DOCSLIB.ORG

Breaking of Galilean Invariance in the Hydrodynamic Formulation of Ferromagnetic Thin Films

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Breaking of Galilean Invariance in the Hydrodynamic Formulation of Ferromagnetic Thin Films week ending PRL 118, 017203 (2017) PHYSICAL REVIEW LETTERS 6 JANUARY 2017 Breaking of Galilean Invariance in the Hydrodynamic Formulation of Ferromagnetic Thin Films Ezio Iacocca,1,2,* T. J. Silva,3 and Mark A. Hoefer1 1Department of Applied Mathematics, University of Colorado, Boulder, Colorado 80309-0526, USA 2Department of Physics, Division for Theoretical Physics, Chalmers University of Technology, 412 96 Gothenburg, Sweden 3National Institute of Standards and Technology, Boulder, Colorado 80305-3328, USA (Received 30 June 2016; published 5 January 2017) Microwave magnetodynamics in ferromagnets are often studied in the small-amplitude or weakly nonlinear regime corresponding to modulations of a well-defined magnetic state. However, strongly nonlinear regimes, where the aforementioned approximations are not applicable, have become exper- imentally accessible. By reinterpreting the governing Landau-Lifshitz equation of motion, we derive an exact set of equations of dispersive hydrodynamic form that are amenable to analytical study even when full nonlinearity and exchange dispersion are included. The resulting equations are shown to, in general, break Galilean invariance. A magnetic Mach number is obtained as a function of static and moving reference frames. The simplest class of solutions are termed uniform hydrodynamic states (UHSs), which exhibit fluidlike behavior including laminar flow at subsonic speeds and the formation of a Mach cone and wave fronts at supersonic speeds. A regime of modulational instability is also possible, where the UHS is violently unstable. The hydrodynamic interpretation opens up novel possibilities in magnetic research. DOI: 10.1103/PhysRevLett.118.017203 Magnetodynamics in thin film ferromagnets has been This Letter shows that the LL equation exactly maps into studied for many decades. Advances in nanofabrication and a DH system of equations, without long-wavelength and the advent of spin transfer [1,2] and spin-orbit torques [3] low-frequency restrictions. The conservative equations are have opened a new frontier of experimentally accessible analogous to the Euler equations of a compressible, isen- nonlinear physics [4–8]. Large-amplitude excitations neg- tropic fluid. The DH equations for a planar ferromagnet ate the use of typical linear or weakly nonlinear analyses admit spin-current-carrying, spatially periodic magnetiza- [9–11], necessitating instead either micromagnetic simu- tion textures termed “uniform hydrodynamic states” lations [12] or analytical approaches suited to strongly (UHSs), providing a continuous interpolation between large nonlinear dynamics. Therefore, an interpretation of the amplitude spin superflows [14–16] and small-amplitude Landau-Lifshitz (LL) equation that includes full nonlinear- spin waves. Within the DH formulation, we prove that ity, yet is amenable to analytical study, would be insightful. planar ferromagnets break Galilean invariance and elucidate A hydrodynamic interpretation was proposed by Halperin their reference-frame-dependent dynamics by identifying and Hohenberg [13] to describe spin waves in anisotropic the linear dispersion relation for spin waves propagating on ferro- and antiferromagnets. Recently, theoretical studies of top of a UHS background. Such symmetry breaking at the thin film ferromagnets with planar anisotropy have identified level of linear spin waves is striking and fundamentally a relationship to superfluidlike hydrodynamic equations different from the nontrivial speed-dependent dynamics of [14–19] supporting large-amplitude modes beyond weakly topological textures due to their inherent nonlinearity, e.g., nonlinear spin wave and macrospin modes [10,11]. However, Walker breakdown for domain wall propagation [35] and these studies are limited to the long-wavelength, low- core reversal in magnetic vortices [36]. In this Letter, we also frequency regime where linear and weakly nonlinear show that static textures can break Galilean invariance for approaches apply. The relaxation of these approximations infinitesimal spin wave excitations that ride on a textured along with the identification of a deep connection between background. To emphasize this novel result, we suggest a magnetodynamics and fluid dynamics brings new perspec- Brillouin light scattering experimental test where broken tives on magnetism and reveals novel physical regimes. Galilean invariance manifests itself as a spin-wave Indeed, nonlinear, dispersive physics are required to describe dispersion shift in the presence of a UHS. superfluids and exotic structures such as solitons, quantized We consider the nondimensionalized LL equation (see vortices, and dispersive shock waves (DSWs) [20–23], Supplemental Material [37]) as exemplified by Bose-Einstein condensates (BECs) ∂m ¼ −m × h − αm × m × h : ð1Þ [20–22,24–34]. To obtain an analytical description of ∂t eff eff large-amplitude magnetic textures, we introduce dispersive Damping is parametrized by the Gilbert constant α, hydrodynamic (DH) equations for a thin-film ferromagnet. m¼M=Ms ¼ðmx;my;mzÞ is the magnetization vector 0031-9007=17=118(1)=017203(6) 017203-1 © 2017 American Physical Society week ending PRL 118, 017203 (2017) PHYSICAL REVIEW LETTERS 6 JANUARY 2017 h ¼ Δm− 2 normalized to the saturation magnetization, and eff limit, i.e., j∇nj ≪ 1, jnj ≪ 1, and juj ≪ 1. As we show σmzzˆ þ h0zˆ is the normalized effective field including below, the full nonlinearity and exchange dispersion ferromagnetic exchange, Δm; total anisotropy determined included in Eqs. (3a) and (3b) are required to describe by σ ¼ sgnðMs − HkÞ, where Hk is the perpendicular the existence and stability regions of magnetic hydro- magnetic anisotropy field, such that σ ¼þ1 (σ ¼ −1) dynamic states and broken Galilean invariance. represents a material with easy-plane (perpendicular mag- Insight can be gained from the homogeneous field netic) anisotropy; and a perpendicular applied field, h0zˆ. ∇h0 → 0, conservative α → 0 limit, where Eqs. (3) become This nondimensionalization of a two-dimensional (2D) thin conservation laws for n and u. Notably, the non-negative film provides a parameter-free description of materials with deviation from vacuum ð1 − n2Þ, or fluid density, is not planar or uniaxial anisotropy. We consider an idealized case conserved. A conservation law for the momentum p ¼ nu where in-plane magnetic anisotropy is negligible; i.e., its can also be obtained, symmetry-breaking contribution only perturbs the leading ∂p ∇n∇nT order solution, similar to domain wall Brownian motion [40]. ¼ ∇ ½ð1 − n2ÞuuTþ∇Pðn; jujÞ þ ∇ ∂t · · 1 − n2 Fluidlike variables are introduced using the canonical Hamiltonian cylindrical transformation [41] nΔn þ 1 j∇nj2 n2j∇nj2 − ∇ 2 þ ; ð Þ 1 − n2 ð1 − n2Þ2 5 n ¼ mz; u ¼ −∇Φ ¼ −∇½arctan ðmy=mxÞ; ð2Þ where the magnetic pressure is defined as where Φ is the azimuthal phase angle. We identify n jnj ≤ 1 u 1 2 2 ( ) as the longitudinal spin density and as the fluid Pðn; jujÞ ¼ ð1 þ n Þðσ − juj Þ − σ: ð6Þ velocity. There are two important features of Eq. (2). First, 2 the flow is irrotational because the velocity originates from Equations (3a) with α ¼ 0, and (5) are analogous to the a phase gradient, i.e., only quantized circulation, such as a time-reversed Euler equations expressing conservation of magnetic vortex [15], is possible. Second, Φ is undefined mass and momentum for a 2D, compressible, isentropic when n ¼1, corresponding to fluid vacuum. fluid with a density- and velocity-dependent pressure P. Utilizing the transformation (2) and standard vector Additionally, the one-dimensional conservative limit of calculus identities, the LL equation (1) can be exactly Eqs. (3a) and (3b) are exactly the equations describing recast as two DH equations [37] polarization waves in two-component spinor Bose gases jnj ∼ 1 ∂n ∂Φ [33,34] and, in the near vacuum ( ), long-wavelength, ¼ ∇ ½ð1 − n2Þu þ αð1 − n2Þ ; ð Þ and low-frequency regime, approximate the mean field ∂t · |fflfflfflfflfflfflffl{zfflfflfflfflfflfflffl} ∂t 3a |fflfflfflfflfflfflfflfflffl{zfflfflfflfflfflfflfflfflffl} dynamics of a BEC [24,44]. This suggests that thin film spin current spin relaxation ferromagnets are ripe for the exploration of nonlinear ∂u Δn nj∇nj2 structures observed in BECs, e.g., “Bosenovas” [25,27] in ¼ ∇½ðσ − juj2Þn − ∇ þ ∂t |fflfflfflfflfflfflfflffl{zfflfflfflfflfflfflfflffl} 1 − n2 ð1 − n2Þ2 attractive (σ ¼ −1), and dark solitons [30], vortices [22], and |fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl} velocity flux DSWs [20] in repulsive (σ ¼þ1) BECs. Some of these dispersion structures have been observed in uniaxial (dissipative drop- 1 – −∇h þ α∇ ∇ ½ð1 − n2Þu : ð Þ lets [5 7]) and planar (vortices [8]) thin film ferromagnets. |{z}0 1 − n2 · 3b As we demonstrate, hydrodynamic states are also supported. |fflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl{zfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflfflffl} potential force Consider an ideal planar thin film ferromagnet (σ ¼þ1) viscous loss and a homogeneous field. Equations (3a) admit a static Equation (3a) is reminiscent of spin density continuity (∂Φ=∂t ¼ 0) solution with nonzero fluid velocity, u ¼ uxˆ, [42] from which we identify the spin density flux as the juj < 1, n ¼ 0, and h0 ¼ 0. These are ground states known spin current as spin-density waves (SDWs) [45] or soliton lattices [15] that minimize both exchange and anisotropy energies; i.e., J ¼ −ð1 − n2Þu: ð Þ s 4 any configuration with juj < 1 is stable when m lies purely Vacuum carries zero spin current. However, maximal spin in plane. SDWs exhibit a periodic structure that affords current is reached when n ¼ 0, identified as the saturation them topological stability
Load more

Recommended publications
  • Cen, Julia.Pdf
    City Research Online City, University of London Institutional Repository Citation: Cen, J. (2019). Nonlinear classical and quantum integrable systems with PT -symmetries. (Unpublished Doctoral thesis, City, University of London) This is the accepted version of the paper. This version of the publication may differ from the final published version. Permanent repository link: https://openaccess.city.ac.uk/id/eprint/23891/ Link to published version: Copyright: City Research Online aims to make research outputs of City, University of London available to a wider audience. Copyright and Moral Rights remain with the author(s) and/or copyright holders. URLs from City Research Online may be freely distributed and linked to. Reuse: Copies of full items can be used for personal research or study, educational, or not-for-profit purposes without prior permission or charge. Provided that the authors, title and full bibliographic details are credited, a hyperlink and/or URL is given for the original metadata page and the content is not changed in any way. City Research Online: http://openaccess.city.ac.uk/ [email protected] Nonlinear Classical and Quantum Integrable Systems with PT -symmetries Julia Cen A Thesis Submitted for the Degree of Doctor of Philosophy School of Mathematics, Computer Science and Engineering Department of Mathematics Supervisor : Professor Andreas Fring September 2019 Thesis Commission Internal examiner Dr Olalla Castro-Alvaredo Department of Mathematics, City, University of London, UK External examiner Professor Andrew Hone School of Mathematics, Statistics and Actuarial Science University of Kent, UK Chair Professor Joseph Chuang Department of Mathematics, City, University of London, UK i To my parents.
    [Show full text]
  • Weak Galilean Invariance As a Selection Principle for Coarse
    Weak Galilean invariance as a selection principle for coarse-grained diffusive models Andrea Cairolia,b, Rainer Klagesb, and Adrian Bauleb,1 aDepartment of Bioengineering, Imperial College London, London SW7 2AZ, United Kingdom; and bSchool of Mathematical Sciences, Queen Mary University of London, London E1 4NS, United Kingdom Edited by David A. Weitz, Harvard University, Cambridge, MA, and approved April 16, 2018 (received for review October 2, 2017) How does the mathematical description of a system change in dif- in the long-time limit, hX 2i ∼ t β with β = 1, for anomalous dif- ferent reference frames? Galilei first addressed this fundamental fusion it scales nonlinearly with β 6=1. Anomalous dynamics has question by formulating the famous principle of Galilean invari- been observed experimentally for a wide range of physical pro- ance. It prescribes that the equations of motion of closed systems cesses like particle transport in plasmas, molecular diffusion in remain the same in different inertial frames related by Galilean nanopores, and charge transport in amorphous semiconductors transformations, thus imposing strong constraints on the dynam- (5–7) that was first theoretically described in refs. 8 and 9 based ical rules. However, real world systems are often described by on the continuous-time random walk (CTRW) (10). Likewise, coarse-grained models integrating complex internal and exter- anomalous diffusion was later found for biological motion (11– nal interactions indistinguishably as friction and stochastic forces. 13) and even human movement (14). Recently, it was established Since Galilean invariance is then violated, there is seemingly no as a ubiquitous characteristic of cellular processes on a molec- alternative principle to assess a priori the physical consistency of a ular level (15).
    [Show full text]
  • Newton's Laws
    Newton’s Laws First Law A body moves with constant velocity unless a net force acts on the body. Second Law The rate of change of momentum of a body is equal to the net force applied to the body. Third Law If object A exerts a force on object B, then object B exerts a force on object A. These have equal magnitude but opposite direction. Newton’s second law The second law should be familiar: F = ma where m is the inertial mass (a scalar) and a is the acceleration (a vector). Note that a is the rate of change of velocity, which is in turn the rate of change of displacement. So d d2 a = v = r dt dt2 which, in simplied notation is a = v_ = r¨ The principle of relativity The principle of relativity The laws of nature are identical in all inertial frames of reference An inertial frame of reference is one in which a freely moving body proceeds with uniform velocity. The Galilean transformation - In Newtonian mechanics, the concepts of space and time are completely separable. - Time is considered an absolute quantity which is independent of the frame of reference: t0 = t. - The laws of mechanics are invariant under a transformation of the coordinate system. u y y 0 S S 0 x x0 Consider two inertial reference frames S and S0. The frame S0 moves at a velocity u relative to the frame S along the x axis. The trans- formation of the coordinates of a point is, therefore x0 = x − ut y 0 = y z0 = z The above equations constitute a Galilean transformation u y y 0 S S 0 x x0 These equations are linear (as we would hope), so we can write the same equations for changes in each of the coordinates: ∆x0 = ∆x − u∆t ∆y 0 = ∆y ∆z0 = ∆z u y y 0 S S 0 x x0 For moving particles, we need to know how to transform velocity, v, and acceleration, a, between frames.
    [Show full text]
  • Teaching and Learning Special Relativity Theory in Secondary and Lower Undergraduate Education: a Literature Review
    PHYSICAL REVIEW PHYSICS EDUCATION RESEARCH 17, 023101 (2021) Teaching and learning special relativity theory in secondary and lower undergraduate education: A literature review Paul Alstein ,* Kim Krijtenburg-Lewerissa , and Wouter R. van Joolingen Freudenthal Institute, Utrecht University, P.O. Box 85170, 3508 AD Utrecht, Netherlands (Received 20 November 2020; accepted 7 June 2021; published 12 July 2021) This review presents an overview and analysis of the body of research on special relativity theory (SRT) education at the secondary and lower undergraduate level. There is currently a growing international interest in implementing SRT in pre-university education as an introduction to modern physics. For this reason, insights into learning opportunities and challenges in SRT education are needed. The field of research in SRT education is still at an early stage, especially at the level of secondary education, and there is a shortage of empirical evaluation of learning outcomes. In order to guide future research directions, there is a need for an overview and synthesis of the results reported so far. We have selected 40 articles and categorized them according to reported learning difficulties, teaching approaches, and research tools. Analysis shows that students at all educational levels experience learning difficulties with the use of frames of reference, the postulates of SRT, and relativistic effects. In the reported teaching sequences, instructional materials, and learning activities, these difficulties are approached from different angles. Some teaching approaches focus on thought experiments to express conceptual features of SRT, while others use virtual environments to provide realistic visualization of relativistic effects. From the reported teaching approaches, three learning objectives can be identified: to foster conceptual understanding, to foster understanding of the history and philosophy of science, and to gain motivation and confidence toward SRT and physics in general.
    [Show full text]
  • 1. Special Relativity (SR) — Introduction Lectures • Introduction
    1. Special Relativity (SR) — Introduction Lectures • Introduction, Invariants • Lorentz transformations • Algebra of the Lorentz group Links • Lecture notes by David Hogg: http://cosmo.nyu.edu/hogg/sr/sr.pdf – or: http://web.vu.lt/ff/t.gajdosik/wop/sr.pdf • Tatsu Takeuchi: http://www.phys.vt.edu/~takeuchi/relativity/notes/ • ”Special Relativity for Particle Physics”: http://web.vu.lt/ff/t.gajdosik/wop/sr4wop.pdf Thomas Gajdosik – World of Particles Special Relativity 1 1. Special Relativity (SR) — Introduction History • 1632: Galileo Galilei describes the principle of relativity: – ”Dialogue concerning the Two Chief World Systems” • 1861: Maxwell’s equations • 1887: Michelson-Morley experiment • 1889 / 1892: Lorentz – Fitzgerald transformation • 1905: Albert Einstein publishes the Theory of Special Relativity: – ”On the Electrodynamics of Moving Bodies” • 1908: Hermann Minkovsky introduces 4D space-time Thomas Gajdosik – World of Particles Special Relativity 2 1. Special Relativity (SR) — Introduction Galilean Invariance: Every physical theory should mathematically look the same to every inertial observer • for Galileo it was the mechanics and kinematics: – water dropping down – throwing a ball or a stone – insects flying – jumping around . Thomas Gajdosik – World of Particles Special Relativity 3 1. Special Relativity (SR) — Introduction Galilean Invariance/ Galilean transformations: t ! t0, ~x ! ~x0 Two inertial observers, O and O0, • measure the same absolute time (i.e.: 1 second = 1 second0) – Time translations: t0 = t + τ, ~x0 = ~x
    [Show full text]
  • CHAPTER 2: Special Theory of Relativity
    The Foucault pendulum in Aggieland What does it show?? Seeing is believing T=10 sec how long is it?? https://sibor.physics.tamu.edu/home/courses/physic s-222-modern-physics/ CHAPTER 2 Special Theory of Relativity ◼ 2.1 The Apparent Need for Ether ◼ 2.2 The Michelson-Morley Experiment ◼ 2.3 Einstein’s Postulates ◼ 2.4 The Lorentz Transformation ◼ 2.5 Time Dilation and Length Contraction ◼ 2.6 Addition of Velocities ◼ 2.7 Experimental Verification ◼ 2.8 Twin Paradox It was found that there was no ◼ 2.9 Space-time displacement of the interference ◼ 2.10 Doppler Effect fringes, so that the result of the experiment was negative and would, ◼ 2.11 Relativistic Momentum therefore, show that there is still a ◼ 2.12 Relativistic Energy difficulty in the theory itself… ◼ 2.13 Computations in Modern Physics - Albert Michelson, 1907 ◼ 2.14 Electromagnetism and Relativity Newtonian (Classical) Relativity Assumption ◼ It is assumed that Newton’s laws of motion must be measured with respect to (relative to) some reference frame. Inertial Reference Frame ◼ A reference frame is called an inertial frame if Newton laws are valid in that frame. ◼ Such a frame is established when a body, not subjected to net external forces, is observed to move in rectilinear (along a straight line) motion at constant velocity. Newtonian Principle of Relativity or Galilean Invariance ◼ If Newton’s laws are valid in one reference frame, then they are also valid in another reference frame moving at a uniform velocity relative to the first system. ◼ This is referred to as the Newtonian principle of relativity or Galilean invariance.
    [Show full text]
  • General Relativity
    Institut für Theoretische Physik der Universität Zürich in conjunction with ETH Zürich General Relativity Autumn semester 2016 Prof. Philippe Jetzer Original version by Arnaud Borde Revision: Antoine Klein, Raymond Angélil, Cédric Huwyler Last revision of this version: September 20, 2016 Sources of inspiration for this course include • S. Carroll, Spacetime and Geometry, Pearson, 2003 • S. Weinberg, Gravitation and Cosmology, Wiley, 1972 • N. Straumann, General Relativity with applications to Astrophysics, Springer Verlag, 2004 • C. Misner, K. Thorne and J. Wheeler, Gravitation, Freeman, 1973 • R. Wald, General Relativity, Chicago University Press, 1984 • T. Fliessbach, Allgemeine Relativitätstheorie, Spektrum Verlag, 1995 • B. Schutz, A first course in General Relativity, Cambridge, 1985 • R. Sachs and H. Wu, General Relativity for mathematicians, Springer Verlag, 1977 • J. Hartle, Gravity, An introduction to Einstein’s General Relativity, Addison Wesley, 2002 • H. Stephani, General Relativity, Cambridge University Press, 1990, and • M. Maggiore, Gravitational Waves: Volume 1: Theory and Experiments, Oxford University Press, 2007. • A. Zee, Einstein Gravity in a Nutshell, Princeton University Press, 2013 As well as the lecture notes of • Sean Carroll (http://arxiv.org/abs/gr-qc/9712019), • Matthias Blau (http://www.blau.itp.unibe.ch/lecturesGR.pdf), and • Gian Michele Graf (http://www.itp.phys.ethz.ch/research/mathphys/graf/gr.pdf). 2 CONTENTS Contents I Introduction 5 1 Newton’s theory of gravitation 5 2 Goals of general relativity 6 II Special Relativity 8 3 Lorentz transformations 8 3.1 Galilean invariance . .8 3.2 Lorentz transformations . .9 3.3 Proper time . 11 4 Relativistic mechanics 12 4.1 Equations of motion . 12 4.2 Energy and momentum .
    [Show full text]
  • 1.1. Galilean Relativity
    1.1. Galilean Relativity Galileo Galilei 1564 - 1642 Dialogue Concerning the Two Chief World Systems The fundamental laws of physics are the same in all frames of reference moving with constant velocity with respect to one another. Metaphor of Galileo’s Ship Ship traveling at constant speed on a smooth sea. Any observer doing experiments (playing billiard) under deck would not be able to tell if ship was moving or stationary. Today we can make the same Even better: Earth is orbiting observation on a plane. around sun at v 30 km/s ! ≈ 1.2. Frames of Reference Special Relativity is concerned with events in space and time Events are labeled by a time and a position relative to a particular frame of reference (e.g. the sun, the earth, the cabin under deck of Galileo’s ship) E =(t, x, y, z) Pick spatial coordinate frame (origin, coordinate axes, unit length). In the following, we will always use cartesian coordinate systems Introduce clocks to measure time of an event. Imagine a clock at each position in space, all clocks synchronized, define origin of time Rest frame of an object: frame of reference in which the object is not moving Inertial frame of reference: frame of reference in which an isolated object experiencing no force moves on a straight line at constant velocity 1.3. Galilean Transformation Two reference frames ( S and S ) moving with velocity v to each other. If an event has coordinates ( t, x, y, z ) in S , what are its coordinates ( t ,x ,y ,z ) in S ? in the following, we will always assume the “standard configuration”: Axes of S and S parallel v parallel to x-direction Origins coincide at t = t =0 x vt x t = t Time is absolute Galilean x = x vt Transf.
    [Show full text]
  • Generalized Galilean Transformations of Tensors and Cotensors with Application to General Fluid Motion
    GENERALIZED GALILEAN TRANSFORMATIONS OF TENSORS AND COTENSORS WITH APPLICATION TO GENERAL FLUID MOTION VÁN P.1;2;3, CIANCIO, V,4 AND RESTUCCIA, L.4 Abstract. Galilean transformation properties of different physical quantities are investigated from the point of view of four dimensional Galilean relativistic (non- relativistic) space-time. The objectivity of balance equations of general heat con- ducting fluids and of the related physical quantities is treated as an application. 1. Introduction Inertial reference frames play a fundamental role in non-relativistic physics [1, 2, 3]. One expects that the physical content of spatiotemporal field theories are the same for different inertial observers, and also for some noninertial ones. This has several practical, structural consequences for theory construction and development [4, 5, 6, 7]. The distinguished role of inertial frames can be understood considering that they are true reflections of the mathematical structure of the flat, Galilean relativistic space-time [8, 9, 10]. When a particular form of a physical quantity in a given Galilean inertial reference frame is expressed by the components of that quantity given in an other Galilean inertial reference frame, we have a Galilean transformation. In a four dimensional representation particular components of the physical quantity are called as timelike and spacelike parts, concepts that require further explanations. In non-relativistic physics time passes uniformly in any reference frame, it is ab- solute. The basic formula of Galilean transformation is related to both time and position: t^= t; x^ = x − vt: (1) Here, t is the time, x is the position in an inertial reference frame K, x^ is the position in an other inertial reference frame K^ and v is the relative velocity of K arXiv:1608.05819v1 [physics.class-ph] 20 Aug 2016 and K^ (see Figure 1).
    [Show full text]
  • Relativity Chap 1.Pdf
    Chapter 1 Kinematics, Part 1 Special Relativity, For the Enthusiastic Beginner (Draft version, December 2016) Copyright 2016, David Morin, [email protected] TO THE READER: This book is available as both a paperback and an eBook. I have made the first chapter available on the web, but it is possible (based on past experience) that a pirated version of the complete book will eventually appear on file-sharing sites. In the event that you are reading such a version, I have a request: If you don’t find this book useful (in which case you probably would have returned it, if you had bought it), or if you do find it useful but aren’t able to afford it, then no worries; carry on. However, if you do find it useful and are able to afford the Kindle eBook (priced below $10), then please consider purchasing it (available on Amazon). If you don’t already have the Kindle reading app for your computer, you can download it free from Amazon. I chose to self-publish this book so that I could keep the cost low. The resulting eBook price of around $10, which is very inexpensive for a 250-page physics book, is less than a movie and a bag of popcorn, with the added bonus that the book lasts for more than two hours and has zero calories (if used properly!). – David Morin Special relativity is an extremely counterintuitive subject, and in this chapter we will see how its bizarre features come about. We will build up the theory from scratch, starting with the postulates of relativity, of which there are only two.
    [Show full text]
  • Notes on Special Relativity Honours-Level Module in Applied Mathematics
    School of Mathematics and Statistics Te Kura M¯ataiTatauranga MATH 466/467 Special Relativity Module T1/T2 2020 Math 466/467: Notes on special relativity Honours-level module in Applied Mathematics Matt Visser School of Mathematics and Statistics, Victoria University of Wellington, Wellington, New Zealand. E-mail: [email protected] URL: http://www.victoria.ac.nz/sms/about/staff/matt-visser Draft form: 3 March 2020; LATEX-ed March 3, 2020; c Matt Visser |VUW| Warning: Semi{Private | Not intended for large-scale dissemination. These notes are provided as a reading module for Math 466/467: Honours-level Applied Mathematics. There are still a lot of rough edges. Semi{Private | Not intended for large-scale dissemination. Math 466/467: Special Relativity Module 2 Contents I Notes: The special relativity 5 1 Minkowski spacetime 5 2 The Lorentz and Poincare groups 9 2.1 Full Lorentz group: 10 2.2 Restricted Lorentz group: 14 2.3 Poincare group: 15 2.4 Explicit Lorentz transformations 16 3 Quaternions (an aside) 21 4 Bi-quaternions (an aside) 24 5 Causal structure 25 6 Lorentzian metric 28 7 Inner product 32 8 Index-based methods for SR 33 9 Relativistic combination of velocities 34 10 Relativistic kinematics 34 11 Relativistic dynamics 38 12 Electromagnetic fields and forces 39 12.1 Lorentz transformations for electromagnetic fields 42 12.1.1 Transformation along the x direction 42 12.1.2 Summary: 44 12.1.3 Transformation along a general direction 44 12.2 Some exercises: 47 12.3 Lorentz force law 48 13 Relativistic scalar potential 54 14
    [Show full text]
  • Transformations and Conservation Laws Galilean Transformation We Mainly Use Inertial Frames in Which a Free Body (No Forces Applied) Moves with a Constant Velocity
    Transformations and conservation laws Galilean transformation We mainly use inertial frames in which a free body (no forces applied) moves with a constant velocity. A frame moving with a constant velocity with respect to an inertial frame is inertial, too. Thus there is an infinite number of inertial frames. The equations of motion are invariant with respect to transformations from one inertial frame to another, and the transformed Lagrange function can differ from the initial one only by an irrelevant full derivative. This is the principle of the Galilean invariance , i.e., invariance with resperct to Galilean transfromations , that is valid in the classical mechanics. K‘ V K Frame K‘ moves with a velocity V = const with respect to frame K O‘ v' = -v V, r' = r − Vt O t' = t Transformation of the Lagrange function of a free particle: m m m m L' = v' 2 = (v − V)2 = v2 − mv • V + V 2 2 2 2 2 ¢ ¥ d £ m 2 - Thus the Lagrange equations are the same in both frames ¡ = L + ¤ − mr • V + V t dt 2 (Prove the same for systems with interaction) 1 Irrelevant full derivative The proof of the Galilean invariance on the previous page (Landau and Lifshitz) is not fully satisfactory since the Largange function in the K‘ frame is expressed as the function of the variables in the K frame. The true check of the Galilean invariance should be that of the covariance of the Lagrange equations, that is, ∂L ∂L' d d = 0 = 0 dt ∂v dt ∂v' under the Galilean transformation with the same functional forms of the Lagrange function.
    [Show full text]