A New Formula of Redshift Vs. Space Expansion and Dark Energy

Total Page:16

File Type:pdf, Size:1020Kb

A New Formula of Redshift Vs. Space Expansion and Dark Energy Journal of Modern Physics, 2021, 12, 229-253 https://www.scirp.org/journal/jmp ISSN Online: 2153-120X ISSN Print: 2153-1196 A New Formula of Redshift vs. Space Expansion and Dark Energy Olivier Serret ESIM Engineer, Cugnaux, France How to cite this paper: Serret, O. (2021) A Abstract New Formula of Redshift vs. Space Expan- sion and Dark Energy. Journal of Modern The speed away of stars and galaxies is traditionally calculated from the rela- Physics, 12, 229-253. tivistic formula according to the measurement of the redshift. It is demon- https://doi.org/10.4236/jmp.2021.123018 strated here another formula for this speed away of stars and galaxies, from Received: December 23, 2020 this same redshift z. After having exposed critiques on the demonstration and Accepted: February 17, 2021 the relativistic use which require the assumption of an expanding universe by Published: February 20, 2021 itself, it is proposed within the framework of neo-Newtonian mechanics the z Copyright © 2021 by author(s) and formula Vc= where V is the speed from the source. This formula has 1+ z Scientific Research Publishing Inc. This work is licensed under the Creative the double characteristic of being equivalent to relativistic predictions for low Commons Attribution International redshifts, but of deviating from them by up to 17% for high redshifts. It is License (CC BY 4.0). consistent with the observation of the anisotropy of the Universe and the http://creativecommons.org/licenses/by/4.0/ Cosmic Microwave Background. It helps to explain Pioneer anomalies. It is Open Access compatible with the constancy in the majority of cases of interference phe- nomena. Finally, it provides a new analysis grid for the observation of super- novae, galaxies and distant pulsars, thus opening up new fields of research on the increase in distances attributed to dark energy and also in other areas of the cosmology. Keywords Redshift, Blueshift, Dark Energy, Radial Velocity, Expansion of the Universe, Anisotropy, Hubble Law, Pioneer Spacecraft, Photon, Wavelength, Frequency, Variable Speed, Celerity of Light 1. Introduction In the past, the stars did not exactly follow the supposedly perfectly circular tra- jectory, it was necessary to imagine the existence of epicycles … until new ellip- tical trajectories were accepted. Today, the distant galaxies not having to exceed DOI: 10.4236/jmp.2021.123018 Feb. 20, 2021 229 Journal of Modern Physics O. Serret the speed of light in spite of the law of Hubble, it is imagined a space which would create itself its own space, and the distant supernovae not following ex- actly the speed away calculated there, it is imagined the existence of a repulsive dark energy … unless we come to accept a new formula for the speeds away as a function of the redshift. This is what we will try to demonstrate in this article. After having recalled the definitions and uses of redshift and wavelength, we will analyze the research status on the relativistic redshift formula. Then we will propose the neo-Newtonian derivation to get to the expression of a slightly modified formula. Finally, we will discuss the consequences or not of this change of formula. 2. Definition and Context The redshift, noted z, is the fringe shift measured on light and electromagnetic waves from moving objects. From this measurement, first the speed away for stars and galaxies is calculated and then their distance is deduced using Hubble’s “law”. Yet, at the horizons of the Universe, by correlating with the distances derived from their luminosity, supernovae appear to be at distances greater than those calculated by the redshift method (see Figure 1). To explain this additional dis- tance speed and therefore this additional distance, it is invoked the existence of a dark energy with a repulsive effect, dark energy which has so far not been able to be directly apprehended. And more simply, why not question the formulas used to calculate the very fast speeds and the far distances? Light and electromagnetic waves in general are characterized by their wave- length λ, their propagation speed c and their frequency f. We can characterize them only by two out of three parameters because they are related to each other by the relation: λ = cf (1) Figure 1. Schematic explanation of Dark Energy. DOI: 10.4236/jmp.2021.123018 230 Journal of Modern Physics O. Serret Since the speed of light in vacuum is assumed to be constant, it has become customary to characterize the electromagnetic waves by only one parameter, the wavelength λ (i.e. a distance). Yet this is the frequency (i.e. a time, or more ex- actly the inverse of time) that we perceive or directly measure. For example, an optical detector does not measure a length, but is excited at certain frequencies. This is why in this article we will favor the explanation by frequencies f (rather than by wavelengths λ). 3. Analysis of the Relativistic Redshift Formula The relativistic expression allowing to deduce the distance speed V from the redshift z is as follows: 2 (11+−z) = − Vc2 (2) (11++z) This formula comes up against two difficulties. 3.1. The Derivation Itself The usual demonstration goes through the following intermediate step [1] [2] [3] [4]: cV− λobs = (3) fobs The problem is that the theory of Relativity postulates that the speed linking the two quantities λobs and fobs is constant and therefore that the numerator must be equal to c in any frame of reference. This means that V should be zero, which is contradictory with a moving source. There are also few much more complex derivations, but the one we have seen [5] is also open to criticism (in this video, there is a mix between Galilean for- mulas and relativistic formulas and the Equation (3) is implicit). 3.2. The Expansion of Space Itself Even admitting the validity of the previous derivation, the relativistic formula only allows to relate the redshift to the speed by making an additional assump- tion, namely the expansion of space itself. This additional assumption does not appear necessary as long as the source does not move away at very high speeds because it is used a simplified formula. But when they are faced with very high speed or high z’s, they end up with an inconsistency that can only be overcome by posing the strange hypothesis of a space that expands by itself. Without this additional assumption, the relativistic Equation (2) of the redshift leads to an inconsistent situation on the propagation speeds [see Appendix 1]. 4. The Neo-Newtonian Derivation 4.1. The Neo-Newtonian Mechanic So what formula should be used between the distance velocities and the fringe DOI: 10.4236/jmp.2021.123018 231 Journal of Modern Physics O. Serret shifts received from high- stars and galaxies? The proposal falls within the framework of neo-Newtonian mechanics which is none other than Newtonian mechanics but without the principle of equivalence between inert mass and gra- vitational mass: thus, the increase of inertial mass as a function of the speed pre- vents the photon from exceeding the celerity c, this means that the speed of the photon would not be constant in any frame of reference. The purpose of this ar- ticle is not to detail Newtonian Mechanics, the reader may consult it in the RELATED LINKS [a]. And as in Newtonian mechanics, it is assumed that the photon is a body of matter that can move in a vacuum, and that there is a fixed or barycentric frame R0. 4.2. The Method of the Derivation The derivation is based on the redshift understood as an effect of the Dopp- ler-Fizeau effect. The Doppler-Fizeau effect can be described as the effect pro- duced by a moving source of electromagnetic waves in which there is an appar- ent upward shift in frequency for observers towards whom the source is ap- proaching and an apparent downward shift in frequency for observers from whom the source is receding. Here is a simplified derivation of the speed away as a function of redshift, the general derivation is given in Appendix 2. Let us take the usual and simplified case of a photon emitted from a source which moves away while the observer is motionless in the fixed frame of reference R0. The pho- tons (A) then (B) are emitted according to the time interval Tsource at the ce- lerity c in the reference frame of the source, but according to neo-Newtonian mechanics they move at the speed (c-V) in the fixed reference frame R0 (see Figure 2) vc= − v photon// R00 photon source source / R (4) v > 0 with source/ R0 . There are two ways to calculate the distance between photons (A) and (B): • The first way is to note that the distance λ between the photons (A) and (B) is the distance DA traveled by the photon (A) during the time Tsource added to the distance dsource traveled by the source until the emission photon (B) (see Figure 3) Figure 2. Velocities of the photon: in black/Ro and in green/source S. DOI: 10.4236/jmp.2021.123018 232 Journal of Modern Physics O. Serret Figure 3. Photons from the moving source to the observer. λ =DdA + source (5) λ = vT∗ + v∗ T A// R00 source source R source (6) • The second way is to consider that the distance between the photons is the propagation distance of the photon (B) until it reaches the position where the photon (A) had been observed at the time of the emission of (B): λ′ = vT∗ B/ R0 obs (7) λ′ = vf B/ R0 obs (8) In neo-Newtonian mechanics, there is no variation in distance or time de- pending on the speed of the frame of reference, the distance between two pho- tons is the same whether it is calculated from the observer or from the source.
Recommended publications
  • 3 the Friedmann-Robertson-Walker Metric
    3 The Friedmann-Robertson-Walker metric 3.1 Three dimensions The most general isotropic and homogeneous metric in three dimensions is similar to the two dimensional result of eq. (43): dr2 ds2 = a2 + r2dΩ2 ; dΩ2 = dθ2 + sin2 θdφ2 ; k = 0; 1 : (46) 1 kr2 − The angles φ and θ are the usual azimuthal and polar angles of spherical coordinates, with θ [0; π], φ [0; 2π). As before, the parameter k can take on three different values: for k = 0, 2 2 the above line element describes ordinary flat space in spherical coordinates; k = 1 yields the metric for S , with constant positive curvature, while k = 1 is AdS and has constant 3 − 3 negative curvature. As in the two dimensional case, the change of variables r = sin χ (k = 1) or r = sinh χ (k = 1) makes the global nature of these manifolds more apparent. For example, − for the k = 1 case, after defining r = sin χ, the line element becomes ds2 = a2 dχ2 + sin2 χdθ2 + sin2 χ sin2 θdφ2 : (47) This is equivalent to writing ds2 = dX2 + dY 2 + dZ2 + dW 2 ; (48) where X = a sin χ sin θ cos φ ; Y = a sin χ sin θ sin φ ; Z = a sin χ cos θ ; W = a cos χ ; (49) which satisfy X2 + Y 2 + Z2 + W 2 = a2. So we see that the k = 1 metric corresponds to a 3-sphere of radius a embedded in 4-dimensional Euclidean space. One also sees a problem with the r = sin χ coordinate: it does not cover the whole sphere.
    [Show full text]
  • From Relativistic Time Dilation to Psychological Time Perception
    From relativistic time dilation to psychological time perception: an approach and model, driven by the theory of relativity, to combine the physical time with the time perceived while experiencing different situations. Andrea Conte1,∗ Abstract An approach, supported by a physical model driven by the theory of relativity, is presented. This approach and model tend to conciliate the relativistic view on time dilation with the current models and conclusions on time perception. The model uses energy ratios instead of geometrical transformations to express time dilation. Brain mechanisms like the arousal mechanism and the attention mechanism are interpreted and combined using the model. Matrices of order two are generated to contain the time dilation between two observers, from the point of view of a third observer. The matrices are used to transform an observer time to another observer time. Correlations with the official time dilation equations are given in the appendix. Keywords: Time dilation, Time perception, Definition of time, Lorentz factor, Relativity, Physical time, Psychological time, Psychology of time, Internal clock, Arousal, Attention, Subjective time, Internal flux, External flux, Energy system ∗Corresponding author Email address: [email protected] (Andrea Conte) 1Declarations of interest: none Preprint submitted to PsyArXiv - version 2, revision 1 June 6, 2021 Contents 1 Introduction 3 1.1 The unit of time . 4 1.2 The Lorentz factor . 6 2 Physical model 7 2.1 Energy system . 7 2.2 Internal flux . 7 2.3 Internal flux ratio . 9 2.4 Non-isolated system interaction . 10 2.5 External flux . 11 2.6 External flux ratio . 12 2.7 Total flux .
    [Show full text]
  • An Analysis of Gravitational Redshift from Rotating Body
    An analysis of gravitational redshift from rotating body Anuj Kumar Dubey∗ and A K Sen† Department of Physics, Assam University, Silchar-788011, Assam, India. (Dated: July 29, 2021) Gravitational redshift is generally calculated without considering the rotation of a body. Neglect- ing the rotation, the geometry of space time can be described by using the spherically symmetric Schwarzschild geometry. Rotation has great effect on general relativity, which gives new challenges on gravitational redshift. When rotation is taken into consideration spherical symmetry is lost and off diagonal terms appear in the metric. The geometry of space time can be then described by using the solutions of Kerr family. In the present paper we discuss the gravitational redshift for rotating body by using Kerr metric. The numerical calculations has been done under Newtonian approximation of angular momentum. It has been found that the value of gravitational redshift is influenced by the direction of spin of central body and also on the position (latitude) on the central body at which the photon is emitted. The variation of gravitational redshift from equatorial to non - equatorial region has been calculated and its implications are discussed in detail. I. INTRODUCTION from principle of equivalence. Snider in 1972 has mea- sured the redshift of the solar potassium absorption line General relativity is not only relativistic theory of grav- at 7699 A˚ by using an atomic - beam resonance - scat- itation proposed by Einstein, but it is the simplest theory tering technique [5]. Krisher et al. in 1993 had measured that is consistent with experimental data. Predictions of the gravitational redshift of Sun [6].
    [Show full text]
  • The Age of the Universe Transcript
    The Age of the Universe Transcript Date: Wednesday, 6 February 2013 - 1:00PM Location: Museum of London 6 February 2013 The Age of The Universe Professor Carolin Crawford Introduction The idea that the Universe might have an age is a relatively new concept, one that became recognised only during the past century. Even as it became understood that individual objects, such as stars, have finite lives surrounded by a birth and an end, the encompassing cosmos was always regarded as a static and eternal framework. The change in our thinking has underpinned cosmology, the science concerned with the structure and the evolution of the Universe as a whole. Before we turn to the whole cosmos then, let us start our story nearer to home, with the difficulty of solving what might appear a simpler problem, determining the age of the Earth. Age of the Earth The fact that our planet has evolved at all arose predominantly from the work of 19th century geologists, and in particular, the understanding of how sedimentary rocks had been set down as an accumulation of layers over extraordinarily long periods of time. The remains of creatures trapped in these layers as fossils clearly did not resemble any currently living, but there was disagreement about how long a time had passed since they had died. The cooling earth The first attempt to age the Earth based on physics rather than geology came from Lord Kelvin at the end of the 19th Century. Assuming that the whole planet would have started from a completely molten state, he then calculated how long it would take for the surface layers of Earth to cool to their present temperature.
    [Show full text]
  • Hubble's Law and the Expanding Universe
    COMMENTARY COMMENTARY Hubble’s Law and the expanding universe Neta A. Bahcall1 the expansion rate is constant in all direc- Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08544 tions at any given time, this rate changes with time throughout the life of the uni- verse. When expressed as a function of cos- In one of the most famous classic papers presented the observational evidence for one H t in the annals of science, Edwin Hubble’s of science’s greatest discoveries—the expand- mic time, ( ), it is known as the Hubble 1929 PNAS article on the observed relation inguniverse.Hubbleshowedthatgalaxiesare Parameter. The expansion rate at the pres- between distance and recession velocity of receding away from us with a velocity that is ent time, Ho, is about 70 km/s/Mpc (where 1 Mpc = 106 parsec = 3.26 × 106 light-y). galaxies—the Hubble Law—unveiled the proportional to their distance from us: more The inverse of the Hubble Constant is the expanding universe and forever changed our distant galaxies recede faster than nearby gal- Hubble Time, tH = d/v = 1/H ; it reflects understanding of the cosmos. It inaugurated axies. Hubble’s classic graph of the observed o the time since a linear cosmic expansion has the field of observational cosmology that has velocity vs. distance for nearby galaxies is begun (extrapolating a linear Hubble Law uncovered an amazingly vast universe that presented in Fig. 1; this graph has become back to time t = 0); it is thus related to has been expanding and evolving for 14 bil- a scientific landmark that is regularly repro- the age of the Universe from the Big-Bang lion years and contains dark matter, dark duced in astronomy textbooks.
    [Show full text]
  • Aspects of Spatially Homogeneous and Isotropic Cosmology
    Faculty of Technology and Science Department of Physics and Electrical Engineering Mikael Isaksson Aspects of Spatially Homogeneous and Isotropic Cosmology Degree Project of 15 credit points Physics Program Date/Term: 02-04-11 Supervisor: Prof. Claes Uggla Examiner: Prof. Jürgen Fuchs Karlstads universitet 651 88 Karlstad Tfn 054-700 10 00 Fax 054-700 14 60 [email protected] www.kau.se Abstract In this thesis, after a general introduction, we first review some differential geom- etry to provide the mathematical background needed to derive the key equations in cosmology. Then we consider the Robertson-Walker geometry and its relation- ship to cosmography, i.e., how one makes measurements in cosmology. We finally connect the Robertson-Walker geometry to Einstein's field equation to obtain so- called cosmological Friedmann-Lema^ıtre models. These models are subsequently studied by means of potential diagrams. 1 CONTENTS CONTENTS Contents 1 Introduction 3 2 Differential geometry prerequisites 8 3 Cosmography 13 3.1 Robertson-Walker geometry . 13 3.2 Concepts and measurements in cosmography . 18 4 Friedmann-Lema^ıtre dynamics 30 5 Bibliography 42 2 1 INTRODUCTION 1 Introduction Cosmology comes from the Greek word kosmos, `universe' and logia, `study', and is the study of the large-scale structure, origin, and evolution of the universe, that is, of the universe taken as a whole [1]. Even though the word cosmology is relatively recent (first used in 1730 in Christian Wolff's Cosmologia Generalis), the study of the universe has a long history involving science, philosophy, eso- tericism, and religion. Cosmologies in their earliest form were concerned with, what is now known as celestial mechanics (the study of the heavens).
    [Show full text]
  • The Reionization of Cosmic Hydrogen by the First Galaxies Abstract 1
    David Goodstein’s Cosmology Book The Reionization of Cosmic Hydrogen by the First Galaxies Abraham Loeb Department of Astronomy, Harvard University, 60 Garden St., Cambridge MA, 02138 Abstract Cosmology is by now a mature experimental science. We are privileged to live at a time when the story of genesis (how the Universe started and developed) can be critically explored by direct observations. Looking deep into the Universe through powerful telescopes, we can see images of the Universe when it was younger because of the finite time it takes light to travel to us from distant sources. Existing data sets include an image of the Universe when it was 0.4 million years old (in the form of the cosmic microwave background), as well as images of individual galaxies when the Universe was older than a billion years. But there is a serious challenge: in between these two epochs was a period when the Universe was dark, stars had not yet formed, and the cosmic microwave background no longer traced the distribution of matter. And this is precisely the most interesting period, when the primordial soup evolved into the rich zoo of objects we now see. The observers are moving ahead along several fronts. The first involves the construction of large infrared telescopes on the ground and in space, that will provide us with new photos of the first galaxies. Current plans include ground-based telescopes which are 24-42 meter in diameter, and NASA’s successor to the Hubble Space Telescope, called the James Webb Space Telescope. In addition, several observational groups around the globe are constructing radio arrays that will be capable of mapping the three-dimensional distribution of cosmic hydrogen in the infant Universe.
    [Show full text]
  • Simulating Gamma-Ray Binaries with a Relativistic Extension of RAMSES? A
    A&A 560, A79 (2013) Astronomy DOI: 10.1051/0004-6361/201322266 & c ESO 2013 Astrophysics Simulating gamma-ray binaries with a relativistic extension of RAMSES? A. Lamberts1;2, S. Fromang3, G. Dubus1, and R. Teyssier3;4 1 UJF-Grenoble 1 / CNRS-INSU, Institut de Planétologie et d’Astrophysique de Grenoble (IPAG) UMR 5274, 38041 Grenoble, France e-mail: [email protected] 2 Physics Department, University of Wisconsin-Milwaukee, Milwaukee WI 53211, USA 3 Laboratoire AIM, CEA/DSM - CNRS - Université Paris 7, Irfu/Service d’Astrophysique, CEA-Saclay, 91191 Gif-sur-Yvette, France 4 Institute for Theoretical Physics, University of Zürich, Winterthurestrasse 190, 8057 Zürich, Switzerland Received 11 July 2013 / Accepted 29 September 2013 ABSTRACT Context. Gamma-ray binaries are composed of a massive star and a rotation-powered pulsar with a highly relativistic wind. The collision between the winds from both objects creates a shock structure where particles are accelerated, which results in the observed high-energy emission. Aims. We want to understand the impact of the relativistic nature of the pulsar wind on the structure and stability of the colliding wind region and highlight the differences with colliding winds from massive stars. We focus on how the structure evolves with increasing values of the Lorentz factor of the pulsar wind, keeping in mind that current simulations are unable to reach the expected values of pulsar wind Lorentz factors by orders of magnitude. Methods. We use high-resolution numerical simulations with a relativistic extension to the hydrodynamics code RAMSES we have developed. We perform two-dimensional simulations, and focus on the region close to the binary, where orbital motion can be ne- glected.
    [Show full text]
  • Galaxies at High Redshift Mauro Giavalisco
    eaa.iop.org DOI: 10.1888/0333750888/1669 Galaxies at High Redshift Mauro Giavalisco From Encyclopedia of Astronomy & Astrophysics P. Murdin © IOP Publishing Ltd 2006 ISBN: 0333750888 Institute of Physics Publishing Bristol and Philadelphia Downloaded on Thu Mar 02 23:08:45 GMT 2006 [131.215.103.76] Terms and Conditions Galaxies at High Redshift E NCYCLOPEDIA OF A STRONOMY AND A STROPHYSICS Galaxies at High Redshift that is progressively higher for objects that are separated in space by larger distances. If the recession velocity between Galaxies at high REDSHIFT are very distant galaxies and, two objects is small compared with the speed of light, since light propagates through space at a finite speed of its value is directly proportional to the distance between approximately 300 000 km s−1, they appear to an observer them, namely v = H d on the Earth as they were in a very remote past, when r 0 the light departed them, carrying information on their H properties at that time. Observations of objects with very where the constant of proportionality 0 is called the high redshifts play a central role in cosmology because ‘HUBBLE CONSTANT’. For larger recession velocities this they provide insight into the epochs and the mechanisms relation is replaced by a more general one calculated from the theory of general relativity. In each cases, the value of GALAXY FORMATION, if one can reach redshifts that are high H enough to correspond to the cosmic epochs when galaxies of 0 provides the recession velocity of a pair of galaxies were forming their first populations of stars and began to separated by unitary distance, and hence sets the rate of shine light throughout space.
    [Show full text]
  • The Anthropic Principle and Multiple Universe Hypotheses Oren Kreps
    The Anthropic Principle and Multiple Universe Hypotheses Oren Kreps Contents Abstract ........................................................................................................................................... 1 Introduction ..................................................................................................................................... 1 Section 1: The Fine-Tuning Argument and the Anthropic Principle .............................................. 3 The Improbability of a Life-Sustaining Universe ....................................................................... 3 Does God Explain Fine-Tuning? ................................................................................................ 4 The Anthropic Principle .............................................................................................................. 7 The Multiverse Premise ............................................................................................................ 10 Three Classes of Coincidence ................................................................................................... 13 Can The Existence of Sapient Life Justify the Multiverse? ...................................................... 16 How unlikely is fine-tuning? .................................................................................................... 17 Section 2: Multiverse Theories ..................................................................................................... 18 Many universes or all possible
    [Show full text]
  • Doppler Boosting and Cosmological Redshift on Relativistic Jets
    Doppler Boosting and cosmological redshift on relativistic jets Author: Jordi Fernández Vilana Advisor: Valentí Bosch i Ramon Facultat de Física, Universitat de Barcelona, Diagonal 645, 08028 Barcelona, Spain. Abstract: In this study our goal was to identify the possible effects that influence with the Spectral Energy Distribution of a blazar, which we deducted that are Doppler Boosting effect and cosmological redshift. Then we investigated how the spectral energy distribution varies by changing intrinsic parameters of the jet like its Lorentz factor, the angle of the line of sight respect to the jet orientation or the blazar redshift. The obtained results showed a strong enhancing of the Spectral Energy Distribution for nearly 0º angles and high Lorentz factors, while the increase in redshift produced the inverse effect, reducing the normalization of the distribution and moving the peak to lower energies. These two effects compete in the observations of all known blazars and our simple model confirmed the experimental results, that only those blazars with optimal characteristics, if at very high redshift, are suitable to be measured by the actual instruments, making the study of blazars with a high redshift an issue that needs very deep observations at different wavelengths to collect enough data to properly characterize the source population. jet those particles are moving at relativistic speeds, producing I. INTRODUCTION high energy interactions in the process. This scenario produces a wide spectrum of radiation that mainly comes, as we can see in more detail in [2], from Inverse Compton We know that active galactic nuclei or AGN are galaxies scattering. Low energy photons inside the jet are scattered by with an accreting supermassive blackhole in the centre.
    [Show full text]
  • (Special) Relativity
    (Special) Relativity With very strong emphasis on electrodynamics and accelerators Better: How can we deal with moving charged particles ? Werner Herr, CERN Reading Material [1 ]R.P. Feynman, Feynman lectures on Physics, Vol. 1 + 2, (Basic Books, 2011). [2 ]A. Einstein, Zur Elektrodynamik bewegter K¨orper, Ann. Phys. 17, (1905). [3 ]L. Landau, E. Lifschitz, The Classical Theory of Fields, Vol2. (Butterworth-Heinemann, 1975) [4 ]J. Freund, Special Relativity, (World Scientific, 2008). [5 ]J.D. Jackson, Classical Electrodynamics (Wiley, 1998 ..) [6 ]J. Hafele and R. Keating, Science 177, (1972) 166. Why Special Relativity ? We have to deal with moving charges in accelerators Electromagnetism and fundamental laws of classical mechanics show inconsistencies Ad hoc introduction of Lorentz force Applied to moving bodies Maxwell’s equations lead to asymmetries [2] not shown in observations of electromagnetic phenomena Classical EM-theory not consistent with Quantum theory Important for beam dynamics and machine design: Longitudinal dynamics (e.g. transition, ...) Collective effects (e.g. space charge, beam-beam, ...) Dynamics and luminosity in colliders Particle lifetime and decay (e.g. µ, π, Z0, Higgs, ...) Synchrotron radiation and light sources ... We need a formalism to get all that ! OUTLINE Principle of Relativity (Newton, Galilei) - Motivation, Ideas and Terminology - Formalism, Examples Principle of Special Relativity (Einstein) - Postulates, Formalism and Consequences - Four-vectors and applications (Electromagnetism and accelerators) § ¤ some slides are for your private study and pleasure and I shall go fast there ¦ ¥ Enjoy yourself .. Setting the scene (terminology) .. To describe an observation and physics laws we use: - Space coordinates: ~x = (x, y, z) (not necessarily Cartesian) - Time: t What is a ”Frame”: - Where we observe physical phenomena and properties as function of their position ~x and time t.
    [Show full text]