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#61
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Eric Gisse ha escrito: Juan R. wrote: Almost all textbooks on GR claim that GR reduces to NG in the linear regime. Is this true? NO because GR-textbooks are wrong in many, many, many aspects. A bold claim. Continue being true. If you read carefully the Wald you discover that in the linear regime one CANNOT derive Newtonian equation of motion, and Wald explain why one may go beyond the linear regime. In fact Wald explain why in the linear regime one obtains a = 0. I haven't been reading Wald much. Just "Spacetime and Geometry" with an occasional look at MTW. One would obtain "a=0" if one was solving the geodesic equation. But since you didn't explain further, I can only guess as to your mening. Then does GR reduces to NG in the nonlinear regime? Again NO. That is because I wasn't talking about the nonlinear regime. It is an approximation for slow moving particles, "small" amounts of mass-energy and a "weak" field which I would not expect to hold under all, most, many, or even a few circumstances. Research on the Newtonian limit follows ways very far from textbooks. Schutz, Bernard F. The Newtonian Limit (1984) Lecture Notes in Physics, 205, 367-391. In his page 368 says "there are at least two reasons why the simple textbook extractions of the newtonian limit are not rigorous" ...because its an approximation in the 3 cases I stated above, and second-order terms and higher are dropped because it is assumed they are small. Or perhaps because the extractions, as he says, are simple. "At least two reasons", but one can prove that there is no posibility for a consistent derivation of the limit (in fact Schutz approach is not correct one). That was addressed here in sci.physics.relativity and also on sci.physics.research at one basic level. Advanced stuff is addressed in article i am preparing. Why does consistancy matter? For example: MTW, to my amusement, details 6 ways to obtain Einstein's field equations. There is more than one route to which you desire, no one is more "correct" than the other. I will explain to you again. Almost all books on GR CLAIM that NG is /obtained/ in the linear regime. That is, almost all textbooks on GR claim that in the linear regime the geodesic equation reduces to Newtonian law. Textbooks 'prove' that. Is this true? NO. As explained in Wald, in the linear regime a = 0 therefore Wald proves JUST the ***contrary*** to usual textbooks. Wald claim that for obtaining Newton law one may go beyond the linear regime. I am treating to explain is that textbooks are wrong and in the same manner that Wald proves just the contrary that other textbooks -i.e. Wald proves that in the linear regime GR does NOT reduce to Newton- i am saiyng that there is other incorrections on the derivations and that GR does NOT reduces to NG. The line of reasoning is next 'detailed'. From less rigorous to more ones. At each stage are corrected the errors of previous stages. Therefore, it is proved as 'correct' at one stage can be proven *incorrect* when more rigorous treatment is done. Typical textbooks: In the linear regime one obtains Newton law Wald textbook: the 'proofs' of others textbook are WRONG because in the linear regime there is no gravitational description: a=0. The correct proof is nonlinear one. Basic literature on Newtonian limit: textbooks 'proofs' including Wald are WRONG. The nonlinear Wald proof is not correct. Derivation may be done via NC theory and specific boundary conditions. For example, Ehlërs boundaries. Those kind of approaches are usually called 'post-Newtonian' (textbook derivation is usually called 'post-Minkowskian'). More advanced literatu Ehërls and others spacetime approaches (weak-NC. strong-NC etc.) are, in rigor, wrong, theoretically flawed, and experimentally incorrect. Correct derivation can be done via aditional equations, for example using Christian restriction for curvature tensor. Juan R: Derivation via Christian restriction for curvature tensor and others similar approaches are also wrong. Etc. When one is not rigorous one claim as in John Baez webpage that "the theorem that GR reduces to NG is proven in any textbook", which is, obviously, false. You are still in the first stage. But people doing research is in the two last stages. [waka waka Carlip waka waka] All very nice, but this supposed conversation between you and Steve Carlip does not appear on any of my searching on google groups in sci.physics.* Perhaps is was only in my head. but i thought was real one. Why do you think that still today people continue publishing articles on the Newtonian limit, why question has been not solved still guy? Probably because the universe in most cases is pretty decently served by the Newtonian limit. Yes, good reply but i was refering to publications on OBTAIN the Newtonian limit instead of publications using the Newtonian limit in astronomy. Juan R. Center for CANONICAL |SCIENCE) |
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#62
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Bilge ha escrito: Can the crap. Eugene starts with the same theory. All he does is perform a unitary transform. Changing representations doesn't change any physics. I already expresed my doubts on you understanding of Eugene theory and your real capacity for evaluating it... Since Eugene already replied to you i will say nothing more Advice: please study topics a bit before claim that work of others is nonsense. Juan R. Center for CANONICAL |SCIENCE) |
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#63
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Juan R. wrote: Eric Gisse ha escrito: Juan R. wrote: Almost all textbooks on GR claim that GR reduces to NG in the linear regime. Is this true? NO because GR-textbooks are wrong in many, many, many aspects. A bold claim. Continue being true. If you read carefully the Wald you discover that in the linear regime one CANNOT derive Newtonian equation of motion, and Wald explain why one may go beyond the linear regime. In fact Wald explain why in the linear regime one obtains a = 0. I haven't been reading Wald much. Just "Spacetime and Geometry" with an occasional look at MTW. One would obtain "a=0" if one was solving the geodesic equation. But since you didn't explain further, I can only guess as to your mening. Then does GR reduces to NG in the nonlinear regime? Again NO. That is because I wasn't talking about the nonlinear regime. It is an approximation for slow moving particles, "small" amounts of mass-energy and a "weak" field which I would not expect to hold under all, most, many, or even a few circumstances. Research on the Newtonian limit follows ways very far from textbooks. Schutz, Bernard F. The Newtonian Limit (1984) Lecture Notes in Physics, 205, 367-391. In his page 368 says "there are at least two reasons why the simple textbook extractions of the newtonian limit are not rigorous" ...because its an approximation in the 3 cases I stated above, and second-order terms and higher are dropped because it is assumed they are small. Or perhaps because the extractions, as he says, are simple. "At least two reasons", but one can prove that there is no posibility for a consistent derivation of the limit (in fact Schutz approach is not correct one). That was addressed here in sci.physics.relativity and also on sci.physics.research at one basic level. Advanced stuff is addressed in article i am preparing. Why does consistancy matter? For example: MTW, to my amusement, details 6 ways to obtain Einstein's field equations. There is more than one route to which you desire, no one is more "correct" than the other. I will explain to you again. Almost all books on GR CLAIM that NG is /obtained/ in the linear regime. That is, almost all textbooks on GR claim that in the linear regime the geodesic equation reduces to Newtonian law. Textbooks 'prove' that. Is this true? NO. As explained in Wald, in the linear regime a = 0 therefore Wald proves JUST the ***contrary*** to usual textbooks. Wald claim that for obtaining Newton law one may go beyond the linear regime. I am treating to explain is that textbooks are wrong and in the same manner that Wald proves just the contrary that other textbooks -i.e. Wald proves that in the linear regime GR does NOT reduce to Newton- i am saiyng that there is other incorrections on the derivations and that GR does NOT reduces to NG. The line of reasoning is next 'detailed'. From less rigorous to more ones. At each stage are corrected the errors of previous stages. Therefore, it is proved as 'correct' at one stage can be proven *incorrect* when more rigorous treatment is done. Typical textbooks: In the linear regime one obtains Newton law Wald textbook: the 'proofs' of others textbook are WRONG because in the linear regime there is no gravitational description: a=0. The correct proof is nonlinear one. Wald obtains the correct potential and the correct definition of acceleration (a = -del*phi) on page 77. MTW and "Spacetime and Geometry" obtain the same metrics as Wald. I fail to see what you are complaining about. Basic literature on Newtonian limit: textbooks 'proofs' including Wald are WRONG. The nonlinear Wald proof is not correct. Derivation may be done via NC theory and specific boundary conditions. For example, Ehlërs boundaries. Those kind of approaches are usually called 'post-Newtonian' (textbook derivation is usually called 'post-Minkowskian'). More advanced literatu Ehërls and others spacetime approaches (weak-NC. strong-NC etc.) are, in rigor, wrong, theoretically flawed, and experimentally incorrect. Correct derivation can be done via aditional equations, for example using Christian restriction for curvature tensor. Juan R: Derivation via Christian restriction for curvature tensor and others similar approaches are also wrong. Etc. When one is not rigorous one claim as in John Baez webpage that "the theorem that GR reduces to NG is proven in any textbook", which is, obviously, false. You are still in the first stage. But people doing research is in the two last stages. [waka waka Carlip waka waka] All very nice, but this supposed conversation between you and Steve Carlip does not appear on any of my searching on google groups in sci.physics.* Perhaps is was only in my head. but i thought was real one. Why do you think that still today people continue publishing articles on the Newtonian limit, why question has been not solved still guy? Probably because the universe in most cases is pretty decently served by the Newtonian limit. Yes, good reply but i was refering to publications on OBTAIN the Newtonian limit instead of publications using the Newtonian limit in astronomy. Juan R. Center for CANONICAL |SCIENCE) |
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#64
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Eugene Stefanovich:
Bilge wrote: Think about what those mean physically. If X causes Y, then the events X and Y are time ordered. Not necessarily. X and Y can be instantaneous and still X is a cause of Y. Only because you failed to think that statement through. It should be obvious that your assertion is wrong, even for a gailiean invariant theory, in which signals can propagate arbitrarily fast, but not instantaneously in the sense you mean. [...] Do you have a proof that in Poincare invariant theories the speed of propagation of interactions is 'c'? or this is simply your belief? Do you have proof that will convince me that 1+1=2, if I refuse to accept anything anyone says? Sure, I can give such a proof, but I can't give a proof you won't reject out of hand to keep from having to admit you're entire ``discovery'' is the result of mistaking the ability to perform a unitary transform for two real degrees of freedom that didn't exist until you made the unitary transform. For example, you reject any explanation, proof or argument in which the words lagrangian, field, phase, or gauge are used as well as some I probably omitted because I don't recall all of your quirks. In short, the only point in trying to explain it to you, _again_ in a different way would be to help you add more items to your knee-jerk rejection list. If you got in a real bind trying to reject it, I expect you would just ``discover'' some new physics and then repeat the request, ad infinitum. [...] The interactions cannot propagate faster since that isn't consistent with the definition of poincare invariance or simultaneity. Not true. That's like trying to say it's possible to perform a rotation on the unit circle by more than 2\pi without going all the way around the circle. Even in a galilean universe, simultaneous events have to be separated in a way which in some sense is further than can be reached by a signal propagating at an arbitrarily large velocity. In addition, if light propagates at `c', charge is conserved. I don't see a connection between charge conservation and the speed of light. I know you don't. You've made that clear by declaring your choice to work in the coulonb gauge, physically significant due to your inability to understand a gauge transformation, and then calling the unphysical result a discovery. Wow! I never would have guessed that by choosing a non-covariant gauge, to make a noncovariant separation of the potentials into transverse, scalar and longitudinal compoenents, the result would be an equally non-covariant coordinate transformation to fix it. To phrase it in terms you really hate, you've taken the photon four- polarization and separated the transverse part into the photon and turned the longitudinal and scalar polariztions into a separate phenomenon. I don't think anyone but you is surprised by the fact that you ``dicovered'' instantaneous propagation of the interaction. The surprise is that you attributed it to new physics rather than attributing it to the physics you left out in the first place. I can easily derive a relativistically invariant theory in which charge is not conserved. So can I, but the difference between your concept of relativistically invariant and everyone else's idea of relativistically invariant, is that yours makes a mockery of the word invariant, while the theory everyone might end up with describes superconductors. In addition, your idea of ``proving'' conservation of charge amounts to declaring it to be true by fiat. I've already pointed that out more than once. [...] As a consequence, charge isn't conserved, Not related. It's amazing how every single misconception you have can be traced back to a single origin - your inability and/or unwillingness to try and grasp the idea of gauge invariance and the cascade of patches you need as a result. |
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#65
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Eugene Stefanovich:
Bilge wrote: The details are in http://arxiv.org/abs/physics/0504062 It's easy to not take me seriously, it's a bit harder to reject the proofs. But you have no such proofs. What you have proven is that any inconsistent assumptions can be glossed over by a superficial argument that asserts the existence of a physical effect due to unphysical degrees of freedom and/or attempting to bury the inconsistency in technical jargon. All you are doing is fooling yourself. Can you point to a specific place in the book where I do that? I've done that on previous occasions. Your goodwill credit is already overextended. Then we can have a meaningful discussion. Based on prior experience and an occasional glance at the threads on sci.physics.research, I doubt it. I'm fairly certain that you are immune to reason. |
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#66
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Eric Gisse ha escrito:
Wald obtains the correct potential and the correct definition of acceleration (a = -del*phi) on page 77. MTW and "Spacetime and Geometry" obtain the same metrics as Wald. I fail to see what you are complaining about. Exactly! You see page 77 of Wald and you think "equation (4.4.21) of Wald is Newtonian law". But it is NOT. I already detailed just some of most basic points on why is NOT Newtonian gravity law in both sci.physics.relativity and sci.physics.research. Since you appear unable to find the posts -including discussion with Carlip- i detail some of post next. The derivation is incorrect as i will prove AGAIN. 1) Derivation in the linear regime is WRONG. In the linear regime a=0; newer (repeat NEWER) a=-grad (Phi). In fact, you see Wald derivation and you believe because you have not revised details -see below- that derivation is correct -just as you cite the MTW- but derivation is INCORRECT. The linear regime predicts a=0 and Newtonian gravity predicts a = - grad(Phi). ***Therefore GR does not reduce to NG in the linear regime***. Usual textbooks are wrong. Then if you cannot understand an elementary derivation WHY are you doing wrong claims? Note i would be not as hard with you if you had claimed "Hey Juan R. I think that you are not correct by this and this". But you categorically claimed "you wrong" even without the most basic understanding of the topic! Again, I remember you that we are doing serious stuff, this is not string theory or general relativity, this is canonical science. If you have time you would read pag 78 of Wald: "If one stays consistently within the linear approximation, one predicts that test bodies are unaffected by gravity. Thus, in obtaining equation (4.4.21) we actualy have gone beyond the linear approximation". That is the reason why i said that Wald derivation is NON-linear, since in the strict rigorous linear regime a=0. All textbooks claiming that in the linear regime a is different from zero are wrong and simply are modifing *reality* for consistency with Newtonian law. Ok, then next Wald claims that in the non-linear regime, the derivation is already correct, but, again, that is not true. 2) Wald (4.4.21) is not Newton equation. The 'Phi' in (4.4.21) is not Newtonian potential it is a retarded LW potential. The 'a' in (4.4.21) is not Newton aceleration because 'x' is not Newtonian 'x'. Moreover 't' in (4.4.21) is not Newtonian time. What is more, (4.4.21) is not a nonrelativistic equation because it contains c in both terms left and right and this is an authentic absurdity. Non relativistic equations do not contain c. Moreover, the metric used by Wald also contains c and does not correspond with Newtonian physics. 3) Moreover functional dependence is wrong. In (4.4.21), phy = phi(x, t). In Newtonian physics, phi = phi(R(t)). Wald simply writes 'phy', without details, and then it appears that one has derived Newtonian law. 4) The fixing of the gauge of the GR phi is done via asymptotic regime. This regime is called 'island universe asumption' and it is wrong, because it is not verified by experimental data. In Christian's own words: "However, physical evidence clearly suggests that we are not living in an 'island universe' " In Penrose's own words: "universe is not 'an island of matter surrounded by emptiness'" Etc. Wald derivation is a complete nonsense. If GR is consistent, the Newtonian limit may BE the c-- infinite limit of GR. But Wald did NOT the c-- infinite limt. Wald only took the slow motion weak field limit. I repeat again that people doing research does not follow textbook wrong derivation. If you take the c-- infinite limit you discover that gravity breaks down and cannot explain Newtonian gravity. This is not so difficult to understand in the c--infinite limit there is no curvature. The metric is (1 -1 -1 -1) Therefore if GR was a consistent theory would have no gravity. Carlip has done an attempt to derive Newtonian limit on both sci.physics.resesarch and sci.physics.relativity but: i) He uses a wrong metric that forces to us to rewritte all relativity. For example, in his nonstandard approach there is no four currents and there is not four space. The EM four 'current' is a strange mixture of densities and true currents in Carlip nonstandard approach. My metric is standard, verifies all experimental data and is consistent with particle physics, special relativity and Maxwell EM. Moreover my chossing of metric is recommended by Astronomical societies. ii) Carlip takes the wrong spacetime (t, x) which looks like (t, x) in the nonrelativisitc limit. That is, Carlip think that in Newtonian physics time is a dimension which violates the most basic understanding of Newtonian physics!!! In my own spacetime (ct, x), the limit is the correct (infinite, x). The zeroth dimension of spacetime collapse, doing time as dimension a wrong concept, and this is good. One recovers time as an evolution parameter (x^0 collapses by t does NOT collapse), WHICH is the correct Newtonian concept of time. In any elementary textbook of mechanics one can verify that the state of the system is (p,q) parametrized for one single evolution parameter t called absolute Newtonian time. iii) By taking the wrong spacetime and wrong limit, Carlip obtains the functional dependence Phi(x,t) when the correct dependence in Newtonian physics is Phi(R(t)) because time is NOT a dimension in Newtonian physics and interactions are not field-theoretic ones. Moreover, there are difficulties with the use of Phi(x,t) for example violation of causality in the transition to stationary regimes, etc. My work on gravity corrects this and one obtains the correct functional dependence without lack of continuity, etc. iv) Carlip choosing of wrong spacetime and wrong metric does that he obtains a nonzero 00-connection. This is wrong. In GR, the covariant derivatives are physical derivatives, therefore in Carlip approach the only measured (physical) derivatives are covariant = usual partial ones + 00-connection. This is of course WRONG, any textbook of Newtonian mechanics explains that the correct derivatives are usual partial ones. In my own work, the 00-connection is zero therefore Newtonian derivatives are partial ones. This is correct. v) The scalar curvature in Carlip approach is R = R_00/g_00. Since he introduces the c^2 term into g_00, in the limit he obtains R -- 0. That is, in GR, gravity is spacetime curvature, even ignoring all four points of above doing Carlip derivation just wrong, one obtains that in the nonrelativistic limit the curvature of spacetime is ZERO. If A is the cause of B, then elimination of A may eliminate B. The curvature interpretation of GR is not only artificial (as proved by teleparallel gravity or FTG) is also incorrect. In my own metric, the curvature is zero as correspond to Newtonian physics. Are you heard in some textbook of Newtonian physics that spacetime, time, or space is curved? vi) In the derivation from GR one may fix the 'gauge'. Carlip uses asymptotic limit. This is again wrong. As explained by Christian, Penrose and others, the island asumptions is ***experimentally*** false. Other people, as Christian, does use of aditional equations and constraints do NOT derived from GR. There is still more points and very very sophisticated that i do not discuss with Carlip, but since he is unable to recognize difference between a Newtonian potential (R(t)) and the nonrelativistic limit of a retarded LW field (x, t), i consider unnecesary to discuss advanced stuff with him. Juan R. Center for CANONICAL |SCIENCE) |
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#67
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Eugene Stefanovich:
Eric Gisse wrote: I was simply thinking in terms of photons being the mediators of electromagnetic interactions. This often repeated statement can be easily disproved experimentally. Take a van der Graaf generator with two highly charged balls in evacuated room. There is certainly a strong electrostatic force acting between the two balls. Now try to catch any of those photons that supposedly mediate this interaction. You can fill the room with photomultipliers, photographic plates, cameras, whatever, but you will not detect a single real photon. Duh. Now that your misreprentation of a virtual photon explains why your misreprentation is wrong, try your argument again within the context of the actual theory. So, if there is something that mediates EM interaction it is not the real observable photon. Some people call this mediator "virtual photon" pointing to the fact that these "photons" cannot be directly observed. Oddly enough, the ONLY part of ``virtual photon'' that you really have an issue with is the word virtual. If you'll recall, I asked you to explain how you thought it was possible for the neutron to decay, given that the mass of the W is 83 GeV, and your reply was exactly the same as the popularized explanation of a virtual particle, i.e., the uncertainty relations permitting the short term violation of conservation of energy. After I pointed that out, you simply denied that had any connection to a virtual W. This means that there exists a substance that penetrates everywhere, effects real things, but cannot be directly observed. This looks very much like long forgotten aether. Only to you. As history showed us, physics is doing much better if such unobservable "substances" like aether or virtual photons are removed from the theory and the theory is formulated in terms of directly observable things, like real physical photons, electrons, etc. Please explain precisely how to observe a real electron. Every signal which is observed from a detector is observed through the forces produced by virtual interactions, i.e., the motion of an indicator on a meter, the chemical reactions in ones retina which propagate via more chemical reactions through the visual cortex, etc. I could claim the exact opposite with greater veracity. Give me a single example of any observation in which the final step in the observation involves any of the free particles you call real. |
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#68
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Bilge your words sound as when D'Alemembert 'proved' that Newton was
wrong. Or perhaps as when Feynman sure in public that parity violation phenomena was imposible, just after was found. I do not believe on all of Eugene theory, but he is correct in several ways. I unknow what kind of discussions were maintained in the past, but i know recent dicussion on quantum fields on sci.physics.research and nobody here provided serious stuff. Only i dislike... which is not a scientific argument. Seeing the couple of mistakes you have done here in just a few posts. I am rather skeptic you can valuate Eugene's proposal in deep. In fact, you continue to believe that instantaneous interaction, in the sense of AAAD, needs of a signal travelling faster than c and therefore violating special relativity, which is, excuseme the 'hard' words, an authentic absurdity. How can you accuse to Eugene of 'do not hear criticism of others' if you still has not replied none of questions i did to you. You have not proved that PRE article cited above is wrong. You have not write relativisitc uncertainty You have not write relativistic wave equation for an electron Etc. Juan R. Center for CANONICAL |SCIENCE) |
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#69
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In article .com,
Juan R. wrote: Gregory L. Hansen ha escrito: Quantum field theory is a theory of fields. It has a particle interpretation, but the fundamental entity is the field. Virtual particles are the expression of the field in momentum eigenstates. When momentum is transferred from the field to an electron, we say a virtual photon was exchanged. The virtual photons are the interactions that the field could be involved in, they're not an accounting of the interactions that have been completed. Precisely Weinberg begins from particles and then obtains the fields. Weinberg does not claim that the field was fundamental as many textbooks incorrectly does. However, the field approach is not posible in bounded states and this is the reason that quantum field theory is defined only for isolated particles (S-matrix). Not possible in bounded states? I'm suspicious of that claim! When you churn the Lagrangian through the Euler-Lagrange equations you get an equation of motion like the Dirac equation with electromagnetic interaction. There's nothing inherently S-matrix about it until you specialize to high energies. -- "Then they placed the ark of the Lord on the cart; along with the box containing the golden mice and the images of the hemorrhoids." -- 1 Samuel 6:11 |
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#70
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In article om,
Juan R. wrote: Gregory L. Hansen ha escrito: What effect does the 00 component of the metric have on a test particle? How does that compare with the effect of a Newtonian gravitational potential? In the weak field limit, how large, and how important, are the other components of the metric compared with the 00 component? That was addressed both here and in sci.physics.research. And I trust that you'd demonstrated an acceleration proportional to the mass of the source, and inversely proportional to the square of the distance. -- "I fart for joy and I laugh more than if I had cast my old age, as a serpent does its skin." -- Aristophanes, Peace, 421 BC |
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