息科学等几乎所有 的科学技术领域。计算电磁场研究的内容涉及面很广,与电磁场要解决的是实际电磁场工程中越来越复杂的建模 与仿真、优化设计等问题;而电磁场工程也为之提供实验结果,以验证其计算结果的正确性。 对电磁场理论而言,计算电磁场可以为其研究提供进行复杂的数值及解析运算的方法、手段 和计算结果;而电磁场理论则为计算电磁场问题提供了电磁规律、数学方程,进而验证其计 算结果。计算电磁场对电磁场理论发展的影响决不仅仅是提供一个计算工具而已,而是使整 个电磁场理论发生了革命性的变化。毫不夸张地说,近二三十年来,电磁场理论的发展,无 一不是与计算电磁场的发展相联系的。目前,计算电磁场已成为对复杂体系的电磁规律、电 磁性质进行研究的重要手段,为电磁场理论的深人研究开辟了新的途径,并极大地推动了电 磁场工程的发展。
在一个电磁系统中,电场和磁场的计算对于完成该系统的有效设计是极端重要的。为了 分析电磁场,我们从所涉及的数学公式人手。依据电磁系统的特性,拉普拉斯方程和泊松方 程只能适合于描述静态和准静态(低频)运行条件下的情况。但是,在高频应用中,则必须 在时域或频域中求解波动方程,以做到准确地预测电场和磁场,在任何情况下,满足边界条 件的一个或多个偏微分方程的解,因此,计算电磁系统内部和周围的电场和磁场都是必要的。

量子力学学习课件第三章英文版

量子力学学习课件第三章英文版
(1) hermitian? In this case: As is the usual polar coordinate:
On the interval
(2) The eigenvalue equation, The general solution is By using periodic boundary condition
Therefore, the set of all square-integrable functions, on a specified interval,
constitutes a (much smaller) vector space.
Mathematicians call it L2(a,b), while physicists call it Hilbert space.
the addition and the inner product
The inner product of two vectors, which generalizes the dot product in three dimensions, is defined by
2. Linear transformations
In an N-dimensional space, the vector is represented by a N-number of its components, with respect to a specified orthonormal basis:
We can define operations on vectors:
Some important concepts
On state
we measure an observable Q.

无线电力传输的电车辆应用-英文

无线电力传输的电车辆应用-英文

Wireless Power Transfer for Electric Vehicle ApplicationsSiqi Li,Member,IEEE,and Chunting Chris Mi,Fellow,IEEEAbstract—Wireless power transfer(WPT)using magnetic resonance is the technology which could set human free from the annoying wires.In fact,the WPT adopts the same basic theory which has already been developed for at least30 years with the term inductive power transfer.WPT tech-nology is developing rapidly in recent years.At kilowatts power level,the transfer distance increases from several mil-limeters to several hundred millimeters with a grid to load efficiency above90%.The advances make the WPT very attractive to the electric vehicle(EV)charging applications in both stationary and dynamic charging scenarios.This paper reviewed the technologies in the WPT area applicable to EV wireless charging.By introducing WPT in EVs,the obstacles of charging time,range,and cost can be easily mitigated.Battery technology is no longer relevant in the mass market penetration of EVs.It is hoped that researchers could be encouraged by the state-of-the-art achievements,and push forward the further development of WPT as well as the expansion of EV.Index Terms—Dynamic charging,electric vehicle(EV), inductive power transfer(IPT),safety guidelines,stationary charging,wireless power transfer(WPT).I.I NTRODUCTIONF OR energy,environment,and many other reasons,theelectrification for transportation has been carrying out for many years.In railway systems,the electric locomotives have already been well developed for many years.A train runs on a fixed track.It is easy to get electric power from a conductor rail using pantograph sliders.However,for electric vehicles(EVs), the highflexibility makes it not easy to get power in a similar way.Instead,a high power and large capacity battery pack is usually equipped as an energy storage unit to make an EV to operate for a satisfactory distance.Until now,the EVs are not so attractive to consumers even with many government incentive ernment subsidy and tax incentives are one key to increase the market share of EV today.The problem for an electric vehicle is nothing else but the electricity storage technology,which requires a battery which is the bottleneck today due to its unsatisfactory energy density,limited life time and high cost. Manuscript received February2,2014;revised April6,2014;accepted April18,2014.Date of publication April23,2014;date of current ver-sion January29,2015.Recommended for publication by Associate Editor ler.S.Li is with the Department of Electrical Engineering,Kunming Uni-versity of Science and Technology,Kunming650500,China(e-mail: lisiqi@).C. C.Mi is with the Department of Electrical and Computer Engineering,University of Michigan,Dearborn,MI48128USA(e-mail: chrismi@).Color versions of one or more of thefigures in this paper are available online at .Digital Object Identifier10.1109/JESTPE.2014.2319453In an EV,the battery is not so easy to design because of the following requirements:high energy density,high power density,affordable cost,long cycle life time,good safety, and reliability,should be met simultaneously.Lithium-ion batteries are recognized as the most competitive solution to be used in electric vehicles[1].However,the energy density of the commercialized lithium-ion battery in EVs is only 90–100Wh/kg for afinished pack[2].1This number is so poor compared with gasoline,which has an energy density about 12000Wh/kg.To challenge the300-mile range of an internal combustion engine power vehicle,a pure EV needs a large amount of batteries which are too heavy and too expensive. The lithium-ion battery cost is about500$/kWh at the present time.Considering the vehicle initial investment,maintenance, and energy cost,the owning of a battery electric vehicle will make the consumer spend an extra1000$/year on average compared with a gasoline-powered vehicle[1].Besides the cost issue,the long charging time of EV batteries also makes the EV not acceptable to many drivers.For a single charge, it takes about one half-hour to several hours depending on the power level of the attached charger,which is many times longer than the gasoline refueling process.The EVs cannot get ready immediately if they have run out of battery energy. To overcome this,what the owners would most likely do is tofind any possible opportunity to plug-in and charge the battery.It really brings some trouble as people may forget to plug-in andfind themselves out of battery energy later on. The charging cables on thefloor may bring tripping hazards. Leakage from cracked old cable,in particular in cold zones, can bring additional hazardous conditions to the owner.Also, people may have to brave the wind,rain,ice,or snow to plug-in with the risk of an electric shock.The wireless power transfer(WPT)technology,which can eliminate all the charging troublesome,is desirable by the EV owners.By wirelessly transferring energy to the EV,the charging becomes the easiest task.For a stationary WPT system,the drivers just need to park their car and leave.For a dynamic WPT system,which means the EV could be powered while driving;the EV is possible to run forever without a stop. Also,the battery capacity of EVs with wireless charging could be reduced to20%or less compared to EVs with conductive charging.Although the market demand is huge,people were just wondering whether the WPT could be realized efficiently at1Although lithium ion battery can achieve up to200Wh/kg for individual cells,the battery pack requires structure design,cooling,and battery manage-ment systems.The over energy density of a battery pack is much lower than the cell density.2168-6777©2014IEEE.Personal use is permitted,but republication/redistribution requires IEEE permission.See /publications_standards/publications/rights/index.html for more information.a reasonable cost.The research team from MIT published a paper in Science[3],in which60W power is transferred at a2-m distance with the so called strongly coupled magnetic resonance theory.The result surprised the academia and the WPT quickly became a hot research area.A lot of interesting works were accomplished with different kinds of innovative circuit,as well as the system analysis and control[4]–[9].The power transfer path can even be guided using the domino-form repeaters[10],[11].In order to transfer power more efficiently and further,the resonant frequency is usually selected at MHz level,and air-core coils are adopted.When the WPT is used in the EV charging,the MHz frequency operation is hard to meet the power and efficiency criteria.It is inefficient to convert a few to a few hundred kilowatts power at MHz frequency level using state-of-the-art power electronics devices.Moreover,air-core coils are too sensitive to the surrounding ferromagnetic objects.When an air-core coil is attached to a car,the magneticflux will go inside the chassis causing high eddy current loss as well as a significant change in the coil parameters.To make it more practical in the EV charging,ferrite as a magneticflux guide and aluminum plate as a shield are usually adopted in the coil design[12].With the lowered frequency to less than100kHz, and the use of ferrite,the WPT system is no different from the inductive power transfer(IPT)technology which has been developed for many years[13]–[39].In fact,since the WPT is based on the nonradiative and near-field electromagnetic,there is no difference with the traditional IPT which is based on magneticfield coupling between the transmitting and receiving coils.The IPT system has already been proposed and applied to various applications,such as underwater vehicles[32]–[34], mining systems[16],cordless robots in automation production lines[36]–[39],as well as the charging of electric vehicles [13],[14],[25]–[27].Recently,as the need of EV charging and also the progress in technology,the power transfer distance increases from several millimeters to a few hundred millimeters at kilowatts power level[12],[14],[40]–[60].As a proof-of-concept of a roadway inductively powered EV,the Partners for Advance Transit and Highways(PATH)program was conducted at the UC Berkeley in the late1970s[14],[54].A60kW, 35-passanger bus was tested along a213m long track with two powered sections.The bipolar primary track was supplied with1200A,400Hz ac current.The distance of the pickup from the primary track was7.6cm.The attained efficiency was around60%due to limited semiconductor technology.During the last15years,researchers at Auckland University have focused on the inductive power supply of movable objects. Their recent achievement in designing pads for the stationary charging of EV is worth noting.A766mm×578mm pad that delivers5kW of power with over90%efficiency for distances about200mm was reported[48],[55].The achieved lateral and longitudinal misalignment tolerance is 250and150mm,respectively.The knowledge gained from the on-line electric vehicle(OLEV)project conducted at the Korea Advanced Institute of Science and Technology(KAIST) also contributes to the WPT design.Three generations of OLEV systems have been built:a light golf cart as thefirst Fig.1.Typical wireless EV charging system.generation,a bus for the second,and an SUV for the third. The accomplishment of the second and the third is noteworthy: 60kW power transfer for the buses and20kW for the SUVs with efficiency of70%and83%,respectively;allowable vertical distance and lateral misalignment up to160mm and up to200mm,respectively[56],[57].In the United States, more and more public attention was drawn to the WPT since the publication of the2007Science paper[3].The WiTricity Corporation with technology from MIT released their WiT-3300development kit,which achieves90%efficiency over a 180mm gap at3.3kW output.Recently,a wireless charging system prototype for EV was developed at Oak Ridge National Laboratory(ORNL)in the United States.The tested efficiency is nearly90%for3kW power delivery[53].The research at the University of Michigan–Dearborn achieved a200mm distance,8kW WPT system with dc to dc efficiency as high as95.7%[61].From the functional aspects,it could be seen that the WPT for EV is ready in both stationary and dynamic applications.However,to make it available for large-scale commercialization,there is still abundant work to be done on the performance optimization,setup of the industrial standards, making it more cost effective,and so on.This paper starts with the basic WPT theory,and then gives a brief overview of the main parts in a WPT system, including the magnetic coupler,compensation network,power electronics converter,study methodology,and its control,and some other issues like the safety considerations.By introduc-ing the latest achievements in the WPT area,we hope the WPT in EV applications could gain a widespread acceptance in both theoretical and practical terms.Also,we hope more researchers could have an interest and make more brilliant contributions in the developing of WPT technology.II.F UNDAMENTAL T HEORYA typical wireless EV charging system is shown in Fig.1. It includes several stages to charge an EV wirelessly.First, the utility ac power is converted to a dc power source by an ac to dc converter with power factor correction.Fig.2.General two-coil WPT system.Then,the dc power is converted to a high-frequency ac todrive the transmitting coil through a compensation network.Considering the insulation failure of the primary side coil,a high-frequency isolated transformer may be inserted betweenthe dc-ac inverter and primary side coil for extra safety andprotection.The high-frequency current in the transmitting coilgenerates an alternating magneticfield,which induces an acvoltage on the receiving coil.By resonating with the secondarycompensation network,the transferred power and efficiencyare significantly improved.At last,the ac power is rectifiedto charge the battery.Fig.1shows that a wireless EV chargerconsists of the following main parts:1)the detached(or separated,loosely coupled)transmittingand receiving ually,the coils are built withferrite and shielding structure,in the later sections,theterm magnetic coupler is used to represent the entirety,including coil,ferrite,and shielding;2)the compensation network;3)the power electronics converters.The main difference between a wireless charger and aconventional conductive or wired charger is that a transformeris replaced by a set of loosely couple coils.To give a quickidea of the WPT principle,the coil and the compensationnetwork are pulled out separately,as shown in Fig.2,whereL1represents the self-inductance of the primary side transmit-ting coil and L2represents the self-inductance of the receivingcoil;˙I1and˙I2are the current in the two coils;˙U12is thevoltage in the secondary coil that is induced by the currentin the primary side coil.˙U21is the voltage in the primarycoil that is induced by the current in secondary side coil dueto coupling,or mutual inductance between the primary andsecondary coils.S1and S2are the apparent power goes intoL1and L2,respectively.S3and S4are the apparent powerprovided by the power converter.S12and S21represent theapparent power exchange between the two coils.The form ofthe compensation network is not specified.The characteristicsof the compensation network will be discussed later.As shown in Fig.2,neglecting the coil resistance andmagnetic losses,we can calculate the simplified form ofexchanged complex power from L1to L2˙S12=−˙U12˙I∗2=−jωM˙I1˙I∗2=ωM I1I2sinϕ12−jωM I1I2cosϕ12(1)˙S21=−˙U21˙I∗1=−jωM˙I2˙I∗1=−ωM I1I2sinϕ12−jωM I1I2cosϕ12(2)where I1and I2are the root mean square value andϕ12isthe phase difference between˙I1and˙I2.The active powertransfer from the primary side to the secondary side can beexpressed asP12=ωM I1I2sinϕ12.(3)The system shown in Fig.2can transfer active power inboth directions.In the analysis below,we assume the poweris transferred from L1to L2.Whenϕ12=π/2,which means˙I1leads˙I2by a quarter cycle,the maximum power can betransferred from L1to L2.The total complex power goes into the two-coil system is˙S=˙S1+˙S2=jωL1˙I1+ωM˙I2˙I∗1+jωL2˙I2+ωM˙I1˙I∗2=jωL1I21+L2I22+2M I1I2cosϕ12.(4)Therefore,the total reactive power goes into the two-coilsystem isQ=ωL1I21+L2I22+2M I1I2cosϕ12.(5)For a traditional transformer,the reactive power representsthe magnetizing power.Higher magnetizing power bringshigher copper and core loss.To increase the transformerefficiency,the ratio between the active power and reactivepower should be maximized.The ratio is defined byf(ϕ12)=|P12||Q|=ωM I1I2sinϕ12ωL1I21+ωL2I22+2ωM I1I2cosϕ12=k1−cos2ϕ12L1L2I1I2+L2L1I2I1+2k cosϕ21=k1−cos2ϕ12x+1x+2k cosϕ12(6)whereπ/2<ϕ12<πx=L1L2I1I2>0k is the coupling coefficient between L1and L2.To achieve the maximum value of f(ϕ12),we solve thefollowing equations:∂∂ϕ12f(ϕ12)=0,∂2∂2ϕ12f(ϕ12)<0(7)and the solutions arecosϕ12=−2kx+1x,sinϕ12=1−4k2x+1x2.(8)When k is close to1,it is a traditional transformer.In this case,if˙I2is an induced current by˙I1,x will be close to1. Thus,cosϕ12≈−1.The phase difference between˙I1and˙I2 is nearly180°.While for WPT,k is close to0.f(ϕ12)is maximized at sinϕ12=1,at which point the transferred power is also maximized.The phase between˙I1and˙I2is around90°instead of180°.Hence we can see the difference between the tightly and the loosely coupled coils.The degree of coupling affects the design of the compensa-tion network.Taking the series–series topology as an example, there are two ways to design the resonant capacitor.One way is design the capacitor to resonate with the leakage inductance [46],[62]which could achieve a higher f(ϕ12).Another way is to resonate with the coil self-inductance[27],[41],[63] which could maximum the transferred power at a certain coil current.When the coupling is tight with a ferrite,like k>0.5, it is important to increase f(ϕ12)to achieve better efficiency. In this case,resonate with the coil self inductance,which makesϕ12=π/2and lowers f(ϕ12),is not recommended. Otherwise the magnetizing loss may significantly increase. When the capacitor resonates with the leakage inductance,it is like the leakage inductance is compensated.This makes the transformer perform as a traditional one and increases f(ϕ12). However,the overall system does not work at a resonant mode.When the coupling is loose,like k<0.5,which is the case for the EV wireless charging,usually the capacitor is tuned with the self inductance to make the system working at a resonate mode to achieve maximum transferred power at a certain coil current.In this case,most of the magnetic field energy is stored in the large air gap between the two coils.The hysteresis loss in the ferrite is not so relative to the magnetizing power.However,the loss in the copper wire is proportional to the square of the conducting current. To efficiently transfer more power at a certain coil current,the induced current˙I2should lag˙I1by90°.Since the induced voltage˙U12on the receiving coil lags˙I1by90°,˙U12and˙I2 should be in phase.The secondary side should have a pure resistive characteristic seen from˙U12at the frequency of˙I1. At the meanwhile,the primary side input apparent power S3 should be minimized.At cosϕ12=0,the complex power˙S1is˙S1=jωL1I21+ωM I1I2.(9) Ideally,the primary side compensation network should cancel the reactive power and make S3=ω0M I1I2,where ω0is the resonant frequency.From the above analysis,we see for a certain transferred power,it is necessary to make the secondary side resonant to reduce the coil volt-ampere(V A) rating,which reduces the loss in the coils;and to make the primary side resonant to reduce the power electronics converter V A rating,which reduces the loss in the power converter. Therefore,we transfer power at the magnetic resonance. With the above analysis,we can calculate the power transfer efficiency between the two coils at the resonant frequency.We haveU12=I2(R2+R Le)=ωM I1=ωkL1L2I1(10) where R2is the secondary winding resistance and R Le is the equivalent load resistance.By defining the quality factor of the two coils, Q1=ωL1/R1,Q2=ωL2/R2,the transferred efficiency can be expressed asη=I22R LeI21R1+I22R2+I22R Le=R Le(R2+R Le)2k2Q1Q2R2+R2+R Le.(11)By defining a=R Le/R2,we obtain the expression of efficiency as a function of aη(a)=1a+1a+2k2Q1Q2+1a+1.(12)The maximum efficiency is obtained by solving the follow-ing equations:∂∂aη(a)=0,∂2∂2aη(a)<0.(13) The maximum efficiencyηmax=k2Q1Q21+1+k2Q1Q22is achieved at aηmax=1+k2Q1Q21/2.In[64],the maximum efficiency is also derived based on several different kinds of compensation network.The results are identical and accord with the above results.The analysis here does not specify a particular compensation form.It can be regarded as a general formula to evaluate the coil performance and estimate the highest possible power transfer efficiency. In EV wireless charging applications,the battery is usu-ally connected to the coil through a diode-bridge rectifier. Most of the time,there is some reactive power required. The reactive power can be provide by either the coil or the compensation network like a unit-power-factor pickup.The battery could be equivalent to a resistance R b=U b/I b,where U b and I b is the battery voltage and current,respectively. If the battery is connected to the rectifier directly in a series-series compensation form,the equivalent ac side resistance could be calculated by R ac=8/π2·R b.Thus,a battery load could be converted to a resistive load.The R ac equation is different for different battery connection style,like with or without dc/dc converter,parallel or series compensation. Most of the time,the equivalent R ac could be derived.Some typical equivalent impendence at the primary side is given in paper[42].By calculating the equivalent ac resistances,the above equations could also be applied to a battery load with rectifier.For stationary EV wireless charging,the coupling between the two coils is usually around0.2.If both the sending and receiving coils have a quality factor of300,the theoretical maximum power transfer efficiency is about96.7%.More efficiency calculations under different coupling and quality factors are shown in Fig.3.Fig.3.Theoretical maximum transfer efficiency between two coils.III.M AGNETIC C OUPLER D ESIGNTo transfer power wirelessly,there are at least two magnetic couplers in a WPT system.One is at the sending side,named primary coupler.The other is at the receiving side,named pickup coupler.Depending on the application scenarios,the magnetic coupler in a WPT for an EV could be either a pad or a track form.For higher efficiency,it is important to have high coupling coefficient k and quality factor Q. Generally,for a given structure,the larger the size to gap ratio of the coupler is,the higher the k is;the thicker the wire and the larger the ferrite section area is,the higher the Q is. By increasing the dimensions and materials,higher efficiency can be achieved.But this is not a good engineering approach. It is preferred to have higher k and Q with the minimum dimensions and cost.Since Q equalsωL/R,high frequency is usually adopted to increase the value of Q.The researchers at Massachusetts Institute of Technology(MIT)used a frequency at around10MHz and the coil Q value reached nearly 1000[3].In high power EV WPT applications,the frequency is also increased to have these benefits.In Bolger’s early design,the frequency is only180Hz[13].A few years later, a400Hz frequency EV WPT system was designed by System Control Technology[14].Neither180Hz nor400Hz is high enough for a loosely coupled system.Huge couplers were employed in the two designs.Modern WPT system uses at least10kHz frequency[15].As the technical progress of power electronics,100kHz could be achieved[65]at high power level.The WiTricity Company with the technology from MIT adopts145kHz in their design.In the recent researches and applications,the frequency adopted in an EV WPT system is between20and150kHz to balance the efficiency and cost.At this frequency,to reduce the ac loss of copper coils, Litz wire is usually adopted.Besides the frequency,the coupling coefficient k is sig-nificantly affected by the design of the magnetic couplers, which is considered one of the most important factors in a WPT system.With similar dimensions and materials,different coupler geometry and configuration will have a significant difference of coupling coefficient.A better coupler design may lead to a50%–100%improvement compared with some nonoptimal designs[48].Fig.4.Mainflux path of double-sided and single-sided coupler.(a)Double-sided type.(b)Single-sided type.A.Coupler in the Stationary ChargingIn a stationary charging,the coupler is usually designed in a pad form.The very early couplers are just like a simple split core transformer[19],[38],[56].Usually this kind of design could only transfer power through a very small gap. To meet the requirements for EV charging,the deformations from spilt core transformers and new magnetic coupler forms are presented for large gap power transfer[12],[31],[37],[42], [47]–[50],[66]–[71].According to the magneticflux dis-tribution area,the coupler could be classified as the double-sided and single-sided types.For the double-sided type,theflux goes to both sides of the coupler[12], [31],[67].Aflattened solenoid inductor form is pro-posed in[12]and[67].Because theflux goes through the ferrite like through a pipe,it is also called aflux-pipe coupler.To prevent the eddy current loss in the EV chassis,an aluminum shielding is usually added which bring a loss of1%–2%[12].When the shielding is added, the quality factor of aflux-pipe coupler reduces from 260to86[48].The high shielding loss makes the double-sided coupler not the optimal choice.For the single-sided coupler, most of theflux exists at only one side of the coupler.As shown in Fig.4,the mainflux pathflows through the ferrite in a single-sided coupler.Unlike the double-sided coupler having half of the mainflux at the back,the single-sided coupler only has a leakageflux in the back.This makes the shielding effort of a single-sided type much less.Two typical single-sidedflux type pads are shown in Fig.5. One is a circular unipolar pad[47].Another one is a rectan-gular bipolar pad proposed by University of Auckland,which is also named DD pad[48].Besides the mechanical support material,a single-sided pad is composed of three layers.The top layer is the coil.Below the coil,a ferrite layer is inserted for the purpose of enhancing and guiding theflux.At the bottom is a shielding layer.To transfer power,the two pads are put closed with coil to coil.With the shielding layer, most of the high-frequency alternating magneticflux can be confined in the space between the two pads.A fundamental flux path concept was proposed in theflux pipe paper[67].Fig. 5.Two typical single-sidedflux type pads.(a)Circular pad.(b)DD pad.Theflux path height of a circular pad is about one-fourth ofthe pad’s diameter.While for a DD pad,the height is abouthalf of the pad’s length.For a similar size,a DD pad has asignificant improvement in the coupling.The charge zone fora DD pad could be about two times larger than a circular padwith similar material cost.The DD pad has a good tolerant inthe y-direction.This makes the DD pad a potential solutionfor the dynamic charging when the driving direction is alongwith the y-axis.However,there is a null point for DD pad inthe x-direction at about34%misalignment[48].To increasethe tolerant in x-direction,an additional quadrature coil namedQ coil is proposed to work together with the DD pad,whichis called DDQ pad[48],[49],[68].With a DDQ receivingpad on a DD sending pad,the charge zone is increased tofivetimes larger than the circular configuration.As the additionalQ coil in the receiver side,the DDQ over DD configurationuses almost two times copper compared with the circularone[48].A variant of a DDQ pad,which is called a newbipolar pad,was also proposed by University of Auckland[49],[50].By increasing the size of each D pad and havingsome overlap between the two D coils,the new bipolar padcould have a similar performance of a DDQ pad with25%less copper.With all the efforts,at200mm gap,the cou-pling between the primary and secondary pads could achieve0.15–0.3with an acceptable size for an EV.Referred to Fig.3,at this coupling level,efficiency above90%could possibly beachieved.B.Coupler in the Dynamic ChargingThe dynamic charging,also called the OLEVs[56]orroadway powered electric vehicles[14],is a way to chargethe EV while driving.It is believed that the dynamic chargingcan solve the EVs’range anxiety,which is the main reasonlimits the market penetration of EVs.In a dynamic chargingsystem,the magnetic components are composed of a primaryside magnetic coupler,which is usually buried under the road,and a secondary side pickup coil,which is mounted under anEV chassis.There are mainly two kinds of primary magneticcoupler in the dynamic charging.Thefirst kind is a long trackcoupler[26],[31],[57],[70],[72]–[76].When an EV withaFig.6.Top view of W-shape and I-shape track configuration.pickup coil is running along with the track,continues powercan be transferred.The track can be as simple as just twowires[37],[77],or an adoption of ferrites with U-type orW-type[26],[56]to increase the coupling and power trans-fer distance.Further,a narrow-width track design with anI-type ferrite was proposed by KAIST[72],[73].The dif-ferences between the W-type and I-type are shown in Fig.6.For W-type configuration,the distribution area of the ferrite Wdetermines the power transfer distance,as well as the lateraldisplacement.The total width of W-type should be about fourtimes the gap between the track and the pickup coil.For I-typeconfiguration,the magnetic pole alternates along with the road.The pole distance W1is optimized to achieve better coupling atthe required distance.The width of pickup coil W2is designedto meet the lateral misalignment requirement.The relationbetween track width and transfer distance is decoupled andthe track can be built at a very narrow form.The width forU-type and W-type is140and80cm,respectively[73].ForI-type,it could be reduced to only10cm with a similar powertransfer distance and misalignment capacity.35kW power wastransferred at a200mm gap and240mm displacement usingthe I-type configuration[73].With the narrowed design,theconstruction cost could be reduced.Also,the track is far awayfrom the road side,the electromagneticfield strength exposedto pedestrians can also be reduced.The problem of the track design is that the pickup coil onlycovers a small portion of the track,which makes the couplingcoefficient very small.The poor coupling brings efficiencyand electromagnetic interference(EMI)issues.To reduce theEMI issue,the track is built by segments[52],[70],[75]with a single power converter and a set of switches to powerthe track.The excitation of each segment can be controlledby the switches’ON-OFF state.The electromagneticfieldabove the inactive segments is reduced significantly.However,there is always a high-frequency currentflowing through thecommon supply cables,which lowers the system efficiency.The published systems efficiency is about70%–80%,whichis much lower than the efficiency achieved in the stationarycharging.When each segment is short enough,the track becomes likea pad in the stationary charging,which is the other kind ofthe primary magnetic coupler.Each pad can be driven by anindependent power converter.Thus,the primary pads can beselectively excited without a high-frequency common current.Also,the energized primary pad is covered by the vehicle.Theelectromagneticfield is shielded to have a minimum impact。

HandbookofLinearPartialDifferential EquationsforEngineersRef

HandbookofLinearPartialDifferential EquationsforEngineersRef

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运载火箭故障模式及制导自适应技术应用分析

运载火箭故障模式及制导自适应技术应用分析

第40卷第3期2019年3月宇航学报Journal of AstronauticsVol.40March No.32019运载火箭故障模式及制导自适应技术应用分析常武权,张志国(北京宇航系统工程研究所,北京100076)摘要:为提高制导控制系统在运载火箭全发射任务周期中的智慧水平,提高运载火箭完成任务的鲁棒能力,从不同角度阐述了运载火箭故障模式,创新提出了基于能量属性的故障分类方法。

针对不同级别的能量故障提出了对制导控制系统的功能、性能需求。

尤其针对小、中级别能量故障,简述了运载火箭故障飞行制导自适应方法应用,包含案例及任务目标变更原则等,并分析了制导自适应技术后续工程化应用的实施途径。

基于能量属性的故障分类方法及制导自适应方法可应用于后续中国运载火箭工程研制。

关键词:故障模式;能量属性;自适应制导中图分类号:V448文献标识码:A文章编号:1000-1328(2019)03-0302-08DOI :10.3873/j.issn.1000-1328.2019.03.007Analysis of Fault Modes and Applications of Self-AdaptiveGuidance Technology for Launch VehicleCHANG Wu-quan ,ZHANG Zhi-guo(Beijing Institute of Astronautical Systems Engineering ,Beijing 100076,China )Abstract :In order to develop an intelligent guidance and control system ,which can increase the mission robust performance in the full launch cycle ,this paper provides the launch vehicle fault modes ,and presents a fault classification method based on the energy characteristics firstly.The function and performance requirements to the guidance and control system are put forward for different ranks of energy fault.Especially ,for the small and medium energy faults ,the self-adaptive guidance methods ,including the case and orbit-changing principle ,are introduced ;besides ,the ways of implementation for the applications of the self-adaptive guidance technology are discussed.The fault classification method based on the energy characteristics and the self-adaptive guidance method can be applied to the future launch vehicles of China.Key words :Fault mode ;Energy characteristics ;Self-adaptive guidance收稿日期:2018-03-19;修回日期:2018-08-090引言智慧火箭是传统运载火箭与新一代信息技术的全面有机结合[1]。

基于Hamacher_三角模的对称毕达哥拉斯集成算子及其应用

基于Hamacher_三角模的对称毕达哥拉斯集成算子及其应用

Advances in Applied Mathematics 应用数学进展, 2023, 12(4), 1713-1721 Published Online April 2023 in Hans. https:///journal/aam https:///10.12677/aam.2023.124178基于Hamacher 三角模的对称毕达哥拉斯集成算子及其应用李卓明,张铭皓,张明雪,崔 旭,马振明*临沂大学数学与统计学院,山东 临沂收稿日期:2023年3月24日;录用日期:2023年4月18日;发布日期:2023年4月27日摘要在毕达哥拉斯模糊集和Hamacher 三角模基础上,研究了一类带参数且具有对称性的集成算子。

首先给出了毕达哥拉斯模糊数的对称运算规则;其次,提出了基于Hamacher 三角模的对称毕达哥拉斯集成算子,讨论了它的性质;之后,提出一种决策方法来解决毕达哥拉斯模糊信息环境下的多属性决策问题;最后,用示例验证所给方法的有效性。

关键词Hamacher 三角模,对称毕达哥拉斯集成算子,多属性决策Symmetric Pythagorean Fuzzy Aggregation Operator Based on the Hamacher T-Norm and Its ApplicationZhuoming Li, Minghao Zhang, Mingxue Zhang, Xu Cui, Zhenming Ma *School of Mathematics and Statistics, Linyi University, Linyi ShandongReceived: Mar. 24th , 2023; accepted: Apr. 18th , 2023; published: Apr. 27th, 2023AbstractBased on the Pythagorean fuzzy set and Hamacher triangular norm, a class of aggregation opera-tors with papameters and symmetric is studied. Firstly, the operational rules of Pythagorean fuzzy numbers is provided; secondly, the symmetric Pythagorean fuzzy aggregation operator based on the Hamacher triangular norm is defined, and some properties of it are investigated in detail; af-*通讯作者。

泛函分析中的巴拿赫空间与映射

泛函分析中的巴拿赫空间与映射

泛函分析中的巴拿赫空间与映射泛函分析是数学中的一个重要分支,它研究的是无限维的向量空间及其上的泛函。

在泛函分析的研究中,巴拿赫空间和映射起着重要的作用。

下面将对巴拿赫空间和映射进行详细介绍。

一、巴拿赫空间巴拿赫空间是泛函分析中的一个重要概念,它是完备的赋范向量空间。

巴拿赫空间的定义有多种等价形式,其中最常见的是基于序列的收敛概念。

一个赋范向量空间是巴拿赫空间,当且仅当它中的任意柯西序列都收敛于该空间中的某个元素。

巴拿赫空间的一些基本性质如下:1. 巴拿赫空间是完备的,即任意柯西序列在空间内有极限。

2. 巴拿赫空间是赋范空间的完备化。

3. 巴拿赫空间是Hilbert空间的推广,也是函数空间的推广。

巴拿赫空间在数学中起着重要的作用。

它不仅是泛函分析的重要工具,也在实际问题的建模和分析中有广泛的应用。

巴拿赫空间的研究涉及到近似理论、泛函分析的极限理论等方面。

二、映射映射是函数论的一个基本概念,它是将一个集合中的元素映射到另一个集合中的元素上。

在泛函分析中,我们常常研究连续的映射。

在巴拿赫空间中,映射的概念被广泛应用。

特别地,巴拿赫空间上的线性连续映射被称为算子。

线性算子是巴拿赫空间中的重要对象,它们在函数空间、概率论、微分方程等领域中有广泛的应用。

巴拿赫空间上的映射还有一些重要的性质,如:1. 压缩映射原理:在完备的巴拿赫空间中,若一个映射的收缩因子小于1,那么这个映射在该空间上有唯一不动点。

2. 开映射定理:若一个算子是一个开映射,那么它是一个满映射。

巴拿赫空间与映射之间有着密切的联系。

巴拿赫空间是映射的定义域和值域,映射在巴拿赫空间中的性质和行为也受到巴拿赫空间的限制。

总结:泛函分析中的巴拿赫空间和映射是该领域中的重要概念。

巴拿赫空间作为完备的赋范向量空间,具有许多重要性质,它在数学和实际问题的研究中发挥着至关重要的作用。

映射则是将一个集合中的元素映射到另一个集合中的元素上,巴拿赫空间上的映射具有许多重要性质和应用。

泛函分析中的巴拿赫空间与算子理论

泛函分析中的巴拿赫空间与算子理论

泛函分析中的巴拿赫空间与算子理论泛函分析是数学中的一个重要分支,研究向量空间上的函数和算子,以及对它们的性质和结构进行描述和分析。

巴拿赫空间和算子理论是泛函分析的重要内容之一,它们在数学、物理等领域中有着广泛的应用。

一、巴拿赫空间巴拿赫空间是泛函分析中的一个重要概念,它是一个完备的赋范线性空间。

在巴拿赫空间中,任意的柯西序列都有极限,这使得巴拿赫空间具有良好的完备性质。

巴拿赫空间的定义和性质可以用数学符号来表达。

设X是一个赋范线性空间,在X中,如果任意一个柯西序列都有极限,则称X是一个巴拿赫空间。

巴拿赫空间的一个重要例子是无穷维的赋范空间l^p,其中1 ≤ p < ∞。

在l^p中,p-范数定义为||x||p = (Σ |xi|^p)^(1/p)。

l^p空间在数学分析和概率论中有广泛的应用,特别是在相关的函数空间、Hilbert空间等领域。

二、算子理论算子理论是泛函分析中研究算子和其性质的理论。

算子可以理解为将一个函数映射到另一个函数的操作。

在算子理论中,我们关注的是算子的性质,如线性性、有界性、稠密性等。

线性算子是算子理论中的基础概念。

线性算子可以简单理解为满足线性性质的函数映射。

设X和Y是两个赋范空间,如果一个算子A:X→Y满足对于任意的x, y∈X和c∈K,都有A(x+y) = A(x) + A(y)和A(cx) = cA(x),则称A是一个线性算子。

有界算子是算子理论中的重要概念。

有界算子是一类满足一定条件的线性算子,其范数是有界的。

设X和Y是两个赋范空间,如果一个线性算子A:X→Y满足存在一个常数M>0,使得对于任意的x∈X,有||A(x)|| ≤ M ||x||,则称A是一个有界算子。

巴拿赫-施托尔兹定理是算子理论中的一个重要定理。

它说明了有界线性算子的性质,描述了有界算子的范数和它在一个完备赋范空间中的性质之间的关系。

三、巴拿赫空间与算子理论的应用巴拿赫空间与算子理论在数学、物理等领域中有着广泛的应用。

Relion 615系列应用 RET615 高级保护与控制IED说明书

Relion 615系列应用 RET615 高级保护与控制IED说明书

Transformer Protection and Control RET615 Relion® 615 seriesApplicationRET615 is the advanced protection and control IED for two-winding power transformers and power generator-transformer blocks. RET615 is available in eight standard configurationsto match the most commonly employed power transformer vector groups and to coordinate the applied transformer neutral earthing principles with the relevant earth-fault protection schemes.Protection and controlRET615 features three-phase, multi-slope stabilized (biased) transformer differential protection and an instantaneous stage to provide fast and selective phase-to-phase short-circuit, winding interturn fault and bushing flash-over protection. Besides second harmonic restraint an advanced waveform-based blocking algorithm ensures stability at transformer energization and a fifth harmonic restraint function ensures good protection stability at modest transformer overexcitation. Sensitive restricted earth-fault function (REF) provides single phase-to-earth fault protection even close to the star point of the transformer. Either the conventional high-impedance or a numerical low-impedance principle can be used for protection of the transformer windings. When low-impedance REF protection is used no stabilizing resistors or varistors are needed. In addition, the transforming ratio of the neutral earthing CT may differ from that of the phase current transformers. Due to its unit protection character and absolute selectivity the REF protection does not need to be time graded with other protection schemes, and therefore high-speed fault clearance can be achieved.RET615 also includes thermal overload protection, which supervises the thermal stress of the transformer windings to prevent premature aging of the winding insulation. Multiple stages of short-circuit, phase overcurrent, negative-phase-sequence and earth fault back-up protection are providedfor both the high voltage and the low voltage side of the transformer. Depending on the selected standard configuration the IED also includes three-phase overvoltage protection, three-phase undervoltage protection and earth fault protection based on a measured or calculated residual voltage. Furthermore, RET615 also offers circuit-breaker failure protection. Enhanced with an optional communication card, RET615 offers a fast three-channel arc-fault protection system for arc flash supervision of the circuit-breaker, busbar and cable compartment of metal-enclosed air-insulated indoor switchgears.The optional RTD/mA module offered for the standard configurations A - D allow up to six temperature signals to be measured via the RTD inputs and two transducer derived ana-log signals via the mA inputs. The RTD and mA inputs can be used for measuring the oil temperature at the bottom and top of the transformer and the ambient air temperature. An RTD input can also be used as a direct resistance measuring input for position tracking of an on-load tap changer. Alternatively, tap changer position can be obtained via a mA-transducer. The analog temperature or tap changer position values can, if required, be sent using analog horizontal GOOSE messaging to other IEDs.RET615 is a dedicated transformer protection and control IED for power transformers, unit and step-up transformers including power generator-transformer blocks in utility and industry power distribution systems. RET615 is a member of ABB’s Relion® protection and control product family and its 615 series. The 615 series IEDs are characterized by their compactness and withdrawable-unit design. Re-engineered from the ground up, the 615 series has been designed to unleash the full potential of the IEC 61850 standardfor communication and interoperability between substation automation devices.RET615 also integrates functionality for the control of theHV-side circuit breaker via the front panel HMI or by means of remote controls.A standard configuration can be adjusted using the signal matrix functionality (SMT) or the optional graphical application configuration functionality (ACT) of the Protection and Control IED Manager PCM600. The ACT supports creation of multi-layer logic by combining function blocks along with timers and flip-flops. By combining protection and logic functions the IED can be modified to exactly fit the application.Standardized communicationRET615 features genuine support for the new IEC 61850 standard for inter-device substation communication. It also supports the DNP3, the IEC 60870-5-103 protocol and the industry standard Modbus® protocol. For redundancy theIED offers an optional second Ethernet bus. The second bus forms a cost efficient communication loop controlled by a managed switch. The redundant solution eliminates single point of failure concerns and improves the reliability of the communication. It can be built on the Ethernet basedIEC 61850, Modbus® and DNP3 protocols.The implementation of the IEC 61850 standard in RET615 covers both vertical and horizontal communication, including GOOSE messaging with both binary and analog signals and parameter setting according to IEC 61850-8-1. For accurate time stamping RET615 supports synchronization over Ethernet using SNTP or over a separate bus using IRIG-B. Pre-emptive condition monitoringFor continuous control of its operational availability RET615 features a comprehensive set of monitoring functions to supervise the IED itself, the CB trip circuit and the circuit breaker.Single line diagramThe 615 series IEDs with large graphical display offer customizable single line mimic diagrams (SLD) with position indication for the switching devices. The IED can also display measured values provided by the chosen standard configuration. The SLD is also available via the web-browser based HMI. The default SLD can be modified according to user needs using the graphical display editor of PCM600.For more information see RET615 Product Guide or contact us: ABB Oy, Distribution AutomationP.O. Box 699FI-65101 VAASA, FinlandPhone: +358 10 22 11Fax: +358 10 22 41094/substationautomationI2>4651P-13I>ARC50L3I>>>50P/51PIoLo>87NL Io>>51N-2Io> BF51NBF ARC50NL3I>>>50P/51PMAP MAP 3I>51P-1 3I>>51P-2Io3I>>51P-23θ>T49T I2>463I>BF51BF3I>T87TIo>51N-1Io1) Optional1)1)1)Protection function overview of the A configuration of RET615.。

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4
It remains to check that (6) entails λ2j −1 (f (AE )) ≤ λj (f (A)E ). This follows from the forthcoming elementary observation. Proposition 1.2. Let X , Y be Hermitians such that UY U∗ + V Y V ∗ X≤ 2 for some unitaries U , V . Then, for j = 1, 2, . . . , λ2j −1 (X ) ≤ λj (Y ). 2
Abstract. We establish several convexity results for Hermitian matrices. For instance: Let A, B be Hermitian and let f be a convex function. If X and Y stands for f ({A + B }/2) and {f (A) + f (B )}/2 respectively, then there exist unitaries U , V such that UY U∗ + V Y V ∗ . 2 This is nothing but the matrix version of the scalar convexity inequality X≤ f a+b 2 ≤ f (a) + f (b) . 2
As a consequence we get, λ2j −1 (X ) ≤ λj (Y ), where λj (·) are the eigenvalues arranged in decreasing order. Keywords: Hermitian operators, eigenvalues, operator inequalities, Jensen’s inequality Mathematical subjects classification: 47A30 47A63
∗ 0 U0 . 0 V0∗
Besides we note that, still in respect with the decomposition E = E ′ ⊕ E ′′ , f (A)E ′ 0 So, letting U= we get f (AE ) ≤ U f (A)E U ∗ + V f (A)E V ∗ . 2 (6) U0 0 0 V0 and V = U0 0 0 − V0 0 f (A)E ′′ = 1 2 I 0 f (A)E 0 I I 0 I 0 + f (A)E 0 I 0 −I I 0 0 −I .
When f is convex and monotone, we showed [2] that (2) can be extended to an operator inequality: There exists a unitary U such that f A+B 2 ≤U·
1Байду номын сангаас
f (A) + f (B ) · U∗ 2
Hermitian operators and convex functions
arXiv:math/0601318v2 [math.OA] 16 Jan 2006
Jean-Christophe Bourin E-mail: bourinjc@club-internet.fr Universit´ e de Cergy-Pontoise, d´ ept. de Math´ ematiques 2 rue Adolphe Chauvin, 95302 Pontoise, France
Introduction
The main aim of this paper is to give a matrix version of the scalar inequality f a+b 2 ≤ f (a) + f (b) 2 (1)
for convex functions f on the real line. Capital letters A, B . . . Z mean n-by-n complex matrices, or operators on a finite dimensional Hilbert space H; I stands for the identity. When A is positive semidefinite, resp. positive definite, we write A ≥ 0, resp. A > 0. A classical matrix version of (1) is von Neuman’s Trace Inequality: For Hermitians A, B , Tr f A+B 2 ≤ Tr f (A) + f (B ) 2 (2)
1. Compressions
Our substitute to (4) for general convex functions (on the real line) is: Theorem 1.1. Let A be Hermitian, let E be a subspace and let f be a convex function. Then, there exist unitaries U , V on E such that U f (A)E U ∗ + V f (A)E V ∗ . f (AE ) ≤ 2 Consequently, for j = 1, 2, . . . , λ2j −1 (f (AE )) ≤ λj (f (A)E ).
3
Proof. We may find spectral subspaces E ′ and E ′′ for AE and a real r such that (i) E = E ′ ⊕ E ′′ , (ii) the spectrum of AE ′ lies on (−∞, r ] and the spectrum of AE ′′ lies on [r, ∞), (iii) f is monotone both on (−∞, r ] and [r, ∞). Let k be an integer, 1 ≤ k ≤ dim E ′ . There exists a spectral subspace F ⊂ E ′ for AE ′ (hence for f (AE ′ )), dim F = k, such that λk [f (AE ′ )] =
(3)
2
We also established similar inequalities involving more general convex combinations. These inequalities are equivalent to an inequality for compressions. Recall that given an operator Z and a subspace E with corresponding orthoprojection E , the compression of Z onto E , denoted by ZE , is the restriction of EZ to E . Inequality (3) can be derived from: For every Hermitian A, subspace E and monotone convex function f , there exists a unitary operator U on E such that f (AE ) ≤ U f (A)E U ∗ . (4) Inequalities (3) and (4) are equivalent to inequalities for eigenvalues. For instance (4) can be rephrased as λj (f (AE )) ≤ λj (f (A)E ), j = 1, 2, . . . where λj (·), j = 1, 2, . . . are the eigenvalues arranged in decreasing order and counted with their multiplicities. Having proved an inequality such as (3) for monotone convex functions, it remains to search counterparts for general convex functions. We derived from (3) the following result for even convex functions f : Given Hermitians A, B , there exist unitaries U , V such that U f (A)U ∗ + V f (B )V ∗ A+B . (5) ≤ f 2 2 This generalizes a wellknown inequality for the absolute value, |A + B | ≤ U |A|U ∗ + V |B |V ∗ We do not know whether (5) is valid for all convex functions. In Section 1 we present a counterpart of (4) for all convex functions. This will enable us to give, in Section 2, a quite natural counterpart of (3) for all convex functions. Though (3) can be proven independently of (4) -and the same for the counterparts-, we have the feeling that in the case of general convex functions, the approach via compressions is more illuminating.
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