Hilbert's Final Form of the Field Equations for General Relativity?
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												  Abraham-Solution to Schwarzschild Metric Implies That CERN Miniblack Holes Pose a Planetary RiskAbraham-Solution to Schwarzschild Metric Implies That CERN Miniblack Holes Pose a Planetary Risk O.E. Rössler Division of Theoretical Chemistry, University of Tübingen, 72076 F.R.G. Abstract A recent mathematical re-interpretation of the Schwarzschild solution to the Einstein equations implies global constancy of the speed of light c in fulfilment of a 1912 proposal of Max Abraham. As a consequence, the horizon lies at the end of an infinitely long funnel in spacetime. Hence black holes lack evaporation and charge. Both features affect the behavior of miniblack holes as are expected to be produced soon at the Large Hadron Collider at CERN. The implied nonlinearity enables the “quasar-scaling conjecture.“ The latter implies that an earthbound minihole turns into a planet-eating attractor much earlier than previously calculated – not after millions of years of linear growth but after months of nonlinear growth. A way to turn the almost disaster into a planetary bonus is suggested. (September 27, 2007) “Mont blanc and black holes: a winter fairy-tale.“ What is being referred to is the greatest and most expensive and potentially most important experiment of history: to create miniblack holes [1]. The hoped-for miniholes are only 10–32 cm large – as small compared to an atom (10–8 cm) as the latter is to the whole solar system (1016 cm) – and are expected to “evaporate“ within less than a picosecond while leaving behind a much hoped-for “signature“ of secondary particles [1]. The first (and then one per second and a million per year) miniblack hole is expected to be produced in 2008 at the Large Hadron Collider of CERN near Geneva on the lake not far from the white mountain.
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												  Einstein, Nordström and the Early Demise of Scalar, Lorentz Covariant Theories of GravitationJOHN D. NORTON EINSTEIN, NORDSTRÖM AND THE EARLY DEMISE OF SCALAR, LORENTZ COVARIANT THEORIES OF GRAVITATION 1. INTRODUCTION The advent of the special theory of relativity in 1905 brought many problems for the physics community. One, it seemed, would not be a great source of trouble. It was the problem of reconciling Newtonian gravitation theory with the new theory of space and time. Indeed it seemed that Newtonian theory could be rendered compatible with special relativity by any number of small modifications, each of which would be unlikely to lead to any significant deviations from the empirically testable conse- quences of Newtonian theory.1 Einstein’s response to this problem is now legend. He decided almost immediately to abandon the search for a Lorentz covariant gravitation theory, for he had failed to construct such a theory that was compatible with the equality of inertial and gravitational mass. Positing what he later called the principle of equivalence, he decided that gravitation theory held the key to repairing what he perceived as the defect of the special theory of relativity—its relativity principle failed to apply to accelerated motion. He advanced a novel gravitation theory in which the gravitational potential was the now variable speed of light and in which special relativity held only as a limiting case. It is almost impossible for modern readers to view this story with their vision unclouded by the knowledge that Einstein’s fantastic 1907 speculations would lead to his greatest scientific success, the general theory of relativity. Yet, as we shall see, in 1 In the historical period under consideration, there was no single label for a gravitation theory compat- ible with special relativity.
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												  Equivalence Principle (WEP) of General Relativity Using a New Quantum Gravity Theory Proposed by the Authors Called Electro-Magnetic Quantum Gravity Or EMQG (RefWHAT ARE THE HIDDEN QUANTUM PROCESSES IN EINSTEIN’S WEAK PRINCIPLE OF EQUIVALENCE? Tom Ostoma and Mike Trushyk 48 O’HARA PLACE, Brampton, Ontario, L6Y 3R8 [email protected] Monday April 12, 2000 ACKNOWLEDGMENTS We wish to thank R. Mongrain (P.Eng) for our lengthy conversations on the nature of space, time, light, matter, and CA theory. ABSTRACT We provide a quantum derivation of Einstein’s Weak Equivalence Principle (WEP) of general relativity using a new quantum gravity theory proposed by the authors called Electro-Magnetic Quantum Gravity or EMQG (ref. 1). EMQG is manifestly compatible with Cellular Automata (CA) theory (ref. 2 and 4), and is also based on a new theory of inertia (ref. 5) proposed by R. Haisch, A. Rueda, and H. Puthoff (which we modified and called Quantum Inertia, QI). QI states that classical Newtonian Inertia is a property of matter due to the strictly local electrical force interactions contributed by each of the (electrically charged) elementary particles of the mass with the surrounding (electrically charged) virtual particles (virtual masseons) of the quantum vacuum. The sum of all the tiny electrical forces (photon exchanges with the vacuum particles) originating in each charged elementary particle of the accelerated mass is the source of the total inertial force of a mass which opposes accelerated motion in Newton’s law ‘F = MA’. The well known paradoxes that arise from considerations of accelerated motion (Mach’s principle) are resolved, and Newton’s laws of motion are now understood at the deeper quantum level. We found that gravity also involves the same ‘inertial’ electromagnetic force component that exists in inertial mass.
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												  Max Abraham's and Tullio Levi-Civita's Approach to EinsteinAlma Mater Studiorum Universita` di · Bologna DOTTORATO DI RICERCA IN Matematica Ciclo XXV Settore concorsuale di afferenza: 01/A4 Settore Scientifico disciplinare: MAT/07 Max Abraham’s and Tullio Levi-Civita’s approach to Einstein Theory of Relativity Presentata da: Michele Mattia Valentini Coordinatore Dottorato: Relatore: Chiar.ma Prof.ssa Chiar.mo Prof. Giovanna Citti Sandro Graffi Esame finale anno 2014 Introduction This thesis deals with the theory of relativity and its diffusion in Italy in the first decades of the XX century. Albert Einstein’s theory of Special and General relativity is deeply linked with Italy and Italian scientists. Not many scientists really involved themselves in that theory understanding, but two of them, Max Abraham and Tullio Levi-Civita left a deep mark in the theory development. Max Abraham engaged a real battle against Ein- stein between 1912 and 1914 about electromagnetic theories and gravitation theories, while Levi-Civita played a fundamental role in giving Einstein the correct mathematical instruments for the general relativity formulation since 1915. Many studies have already been done to explain their role in the develop- ment of Einstein theory from both a historical and a scientific point of view. This work, which doesn’t have the aim of a mere historical chronicle of the events, wants to highlight two particular perspectives. 1. Abraham’s objections against Einstein focused on three important con- ceptual kernels of theory of relativity: the constancy of light speed, the relativity principle and the equivalence hypothesis. Einstein was forced by Abraham to explain scientific and epistemological reasons of the formulation of his theory.
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												  Ether and Electrons in Relativity Theory (1900-1911) Scott WalterEther and electrons in relativity theory (1900-1911) Scott Walter To cite this version: Scott Walter. Ether and electrons in relativity theory (1900-1911). Jaume Navarro. Ether and Moder- nity: The Recalcitrance of an Epistemic Object in the Early Twentieth Century, Oxford University Press, 2018, 9780198797258. hal-01879022 HAL Id: hal-01879022 https://hal.archives-ouvertes.fr/hal-01879022 Submitted on 21 Sep 2018 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. Ether and electrons in relativity theory (1900–1911) Scott A. Walter∗ To appear in J. Navarro, ed, Ether and Modernity, 67–87. Oxford: Oxford University Press, 2018 Abstract This chapter discusses the roles of ether and electrons in relativity the- ory. One of the most radical moves made by Albert Einstein was to dismiss the ether from electrodynamics. His fellow physicists felt challenged by Einstein’s view, and they came up with a variety of responses, ranging from enthusiastic approval, to dismissive rejection. Among the naysayers were the electron theorists, who were unanimous in their affirmation of the ether, even if they agreed with other aspects of Einstein’s theory of relativity. The eventual success of the latter theory (circa 1911) owed much to Hermann Minkowski’s idea of four-dimensional spacetime, which was portrayed as a conceptual substitute of sorts for the ether.
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												  PPN FormalismPPN formalism Hajime SOTANI 01/07/2009 21/06/2013 (minor changes) University of T¨ubingen PPN formalism Hajime Sotani Introduction Up to now, there exists no experiment purporting inconsistency of Einstein's theory. General relativity is definitely a beautiful theory of gravitation. However, we may have alternative approaches to explain all gravitational phenomena. We have also faced on some fundamental unknowns in the Universe, such as dark energy and dark matter, which might be solved by new theory of gravitation. The candidates as an alternative gravitational theory should satisfy at least three criteria for viability; (1) self-consistency, (2) completeness, and (3) agreement with past experiments. University of T¨ubingen 1 PPN formalism Hajime Sotani Metric Theory In only one significant way do metric theories of gravity differ from each other: ! their laws for the generation of the metric. - In GR, the metric is generated directly by the stress-energy of matter and of nongravitational fields. - In Dicke-Brans-Jordan theory, matter and nongravitational fields generate a scalar field '; then ' acts together with the matter and other fields to generate the metric, while \long-range field” ' CANNOT act back directly on matter. (1) Despite the possible existence of long-range gravitational fields in addition to the metric in various metric theories of gravity, the postulates of those theories demand that matter and non-gravitational fields be completely oblivious to them. (2) The only gravitational field that enters the equations of motion is the metric. Thus the metric and equations of motion for matter become the primary entities for calculating observable effects.
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												  The Confrontation Between General Relativity and ExperimentThe Confrontation between General Relativity and Experiment Clifford M. Will Department of Physics University of Florida Gainesville FL 32611, U.S.A. email: [email protected]fl.edu http://www.phys.ufl.edu/~cmw/ Abstract The status of experimental tests of general relativity and of theoretical frameworks for analyzing them are reviewed and updated. Einstein’s equivalence principle (EEP) is well supported by experiments such as the E¨otv¨os experiment, tests of local Lorentz invariance and clock experiments. Ongoing tests of EEP and of the inverse square law are searching for new interactions arising from unification or quantum gravity. Tests of general relativity at the post-Newtonian level have reached high precision, including the light deflection, the Shapiro time delay, the perihelion advance of Mercury, the Nordtvedt effect in lunar motion, and frame-dragging. Gravitational wave damping has been detected in an amount that agrees with general relativity to better than half a percent using the Hulse–Taylor binary pulsar, and a growing family of other binary pulsar systems is yielding new tests, especially of strong-field effects. Current and future tests of relativity will center on strong gravity and gravitational waves. arXiv:1403.7377v1 [gr-qc] 28 Mar 2014 1 Contents 1 Introduction 3 2 Tests of the Foundations of Gravitation Theory 6 2.1 The Einstein equivalence principle . .. 6 2.1.1 Tests of the weak equivalence principle . .. 7 2.1.2 Tests of local Lorentz invariance . .. 9 2.1.3 Tests of local position invariance . 12 2.2 TheoreticalframeworksforanalyzingEEP. ....... 16 2.2.1 Schiff’sconjecture ................................ 16 2.2.2 The THǫµ formalism .............................
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												  Doing Physics with QuaternionsDoing Physics with Quaternions Douglas B. Sweetser ©2005 doug <[email protected]> All righs reserved. 1 INDEX Introduction 2 What are Quaternions? 3 Unifying Two Views of Events 4 A Brief History of Quaternions Mathematics 6 Multiplying Quaternions the Easy Way 7 Scalars, Vectors, Tensors and All That 11 Inner and Outer Products of Quaternions 13 Quaternion Analysis 23 Topological Properties of Quaternions 28 Quaternion Algebra Tool Set Classical Mechanics 32 Newton’s Second Law 35 Oscillators and Waves 37 Four Tests of for a Conservative Force Special Relativity 40 Rotations and Dilations Create the Lorentz Group 43 An Alternative Algebra for Lorentz Boosts Electromagnetism 48 Classical Electrodynamics 51 Electromagnetic Field Gauges 53 The Maxwell Equations in the Light Gauge: QED? 56 The Lorentz Force 58 The Stress Tensor of the Electromagnetic Field Quantum Mechanics 62 A Complete Inner Product Space with Dirac’s Bracket Notation 67 Multiplying quaternions in Polar Coordinate Form 69 Commutators and the Uncertainty Principle 74 Unifying the Representations of Integral and Half−Integral Spin 79 Deriving A Quaternion Analog to the Schrödinger Equation 83 Introduction to Relativistic Quantum Mechanics 86 Time Reversal Transformations for Intervals Gravity 89 Unified Field Theory by Analogy 101 Einstein’s vision I: Classical unified field equations for gravity and electromagnetism using Riemannian quaternions 115 Einstein’s vision II: A unified force equation with constant velocity profile solutions 123 Strings and Quantum Gravity 127 Answering Prima Facie Questions in Quantum Gravity Using Quaternions 134 Length in Curved Spacetime 136 A New Idea for Metrics 138 The Gravitational Redshift 140 A Brief Summary of Important Laws in Physics Written as Quaternions 155 Conclusions 2 What Are Quaternions? Quaternions are numbers like the real numbers: they can be added, subtracted, multiplied, and divided.
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												  1. IntroductionBeichler (1) Preliminary paper for Vigier IX Conference June 2014 MODERN FYSICS PHALLACIES: THE BEST WAY NOT TO UNIFY PHYSICS JAMES E. BEICHLER Research Institute for Paraphysics, Retired P.O. Box 624, Belpre, Ohio 45714 USA [email protected] Too many physicists believe the ‘phallacy’ that the quantum is more fundamental than relativity without any valid supporting evidence, so the earliest attempts to unify physics based on the continuity of relativity have been all but abandoned. This belief is probably due to the wealth of pro-quantum propaganda and general ‘phallacies in fysics’ that were spread during the second quarter of the twentieth century, although serious ‘phallacies’ exist throughout physics on both sides of the debate. Yet both approaches are basically flawed because both relativity and the quantum theory are incomplete and grossly misunderstood as they now stand. Had either side of the quantum versus relativity controversy sought common ground between the two worldviews, total unification would have been accomplished long ago. The point is, literally, that the discrete quantum, continuous relativity, basic physical geometry, theoretical mathematics and classical physics all share one common characteristic that has never been fully explored or explained – a paradoxical duality between a dimensionless point (discrete) and an extended length (continuity) in any dimension – and if the problem of unification is approached from an understanding of how this paradox relates to each paradigm, all of physics and indeed all of science could be unified under a single new theoretical paradigm. Keywords: unification, single field theory, unified field theory, quantized space-time, five-dimensional space-time, quantum, relativity, hidden variables, Einstein, Kaluza, Klein, Clifford 1.
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												  On the Shoulders of Giants: a Brief History of Physics in Göttingen1 6 ON THE SHO UL DERS OF G I A NTS : A B RIEF HISTORY OF P HYSI C S IN G Ö TTIN G EN On the Shoulders of Giants: a brief History of Physics in Göttingen 18th and 19th centuries Georg Ch. Lichtenberg (1742-1799) may be considered the fore- under Emil Wiechert (1861-1928), where seismic methods for father of experimental physics in Göttingen. His lectures were the study of the Earth's interior were developed. An institute accompanied by many experiments with equipment which he for applied mathematics and mechanics under the joint direc- had bought privately. To the general public, he is better known torship of the mathematician Carl Runge (1856-1927) (Runge- for his thoughtful and witty aphorisms. Following Lichtenberg, Kutta method) and the pioneer of aerodynamics, or boundary the next physicist of world renown would be Wilhelm Weber layers, Ludwig Prandtl (1875-1953) complemented the range of (1804-1891), a student, coworker and colleague of the „prince institutions related to physics proper. In 1925, Prandtl became of mathematics“ C. F. Gauss, who not only excelled in electro- the director of a newly established Kaiser-Wilhelm-Institute dynamics but fought for his constitutional rights against the for Fluid Dynamics. king of Hannover (1830). After his re-installment as a profes- A new and well-equipped physics building opened at the end sor in 1849, the two Göttingen physics chairs , W. Weber and B. of 1905. After the turn to the 20th century, Walter Kaufmann Listing, approximately corresponded to chairs of experimen- (1871-1947) did precision measurements on the velocity depen- tal and mathematical physics.
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												  General RelativityInstitut 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 .
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												  Einstein's Pathway to the Equivalence Principle 1905-1907Einstein's Pathway to the Equivalence Principle 1905-1907 Galina Weinstein Between 1905 and 1907, Einstein first tried to extend the special theory of relativity in such a way so as to explain gravitational phenomena. This was the most natural and simplest path to be taken. These investigations did not fit in with Galileo's law of free fall. This law, which may also be formulated as the law of the equality of inertial and gravitational mass, was illuminating Einstein, and he suspected that in it must lie the key to a deeper understanding of inertia and gravitation. He imagined an observer freely falling from the roof of a house; for the observer there is during the fall – at least in his immediate vicinity – no gravitational field. If the observer lets go of any bodies, they remain relative to him, in a state of rest or uniform motion, regardless of their particular chemical and physical nature. The observer is therefore justified in interpreting his state as being "at rest". Newton realized that Galileo's law of free fall is connected with the equality of the inertial and gravitational mass; however, this connection was accidental. Einstein said that Galileo's law of free fall can be viewed as Newton's equality between inertial and gravitational mass, but for him the connection was not accidental. Einstein's 1907 breakthrough was to consider Galileo's law of free fall as a powerful argument in favor of expanding the principle of relativity to systems moving non- uniformly relative to each other. Einstein realized that he might be able to generalize the principle of relativity when guided by Galileo's law of free fall; for if one body fell differently from all others in the gravitational field, then with the help of this body an observer in free fall (with all other bodies) could find out that he was falling in a gravitational field.