The Dynamical Velocity Superposition Effect in the Quantum-Foam In
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Measurement of the Speed of Gravity
Measurement of the Speed of Gravity Yin Zhu Agriculture Department of Hubei Province, Wuhan, China Abstract From the Liénard-Wiechert potential in both the gravitational field and the electromagnetic field, it is shown that the speed of propagation of the gravitational field (waves) can be tested by comparing the measured speed of gravitational force with the measured speed of Coulomb force. PACS: 04.20.Cv; 04.30.Nk; 04.80.Cc Fomalont and Kopeikin [1] in 2002 claimed that to 20% accuracy they confirmed that the speed of gravity is equal to the speed of light in vacuum. Their work was immediately contradicted by Will [2] and other several physicists. [3-7] Fomalont and Kopeikin [1] accepted that their measurement is not sufficiently accurate to detect terms of order , which can experimentally distinguish Kopeikin interpretation from Will interpretation. Fomalont et al [8] reported their measurements in 2009 and claimed that these measurements are more accurate than the 2002 VLBA experiment [1], but did not point out whether the terms of order have been detected. Within the post-Newtonian framework, several metric theories have studied the radiation and propagation of gravitational waves. [9] For example, in the Rosen bi-metric theory, [10] the difference between the speed of gravity and the speed of light could be tested by comparing the arrival times of a gravitational wave and an electromagnetic wave from the same event: a supernova. Hulse and Taylor [11] showed the indirect evidence for gravitational radiation. However, the gravitational waves themselves have not yet been detected directly. [12] In electrodynamics the speed of electromagnetic waves appears in Maxwell equations as c = √휇0휀0, no such constant appears in any theory of gravity. -
Relativity and Fundamental Physics
Relativity and Fundamental Physics Sergei Kopeikin (1,2,*) 1) Dept. of Physics and Astronomy, University of Missouri, 322 Physics Building., Columbia, MO 65211, USA 2) Siberian State University of Geosystems and Technology, Plakhotny Street 10, Novosibirsk 630108, Russia Abstract Laser ranging has had a long and significant role in testing general relativity and it continues to make advance in this field. It is important to understand the relation of the laser ranging to other branches of fundamental gravitational physics and their mutual interaction. The talk overviews the basic theoretical principles underlying experimental tests of general relativity and the recent major achievements in this field. Introduction Modern theory of fundamental interactions relies heavily upon two strong pillars both created by Albert Einstein – special and general theory of relativity. Special relativity is a cornerstone of elementary particle physics and the quantum field theory while general relativity is a metric- based theory of gravitational field. Understanding the nature of the fundamental physical interactions and their hierarchic structure is the ultimate goal of theoretical and experimental physics. Among the four known fundamental interactions the most important but least understood is the gravitational interaction due to its weakness in the solar system – a primary experimental laboratory of gravitational physicists for several hundred years. Nowadays, general relativity is a canonical theory of gravity used by astrophysicists to study the black holes and astrophysical phenomena in the early universe. General relativity is a beautiful theoretical achievement but it is only a classic approximation to deeper fundamental nature of gravity. Any possible deviation from general relativity can be a clue to new physics (Turyshev, 2015). -
Arxiv:Gr-Qc/0507001V3 16 Oct 2005
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by University of Missouri: MOspace February 7, 2008 3:29 WSPC/INSTRUCTION FILE ijmp˙october12 International Journal of Modern Physics D c World Scientific Publishing Company Gravitomagnetism and the Speed of Gravity Sergei M. Kopeikin Department of Physics and Astronomy, University of Missouri-Columbia, Columbia, Missouri 65211, USA [email protected] Experimental discovery of the gravitomagnetic fields generated by translational and/or rotational currents of matter is one of primary goals of modern gravitational physics. The rotational (intrinsic) gravitomagnetic field of the Earth is currently measured by the Gravity Probe B. The present paper makes use of a parametrized post-Newtonian (PN) expansion of the Einstein equations to demonstrate how the extrinsic gravitomag- netic field generated by the translational current of matter can be measured by observing the relativistic time delay caused by a moving gravitational lens. We prove that mea- suring the extrinsic gravitomagnetic field is equivalent to testing relativistic effect of the aberration of gravity caused by the Lorentz transformation of the gravitational field. We unfold that the recent Jovian deflection experiment is a null-type experiment testing the Lorentz invariance of the gravitational field (aberration of gravity), thus, confirming existence of the extrinsic gravitomagnetic field associated with orbital motion of Jupiter with accuracy 20%. We comment on erroneous interpretations of the Jovian deflection experiment given by a number of researchers who are not familiar with modern VLBI technique and subtleties of JPL ephemeris. We propose to measure the aberration of gravity effect more accurately by observing gravitational deflection of light by the Sun and processing VLBI observations in the geocentric frame with respect to which the Sun arXiv:gr-qc/0507001v3 16 Oct 2005 is moving with velocity ∼ 30 km/s. -
Effect of the Earth's Time-Retarded Transverse Gravitational Field On
-1- Effect of the Earth’s Time-Retarded Transverse Gravitational Field on Spacecraft Flybys (Version 3) J. C. Hafele1 ______________________________________________________________________________ In 2008 a group of NASA scientists reported an anomalous change in the speed of six spacecraft flybys of the Earth. The reported speed change for the NEAR spacecraft flyby is 13.460.01 mm/s. It is known that general relativity theory reduces to classical time-retarded electromagnetic field theory in the linearized approximation. This report shows that time-retarded field theory applied to the Earth’s transverse gravitational field gives rise to a small change in the speed of a spacecraft during a flyby. The speed change depends on the time dependence of the transverse gravitational field, which generates an induction field that is proportional to the time derivative of the transverse field. If the corresponding speed for the induction field is set equal to (4.1300.003) times the Earth’s equatorial rotational surface speed, and the speed of the Earth’s gravitational field is set equal to (1.0600.001) times the vacuum speed of light, the calculated value for the speed change for the NEAR flyby agrees exactly with the observed value. Similar results are found for the remaining five flybys. ______________________________________________________________________________ Key Words: time-retarded gravity; transverse gravity; speed of gravity; flyby anomaly 1. INTRODUCTION It has long been known that electromagnetic fields propagate at the speed of light. The actual speed of light depends on whether the field is propagating in a vacuum or in a material medium. In either case, to calculate the electromagnetic fields of a moving point-charge, the concept of “time retardation” must be used.(1) Time retardation is necessary because it takes a certain amount of time for causal physical fields to propagate from a moving point-source to a distant field point. -
Physics/0409010V1 [Physics.Gen-Ph] 1 Sep 2004 Ri Ihteclsilshr Sntfound
Physical Interpretations of Relativity Theory Conference IX London, Imperial College, September, 2004 ............... Mach’s Principle II by James G. Gilson∗ School of Mathematical Sciences Queen Mary College University of London October 29, 2018 Abstract 1 Introduction The question of the validity or otherwise of Mach’s The meaning and significance of Mach’s Principle Principle[5] has been with us for almost a century and and its dependence on ideas about relativistic rotat- has been vigorously analysed and discussed for all of ing frame theory and the celestial sphere is explained that time and is, up to date, still not resolved. One and discussed. Two new relativistic rotation trans- contentious issue is, does general[7] relativity theory formations are introduced by using a linear simula- imply that Mach’s Principle is operative in that theo- tion for the rotating disc situation. The accepted retical structure or does it not? A deduction[4] from formula for centrifugal acceleration in general rela- general relativity that the classical Newtonian cen- tivity is then analysed with the use of one of these trifugal acceleration formula should be modified by transformations. It is shown that for this general rel- an additional relativistic γ2(v) factor, see equations ativity formula to be valid throughout all space-time (2.11) and (2.27), will help us in the analysis of that there has to be everywhere a local standard of ab- question. Here I shall attempt to throw some light solutely zero rotation. It is then concluded that the on the nature and technical basis of the collection of field off all possible space-time null geodesics or pho- arXiv:physics/0409010v1 [physics.gen-ph] 1 Sep 2004 technical and philosophical problems generated from ton paths unify the absolute local non-rotation stan- Mach’s Principle and give some suggestions about dard throughout space-time. -
New Varying Speed of Light Theories
New varying speed of light theories Jo˜ao Magueijo The Blackett Laboratory,Imperial College of Science, Technology and Medicine South Kensington, London SW7 2BZ, UK ABSTRACT We review recent work on the possibility of a varying speed of light (VSL). We start by discussing the physical meaning of a varying c, dispelling the myth that the constancy of c is a matter of logical consistency. We then summarize the main VSL mechanisms proposed so far: hard breaking of Lorentz invariance; bimetric theories (where the speeds of gravity and light are not the same); locally Lorentz invariant VSL theories; theories exhibiting a color dependent speed of light; varying c induced by extra dimensions (e.g. in the brane-world scenario); and field theories where VSL results from vacuum polarization or CPT violation. We show how VSL scenarios may solve the cosmological problems usually tackled by inflation, and also how they may produce a scale-invariant spectrum of Gaussian fluctuations, capable of explaining the WMAP data. We then review the connection between VSL and theories of quantum gravity, showing how “doubly special” relativity has emerged as a VSL effective model of quantum space-time, with observational implications for ultra high energy cosmic rays and gamma ray bursts. Some recent work on the physics of “black” holes and other compact objects in VSL theories is also described, highlighting phenomena associated with spatial (as opposed to temporal) variations in c. Finally we describe the observational status of the theory. The evidence is slim – redshift dependence in alpha, ultra high energy cosmic rays, and (to a much lesser extent) the acceleration of the universe and the WMAP data. -
A Gravitomagnetic Thought Experiment for Undergraduates Karlsson, Anders
A gravitomagnetic thought experiment for undergraduates Karlsson, Anders 2006 Link to publication Citation for published version (APA): Karlsson, A. (2006). A gravitomagnetic thought experiment for undergraduates. (Technical Report LUTEDX/(TEAT-7150)/1-7/(2006); Vol. TEAT-7150). [Publisher information missing]. Total number of authors: 1 General rights Unless other specific re-use rights are stated the following general rights apply: Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal Read more about Creative commons licenses: https://creativecommons.org/licenses/ Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. LUND UNIVERSITY PO Box 117 221 00 Lund +46 46-222 00 00 CODEN:LUTEDX/(TEAT-7150)/1-7/(2006) A gravitomagnetic thought experiment for undergraduates Anders Karlsson Electromagnetic Theory Department of Electrical and Information Technology Lund University Sweden Anders Karlsson Department of Electrical and Information Technology Electromagnetic Theory Lund University P.O. Box 118 SE-221 00 Lund Sweden Editor: Gerhard Kristensson c Anders Karlsson, Lund, November 2, 2006 1 Abstract The gravitomagnetic force is the gravitational counterpart to the Lorentz force in electromagnetics. -
General Relativity and Spatial Flows: I
1 GENERAL RELATIVITY AND SPATIAL FLOWS: I. ABSOLUTE RELATIVISTIC DYNAMICS* Tom Martin Gravity Research Institute Boulder, Colorado 80306-1258 [email protected] Abstract Two complementary and equally important approaches to relativistic physics are explained. One is the standard approach, and the other is based on a study of the flows of an underlying physical substratum. Previous results concerning the substratum flow approach are reviewed, expanded, and more closely related to the formalism of General Relativity. An absolute relativistic dynamics is derived in which energy and momentum take on absolute significance with respect to the substratum. Possible new effects on satellites are described. 1. Introduction There are two fundamentally different ways to approach relativistic physics. The first approach, which was Einstein's way [1], and which is the standard way it has been practiced in modern times, recognizes the measurement reality of the impossibility of detecting the absolute translational motion of physical systems through the underlying physical substratum and the measurement reality of the limitations imposed by the finite speed of light with respect to clock synchronization procedures. The second approach, which was Lorentz's way [2] (at least for Special Relativity), recognizes the conceptual superiority of retaining the physical substratum as an important element of the physical theory and of using conceptually useful frames of reference for the understanding of underlying physical principles. Whether one does relativistic physics the Einsteinian way or the Lorentzian way really depends on one's motives. The Einsteinian approach is primarily concerned with * http://xxx.lanl.gov/ftp/gr-qc/papers/0006/0006029.pdf 2 being able to carry out practical space-time experiments and to relate the results of these experiments among variously moving observers in as efficient and uncomplicated manner as possible. -
The Newtonian and Relativistic Theory of Orbits and the Emission of Gravitational Waves
108 The Open Astronomy Journal, 2011, 4, (Suppl 1-M7) 108-150 Open Access The Newtonian and Relativistic Theory of Orbits and the Emission of Gravitational Waves Mariafelicia De Laurentis1,2,* 1Dipartimento di Scienze Fisiche, Universitá di Napoli " Federico II",Compl. Univ. di Monte S. Angelo, Edificio G, Via Cinthia, I-80126, Napoli, Italy 2INFN Sez. di Napoli, Compl. Univ. di Monte S. Angelo, Edificio G, Via Cinthia, I-80126, Napoli, Italy Abstract: This review paper is devoted to the theory of orbits. We start with the discussion of the Newtonian problem of motion then we consider the relativistic problem of motion, in particular the post-Newtonian (PN) approximation and the further gravitomagnetic corrections. Finally by a classification of orbits in accordance with the conditions of motion, we calculate the gravitational waves luminosity for different types of stellar encounters and orbits. Keywords: Theroy of orbits, gravitational waves, post-newtonian (PN) approximation, LISA, transverse traceless, Elliptical orbits. 1. INTRODUCTION of General Relativity (GR). Indeed, the PN approximation method, developed by Einstein himself [1], Droste and de Dynamics of standard and compact astrophysical bodies could be aimed to unravelling the information contained in Sitter [2, 3] within one year after the publication of GR, led the gravitational wave (GW) signals. Several situations are to the predictions of i) the relativistic advance of perihelion of planets, ii) the gravitational redshift, iii) the deflection possible such as GWs emitted by coalescing compact binaries–systems of neutron stars (NS), black holes (BH) of light, iv) the relativistic precession of the Moon orbit, that driven into coalescence by emission of gravitational are the so–called "classical" tests of GR. -
The Confrontation Between General Relativity and Experiment
The 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 ............................. -
Arxiv:1007.1861V1 [Gr-Qc] 12 Jul 2010 Feulms N Hp.Temaueeto Uhagravito-Mag a Such of Measurement 10 the Is Shape
A laser gyroscope system to detect the Gravito-Magnetic effect on Earth A. Di Virgilio∗ INFN Sez. di Pisa, Pisa, Italy K. U. Schreiber and A. Gebauer† Technische Universitaet Muenchen, Forschungseinrichtung Satellitengeodaesie Fundamentalstation Wettzell, 93444 Bad K¨otzting, Germany J-P. R. Wells‡ Department of Physics and Astronomy, University of Canterbury, PB4800, Christchurch 8020, New Zealand A. Tartaglia§ Polit. of Torino and INFN, Torino, Italy J. Belfi and N. Beverini¶ Univ. of Pisa and CNISM, Pisa, Italy A.Ortolan∗∗ Laboratori Nazionali di Legnaro, INFN Legnaro (Padova), Italy Large scale square ring laser gyros with a length of four meters on each side are approaching a sensitivity of 1 10−11rad/s/√Hz. This is about the regime required to measure the gravito- magnetic effect (Lense× Thirring) of the Earth. For an ensemble of linearly independent gyros each measurement signal depends upon the orientation of each single axis gyro with respect to the rotational axis of the Earth. Therefore at least 3 gyros are necessary to reconstruct the complete angular orientation of the apparatus. In general, the setup consists of several laser gyroscopes (we would prefer more than 3 for sufficient redundancy), rigidly referenced to each other. Adding more gyros for one plane of observation provides a cross-check against intra-system biases and furthermore has the advantage of improving the signal to noise ratio by the square root of the number of gyros. In this paper we analyze a system of two pairs of identical gyros (twins) with a slightly different orientation with respect to the Earth axis. The twin gyro configuration has several interesting properties. -
An Essay on the Coriolis Force
James F. Price Woods Hole Oceanographic Institution Woods Hole, Massachusetts, 02543 http:// www.whoi.edu/science/PO/people/jprice [email protected] Version 3.3 January 10, 2006 Summary: An Earth-attached and thus rotating reference frame is almost always used for the analysis of geophysical flows. The equation of motion transformed into a steadily rotating reference frame includes two terms that involve the rotation vector; a centrifugal term and a Coriolis term. In the special case of an Earth-attached reference frame, the centrifugal term is exactly canceled by gravitational mass attraction and drops out of the equation of motion. When we solve for the acceleration seen from an Earth-attached frame, the Coriolis term is interpreted as a force. The rotating frame perspective gives up the properties of global momentum conservation and invariance to Galilean transformation. Nevertheless, it leads to a greatly simplified analysis of geophysical flows since only the comparatively small relative velocity, i.e., winds and currents, need be considered. The Coriolis force has a simple mathematical form, 2˝ V 0M , where ˝ is Earth’s rotation vector, V 0 is the velocity observed from the rotating frame and M is the particle mass. The Coriolis force is perpendicular to the velocity and can do no work. It tends to cause a deflection of velocity, and gives rise to two important modes of motion: (1) If the Coriolis force is the only force acting on a moving particle, then the velocity vector of the particle will be continually deflected and rotate clockwise in the northern hemisphere and anticlockwise in the southern hemisphere.