tisdag 29 november 2011

Poincare and Einstein, two giants.

"If we were not ignorant there would be no probability, there could only be certainty. But our ignorance cannot be absolute, for then there would be no longer any probability at all. Thus the problems of probability may be classed according to the greater or less depth of our ignorance. "Mathematics is not the study of objects, but instead, the relations (isomorphisms for instance) between them.

"Good theories are flexible. Those which have a rigid form and which can not change that form without collapsing really have too little vitality. But if a theory is solid, then it can be cast in diverse forms, it resists all attacks, and its essential meaning remains unaffected. The objections to them, therefore, far from annihilating them, actually serve them, since they allow such theories to develop all the virtues which were latent in them. The theory of Lorentz is one such " (My comment; TGD is usually accused for being a flexible theory).

Henry Poincaré


There has been no Nobel Prize awarded for the theory of relativity? Got the wrong man the Nobel Prize? Poincare was dead, otherwise he would have, [Lorentz (Nobel 1902 for his electron), Michelson (Nobel 1907), Minkowski (?), Planck (Nobel 1918)] the prize shared with Einstein (Nobel 1921)?

Would this have made the history go otherwise? Henri Poincaré died from embolism and cancer in 1912.

When the Michelson–Morley experiment failed to show the presence of “lumineferous ether” (if the ether did exist, the experiment would show that light moving in the same direction as the Earth was traveling faster than light moving at right angles to it) the physics community began a scramble to account for the findings, and took Einstein to unravel the mystery and a new era of physics was born. In fact Poincare was the one starting doubt the 'ether' and its 'dragging effect'.
The Relative Motion of the Earth and the Luminiferous Ether (1881)
On the Relative Motion of the Earth and the Luminiferous Ether (1887)
The Theory of Electrons and the Propagation of Light (1902)
At the end of the 19th century, when the detection (at the second order) by the Michelson Morley experience of the absolute motion “in the ether” of the Earth failed, the science was under trouble. This was the greatest missing experiment ever.

The wikipedia article 'Special Relativity' says: Instead of providing insight into the properties of the aether, Michelson and Morley's article in the American Journal of Science reported the measurement to be as small as one-fortieth of the expected displacement but "since the displacement is proportional to the square of the velocity" they concluded that the measured velocity was "probably less than one-sixth" of the expected velocity of the Earth's motion in orbit and "certainly less than one-fourth." Although this small "velocity" was measured, it was considered far too small to be used as evidence of speed relative to the aether, and it was later said to be within the range of an experimental error that would allow the speed to actually be zero. Though Kennedy later also carried out an experiment at Mount Wilson, finding 1/10 the drift measured by Miller, and no seasonal effects, Miller's findings were considered important at the time, and were discussed by Michelson, Lorentz and others at a meeting reported in 1928. There was general agreement that more experimentation was needed to check Miller's results. Lorentz recognised that the results, whatever their cause, did not quite tally with either his or Einstein's versions of special relativity. Einstein was not present at the meeting and felt the results could be dismissed as experimental error. To date, no-one has been able to replicate Miller's results, and modern experimental accuracies are considered to have ruled them out.
Note: Poincare was not mentioned here. Note also the Gruisenick experiment 1, 2, that found differencies, still unconfirmed (Miller-type?). Not mentioned in the modern laser experiments either.

In History of special relativity Poincare was a central name.
Poincare (1895, 1900a) argued that experiments like that of Michelson-Morley show the impossibility of detecting the absolute motion of matter, i.e., the relative motion of matter in relation to the aether. He called this the "principle of relative motion." In the same year he interpreted Lorentz's local time as the result of a synchronization procedure based on light signals.
He assumed that 2 observers A and B, which are moving in the aether, synchronize their clocks by optical signals. Since they believe themselves to be at rest, they must consider only the transmission time of the signals and then cross-reference their observations to examine whether their clocks are synchronous. However, from the point of view of an observer at rest in the aether, the clocks are not synchronous and indicate the local time
\scriptstyle{t'=t-{vx}/{c^2}}. But because the moving observers do not know anything about their movement, they do not recognize this. So, contrary to Lorentz, Poincaré-defined local time can be measured and indicated by clocks. Therefore, in his recommendation of Lorentz for the Nobel Prize in 1902, Poincaré argued that Lorentz has convincingly explained the negative outcome of the aether drift experiments by inventing the "diminished time", i.e. that two events at different place could appear as simultaneous, although they are not simultaneous in reality.

This reminds me of the neutrino faster than light - speed. A new paradigm shift too?

The constancy of the speed of light was postulated by Albert Einstein in 1905, motivated by Maxwell's theory of electromagnetism and the lack of evidence for the luminiferous ether but not, contrary to widespread belief, by the null result of the Michelson–Morley experiment. However the null result of the Michelson–Morley experiment helped the notion of the constancy of the speed of light gain widespread and rapid acceptance.
"Test Light Speed in Mile Long Vacuum Tube." Popular Science Monthly, September 1930, p. 17-18.

No Nobel for Relativity.
When Albert Einstein got the Nobel Prize, no mention of relativity was made : The Nobel Prize in Physics 1921 was awarded to Albert Einstein "for his services to Theoretical Physics, and especially for his discovery of the law of the photoelectric effect".

Actually, a Nobel Prize for special relativity (SR) could well have been awarded already in the period 1905-1910. But then, it would have been impossible to ignore the role of Henri Poincaré. Who was against a Nobel Prize including Poincaré? He was not only "a mathematician" ("not a physicist"), as seen by some, but also the first cousin of the French politician Raymond Poincaré, who in 1913 became the President of the French Republic.

Poincare versus Einstein by Roger J Anderton, 2010: Poincare was working on the same ideas as Einstein. Poincare’s theory came before Einstein’s theory, and is a more general theory than Einstein’s theory. There are similarities and differences between Einstein’s SR with Poincare’s theory. Poincare’s theory is just Newtonian physics.
Jaques Fric: “[Poincare] set up all the basic concepts of SR, several years before Einstein did in his the famous paper.

As is well known Einstein did not cite references in his famous paper.


At least the Relativity principle as well as the method for synchronizing clocks are borrowed from Poincaré published papers (1898-1902). This should explain why Einstein was not awarded the Nobel Prize for the Relativity, but for the photo-electric effect!i.e. there was dispute over whose theory it was!

The ether, time, speed of light - and invariance.
In 1895 Lorentz
suggested that moving bodies should experience a “physical” contraction, compute what it would be in accordance to the Michelson Morley experience and set up a theory on this basis.

Length Contraction (wikipedia): Not only the electrostatic fields, but also the molecular forces are affected in such a way that the dimension of a body in the line of motion is less by the value v2 / (2c2) than the dimension perpendicularly to the line of motion. However, an observer co-moving with the earth would not notice this contraction, because all other instruments contract at the same ratio. In 1895 Lorentz proposed three possible explanation for this relative contraction:
  • The body contracts in the line of motion and preserves its dimension perpendicularly to it.
  • The dimension of the body remains the same in the line of motion, but it expands perpendicularly to it.
  • The body contracts in the line of motion, and expands at the same time perpendicularly to it.
Although the possible connection between electrostatic and intermolecular forces was used by Lorentz as a plausibility argument, the contraction hypothesis was soon considered as purely ad hoc. It is also important that this contraction only affected the space between the electron but not the electrons themselves, therefore the name "intermolecular hypotheses" was sometimes used of this effect. The so called Length contraction without expansion perpendicularly to the line of motion and by the precise value l=l_0 \cdot \sqrt{1- v^2 / c^2} (where l0 is the length at rest in the ether) was given by Larmor in 1897 and by Lorentz in 1904. In the same year Lorentz also argued that also electrons themselves are affected by this contraction. For further development of this concept, see the section Lorentz transformation.

Poincare: “ I am not satisfied with the explanation (physical contraction) of the negative result of the Michelson experiment by the Lorentz theory, I would say that the laws of optics are only depending on the relative motion of the involved bodies”.


A number of ordinary mechanical quantities take on a different form as the speed approaches the speed of light. At what energies is a particle relativistic? See the equations. The relativistic kinetic energy, the relativistic momentum, the exact expression for pc in terms of kinetic energy, and the photon energy expression E = hc/l = pc when the rest mass energy is negligible compared to the kinetic energy.

Poincaré did not accept the ad hoc "length contraction" hypothesis by FitzGerald and Lorentz. It led to a friendly controversy with Lorentz , mainly about the concept of absolute Space and absolute Time, brought forth by Mach. Poincare emphasised that the Lorentz contraction was just made for adjusting the theory to the experience. Lorentz reported this point of view of Poincaré, in his theory of electromagnetism (1904). “Poincaré has objected to the existing theory of electric and optical phenomena in moving bodies that, in order to explain Michelson’s negative result, the introduction of a new hypothesis has been required, and that the same necessity may occur each time new facts will be brought to light. Surely this course of inventing special hypotheses for each new experimental result is somewhat artificial. It would be more satisfactory if it were possible to show by means of certain assumptions and without neglecting terms of one order of magnitude or another, that many electromagnetic actions are entirely independent of the motion of the system…..”
Can the Lorentz - Fitzgerald Contraction Hypothesis be Real? (2005?).
After rejecting the reality of ether, the relativistic length contraction in SRT was no longer the result of certain forces (real or fictitious), and didn’t need any additional propositions concerning the structure of matter or the nature of the ether. In short, relativistic length contraction became a kinematics effect. The textbook methods for studying the well-known examples in electrodynamics are based on two hypotheses: the Lorentz-Fitzgerald contraction, and the relativistic length contraction. Given that the Lorentz-Fitzgerald contraction was an ad-hoc and theoretically unproven concept, so might the method given in this work be considered which provides some theoretical justification. Thus, regardless of whatever else one may believe about relativistic length contraction, we are led to believe that the Lorentz-Fitzgerald contraction is real.
History of SR: Lange (1885) was the first to coin the expression inertial frame of reference and inertial time scale as operational replacements for absolute space and time, by defining "a reference frame in which a mass point thrown from the same point in three different (non co-planar) directions follows rectilinear paths each time it is thrown is called a inertial frame".

And in 1902, Henri Poincaré published the philosophical and popular-science book "Science and Hypothesis", which included: philosophical assessments on the relativity of space, time, and simultaneity; the opinion that a violation of the Relativity Principle can never be detected; the possible non-existence of the aether but also some arguments supporting the aether; many remarks on non-Euclidean geometry. Poincaré devoted a full chapter to the relativity principle:
“There is no absolute uniform motion, no physical experience can therefore detect any inertial motion (no force felt), there is no absolute time, saying that two events have the same duration is conventional, as well as saying they are simultaneous is purely conventional as they occur in different places.” One can still keep in mind the concept of ether, if it helps for thinking, but it is a unphysical concept, it is a metaphysical concept.

Poincare points out that the “form” of the Lorentz formulae can be demonstrated from the Relativity principle alone, and therefore are implied by this principle alone (with a parameter to specify, related to “c” for the SR), only one hypothesis is required, instead of the local time and the associated three new hypothesis of the article of Lorentz (1904). In The Principles of Mathematical Physics (1904), Poincaré drew some consequences from Lorentz's theory and defined (in modification of Galileo's Relativity Principle and Lorentz's Theorem of Corresponding States) the following principle: "The Principle of Relativity, according to which the laws of physical phenomena must be the same for a stationary observer as for one carried along in a uniform motion of translation, so that we have no means, and can have none, of determining whether or not we are being carried along in such a motion." He also specified his clock synchronization method and explained the possibility of a "new method" or "new mechanics", in which no velocity can surpass that of light for all observers. However, he critically noted that the Relativity Principle, Newton's action and reaction, the Conservation of Mass, and the Conservation of Energy are not fully established and are even threatened by some experiments (prefiguring Noether theorem: 1915).

Cohn illustrated (like Joseph Larmor in the same year) this Lorentz transformation by using rods and clocks: If they are at rest in the aether, they indicate the true length and time, and if they are moving, they indicate contracted and dilated values. Like Poincaré, Cohn defined local time as the time, which is based on the assumption of isotropic propagation of light. Contrary to Lorentz and Poincaré it was noticed by Cohn, that within Lorentz's theory the separation of "real" and "apparent" coordinates is artificial, because no experiment can distinguish between them.

Henri Poincaré (1898) in his paper The Measure of Time drew some important consequences of this process and explained that astronomers, in determining the speed of light, simply assume that light has a constant speed, and that this speed is the same in all directions. Without this postulate it would be impossible to infer the speed of light from astronomical observations, as Rømer did based on observations of the moons of Jupiter. Poincaré also noted that the propagation speed of light can be (and in practice often is) used to define simultaneity between spatially separate events. He concluded by saying, that "The simultaneity of two events, or the order of their succession, the equality of two durations, are to be so defined that the enunciation of the natural laws may be as simple as possible. In other words, all these rules, all these definitions are only the fruit of an unconscious opportunism."

Lorentz argued that there exists only electromagnetic mass, not mechanical mass, and derived the correct expression for longitudinal and transverse mass. And using the electromagnetic momentum, he could explain the negative result of the Trouton-Noble experiment, in which a charged parallel-plate capacitor moving through the aether should orient itself perpendicular to the motion. Also the Experiments of Rayleigh and Brace could be explained. Another important step was the postulate that the Lorentz Transformation has to be valid for non-electrical forces as well.

Wien (1903) recognized an important consequence of the velocity dependence of mass. He argued that superluminal velocities were impossible, because that would require an infinite amount of energy — the same was already noted by Thomson (1893) and Searle (1897). And in June 1904, after he had read Lorentz's 1904 paper, he noticed the same in relation to length contraction, because at superluminal velocities the factor
\scriptstyle{\sqrt{1-{v^2}/{c^2}}} becomes imaginary.


The fringe-shift effect (used today in laser gyroscopes) found in M-M exp. as described in wikipedia SR article. (Note, no mention of Poincare. How could they write about this without mention of his qritique?)
The explanation was found in the
FitzGerald–Lorentz contraction, also simply called length contraction. According to this physical law all objects physically contract along the line of motion (originally thought to be relative to the aether), so while the light may indeed transit slower on that arm, it also ends up travelling a shorter distance that exactly cancels out the drift. In 1932 the Kennedy–Thorndike experiment modified the Michelson–Morley experiment by making the path lengths of the split beam unequal, with one arm being very short. In this version a change of the velocity of the earth would still result in a fringe shift except if also the predicted time dilation is correct. Once again, no effect was seen, which they presented as evidence for both length contraction and time dilation, both key effects of relativity.
Einstein derived the FitzGerald–Lorentz contraction from the relativity postulate; thus his description of special relativity was also consistent with the apparently null results of most experiments (though not, as was recognized at the 1928 meeting, with Miller's observed seasonal effects). Today special relativity is generally considered the "solution" to the Michelson–Morley null result. However, this was not universally recognized at the time. As late as 1920, Einstein himself still spoke of a different concept of ether that was not a "ponderable medium" but something of significance nonetheless.

Poincare defines the way to synchronise all the clocks of an inertial frame, by using light signals (1900: La théorie de Lorentz et le principe de réaction, J.Bosscha).

In 1904 at the St Louis conference, he proposes to add the Relativity principle to the five classical “universal” principles of the physics.

At last but not at least, In 1900, he noticed that the recoil of a radiation, of energy E, is m = E/c² [Poincaré, op.cit.t IX p 471] which is nothing else that the famous E = mc². We can see that in 1905 Poincaré, in different articles, had set up all the basic concepts of the special Relativity even though he did not summarize all of them in the framework of a formal theory as Einstein did.

I would like to draw attention to the fact that the Principle of Relativity is part of
Newtonian physics (
no, says other). It is only the addition of the idea of constancy of lightspeed that has caused the problems with thinking there is another theory SR different to Newtonian physics.
So working just from the Principle of Relativity without the lightspeed constancy, he is working within the context of Newtonian physics.

Poincaré as a mathematician had a clear formal approach of the Relativity principle. He states first that inertial frames are homogenous allowing to express each coordinate (x,t) of one frame as a linear function of the coordinates of the other frame (x’,t’) and vice versa. He had previously rotated one axis by 180 ° in order to have a full symmetrical situation. This results in four relations with eight unknown parameters. The symmetry of the situation reduces them to four and using relations leaves the equations with only one undetermined parameter, function of the relative speed. The form of this last parameter can be computed taking into account that into a group, by definition, operation by two elements is an element of the group. He never used the statement constancy of lightspeed, though. Just homogenous isotropic and anisotropic space!
Enrico Giannetto The rise of Special Relativity: Henri Poincaré’s works before Einstein, 1998: Without the absurd "length contraction" hypothesis, the Michelson-Morley experiment UNEQUIVOCALLY confirms the equation c'=c+v given by Newton's emission theory of light and showing how the speed of light varies with v, the speed of the emitter relative to the observer, and refutes the assumption that the speed of light is independent of the speed of the light source (Einstein's 1905 light postulate).

Poincares Model.
Back to Poincare's math:

x'=(x-Vt) (1-V²/K)-1/2 ; y'=y ; z'=z

t'=[(t-(Vx/K)] (1-V²/K)-1/2

V is the relative velocity of the two frames and K is a parameter having the dimension of a square of a speed which, is the maximum possible value of V (to keep the equation real) . Whether K = c², we recognize the Lorentz equations, whether K = infinity, it is Newton.

The interesting thing is that each value of K (continuous parameter) defines a continuous family (with a group structure) of inertial frames.

Poincaré understood that such Relativity principle reflects symmetry properties of the physical laws: invariance of physical laws under a group of transformations: the Poincaré group, including three spatial rotations, three hyperbolic rotations (boosts) and four translations, conferring to the Minkowski space (SR spacetime), the maximum possible number of symmetries : n( n+1)/2 = 10.

For d−1∈ℕ, d-dimensional Minkowski space is the Lorentzian manifold whose underlying smooth manifold is the Cartesian space ℝ d and whose pseudo-Riemannian metric is at each point the Minkowski metric. This is naturally a spacetime.
Theorem. Minkowski spacetimes is a stable? solution of the vacuum Einstein equations.
Reissner-Nordström spacetime is a generalization? What are called Einstein’s equations are the equations of motion of gravity: the Euler-Lagrange equations induced by the Einstein-Hilbert action. Einstein's vacuum fi eld equation, in analogy with Laplace vacuum field formulation of Newtonian theory can be formulated as the statement that the trace of the relativistic analogue of wave is zero. Compare to the knots again. In Synthetic Differential Geometry (SDG), the reals R have the structure of a (non-trivial) ring, not a field, and the main axiom states one of the basic insights, namely, that \in the in finitely small, every curve is a line in a unique way." This gives hidden dimensions (in 26D model) and curvature that doesn't obey ordinary laws at quantum level (in TGD). The c.c.
Gonzalo Reyes, A derivation of Einstein’s vacuum field equations (pdf)
J.K. Webb et al. 2010: Indications of a Spatial Variation of the Fine Structure Constant
He showed that the transformations are a consequence of the Principle of Least Action and developed the properties of the Poincaré stresses. He demonstrated in more detail the group characteristics of the transformation, which he called the Lorentz group, and he showed that the combination \scriptstyle{x^2+y^2+z^2-c^2t} is invariant. While elaborating his gravitational theory, he said the Lorentz transformation is merely a rotation in four-dimensional space about the origin, by introducing \scriptstyle{ct\sqrt{-1}} as a fourth imaginary coordinate.
The theory of Lorentz and the principle of reaction (1900)
Compare to the knot theory where the result also is invariant, only the path varies.

Poincare group, ISO(p,1) is the isometry group of Minkowski spacetime of dimension d+1: the group of affine transformations on ℝ 4 which preserve the Minkowski "metric". The norm of Minkowski is quadratic. The group elements are multiplied by composing maps. The Poincaré group G may also be described as a semidirect product (ℝ⊕ℝ 3)⋊O(1,3) where O(1,3), the Lorentz group, consists of all linear transformations L:ℝ 4→ℝ 4 that preserve the Minkowski inner product of signature (1,3). The Lorentz group is a 6-dimensional Lie group. It has four connected components.

This is obviously, the modern approach. Time is the 'dragging' i-factor (ether?)?


Einstein, more intuitive and sticking to physical principles, first states the two postulates: Relativity principle (borrowed to Poincaré) and constancy of light speed in all Galilean frames. Then he studies the methods for synchronizing clocks in a frame ( borrowed to Poincaré) , allowing also to define space milestones ( with the help of the constant light speed).

Then, after defining exactly the terminology, he considers a moving frame and writes the relations between the coordinates of the two frames by considering the clock synchronisation equation in the two different frames derived from the light speed constancy. The paper of Einstein is a more extensive treaty about Relativity, as in addition to the demonstration of the Lorentz formula, he considers also the cinematic, and the dynamic of the electron, it is a first synthesis about the theory of special relativity and its implications. ( E = mc² will come later in a second paper).


So, why
is the work of Poincaré in Special Relativity so ignored ?
Poincaré did not realize the revolution implied by this new theory, as he had many others topics of interest especially in mathematics. His formal (maybe too speculative) approach did not reflect the “physical reality” implied by the theory. His position on the ether remains quite ambiguous, as he did not reject definitely the concept as Einstein did (at the beginning, as later Einstein had a more ambiguous position too, ether being a “hard to kill “concept). In some following papers, he expresses some doubts about the universality of the Relativity principle. In addition, he never published a so extensive treaty as Einstein, whose approach was more physical, more practical, closer to the physical reality [for that time]...

Poincare was shy. He let other become famous in his place, as Fuchs, Lorentz, maybe Einstein...
Einstein was young, bold, unknown at that time, and therefore took over the whole thing.


Einstein has always denied to have known Poincaré publications. It’s hard to believe as his friends Maurice Solovine and Carl Seelig, report Einstein had read the Poincaré book “La Science et l'hypothèse” (no absolute time, no absolute space, no ether ... ) around 1902-1904. This book was commented at their reading commitee « Académie Olympia » during several weeks (ref. 8, pages 129 et 139 ; ref. 9, page VIII and ref. 17, page 30). His position at the Swiss office patent in charge of “electromagnetism” implied that part of his job was to read and summarize the main publications on this topic (he summarized several papers from the French “Academie des sciences”).

At the end of his life, Einstein wrote in 1955 in a letter to Carl Seelig: «There is no doubt, if we look back to the development of the Relativity theory, special Relativity was about to be discovered in 1905. Lorentz already noticed that the transformations (named Lorentz transformations) were essential in the Maxwell theory and Poincaré had gone even further. At that time I only knew Lorentz work of 1895, but I knew neither Lorentz nor Poincaré further work. This why I can say that my work of 1905 was independent » (ref 8, page 11).

Anyway, Einstein had a different approach, he popularised the Special Relativity, and developed “ alone” the General Relativity ( even though Hilbert derived the field equation of GR a few days before Einstein, but by using Einstein work so the equation was rightly attributed to Einstein) .

When the Nobel Committee decided to award Einstein the price, Lorentz, who was a member, objected that it was Poincaré who had found the full group of transformations of the SR, and it would be unfair not to associate him. But as Poincaré was dead at that time, Einstein was awarded the Nobel price for his work on the photo electric effect: That’s diplomacy…

Poincare and gravity.
Pentcho Valev: Look at the formulae used by Poincaré in his articles : Poincaré had already formulated special relativity before Einstein, and was already considering the possibility to extend it to gravity (where Einstein was struck for the rest of his life). There had also been the contribution by Lorentz - precisely the relativity principle that Poincaré formulated as early as 1895.

H. Poincaré appreciated Einstein's efforts on explaining popularly the principle of relativity but he called it a "mechanics of Lorentz'" because it was H.Lorentz who, step by step, was approaching this new physical description basing on experimental data. In addition, apart from playing with (x,t), there were equations of motion with severe problems (self-action, radiation resistance) not resolved even today.

Poincaré supported 1905 the Lorentz transformation against an alternative theory by Langevin. He also pointed out that the gravitational interaction had to travel at the speed of light, and even spoke about "gravitational waves". Perhaps people around Langevin did not like Poincaré's attitude. In any case, he was forced to send to the Circolo Matematico di Palermo his long paper "Sur la dynamique de l'électron", and this delayed its publication.
On the Dynamics of the Electron (1906)
Mayeul Arminjon: Lorentz-Poincaré relativity and a scalar theory of gravitation (2007?)
Poincaré's version of the relativity principle was different from Einstein's (1905), indeed Poincaré's version (1904) was this: "The laws of physical phenomenons must be the same, whether for a fixed observer, as also for one dragged in a motion of uniform translation, so that we do not and cannot have any mean to discern whether or not we are dragged in a such motion." This formulation does not preclude in any way the possibility that there might be an absolute meaning to the words "fixed" and "moving". In essential features the Poincare model gives SR too, proved by many.

Today this motion is interpreted as 70% dark energy in our universe, because of the ever increasing acceleration, oddly without ceasing energy from the vacuum.
Apart from the historical aspect, it is important for physics research to realize that the physics of special relativity was found by scientists who based their work on the concept of ether. Indeed today's physics makes it obvious that vacuum has physical properties.

14 kommentarer:

  1. http://isbnbookfinder.com/Broader-view-of-relativity-General-implications-of-Lorentz-and-Poincare-invariance/p142439/

    Broader view of relativity: General implications of Lorentz and Poincare invariance
    Hsu J.P., Hsu L. 2006.
    "A Broader View of Relativity" shows that there is still new life in old physics. The book examines the historical context and theoretical underpinnings of Einstein's theory of special relativity and describes Broad Relativity, a generalized theory of coordinate transformations between inertial reference frames that includes Einstein's special relativity as a special case. It shows how the principle of relativity is compatible with multiple concepts of physical time and how these different procedures for clock synchronization can be useful for thinking about different physical problems, including many-body systems and the development of a Lorentz-invariant thermodynamics. Broad relativity also provides new answers to old questions such as the necessity of postulating the constancy of the speed of light and the viability of Reichenbach's general concept of time. The book also draws on the idea of limiting-four-dimensional symmetry to describe coordinate transformations and the physics of particles and fields in non-inertial frames, particularly those with constant linear accelerations. This new edition expands the discussion on the role that human conventions and unit systems have played in the historical development of relativity theories and includes new results on the implications of broad relativity for clarifying the status of constants that are truly fundamental and inherent properties of our universe.

    Einstein 1905-2005. Poincare Seminar 2005
    Olivier Darrigol, Thibault Damour, Vincent Rivasseau

    From the Back Cover

    The Poincaré Seminar is held twice a year at the Institute Henri Poincaré in Paris. The goal of this seminar is to provide up-to-date information about general topics of great interest in physics. Both the theoretical and experimental results are covered, with some historical background. Particular care is devoted to the pedagogical nature of the presentation. This volume is devoted to Einstein's 1905 papers and their legacy. After a presentation of Einstein's epistemological approach to physics, and the genesis of special relativity, a centenary perspective is offered. The geometry of relativistic spacetime is explained in detail. Single photon experiments are presented, as a spectacular realization of Einstein's light quanta hypothesis. A previously unpublished lecture by Einstein, which presents an illuminating point of view on statistical physics in 1910, at the dawn of quantum mechanics, is reproduced. The volume ends with an essay on the historical, physical and mathematical aspects of Brownian motion.

    Contributing authors:

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    Henri Poincare and Relativity Theory
    A.A. Logunov, 2005.

    Science and hypothesis
    Henri Poincare, 1905
    Nontechnical essays on hypothesis in physical theory, concept of number, magnitude, force, intuition vs. logic, more. Chapters include "On the Nature of Mathematical Reasoning," "Mathematical Magnitude and Experiment," "Non-Euclidean Geometries," "Space and Geometry," "Experiment and Geometry," The Classical Mechanics," "Energy and Thermo-Dynamics," "Hypotheses in Physics," and "The Calculus of Probabilities."

    SvaraRadera
  2. Did Poincaré discover Special Relativity? December 18, 2011. http://physicsforme.wordpress.com/2011/12/18/did-poincare-discover-special-relativity/Physics4me blog,

    Emily Adlam
    Henri Poincare’s work on mathematical features of the Lorentz transformations was an important precursor to the development of special relativity.
    In this paper I compare the approaches taken by Poincare and Einstein, aiming to come to an understanding of the philosophical ideas underlying their methods.
    In section (1) I assess Poincare’s contribution, concluding that although he inspired much of the mathematical formalism of special relativity, he cannot be credited with an overall conceptual grasp of the theory.
    In section (2) I investigate the origins of the two approaches, tracing differences to a disagreement about the appropriate direction for explanation in physics;
    I also discuss implications for modern controversies regarding explanation in the philosophy of special relativity.
    Finally, in section (3) I consider the links between Poincare’s philosophy and his science, arguing that apparent inconsistencies in his attitude to special relativity can be traced back to his acceptance of a `convenience thesis’ regarding conventions…..
    Read more: http://arxiv.org/pdf Posted to arxive 14.12.

    The crucial difference between these formulations is that Poincar´e finds
    it necessary to refer to an observer, while Einstein does not.

    SvaraRadera
  3. cont.
    In contrast to Einstein, who denied the existence
    of absolute motion, Poincar´e denied the possibility to detect it.’ (2005)
    As a result Einstein’s principle leads to stronger constraints: for Einstein, there can be no difference at all between the forms of the laws of nature in different inertial frames, whereas Poincar´e can accept that the laws of nature take one form relative to a privileged frame and a more complicated form relative to all other frames, provided they work together in such a way that this difference between frames does not have any observable consequences.
    However, the importance to be attached to this distinction turns upon our understanding of what is meant by a ’law of nature.’ Poincar´e was famously a conventionalist, and therefore held a view of lawhood which may appear to make the two principles equivalent after all.

    Conclusions
    Poincar´e’s contributions to the field of special relativity were undoubtedly invaluable, but nonetheless those contributions do not constitute an independent discovery of the theory. His conceptual grasp of certain elements, particularly the Lorentz transformations, was very different to Einstein’s - and this does not constitute merely a small difference in interpretation, but a substantive disagreement about the possible applications of the transformations.
    I have suggested that the root of this conceptual difference lies in a disagreement over the appropriate direction of explanation; for Poincar´e, the relativity principle is to be explained by invoking microscopic phenomena, whereas Einstein showed that the relativity principle can be taken as basic and used to explain the form of the laws governing microscopic phenomena.
    This has important consequences for issues concerning explanation in special relativity a return to the approach of 1905 may help to resolve issues concerning the role of Minkowski spacetime in relativistic explanations.

    Finally, I have argued that Poincar´e’s choice to restrict his scientific explanations to traditional forms was related to certain conventionalist doctrines that he held, particularly the convenience thesis. This thesis led Poincar´e to maintain that science should not question the conventional framework within which it is mandated to work, and as a consequence, he was unwilling to give up the conventional framework of explanation. Therefore an explanatory approach like Einstein’s was unavailable to him and he never appreciated the interesting possibilities that arise from a willingness to explain in non-traditional ways.

    Compare also to the new 'superstar' in physics http://www.physics.uq.edu.au/download/tamarad/papers/thesis_complete.pdf

    SvaraRadera
  4. http://espacioytiempo.net/modulos/archivos/files/INCONSISTENCY%20OF%20LORENTZ%20TRANSFORMATION.pdf

    SvaraRadera
  5. http://backreaction.blogspot.com/2007/04/henri-poincar.html

    SvaraRadera
  6. http://www.jstor.org/stable/10.1086/430652
    Despite the scarcity of relevant documents, the last twenty years have brought significant progress in our understanding of Albert Einstein’s and Henri Poincaré’s contributions to relativity theory. A number of circumstances have made this possible: the authoritative edition of Einstein’s collected papers for the years 1879–1909, the discovery of the correspondence between Einstein and Mileva Marić, better knowledge of the earlier history of electrodynamics, closer analysis of Poincaré’s criticism of electrodynamics at the turn of the century, and attention to his and Einstein’s involvement in technologies of time measurement. One benefit of this progress is that we now have a more precise idea of the similarities and differences between the two thinkers’ contributions to relativity theory. Yet the historical connection between these contributions remains highly mysterious.1

    Curiosity about this connection seems legitimate, not to agitate pointless priority debates, but because our understanding of the origins of modern physics strongly depends on comparisons between Einstein’s and other theorists’ approaches to the major problems of early twentieth‐century physics. The inclination to deem Einstein’s contributions a priori singular and superior to any others has long obscured the endeavors of his contemporaries as well as the nature of his own reflections. This is especially true for relativity theory and its primary context, the electrodynamics of moving bodies. Once this sort of prejudice has been eliminated, the interesting question no longer is whether a contemporary of Einstein got it right or wrong—using Einstein as a gauge—but how the similarities and dissimilarities between his and Einstein’s approaches can be explained.

    SvaraRadera
  7. http://www.maa.org/mathland/mathtrek_11_15_99.html
    http://www.maa.org/mathland/mathtrek_8_23_99.html
    http://en.wikipedia.org/wiki/Three-body_problem

    SvaraRadera
  8. From a FB discussion:
    Phil Warnell: ‎Ulla, I'm not certain what your question is yet the main difference between Poincare and Einstein is the former believed in the existence of a fixed frame of reference while the latter did not. The truth in this case as with many tings in science still waiting to be discovered.

    Philip Gibbs: Poincare did not believe in a fixed frame of reference. That was the case for lorentz and others. Poincare understood relativity but thought that it was simpler and more appropriate to assume a fixed frame of reference by convention. It is hard to appreciate his position now but that was his philosophy. It was especially wrong for the case of curved spacetime and general relativity where he understood non-Euclidean geometry but said that a Euclidean frame could always be imposed and would be simpler.


    Emily Adlam, Poincar´e and Special Relativity. http://arxiv.org/PS_cache/arxiv/pdf/1112/1112.3175v1.pdf
    Finally, in section (3) I consider the links between Poincar´e’s philosophy and his science, arguing that apparent inconsistencies in his attitude to special relativity can be traced back to his acceptance of a ‘convenience thesis’ regarding conventions.

    SvaraRadera
  9. Dear Ulla,
    I admire your efforts a lot on introducing TGD. Certainly you take a lot of time on searching in internet and find interesting links.
    I know I can learn from you a lot not only in biological aspects of TGD but even in physics;-). (Although it is difficult to distinguish between biology and physics in TGD!)
    Postings about Poincare and Einstein or knot theory were interesting and new for me and lead to some discussion with my friend about it. I’d like to know why did you start from knots theory and then Poincare and Einstein in TGD lessons and what process do you want to continuing on the way? And when will you start TGD quantum biology in your viewpoint? (I’m very thirsty about it ;-)).

    SvaraRadera
  10. Thanks Hamed :)

    Sometimes I must admit I feel very ridiculous, when I think at me explaining physics. I am a biologist at heart.

    TGD is a beautiful theory, but there are missing something very important, a link to mainstream physics, especially the path to how TGD got the form it has. That I try to fill in. It will take a long time, when I must learn at the same time, and I have also ordinary work to do. From somewhere I must earn my money too :)

    During the years I have studied TGD I have learned that there is no way to circumwent its foundations, that is a Poincare invariant theory of gravity. I have hoped I could have someone else, more qualified doing that work, but seems I must do it myself. In my first post I outlined the necessary lessons I will do, but between them there must be the left-out material. Otherwise it will be no point in my work, and TGD will be just as good. Matti also use a hopeless language that I try to make more popular. I don't want to use words I don't know what they stand for.

    Biology is physics at ground. Not only in TGD. I am very fond of quantum biology, but it has to wait until the basement is explained. As you see in post 1 it is a long way there.

    The very basis for TGD is the trinity, which in fact is a knot (SR) at basement. From this 'knot' the Poincare invariant gravity must arise. Those two are very important. GR is also obligately necessary. So I look at Einstein and Poincare and how GR and SR got the form it has and if there could be other interpretations that lead to a TGD form of theory. I try to make this all logical, and I have many posts almost ready, but considering I handle another persons 'Work of Life' I must be cautious and careful so there is no big error and misunderstandings. Undoubtedly there will be some, and then I hope you or someone else shout, look out! I don't want to do harm.

    Glad you like it. Without feedback it is hard to figure out is it good or bad. I am also very fascinated of this all.

    SvaraRadera
  11. Thanks Ulla,
    I think when I read your first posting some Months ago, I didn’t read the part of it carefully. I wish success for you in your process, and if I know something that maybe useful for the lessons, I will comment that.
    I believe that scientists are in an incorrect way and every year they throw away billions dollars in experiments. This is a tragic disaster :(. We should fight against it cautious and patiently. I’m very glad when see I’m not alone and some people like you are in this way.
    For first time I found TGD in internet it was 2006 (I’m very thankful to GOD for that) and I was at high school. At that time my writing and reading English was very poor (in eastern countries the language isn’t as popular as western countries) And also because of hard language of TGD, it was taking very long time when I was reading only some papers about TGD, But I was very interested in. at the years when I was reading my courses of university, I tried to learn a few mathematical Prerequisites for TGD and at the same time I followed a lot of TGD postings and comments from Matti’s blog. My reading and writing improved gradually (with the help of TGD :)) and now I can communicate with Matti and you(although it is not simple for me yet).
    I hadn’t a regular study about TGD until two weeks ago. Now I’m struggling all day long with TGD :).
    If it will be possible, I’m going to choose TGD theory for subject of my MSc thesis and continue it for PhD. (I’m at first year of MSc now). I’m happy that I can learn from you (in your viewpoint) about TGD too.

    SvaraRadera
  12. Yes, it is important to realize this is my viewpoints.

    Thanks for your words. I am struggling too. Hope he would appreciate it :) And the rest of the world too.

    SvaraRadera
  13. http://www.fisica.net/relatividade/stephen_hawking_a_brief_history_of_time.pdf

    Hawkings 'A Brief History of Time'.look what he writes!

    Between 1887 and 1905 there were several attempts, most notably by the Dutch physicist Hendrik Lorentz, to explain the result of the Michelson-Morley experiment in terms of objects contracting and clocks slowing down when they moved through the ether. However, in a famous paper in 1905, a hitherto unknown clerk in the Swiss patent office, Albert Einstein, pointed out that the whole idea of an ether was unnecessary, providing one was willing to abandon the idea of absolute time. A similar point was made a few weeks later by a leading French mathematician, Henri Poincare. Einstein’s arguments were closer to physics than those of Poincare, who regarded this problem as mathematical. Einstein is usually given the credit for the new theory, but Poincare is remembered by having his name attached to an important part of it.

    Is this the way he deals with truth? What is truth?

    SvaraRadera
  14. It is not widely known that Einstein had doubts, increasing with time, about the way he formulated his special theory of relativity in 1905. Physical Relativity examines the grounds of these doubts and related misgivings on the part of a handful of physicists and philosophers in the course of the twentieth century. Harvey Brown defends an interpretation of relativity theory, and hence of the nature of space and time, that combines Einstein's insights with those of his immediate precursors, who today are widely regarded as having had the right ideas for the wrong reasons. Appearing in the centennial year of Einstein's celebrated paper on special relativity, Physical Relativity is an unusual, critical examination of Einstein's thinking that will be of great interest to philosophers of physics, physicists, and historians of science.

    http://books.google.ca/books/about/Physical_relativity.html?id=_6Dauvr3czYC&redir_esc=y Physical relativity Harvey R. Brown, 2005 and 2007.

    SvaraRadera