Table of Contents

Total Page:16

File Type:pdf, Size:1020Kb

Table of Contents Contents 1 Minkowski Spacetime .......................................... 1 1.1 Introduction ............................................... 1 1.2 The Four Dimensions ....................................... 2 1.2.1 Spacetime as an Affine Space .......................... 2 1.2.2 A Few Notations ..................................... 3 1.2.3 Affine Coordinate System ............................. 4 1.2.4 Constant c .......................................... 4 1.2.5 Newtonian Spacetime ................................ 5 1.3 Metric Tensor .............................................. 6 1.3.1 Scalar Product on Spacetime ........................... 7 1.3.2 Matrix of the Metric Tensor ........................... 9 1.3.3 Orthonormal Bases ................................... 10 1.3.4 Classification of Vectors with Respect to g ............... 11 1.3.5 Norm of a Vector .................................... 11 1.3.6 Spacetime Diagrams ................................. 12 1.4 Null Cone and Time Arrow .................................. 15 1.4.1 Definitions .......................................... 15 1.4.2 Two Useful Lemmas ................................. 15 1.4.3 Classification of Unit Vectors .......................... 16 1.5 Spacetime Orientation....................................... 19 1.6 Vector / Linear Form Duality ................................. 21 1.6.1 Linear Forms and Dual Space .......................... 21 1.6.2 Metric Duality....................................... 22 1.7 Minkowski Spacetime ....................................... 23 1.8 Before Going Further... ...................................... 26 2 Worldlines and Proper Time .................................... 29 2.1 Introduction ............................................... 29 2.2 Worldline of a Particle ...................................... 29 2.3 Proper Time ............................................... 31 2.3.1 Definition .......................................... 31 xvii xviii Contents 2.3.2 Ideal Clock ......................................... 34 2.4 Four-Velocity and Four-Acceleration .......................... 35 2.4.1 Four-Velocity ....................................... 35 2.4.2 Four-Acceleration .................................... 37 2.5 Photons ................................................... 39 2.5.1 Null Geodesics ...................................... 39 2.5.2 Light Cone ......................................... 40 2.6 Langevin’s Traveller and Twin Paradox ........................ 40 2.6.1 Twins’ Worldlines ................................... 41 2.6.2 Proper Time of each Twin ............................. 43 2.6.3 The “Paradox” ...................................... 44 2.6.4 4-Velocity and 4-Acceleration.......................... 46 2.6.5 A Round Trip to the Galactic Centre .................... 50 2.6.6 Experimental Verifications ............................ 53 2.7 Geometrical Properties of a Worldline ......................... 56 2.7.1 Timelike Geodesics .................................. 56 2.7.2 Vector Field along a Worldline ......................... 57 2.7.3 Curvature and Torsions ............................... 58 3 Observers ..................................................... 63 3.1 Introduction ............................................... 63 3.2 Simultaneity and Measure of Time ............................ 64 3.2.1 The Problem ........................................ 64 3.2.2 Einstein-Poincare´ Simultaneity ......................... 65 3.2.3 Local Rest Space .................................... 66 3.2.4 Nonexistence of Absolute Time ........................ 69 3.2.5 Orthogonal Projector onto the Local Rest Space .......... 70 3.2.6 Euclidean Character of the Local Rest Space ............. 73 3.3 Measuring Spatial Distances ................................. 73 3.3.1 Synge Formula ...................................... 74 3.3.2 Born’s Rigidity Criterion .............................. 75 3.4 Local Frame ............................................... 77 3.4.1 Local Frame of an Observer ........................... 77 3.4.2 Coordinates with Respect to an Observer ................ 79 3.4.3 Reference Space of an Observer ........................ 81 3.5 Four-Rotation of a Local Frame............................... 82 3.5.1 Variation of the Local Frame along the Worldline ......... 82 3.5.2 Orthogonal Decomposition of Antisymmetric Bilinear Forms 84 3.5.3 Application to the Variation of the Local Frame ........... 87 3.5.4 Inertial Observers .................................... 90 3.6 Derivative of a Vector Field along a Worldline .................. 91 3.6.1 Absolute Derivative .................................. 91 3.6.2 Derivative with Respect to an Observer .................. 91 3.6.3 Fermi-Walker Derivative .............................. 92 3.7 Locality of an Observer’s Frame .............................. 93 Contents xix 4 Kinematics 1: Motion with Respect to an Observer . 97 4.1 Introduction ............................................... 97 4.2 Lorentz Factor ............................................. 98 4.2.1 Definition .......................................... 98 4.2.2 Expression in Terms of the 4-Velocity and the 4-Acceleration101 4.2.3 Time Dilation ....................................... 103 4.3 Velocity Relative to an Observer .............................. 104 4.3.1 Definition .......................................... 104 4.3.2 4-Velocity and Lorentz Factor in Terms of the Velocity ..... 106 4.3.3 Maximum Relative Velocity ........................... 109 4.3.4 Component Expressions .............................. 110 4.4 Experimental Verifications of Time Dilation .................... 111 4.4.1 Atmospheric Muons .................................. 111 4.4.2 Other Tests ......................................... 113 4.5 Acceleration Relative to an Observer .......................... 113 4.5.1 Definition .......................................... 113 4.5.2 Relation to the Second Derivative of the Position Vector .... 114 4.5.3 Expression of the 4-acceleration ........................ 117 4.6 Photon Motion ............................................. 121 4.6.1 Propagation Direction of a Photon ...................... 121 4.6.2 Velocity of Light ..................................... 122 4.6.3 Experimental Tests of the Invariance of the Velocity of Light 125 5 Kinematics 2: Change of Observer ...............................133 5.1 Introduction ............................................... 133 5.2 Relations between Two Observers ............................. 133 5.2.1 Reciprocity of the Relative Velocity ..................... 134 5.2.2 Length Contraction................................... 136 5.3 Law of Velocity Composition ................................ 139 5.3.1 General Form ....................................... 139 5.3.2 Decomposition in Parallel and Transverse Parts ........... 141 5.3.3 Collinear Velocities .................................. 144 5.3.4 Alternative Formula .................................. 145 5.3.5 Experimental Verification: Fizeau Experiment ............ 146 5.4 Law of Acceleration Composition ............................. 148 5.5 Doppler Effect ............................................. 150 5.5.1 Derivation .......................................... 151 5.5.2 Experimental Verifications ............................ 153 5.6 Aberration ................................................ 154 5.6.1 Theoretical Expression ............................... 155 5.6.2 Distortion of the Celestial Sphere ....................... 158 5.6.3 Experimental Verifications ............................ 158 5.7 Images of Moving Objects ................................... 160 5.7.1 Image and Instantaneous Position....................... 160 5.7.2 Apparent Rotation ................................... 161 xx Contents 5.7.3 Image of a Sphere .................................... 163 5.7.4 Superluminal Motions ................................ 166 6 Lorentz Group .................................................169 6.1 Introduction ............................................... 169 6.2 Lorentz Transformations .................................... 169 6.2.1 Definition and characterization ......................... 169 6.2.2 Lorentz Group....................................... 171 6.2.3 Properties of Lorentz Transformations ................... 172 6.3 Subgroups of O(3,1) ........................................ 174 6.3.1 Proper Lorentz Group SO(3,1) ......................... 174 6.3.2 Orthochronous Lorentz Group ......................... 175 6.3.3 Restricted Lorentz Group ............................. 176 6.3.4 Reduction of the Lorentz Group to SOo(3,1) ............. 176 6.4 Classification of Restricted Lorentz Transformations ............. 178 6.4.1 Invariant Null Direction ............................... 178 6.4.2 Decomposition with Respect to an Invariant Null Direction . 179 6.4.3 Spatial Rotations..................................... 183 6.4.4 Lorentz Boosts ...................................... 185 6.4.5 Null Rotations ....................................... 187 6.4.6 Four-Screws ........................................ 189 6.4.7 Eigenvectors of a Restricted Lorentz Transformation ...... 190 6.4.8 Summary ........................................... 191 6.5 Polar Decomposition ........................................ 193 6.5.1 Statement and Demonstration .......................... 193 6.5.2 Explicit Forms ...................................... 194 6.6 Properties of Lorentz Boosts ................................. 196 6.6.1 Kinematical
Recommended publications
  • Resolution of the Ehrenfest Paradox in the Dynamic Interpretation of Lorentz Invariance F
    Resolution of the Ehrenfest Paradox in the Dynamic Interpretation of Lorentz Invariance F. Winterberg University of Nevada, Reno, Nevada 89557-0058, USA Z. Naturforsch. 53a, 751-754 (1998); received July 14, 1998 In the dynamic Lorentz-Poincare interpretation of Lorentz invariance, clocks in absolute motion through a preferred reference system (resp. aether) suffer a true contraction and clocks, as a result of this contraction, go slower by the same amount. With the one-way velocity of light unobservable, there is no way this older pre-Einstein interpretation of special relativity can be tested, except in cases involv- ing rotational motion, where in the Lorentz-Poincare interpretation the interaction symmetry with the aether is broken. In this communication it is shown that Ehrenfest's paradox, the Lorentz contraction of a rotating disk, has a simple resolution in the dynamic Lorentz-Poincare interpretation of Lorentz invariance and can perhaps be tested against the prediction of special relativity. One of the oldest and least understood paradoxes of contraction. With all clocks understood as light clocks special relativity is the Ehrenfest paradox [ 1 ], the Lorentz made up of Lorentz-contraded rods, clocks in absolute contraction of a rotating disk, whereby the ratio of cir- motion go slower by the same amount. For an observer cumference of the disk to its diameter should become less in absolute motion against the preferred reference than n. The paradox gave Einstein the idea that in accel- system, the contraction and time dilation observed on an erated frames of reference the metric is non-euclidean object at rest in this reference system is there explained and that by reason of his principle of equivalence the as an illusion caused by the Lorentz contraction and time same should be true in the presence of gravitational fields.
    [Show full text]
  • Relativistic Rigid Systems and the Cosmic Expansion
    Noname manuscript No. (will be inserted by the editor) Relativistic rigid systems and the cosmic expansion Luciano Combi* · Gustavo E. Romero Received: date / Accepted: date Abstract We analyze the necessary conditions for a body to remain rigid in an expanding cosmological Universe. First, we establish the main theorems and definitions for having a rigid body in a general spacetime as well as the new concept of quasilocal rigidity. We apply the obtained results to a homogeneous universe exploring the differences with flat spacetime. We discuss how the concept of rigid body helps to understand the expansion of space in cosmology. Finally, using a rigid system as a reference frame, we calculate the gravitational energy, and we compare it with previous results in the literature. Keywords Cosmology · Rigidity · Expansion · Gravitational energy 1 Introduction A rigid body is a physical system that cannot be deformed, i.e. a body in which distances between its parts are constant. In Newtonian physics, rigidity is well- defined and essentially non-local; for instance, if we push a rigid body, each part must move in a way that that distances remain invariant. This implies that the interaction between all parts must be instantaneous. In Relativity, this is prohibited by the causal structure of spacetime, i.e. nothing can move faster than light. In 1909, a few years after Einstein's presentation of Special Relativity, Born proposed the first definition of relativistic rigidity [1]. He showed that L. Combi* Instituto Argentino de Radioastronom´ıa,C.C. No. 5, 1894, Villa Elisa, Argentina Tel.: +54-45-678910 E-mail: [email protected] G.E.
    [Show full text]
  • Quantum Optics and Relativistic Motion with Superconducting Circuits
    THESIS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY Quantum optics and relativistic motion with superconducting circuits Joel Lindkvist Applied Quantum Physics Laboratory Department of Microtechnology and Nanoscience CHALMERS UNIVERSITY OF TECHNOLOGY G¨oteborg, Sweden 2015 Quantum optics and relativistic motion with superconducting circuits JOEL LINDKVIST ISBN 978-91-7597-300-5 c JOEL LINDKVIST, 2015 Doktorsavhandlingar vid Chalmers tekniska h¨ogskola Ny serie nr 3981 ISSN 0346-718X Applied Quantum Physics Laboratory Department of Microtechnology and Nanoscience - MC2 Chalmers University of Technology SE-412 96 G¨oteborg, Sweden Telephone +46 (0)31 772 1000 www.chalmers.se Author email: [email protected] ISSN 1652-0769 Technical Report MC2-323 Printed by Chalmers Reproservice G¨oteborg, Sweden 2015 Quantum optics and relativistic motion with superconducting circuits JOEL LINDKVIST Applied Quantum Physics Laboratory Department of Microtechnology and Nanoscience Chalmers University of Technology Abstract Superconducting microwave circuits provide a versatile platform for study- ing quantum optics with artificial atoms, mainly motivated by applications in quantum information. In addition, the circuits are promising for simu- lation of relativistic phenomena. This thesis is based on theoretical work along both these lines. Firstly, we consider a transmon coupled to an open transmission line. Using circuit quantization techniques and the master equation formalism, we theoretically describe scattering of coherent microwaves states on the transmon. The results agree with various recent experiments. As an exam- ple, we see a photon number redistribution leading to antibunching in the reflected field and superbunching in the transmitted field. Inspired by these results, we further investigate the possibility of generating single-photon states on demand in the system.
    [Show full text]
  • Talking at Cross-Purposes. How Einstein and Logical Empiricists Never Agreed on What They Were Discussing About
    Talking at Cross-Purposes. How Einstein and Logical Empiricists never Agreed on what they were Discussing about Marco Giovanelli Abstract By inserting the dialogue between Einstein, Schlick and Reichenbach in a wider network of debates about the epistemology of geometry, the paper shows, that not only Einstein and Logical Empiricists came to disagree about the role, principled or provisional, played by rods and clocks in General Relativity, but they actually, in their life-long interchange, never clearly identified the problem they were discussing. Einstein’s reflections on geometry can be understood only in the context of his “measuring rod objection” against Weyl. Logical Empiricists, though carefully analyzing the Einstein-Weyl debate, tried on the contrary to interpret Einstein’s epistemology of geometry as a continuation of the Helmholtz-Poincaré debate by other means. The origin of the misunderstanding, it is argued, should be found in the failed appreciation of the difference between a “Helmhotzian” and a “Riemannian” tradition. The epistemological problems raised by General Relativity are extraneous to the first tradition and can only be understood in the context of the latter, whose philosophical significance, however, still needs to be fully explored. Keywords: Logical Empiricism Moritz Schlick, Hans Reichenbach, Albert Einstein, Hermann Weyl, Epistemology of Geometry 1. Introduction on the notion of rigid bodies in Special Relativity (§2.1) and most of all those between Einstein, Herman Weyl Mara Beller in her classical Quantum dialogue (Beller, and Walter Dellänbach (§3) on the role of rigid rods and 1999) famously suggested a “dialogical” approach to the clocks in General Relativity (§2.2) around the 1920s.
    [Show full text]
  • Visualization of Thomas-Wigner Rotations 2
    Visualization of Thomas-Wigner rotations G. Beyerle Caputh, Germany E-mail: [email protected] Abstract. It is well known that a sequence of two non-collinear pure Lorentz transformations (boosts) is not a boost again, but involves a spatial rotation, the Wigner or Thomas-Wigner rotation. The formation of this rotation is visually illustrated by moving a Born-rigid object on a closed trajectory in several sections. Within each section the boost’s proper time duration is assumed to be the same and the object’s centre accelerates uniformly. Born-rigidity implies that the stern of this object accelerates faster than its bow. It is shown that at least five boosts are required to return the object’s centre to its start position. With these assumptions, the Thomas- Wigner rotation angle depends on a single parameter only, the maximum speed reached within each boost section. The visualization highlights the close relationship between the Thomas-Wigner rotation and the relativity of simultaneity. Furthermore, it is illustrated that accelerated motion implies the formation of an event horizon. The event horizons associated with the five boosts constitute a boundary to the rotated Born-rigid object and ensure its finite size. arXiv:1706.02755v1 [physics.class-ph] 6 Jun 2017 Visualization of Thomas-Wigner rotations 2 1. Introduction In 1926 the British physicist Llewellyn Hilleth Thomas (1903–1992) resolved a discrepancy between observed line splittings of atomic spectra in an external magnetic field (Zeeman effect) and theoretical calculations at that time [see e.g. Tomonaga, 1997]. Thomas’ analysis [Thomas, 1926, 1927] explains the observed deviations in terms of a special relativistic effect [Einstein, 1905].
    [Show full text]
  • Simultaneity and Precise Time in Rotation
    universe Article Simultaneity and Precise Time in Rotation Don Koks Defence Science and Technology Group, CEWD 205 Labs, P.O. Box 1500, Edinburgh SA 5111, Australia; [email protected] Received: 4 October 2019; Accepted: 12 November 2019; Published: 16 December 2019 Abstract: I analyse the role of simultaneity in relativistic rotation by building incrementally on its role in simpler scenarios. Historically, rotation has been analysed in 1+1 dimensions; but my stance is that a 2+1-dimensional treatment is necessary. This treatment requires a discussion of what constitutes a frame, how coordinate choices differ from frame choices, and how poor coordinates can be misleading. I determine how precisely we are able to define a meaningful time coordinate on a gravity-free rotating Earth, and discuss complications due to gravity on our real Earth. I end with a critique of several statements made in relativistic precision-timing literature, that I maintain contradict the tenets of relativity. Those statements tend to be made in the context of satellite-based navigation; but they are independent of that technology, and hence are not validated by its success. I suggest that if relativistic precision-timing adheres to such analyses, our civilian timing is likely to suffer in the near future as clocks become ever more precise. Keywords: rotating disk; clock synchronisation; precise timing; Sagnac effect; accelerated frame; circular twin paradox; Selleri’s paradox PACS: 03.30.+p MSC: 83A05 1. Introduction The analysis of relativistic rotation has evolved from a theoretical problem to a practical one in recent years as clock technology has grown ever more precise, and the question of what constitutes “the best time” on a rotating Earth becomes more urgent to resolve.
    [Show full text]
  • Fritz Hasenöhrl and E=Mc2
    Eur. Phys. J. H DOI: 10.1140/epjh/e2012-30061-5 THE EUROPEAN PHYSICAL JOURNAL H Fritz Hasen¨ohrl and E = mc2 Stephen Boughna Haverford College, 19041 Haverford, PA, USA Received 28 November 2012 / Received in final form 17 December 2012 Published online 21 January 2013 c EDP Sciences, Springer-Verlag 2013 Abstract. In 1904, the year before Einstein’s seminal papers on special relativity, Austrian physicist Fritz Hasen¨ohrl examined the properties of blackbody radiation in a moving cavity. He calculated the work nec- essary to keep the cavity moving at a constant velocity as it fills with radiation and concluded that the radiation energy has associated with E 3 mc2 it an apparent mass such that = 8 . In a subsequent paper, also in 1904, Hasen¨ohrl achieved the same result by computing the force necessary to accelerate a cavity already filled with radiation. In early E 3 mc2 1905, he corrected the latter result to = 4 . This result, i.e., m 4 E/c2 = 3 , has led many to conclude that Hasen¨ohrl fell victim to the same “mistake” made by others who derived this relation between the mass and electrostatic energy of the electron. Some have attributed the mistake to the neglect of stress in the blackbody cavity. In this pa- per, Hasen¨ohrl’s papers are examined from a modern, relativistic point of view in an attempt to understand where he went wrong. The primary mistake in his first paper was, ironically, that he didn’t account for the loss of mass of the blackbody end caps as they radiate energy into the cavity.
    [Show full text]
  • A Modern View of the Classical Herglotz-Noether Theorem
    A modern view of the classical Herglotz-Noether theorem Ziyang Hu∗ D.A.M.T.P. University of Cambridge 13th November 2018 Abstract In this paper we give a new proof, valid for all dimensions, of the classical Herglotz- Noether theorem that all rotational shear-free and expansion-free flows (rotational Born- rigid flows) in Minkowski spacetime are generated by Killing vector fields (isometric flows). This is aimed as an illustration of a general framework for working with problems that can be described as a structure-preserving submersion, which we will describe in a subsequent paper. arXiv:1004.1935v3 [math-ph] 24 Aug 2010 ∗[email protected] 1 Contents 1 Introduction 3 1.1 Historyandpreviousresults . .... 3 1.2 Relation to the AdS/CFT correspondence . ..... 6 1.3 Newresultsanddevelopment . 6 2 Riemannian geometry 6 2.1 Coframes ..................................... 6 2.2 Covariantderivatives. ... 9 3 Flow in an orthonormal frame 10 3.1 Rigidflow..................................... 12 3.2 Conditions for isometric rigid flow . ..... 14 3.3 Relationstofluidmechanics . 15 4 Intrinsic geometry and integrability of rigid flow 15 4.1 GaussandCodazziequations . 16 4.2 (Non-)integrability of the base space . ....... 16 4.3 Connection and curvature for the base space . ....... 18 5 Generalisations to the Herglotz-Noether theorem 20 6 Conclusion 21 References 22 2 1 Introduction 1.1 History and previous results Man has studied rigid motion since antiquity. The concept of rigid motion relevant to us, though, begins only within the framework of Newtonian mechanics. Using modern language, the way of defining such a motion is by considering a body B as a Riemannian manifold (possibly with boundary), the ambient space M also as a Riemannian manifold (usually just Euclidean space) and a map i depending on a parameter t “time” taken values in R, for which the map i(t) : B → M (1.1) obtained by fixing the first argument in i : R × B → M is an isometric embedding for all t in a relevant domain.
    [Show full text]
  • Rigid Motion in Special Relativity
    SCIREA Journal of Physics ISSN: 2706-8862 http://www.scirea.org/journal/Physics April 19, 2021 Volume 6, Issue 1, February 2021 Rigid Motion in Special Relativity Stuart Boehmer Wichita, Kansas, United States Email: [email protected]; [email protected] Abstract We solve the problem of rigid motion in special relativity in completeness, forswearing the use of the 4-D geometrical methods usually associated with relativity, for pedagogical reasons. We eventually reduce the problem to a system of coupled linear nonhomogeneous ordinary differential equations. We find that any rotation of the rigid reference frame must be independent of time. We clarify the issues associated with Bell’s notorious rocket paradox and we discuss the problem of hyperbolic motion from multiple viewpoints. We conjecture that any rigid accelerated body must experience regions of shock in which there is a transition to fluid motion, and we discuss the hypothesis that the Schwarzchild surface of a black hole is just such a shock front. Keywords : rigid body; rigid motion; born rigidity; rotation; acceleration; revolution; Ehrenfest’s paradox; Bell’s rocket paradox; relativity; hyperbolic motion; Schwarzchild solution; black holes 1 1. Introduction In 1910, Born [1] posed the problem of finding the most general rigid motion in special relativity. That is, he wanted to find the relativistic analogue of the classical, , (1) where is the translational velocityand istherotational velocity of the moving rigid reference frame and is the local velocity of the moving rigid frame with respect to the “absolute” frame of reference of Newton, and where and are the Cartesian coordinates and time of the absolute frame.
    [Show full text]
  • Inertial System and Special Relativity Finite Geometrical Field
    Inertial System and Special Relativity Finite Geometrical Field Theory of Matter Motion Part One Xiao Jianhua Natural Science Foundation Research Group, Shanghai Jiaotong University Shanghai, P.R.C Abstract: Special relativity theory is well established and confirmed by experiments. This research establishes an operational measurement way to express the great theory in a geometrical form. This may be valuable for understanding the underlying concepts of relativity theory. In four-dimensional spacetime continuum, the displacement field of matter motion is measurable quantities. Based on these measurements, a finite geometrical field can be established. On this sense, the matter motion in physics is viewed as the deformation of spacetime continuum. Suppose the spacetime continuum is isotropic, based on the least action principle, the general motion equations can be established. In this part, Newton motion and special relativity are discussed. Based on the finite geometrical field theory of matter motion, the Newton motion equation and the special relativity can be derived simply based on the isotropy of spacetime continuum and the definition of inertial system. This research shows that the Lorentz transformation is required by both of the inertial system definition and the time gauge invariance for inertial systems. Hence, the special relativity is the logic conclusion of time invariance in inertial system. The source independent of light velocity supports the isotropy of inertial system rather than the concept of proper time, which not only causes many paradox, such as the twin-paradox, but also causes many misunderstanding and controversial arguments. The singularity of Lorentz transformation is removed in other parts of finite geometrical field theory, where the gravity field, electromagnetic field, and quantum field will be discussed with the time displacement field.
    [Show full text]
  • Proper-Time Measurement in Accelerated Relativistic Systems
    Proper-time measurement in accelerated relativistic systems Uri Ben-Ya'acov School of Engineering, Kinneret Academic College on the Sea of Galilee, D.N. Emek Ha'Yarden 15132, Israel E-mail: [email protected] Abstract. Separate constituents of extended systems measure proper-times on different world-lines. Relating and comparing proper-time measurements along any two such world-lines requires that common simultaneity be possible, which in turn implies that the system is linearly-rigidly moving so that momentary rest frames are identifiable at any stage of the system's journey in space-time. Once momentary rest-frames have been identified, clocks moving on separate world- lines are synchronizable by light-signal communication. The synchronization relations for two clocks are explicitly computed using light-signals exchanged between them. Implications for the clock hypothesis are included. Also, since simultaneity is frame- dependent, incorrect usage of it leads to pseudo-paradoxes. Counter-examples are discussed. Keywords : proper-time; extended relativistic systems; relativistic rigid motion; rapidity; clock hypothesis; relativistic age. 1. Introduction In classical Newtonian mechanics any set of particles may be grouped to form a \system". arXiv:1907.05975v1 [physics.class-ph] 12 Jul 2019 Time is absolute, independent of the referenc-frame, therefore common to all the chosen constituents, and a centre-of-mass (CM) may be unambiguously defined. Relativity theory is closer to reality than Newtonian mechanics, telling us that time measurement is reference-frame-dependent. Then, except for the trivial case of a system whose constituents all move inertially with the same velocity, there is no common time for the system as a whole.
    [Show full text]
  • Expanding Space, Redshifts, and Rigidity Arxiv:1911.05415V1 [Gr-Qc
    Expanding Space, Redshifts, and Rigidity Conceptual issues in cosmology Colin MacLaurin BMath (Hons I), Grad Dip Theol Under the supervision of Prof. Tamara Davis arXiv:1911.05415v1 [gr-qc] 13 Nov 2019 A thesis submitted to the University of Queensland in partial fulfilment of the degree of Master of Science Faculty of Science School of Mathematics and Physics June 2015 Abstract I examine the interpretation of photon redshifts in curved spacetime, as being gravita- tional or Doppler in origin. In Friedmann-Lema^ıtre-Robertson-Walker spacetime, red- shifts between comoving observers are often attributed to \expanding space", whereas in Schwarzschild spacetime, redshifts between static observers are attributed to \grav- itational" causes. Yet various authors have suggested a freely falling observer con- gruence would interpret any redshift as Doppler, whereas a rigid congruence must interpret it as gravitational since there is no relative motion. I realise this proposal by explicitly constructing coordinate systems for rigid motion in the above spacetimes. This includes an extensive analysis of observer-dependent distance measurement in curved spacetime. I also introduce Rindler acceleration, the Milne model, and New- tonian cosmology. Note: This version is from 2015, updated two weeks after formally submitting the thesis. It has been available on my personal website since January 2017. The above abstract is new, along with cosmetic improvements to the references. | CM, 13th Nov. 20191 Disclaimer The work presented in this thesis is, to the best of my knowledge and belief original, except as acknowledged in the text, and has not been submitted either in whole or in part, for a degree at this or any other university.
    [Show full text]