Sir William Rowan Hamilton Life, Achievements, Stature in Physics
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AN INTRODUCTION to LAGRANGIAN MECHANICS Alain
AN INTRODUCTION TO LAGRANGIAN MECHANICS Alain J. Brizard Department of Chemistry and Physics Saint Michael’s College, Colchester, VT 05439 July 7, 2007 i Preface The original purpose of the present lecture notes on Classical Mechanics was to sup- plement the standard undergraduate textbooks (such as Marion and Thorton’s Classical Dynamics of Particles and Systems) normally used for an intermediate course in Classi- cal Mechanics by inserting a more general and rigorous introduction to Lagrangian and Hamiltonian methods suitable for undergraduate physics students at sophomore and ju- nior levels. The outcome of this effort is that the lecture notes are now meant to provide a self-consistent introduction to Classical Mechanics without the need of any additional material. It is expected that students taking this course will have had a one-year calculus-based introductory physics course followed by a one-semester course in Modern Physics. Ideally, students should have completed their three-semester calculus sequence by the time they enroll in this course and, perhaps, have taken a course in ordinary differential equations. On the other hand, this course should be taken before a rigorous course in Quantum Mechanics in order to provide students with a sound historical perspective involving the connection between Classical Physics and Quantum Physics. Hence, the second semester of the sophomore year or the fall semester of the junior year provide a perfect niche for this course. The structure of the lecture notes presented here is based on achieving several goals. As a first goal, I originally wanted to model these notes after the wonderful monograph of Landau and Lifschitz on Mechanics, which is often thought to be too concise for most undergraduate students. -
MA-302 Advanced Calculus 8
Prof. D. P.Patil, Department of Mathematics, Indian Institute of Science, Bangalore Aug-Dec 2002 MA-302 Advanced Calculus 8. Inverse function theorem Carl Gustav Jacob Jacobi† (1804-1851) The exercises 8.1 and 8.2 are only to get practice, their solutions need not be submitted. 8.1. Determine at which points a of the domain of definition G the following maps F have differentiable inverse and give the biggest possible open subset on which F define a diffeomorphism. a). F : R2 → R2 with F(x,y) := (x2 − y2, 2xy) . (In the complex case this is the function z → z2.) b). F : R2 → R2 with F(x,y) := (sin x cosh y,cos x sinh y). (In the complex case this is the function z → sin z.) c). F : R2 → R2 with F(x,y) := (x+ y,x2 + y2) . d). F : R3 → R3 with F(r,ϕ,h) := (r cos ϕ,rsin ϕ,h). (cylindrical coordinates) × 2 2 3 3 e). F : (R+) → R with F(x,y) := (x /y , y /x) . xy f). F : R2 → R2 with F(x,y) := (x2 + y2 ,e ) . 8.2. Show that the following maps F are locally invertible at the given point a, and find the Taylor-expansion F(a) of the inverse map at the point upto order 2. a). F : R3 → R3 with F(x,y,z) := − (x+y+z), xy+xz+yz,−xyz at a =(0, 1, 2) resp. a =(−1, 2, 1). ( Hint : The problem consists in approximating the three zeros of the monic polynomial of degree 3 whose coefficients are close to those of X(X−1)(X−2) resp. -
Carl Gustav Jacob Jacobi
CARL GUSTAV JACOB JACOBI Along with Norwegian Niels Abel, German mathematician Carl Gustav Jacob Jacobi (December 10, 1804 – February 18, 1851) was one of the founders of the theory of elliptic functions, which he described in his 1829 work Fundamenta Nova Theoriae Functionum Ellipticarum (New Foundations of the Theory of Elliptic Functions). His achievements in this area drew praise from Joseph-Louis Lagrange, who had spent some 40 years studying elliptic integrals. Jacobi also investigated number theory, mathematical analysis, geometry and differential equations. His work with determinants, in particular the Hamilton-Jacobi theory, a technique of solving a system of partial differential equations by transforming coordinates, is important in the presentation of dynamics and quantum mechanics. V.I. Arnold wrote of the Hamilton-Jacobi method, “… this is the most powerful method known for exact integration.” Born in Potsdam, Jacobi was the son of a prosperous Jewish banker. His older brother Moritz Hermann Jacobi was a well-known physicist and engineer. The latter worked as a leading researcher at the Academy of Sciences in St. Petersburg. During their lifetimes Moritz was the better known of the two for his work on the practical applications of electricity and especially for his discovery in 1838 of galvanoplastics. Also called electrotyping, it is a process something like electroplating for making duplicate plates of relief, or letterpress, printing. Carl was constantly mistaken for his brother or even worse congratulated for having such a distinguished and accomplished brother. To one such compliment he responded with annoyance, “I am not his brother, he is mine.” Carl Jacobi demonstrated great talent for both languages and mathematics from an early age. -
Fermat's Principle and the Geometric Mechanics of Ray
Fermat’s Principle and the Geometric Mechanics of Ray Optics Summer School Lectures, Fields Institute, Toronto, July 2012 Darryl D Holm Imperial College London [email protected] http://www.ma.ic.ac.uk/~dholm/ Texts for the course include: Geometric Mechanics I: Dynamics and Symmetry, & II: Rotating, Translating and Rolling, by DD Holm, World Scientific: Imperial College Press, Singapore, Second edition (2011). ISBN 978-1-84816-195-5 and ISBN 978-1-84816-155-9. Geometric Mechanics and Symmetry: From Finite to Infinite Dimensions, by DD Holm,T Schmah and C Stoica. Oxford University Press, (2009). ISBN 978-0-19-921290-3 Introduction to Mechanics and Symmetry, by J. E. Marsden and T. S. Ratiu Texts in Applied Mathematics, Vol. 75. New York: Springer-Verlag (1994). 1 GeometricMechanicsofFermatRayOptics DDHolm FieldsInstitute,Toronto,July2012 2 Contents 1 Mathematical setting 5 2 Fermat’s principle 8 2.1 Three-dimensional eikonal equation . 10 2.2 Three-dimensional Huygens wave fronts . 17 2.3 Eikonal equation for axial ray optics . 23 2.4 The eikonal equation for mirages . 29 2.5 Paraxial optics and classical mechanics . 32 3 Lecture 2: Hamiltonian formulation of axial ray optics 34 3.1 Geometry, phase space and the ray path . 36 3.2 Legendre transformation . 39 4 Hamiltonian form of optical transmission 42 4.1 Translation-invariant media . 49 4.2 Axisymmetric, translation-invariant materials . 50 4.3 Hamiltonian optics in polar coordinates . 53 4.4 Geometric phase for Fermat’s principle . 56 4.5 Skewness . 58 4.6 Lagrange invariant: Poisson bracket relations . 63 GeometricMechanicsofFermatRayOptics DDHolm FieldsInstitute,Toronto,July2012 3 5 Axisymmetric invariant coordinates 69 6 Geometry of invariant coordinates 73 6.1 Flows of Hamiltonian vector fields . -
Analogy in William Rowan Hamilton's New Algebra
Technical Communication Quarterly ISSN: 1057-2252 (Print) 1542-7625 (Online) Journal homepage: https://www.tandfonline.com/loi/htcq20 Analogy in William Rowan Hamilton's New Algebra Joseph Little & Maritza M. Branker To cite this article: Joseph Little & Maritza M. Branker (2012) Analogy in William Rowan Hamilton's New Algebra, Technical Communication Quarterly, 21:4, 277-289, DOI: 10.1080/10572252.2012.673955 To link to this article: https://doi.org/10.1080/10572252.2012.673955 Accepted author version posted online: 16 Mar 2012. Published online: 16 Mar 2012. Submit your article to this journal Article views: 158 Citing articles: 1 View citing articles Full Terms & Conditions of access and use can be found at https://www.tandfonline.com/action/journalInformation?journalCode=htcq20 Technical Communication Quarterly, 21: 277–289, 2012 Copyright # Association of Teachers of Technical Writing ISSN: 1057-2252 print/1542-7625 online DOI: 10.1080/10572252.2012.673955 Analogy in William Rowan Hamilton’s New Algebra Joseph Little and Maritza M. Branker Niagara University This essay offers the first analysis of analogy in research-level mathematics, taking as its case the 1837 treatise of William Rowan Hamilton. Analogy spatialized Hamilton’s key concepts—knowl- edge and time—in culturally familiar ways, creating an effective landscape for thinking about the new algebra. It also structurally aligned his theory with the real number system so his objects and operations would behave customarily, thus encompassing the old algebra while systematically bringing into existence the new. Keywords: algebra, analogy, mathematics, William Rowan Hamilton INTRODUCTION Studies of analogy in technical discourse have made important strides in the 30 years since Lakoff and Johnson (1980) ushered in the cognitive linguistic turn. -
Mathematical Genealogy of the Union College Department of Mathematics
Gemma (Jemme Reinerszoon) Frisius Mathematical Genealogy of the Union College Department of Mathematics Université Catholique de Louvain 1529, 1536 The Mathematics Genealogy Project is a service of North Dakota State University and the American Mathematical Society. Johannes (Jan van Ostaeyen) Stadius http://www.genealogy.math.ndsu.nodak.edu/ Université Paris IX - Dauphine / Université Catholique de Louvain Justus (Joost Lips) Lipsius Martinus Antonius del Rio Adam Haslmayr Université Catholique de Louvain 1569 Collège de France / Université Catholique de Louvain / Universidad de Salamanca 1572, 1574 Erycius (Henrick van den Putte) Puteanus Jean Baptiste Van Helmont Jacobus Stupaeus Primary Advisor Secondary Advisor Universität zu Köln / Université Catholique de Louvain 1595 Université Catholique de Louvain Erhard Weigel Arnold Geulincx Franciscus de le Boë Sylvius Universität Leipzig 1650 Université Catholique de Louvain / Universiteit Leiden 1646, 1658 Universität Basel 1637 Union College Faculty in Mathematics Otto Mencke Gottfried Wilhelm Leibniz Ehrenfried Walter von Tschirnhaus Key Universität Leipzig 1665, 1666 Universität Altdorf 1666 Universiteit Leiden 1669, 1674 Johann Christoph Wichmannshausen Jacob Bernoulli Christian M. von Wolff Universität Leipzig 1685 Universität Basel 1684 Universität Leipzig 1704 Christian August Hausen Johann Bernoulli Martin Knutzen Marcus Herz Martin-Luther-Universität Halle-Wittenberg 1713 Universität Basel 1694 Leonhard Euler Abraham Gotthelf Kästner Franz Josef Ritter von Gerstner Immanuel Kant -
Leonhard Euler: His Life, the Man, and His Works∗
SIAM REVIEW c 2008 Walter Gautschi Vol. 50, No. 1, pp. 3–33 Leonhard Euler: His Life, the Man, and His Works∗ Walter Gautschi† Abstract. On the occasion of the 300th anniversary (on April 15, 2007) of Euler’s birth, an attempt is made to bring Euler’s genius to the attention of a broad segment of the educated public. The three stations of his life—Basel, St. Petersburg, andBerlin—are sketchedandthe principal works identified in more or less chronological order. To convey a flavor of his work andits impact on modernscience, a few of Euler’s memorable contributions are selected anddiscussedinmore detail. Remarks on Euler’s personality, intellect, andcraftsmanship roundout the presentation. Key words. LeonhardEuler, sketch of Euler’s life, works, andpersonality AMS subject classification. 01A50 DOI. 10.1137/070702710 Seh ich die Werke der Meister an, So sehe ich, was sie getan; Betracht ich meine Siebensachen, Seh ich, was ich h¨att sollen machen. –Goethe, Weimar 1814/1815 1. Introduction. It is a virtually impossible task to do justice, in a short span of time and space, to the great genius of Leonhard Euler. All we can do, in this lecture, is to bring across some glimpses of Euler’s incredibly voluminous and diverse work, which today fills 74 massive volumes of the Opera omnia (with two more to come). Nine additional volumes of correspondence are planned and have already appeared in part, and about seven volumes of notebooks and diaries still await editing! We begin in section 2 with a brief outline of Euler’s life, going through the three stations of his life: Basel, St. -
Schrödinger's Argument.Pdf
SCHRÖDINGER’S TRAIN OF THOUGHT Nicholas Wheeler, Reed College Physics Department April 2006 Introduction. David Griffiths, in his Introduction to Quantum Mechanics (2nd edition, 2005), is content—at equation (1.1) on page 1—to pull (a typical instance of) the Schr¨odinger equation 2 2 i ∂Ψ = − ∂ Ψ + V Ψ ∂t 2m ∂x2 out of his hat, and then to proceed directly to book-length discussion of its interpretation and illustrative physical ramifications. I remarked when I wrote that equation on the blackboard for the first time that in a course of my own design I would feel an obligation to try to encapsulate the train of thought that led Schr¨odinger to his equation (1926), but that I was determined on this occasion to adhere rigorously to the text. Later, however, I was approached by several students who asked if I would consider interpolating an account of the historical events I had felt constrained to omit. That I attempt to do here. It seems to me a story from which useful lessons can still be drawn. 1. Prior events. Schr¨odinger cultivated soil that had been prepared by others. Planck was led to write E = hν by his successful attempt (1900) to use the then-recently-established principles of statistical mechanics to account for the spectral distribution of thermalized electromagnetic radiation. It was soon appreciated that Planck’s energy/frequency relation was relevant to the understanding of optical phenomena that take place far from thermal equilibrium (photoelectric effect: Einstein 1905; atomic radiation: Bohr 1913). By 1916 it had become clear to Einstein that, while light is in some contexts well described as a Maxwellian wave, in other contexts it is more usefully thought of as a massless particle, with energy E = hν and momentum p = h/λ. -
Hamilton's Principle in Continuum Mechanics
Hamilton’s Principle in Continuum Mechanics A. Bedford University of Texas at Austin This document contains the complete text of the monograph published in 1985 by Pitman Publishing, Ltd. Copyright by A. Bedford. 1 Contents Preface 4 1 Mechanics of Systems of Particles 8 1.1 The First Problem of the Calculus of Variations . 8 1.2 Conservative Systems . 12 1.2.1 Hamilton’s principle . 12 1.2.2 Constraints.......................... 15 1.3 Nonconservative Systems . 17 2 Foundations of Continuum Mechanics 20 2.1 Mathematical Preliminaries . 20 2.1.1 Inner Product Spaces . 20 2.1.2 Linear Transformations . 22 2.1.3 Functions, Continuity, and Differentiability . 24 2.1.4 Fields and the Divergence Theorem . 25 2.2 Motion and Deformation . 27 2.3 The Comparison Motion . 32 2.4 The Fundamental Lemmas . 36 3 Mechanics of Continuous Media 39 3.1 The Classical Theories . 40 3.1.1 IdealFluids.......................... 40 3.1.2 ElasticSolids......................... 46 3.1.3 Inelastic Materials . 50 3.2 Theories with Microstructure . 54 3.2.1 Granular Solids . 54 3.2.2 Elastic Solids with Microstructure . 59 2 4 Mechanics of Mixtures 65 4.1 Motions and Comparison Motions of a Mixture . 66 4.1.1 Motions............................ 66 4.1.2 Comparison Fields . 68 4.2 Mixtures of Ideal Fluids . 71 4.2.1 Compressible Fluids . 71 4.2.2 Incompressible Fluids . 73 4.2.3 Fluids with Microinertia . 75 4.3 Mixture of an Ideal Fluid and an Elastic Solid . 83 4.4 A Theory of Mixtures with Microstructure . 86 5 Discontinuous Fields 91 5.1 Singular Surfaces . -
Leonhard Euler Moriam Yarrow
Leonhard Euler Moriam Yarrow Euler's Life Leonhard Euler was one of the greatest mathematician and phsysicist of all time for his many contributions to mathematics. His works have inspired and are the foundation for modern mathe- matics. Euler was born in Basel, Switzerland on April 15, 1707 AD by Paul Euler and Marguerite Brucker. He is the oldest of five children. Once, Euler was born his family moved from Basel to Riehen, where most of his childhood took place. From a very young age Euler had a niche for math because his father taught him the subject. At the age of thirteen he was sent to live with his grandmother, where he attended the University of Basel to receive his Master of Philosphy in 1723. While he attended the Universirty of Basel, he studied greek in hebrew to satisfy his father. His father wanted to prepare him for a career in the field of theology in order to become a pastor, but his friend Johann Bernouilli convinced Euler's father to allow his son to pursue a career in mathematics. Bernoulli saw the potentional in Euler after giving him lessons. Euler received a position at the Academy at Saint Petersburg as a professor from his friend, Daniel Bernoulli. He rose through the ranks very quickly. Once Daniel Bernoulli decided to leave his position as the director of the mathmatical department, Euler was promoted. While in Russia, Euler was greeted/ introduced to Christian Goldbach, who sparked Euler's interest in number theory. Euler was a man of many talents because in Russia he was learning russian, executed studies on navigation and ship design, cartography, and an examiner for the military cadet corps. -
Principle of Virtual Work
Chapter 1 Principle of virtual work 1.1 Constraints and degrees of freedom The number of degrees of freedom of a system is equal to the number of variables required to describe the state of the system. For instance: • A particle constrained to move along the x axis has one degree of freedom, the position x on this axis. • A particle constrained to the surface of the earth has two degrees of freedom, longitude and latitude. • A wheel rotating on a fixed axle has one degree of freedom, the angle of rotation. • A solid body in free space has six degrees of freedom: a particular atom in the body can move in three dimensions, which accounts for three degrees of freedom; another atom can move on a sphere with the first particle at its center for two additional degrees of freedom; any other atom can move in a circle about the line passing through the first two atoms. No other independent motion of the body is possible. • N atoms moving freely in three-dimensional space collectively have 3N degrees of freedom. 1.1.1 Holonomic constraints Suppose a mass is constrained to move in a circle of radius R in the x-y plane. Without this constraint it could move freely over this plane. Such a constraint could be expressed by the equation for a circle, x2 + y2 = R2. A better way to represent this constraint is F (x; y) = x2 + y2 − R2 = 0: (1.1.1) 1 CHAPTER 1. PRINCIPLE OF VIRTUAL WORK 2 As we shall see, this constraint may be useful when expressed in differential form: @F @F dF = dx + dy = 2xdx + 2ydy = 0: (1.1.2) @x @y A constraint that can be represented by setting to zero a function of the variables representing the configuration of a system (e.g., the x and y locations of a mass moving in a plane) is called holonomic. -
Euler and His Work on Infinite Series
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 44, Number 4, October 2007, Pages 515–539 S 0273-0979(07)01175-5 Article electronically published on June 26, 2007 EULER AND HIS WORK ON INFINITE SERIES V. S. VARADARAJAN For the 300th anniversary of Leonhard Euler’s birth Table of contents 1. Introduction 2. Zeta values 3. Divergent series 4. Summation formula 5. Concluding remarks 1. Introduction Leonhard Euler is one of the greatest and most astounding icons in the history of science. His work, dating back to the early eighteenth century, is still with us, very much alive and generating intense interest. Like Shakespeare and Mozart, he has remained fresh and captivating because of his personality as well as his ideas and achievements in mathematics. The reasons for this phenomenon lie in his universality, his uniqueness, and the immense output he left behind in papers, correspondence, diaries, and other memorabilia. Opera Omnia [E], his collected works and correspondence, is still in the process of completion, close to eighty volumes and 31,000+ pages and counting. A volume of brief summaries of his letters runs to several hundred pages. It is hard to comprehend the prodigious energy and creativity of this man who fueled such a monumental output. Even more remarkable, and in stark contrast to men like Newton and Gauss, is the sunny and equable temperament that informed all of his work, his correspondence, and his interactions with other people, both common and scientific. It was often said of him that he did mathematics as other people breathed, effortlessly and continuously.