Criticism to the Twin's Paradox
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Theoretical Physics
IC/80/166 INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS AW EFFICIENT KORRINGA-KOHN-ROSTOKER METHOD FOR "COMPLEX" LATTICES M. Yussouff and INTERNATIONAL ATOMIC ENERGY R. Zeller AGENCY UNITED NATIONS EDUCATIONAL SCIENTIFIC AND CULTURAL ORGANIZATION 19R0 MIRAMARE-TRIESTE IC/90/166 The well known rapid convergence and precision of the KKR- Green's function method (Korringa 1947, Kohn and Rostocker 1954) International Atomic Energy Agency have made it useful for the calculation of the electronic struc- and United Rations Educational Scientific and Cultural Organization ture of perfect as well as disordered solids (Ham and Segall 1961, IHTEBSATIOHAL CENTRE FOR THEORETICAL PHYSICS Ehrenrelch and Schwartz 1976). Although extensive calculations of this kind exist for cubic crystals (Moruzzi, Janak and Williams 1978), there are so far very few calculations for the equally important class of hexagonal close packed solids. This is due to the computational efforts involved in evaluating the KKR matrix AH EFFICIENT KORRIHGA-KOHH-ROSTOKER METHOD FOR "COMPLEX" LATTICES • elements ATT,{k,E) using the conventional KKR for 'complex' lattices, i.e. crystals with several atoms per unit cell- Some simplifications can be achieved (Bhokare and Yussouff 1972, 1974) for k" vectors International Centre for Theoretical Physics, Trieste, Italy, in symmetry directions but the renewed interest in simplifying the and computations (Segall and Yang 19 80) has arisen in connection with self-consistent calcualtions. Here we describe an efficient modi- R. Zeller Institut fur FeBtkorperforschung der Kernforschungsanlage, fication of the KKR method which is particularly useful for 'complex1 D-5170 Jiilieh, Federal Republic of Germany. lattices. ABSTRACT In our approach, the transformed KKR matrix elements are calcu- We present a modification of the exact KKR-band structure method lated directly using reciprocal space summation. -
The Special Theory of Relativity Lecture 16
The Special Theory of Relativity Lecture 16 E = mc2 Albert Einstein Einstein’s Relativity • Galilean-Newtonian Relativity • The Ultimate Speed - The Speed of Light • Postulates of the Special Theory of Relativity • Simultaneity • Time Dilation and the Twin Paradox • Length Contraction • Train in the Tunnel paradox (or plane in the barn) • Relativistic Doppler Effect • Four-Dimensional Space-Time • Relativistic Momentum and Mass • E = mc2; Mass and Energy • Relativistic Addition of Velocities Recommended Reading: Conceptual Physics by Paul Hewitt A Brief History of Time by Steven Hawking Galilean-Newtonian Relativity The Relativity principle: The basic laws of physics are the same in all inertial reference frames. What’s a reference frame? What does “inertial” mean? Etc…….. Think of ways to tell if you are in Motion. -And hence understand what Einstein meant By inertial and non inertial reference frames How does it differ if you’re in a car or plane at different points in the journey • Accelerating ? • Slowing down ? • Going around a curve ? • Moving at a constant velocity ? Why? ConcepTest 26.1 Playing Ball on the Train You and your friend are playing catch 1) 3 mph eastward in a train moving at 60 mph in an eastward direction. Your friend is at 2) 3 mph westward the front of the car and throws you 3) 57 mph eastward the ball at 3 mph (according to him). 4) 57 mph westward What velocity does the ball have 5) 60 mph eastward when you catch it, according to you? ConcepTest 26.1 Playing Ball on the Train You and your friend are playing catch 1) 3 mph eastward in a train moving at 60 mph in an eastward direction. -
Einstein's Mistakes
Einstein’s Mistakes Einstein was the greatest genius of the Twentieth Century, but his discoveries were blighted with mistakes. The Human Failing of Genius. 1 PART 1 An evaluation of the man Here, Einstein grows up, his thinking evolves, and many quotations from him are listed. Albert Einstein (1879-1955) Einstein at 14 Einstein at 26 Einstein at 42 3 Albert Einstein (1879-1955) Einstein at age 61 (1940) 4 Albert Einstein (1879-1955) Born in Ulm, Swabian region of Southern Germany. From a Jewish merchant family. Had a sister Maja. Family rejected Jewish customs. Did not inherit any mathematical talent. Inherited stubbornness, Inherited a roguish sense of humor, An inclination to mysticism, And a habit of grüblen or protracted, agonizing “brooding” over whatever was on its mind. Leading to the thought experiment. 5 Portrait in 1947 – age 68, and his habit of agonizing brooding over whatever was on its mind. He was in Princeton, NJ, USA. 6 Einstein the mystic •“Everyone who is seriously involved in pursuit of science becomes convinced that a spirit is manifest in the laws of the universe, one that is vastly superior to that of man..” •“When I assess a theory, I ask myself, if I was God, would I have arranged the universe that way?” •His roguish sense of humor was always there. •When asked what will be his reactions to observational evidence against the bending of light predicted by his general theory of relativity, he said: •”Then I would feel sorry for the Good Lord. The theory is correct anyway.” 7 Einstein: Mathematics •More quotations from Einstein: •“How it is possible that mathematics, a product of human thought that is independent of experience, fits so excellently the objects of physical reality?” •Questions asked by many people and Einstein: •“Is God a mathematician?” •His conclusion: •“ The Lord is cunning, but not malicious.” 8 Einstein the Stubborn Mystic “What interests me is whether God had any choice in the creation of the world” Some broadcasters expunged the comment from the soundtrack because they thought it was blasphemous. -
|||GET||| Can the Laws of Physics Be Unified? 1St Edition
CAN THE LAWS OF PHYSICS BE UNIFIED? 1ST EDITION DOWNLOAD FREE Paul Langacker | 9781400885503 | | | | | Can the Laws of Physics be Unified? Answer Key. In American physicist Sheldon Glashow proposed that the weak nuclear forceelectricity and magnetism could arise Can the Laws of Physics Be Unified? 1st edition a partially unified electroweak theory. Law II: The alteration of motion is ever proportional to the motive force impress'd; and is made in the direction of the right line in which that force is impress'd. In the s Mendel Sachs proposed a generally covariant field theory that did not require recourse to renormalisation or perturbation theory. Discoveries are made; models, theories, and laws are formulated; and the beauty of the physical universe is made more sublime for the insights gained. Download as PDF Printable version. Lots of equations, but not much detail explaining exactly what they mean, for that some background is needed. I find that literally inconceivable. These laws are Can the Laws of Physics Be Unified? 1st edition systematically to topics such as phase equilibria, chemical reactions, external forces, fluid-fluid surfaces and interfaces, and anisotropic crystal-fluid interfaces. Cohen and A. The physical universe is enormously complex in its detail. One of her daughters also won a Nobel Prize. Archived from the original PDF on 31 March Thank you for posting a review! And, whereas a law is a postulate that forms the foundation of the scientific method, a theory is the end result of that process. I know of none whatsoever. Paul Langacker is senior scientist at Princeton University, visitor at the Institute for Advanced Study in Princeton, and professor emeritus of physics at the University of Pennsylvania. -
Physics 200 Problem Set 7 Solution Quick Overview: Although Relativity Can Be a Little Bewildering, This Problem Set Uses Just A
Physics 200 Problem Set 7 Solution Quick overview: Although relativity can be a little bewildering, this problem set uses just a few ideas over and over again, namely 1. Coordinates (x; t) in one frame are related to coordinates (x0; t0) in another frame by the Lorentz transformation formulas. 2. Similarly, space and time intervals (¢x; ¢t) in one frame are related to inter- vals (¢x0; ¢t0) in another frame by the same Lorentz transformation formu- las. Note that time dilation and length contraction are just special cases: it is time-dilation if ¢x = 0 and length contraction if ¢t = 0. 3. The spacetime interval (¢s)2 = (c¢t)2 ¡ (¢x)2 between two events is the same in every frame. 4. Energy and momentum are always conserved, and we can make e±cient use of this fact by writing them together in an energy-momentum vector P = (E=c; p) with the property P 2 = m2c2. In particular, if the mass is zero then P 2 = 0. 1. The earth and sun are 8.3 light-minutes apart. Ignore their relative motion for this problem and assume they live in a single inertial frame, the Earth-Sun frame. Events A and B occur at t = 0 on the earth and at 2 minutes on the sun respectively. Find the time di®erence between the events according to an observer moving at u = 0:8c from Earth to Sun. Repeat if observer is moving in the opposite direction at u = 0:8c. Answer: According to the formula for a Lorentz transformation, ³ u ´ 1 ¢tobserver = γ ¢tEarth-Sun ¡ ¢xEarth-Sun ; γ = p : c2 1 ¡ (u=c)2 Plugging in the numbers gives (notice that the c implicit in \light-minute" cancels the extra factor of c, which is why it's nice to measure distances in terms of the speed of light) 2 min ¡ 0:8(8:3 min) ¢tobserver = p = ¡7:7 min; 1 ¡ 0:82 which means that according to the observer, event B happened before event A! If we reverse the sign of u then 2 min + 0:8(8:3 min) ¢tobserver 2 = p = 14 min: 1 ¡ 0:82 2. -
On Radar Time and the Twin ''Paradox''
On radar time and the twin ‘‘paradox’’ Carl E. Dolbya) and Stephen F. Gullb) Astrophysics Group, Cavendish Laboratory, Madingley Road, Cambridge CB3 0HE, United Kingdom ͑Received 23 April 2001; accepted 13 June 2001͒ In this paper we apply the concept of radar time ͑popularized by Bondi in his work on k calculus͒ to the well-known relativistic twin ‘‘paradox.’’ Radar time is used to define hypersurfaces of simultaneity for a class of traveling twins, from the ‘‘immediate turn-around’’ case, through the ‘‘gradual turn-around’’ case, to the ‘‘uniformly accelerating’’ case. We show that this definition of simultaneity is independent of choice of coordinates, and assigns a unique time to any event ͑with which the traveling twin can send and receive signals͒, resolving some common misconceptions. © 2001 American Association of Physics Teachers. ͓DOI: 10.1119/1.1407254͔ INTRODUCTION time’’ ͑and related ‘‘radar distance’’͒ and emphasize that this definition applies not just to inertial observers, but to any It might seem reasonable to suppose that the twin paradox observer in any space–time. We then use radar time to derive has long been understood, and that no confusion remains the hypersurfaces of simultaneity for a class of traveling about it. Certainly there is no disagreement about the relative twins, from the ‘‘immediate turn-around’’ case, through the aging of the two twins, so there is no ‘‘paradox.’’ There is ‘‘gradual turn-around’’ case, to the ‘‘uniformly accelerating’’ also no confusion over ‘‘when events are seen’’ by the two case. -
Quantum Mechanics from General Relativity : Particle Probability from Interaction Weighting
Annales de la Fondation Louis de Broglie, Volume 24, 1999 25 Quantum Mechanics From General Relativity : Particle Probability from Interaction Weighting Mendel Sachs Department of Physics State University of New York at Bualo ABSTRACT. Discussion is given to the conceptual and mathemat- ical change from the probability calculus of quantum mechanics to a weighting formalism, when the paradigm change takes place from linear quantum mechanics to the nonlinear, holistic eld theory that accompanies general relativity, as a fundamental theory of matter. This is a change from a nondeterministic, linear theory of an open system of ‘particles’ to a deterministic, nonlinear, holistic eld the- ory of the matter of a closed system. RESUM E. On discute le changement conceptuel et mathematique qui fait passer du calcul des probabilites de la mecanique quantique a un formalisme de ponderation, quand on eectue le changement de paradigme substituantalam ecanique quantique lineairelatheorie de champ holistique non lineaire qui est associee alatheorie de la relativitegenerale, prise comme theorie fondamentale de la matiere. Ce changement mene d’une theorie non deterministe et lineaire decrivant un systeme ouvert de ‘particules’ a une theorie de champ holistique, deterministe et non lineaire, de la matiere constituant un systeme ferme. 1. Introduction. In my view, one of the three most important experimental discov- eries of 20th century physics was the wave nature of matter. [The other two were 1) blackbody radiation and 2) the bending of a beam of s- tarlight as it propagates past the vicinity of the sun]. The wave nature of matter was predicted in the pioneering theoretical studies of L. -
Relativity Contents.Pdf
Contents 1 Kinematics, Part 1 1 1.1 Motivation . 2 1.1.1 Galilean transformations, Maxwell’s equations . 2 1.1.2 Michelson–Morley experiment . 5 1.2 The postulates . 10 1.3 The fundamental effects . 12 1.3.1 Loss of simultaneity . 12 1.3.2 Time dilation . 17 1.3.3 Length contraction . 23 1.3.4 A few other important topics . 28 1.4 Four instructive examples . 31 1.5 Velocity addition . 35 1.6 Summary . 43 1.7 Problems . 44 1.8 Exercises . 49 1.9 Solutions . 54 2 Kinematics, Part 2 71 2.1 Lorentz transformations . 71 2.1.1 First derivation . 72 2.1.2 Second derivation . 75 2.1.3 The fundamental effects . 78 2.2 Velocity addition . 79 2.2.1 Longitudinal velocity addition . 79 2.2.2 Transverse velocity addition . 80 2.3 The invariant interval . 82 2.4 Minkowski diagrams . 87 2.5 The Doppler effect . 92 2.5.1 Longitudinal Doppler effect . 92 2.5.2 Transverse Doppler effect . 94 2.6 Rapidity . 96 2.6.1 Definition . 96 2.6.2 Physical meaning . 98 2.7 Relativity without c ............................ 99 2.8 Summary . 102 2.9 Problems . 103 2.10 Exercises . 106 2.11 Solutions . 110 iii iv Contents 3 Dynamics 123 3.1 Energy and momentum . 123 3.1.1 Momentum . 124 3.1.2 Energy . 125 3.2 Transformations of E and p . 131 3.3 Collisions and decays . 134 3.4 Particle-physics units . 139 3.5 Force . 140 3.5.1 Force in one dimension . -
Fundamental Nature of the Fine-Structure Constant Michael Sherbon
Fundamental Nature of the Fine-Structure Constant Michael Sherbon To cite this version: Michael Sherbon. Fundamental Nature of the Fine-Structure Constant. International Journal of Physical Research , Science Publishing Corporation 2014, 2 (1), pp.1-9. 10.14419/ijpr.v2i1.1817. hal-01304522 HAL Id: hal-01304522 https://hal.archives-ouvertes.fr/hal-01304522 Submitted on 19 Apr 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution| 4.0 International License Fundamental Nature of the Fine-Structure Constant Michael A. Sherbon Case Western Reserve University Alumnus E-mail: michael:sherbon@case:edu January 17, 2014 Abstract Arnold Sommerfeld introduced the fine-structure constant that determines the strength of the electromagnetic interaction. Following Sommerfeld, Wolfgang Pauli left several clues to calculating the fine-structure constant with his research on Johannes Kepler’s view of nature and Pythagorean geometry. The Laplace limit of Kepler’s equation in classical mechanics, the Bohr-Sommerfeld model of the hydrogen atom and Julian Schwinger’s research enable a calculation of the electron magnetic moment anomaly. Considerations of fundamental lengths such as the charge radius of the proton and mass ratios suggest some further foundational interpretations of quantum electrodynamics. -
A Tale of Two Twins
A tale of two twins L.Benguigui Physics Department and Solid State Institute Technion-Israel Institute of Technology 32000 Haifa Israel Abstract The thought experiment (called the clock paradox or the twin paradox) proposed by Langevin in 1911 of two observers, one staying on earth and the other making a trip toward a Star with a velocity near the light velocity is very well known for its very surprising result. When the traveler comes back, he is younger than the stay on Earth. This astonishing situation deduced form the theory of Special Relativity sparked a huge amount of articles, discussions and controversies such that it remains a particular phenomenon probably unique in Physics. In this article we propose to study it. First, we lookedl for the simplest solutions when one can observe that the published solutions correspond in fact to two different versions of the experiment. It appears that the complete and simple solution of Møller is neglected for complicated methods with dubious validity. We propose to interpret this avalanche of works by the difficulty to accept the conclusions of the Special Relativity, in particular the difference in the times indicated by two clocks, one immobile and the second moving and finally stopping. We suggest also that the name "twin paradox" is maybe related to some subconscious idea concerning conflict between twins as it can be found in the Bible and in several mythologies. 1 Introduction The thought experiment in the theory of Relativity called the "twin paradox" or the "clock paradox" is very well known in physics and even by non-physicists. -
A Short and Transparent Derivation of the Lorentz-Einstein Transformations
A brief and transparent derivation of the Lorentz-Einstein transformations via thought experiments Bernhard Rothenstein1), Stefan Popescu 2) and George J. Spix 3) 1) Politehnica University of Timisoara, Physics Department, Timisoara, Romania 2) Siemens AG, Erlangen, Germany 3) BSEE Illinois Institute of Technology, USA Abstract. Starting with a thought experiment proposed by Kard10, which derives the formula that accounts for the relativistic effect of length contraction, we present a “two line” transparent derivation of the Lorentz-Einstein transformations for the space-time coordinates of the same event. Our derivation make uses of Einstein’s clock synchronization procedure. 1. Introduction Authors make a merit of the fact that they derive the basic formulas of special relativity without using the Lorentz-Einstein transformations (LET). Thought experiments play an important part in their derivations. Some of these approaches are devoted to the derivation of a given formula whereas others present a chain of derivations for the formulas of relativistic kinematics in a given succession. Two anthological papers1,2 present a “two line” derivation of the formula that accounts for the time dilation using as relativistic ingredients the invariant and finite light speed in free space c and the invariance of distances measured perpendicular to the direction of relative motion of the inertial reference frame from where the same “light clock” is observed. Many textbooks present a more elaborated derivation of the time dilation formula using a light clock that consists of two parallel mirrors located at a given distance apart from each other and a light signal that bounces between when observing it from two inertial reference frames in relative motion.3,4 The derivation of the time dilation formula is intimately related to the formula that accounts for the length contraction derived also without using the LET. -
Time Dilation and Length Contraction Shown in Three-Dimensional Space-Time Frames
TIME DILATION AND LENGTH CONTRACTION SHOWN IN THREE-DIMENSIONAL SPACE-TIME FRAMES Tower Chen Division of Mathematical Sciences University of Guam e-mail:[email protected] Zeon Chen e-mail: zeon [email protected] (Received 9 December 2008; accepted 18 February 2009) Abstract In classical Newtonian physics, space and time are abso- lute quantities. Hence, space and time can be treated inde- pendently and discussed separately. With his theory of rel- ativity, Einstein proved that space and time are dependent and must not be treated separately. To maintain this in- terdependency and inseparability of space and time, a three- Concepts of Physics, Vol. VI, No. 2 (2009) 221 dimensional space-time frame, where time is embedded into a spatial coordinate system, has been conceptualized. Utiliz- ing this new type of frame, the concepts of time dilation and length contraction can easily be visualized with intuitive, ge- ometric graphs. The proposed three-dimensional space-time frame is an alternate mathematical frame that can be used to describe the motion of objects. It may also prove to be a use- ful tool in facilitating the understanding of Special Relativity and providing additional insights into space and time. 222 Concepts of Physics, Vol. VI, No. 2 (2009) TIME DILATION AND LENGTH CONTRACTION... 1 Introduction In classical Newtonian physics, the concepts of space and time are absolute. Space is composed of three orthogonal dimensions, and time is represented as a fourth dimension, perpendicular to each of the spatial axes. Both space and time are free to be discussed in- dependent of the other.