That was to Markus, not pryzk.
Did I say that you said it to przyk? I just said that you stated a crackpottery, that's all. I corrected it, yet you persist.
That was to Markus, not pryzk.
Undefined said:...I read the scientific literature and understood naively that light there is "frozen" (not moving much either way) until its energy dissipates and vanishes into quantum fluctuations background. What do you disagree with exactly? You haven't said what your "falls straight out of Scwarzchilds solution EFE" explains about what is happening physically to light there, or say why it was "meaningless" to physicists to think about it and ask questions and discuss it?
Did I say that you said it to przyk? I just said that you stated a crackpottery, that's all. I corrected it, yet you persist.
It is the questions about your "correction" that remain unanswered by you. Please see my above post.
The correction explains why repeating Farsight's claims and arguing with Markus and przyk is wrong.
Unfortunately people who consider themselves to possess some degree of expertise often treat MTW as the "bible" of GR, and sometimes react emotionally when presented with contrary information and evidence.
I am confused what you are trying to say to Farsight, Marcus Hanke. I can think of at least one situation where both local proper and remote frame coordinate speed of light is practically zero. My naive understanding of the professional physics literature says the event horizon of a non-rotating black hole has a location somewhere just above it where light virtually stops moving both ways and just fades away to infinite wavelength while not moving from the spot? No observer can say there is light speed of any kind (except that part of motion vector shared with the black hole's motion through universal space surroundings overall). Where is the null geodesic for that lightwave 'frozen' there and fading to nothingness into the quantum vacuum background fluctuations energy contribution? Can anyone tell me where that fits into what you claim about light speed never being less than 'c' if in that case both proper and remote coordinate speed is effectively 'c'=zero?
First, that's not true, since the purpose of any good textbook, including MTW, is to give students a working understanding of the theory (and not merely tell them what to believe), and most students will consult more than one source when learning general relativity. (Why do you think textbooks tend to be peppered with "exercises"?) It's also not true that everyone learns general relativity from MTW. I didn't, for example. Not that there's all that much variation between textbooks anyway. Anyone who studies from MTW for example will learn pretty much the same general relativity as they would from reading Einstein's 1916 paper.
Second, I find it particularly ironic that you attack MTW since it has a section devoted to the Hamiltonian formulation of general relativity (chapter 21, around section 4). That involves an explicit splitting of spacetime into spacelike slices and is the most formally developed "separate space + time" view of general relativity that I am aware of.
Ad hominems instead of a considered response to my post #158 Markus? Tut tut. What are we to make of that?
And that when Markus gives an unsatisfactory reply, that you press your point.
Rest assured I'll get back to you on it
The speed of light is the same in all references based on experimental data.
The Shapiro delay is the experiment. If light passes between two massive bodies it travels in a straight line, and reaches the detector later than when the bodies aren't there. All local observations will of course show light moving at the speed of light, but the coordinate speed of light varies in a non-inertial reference frame.This has been addressed, I'd say, about 10 times now on this thread alone. The speed of light does not vary. The GIF does not represent what is actually happening, thus it is nonsensical, as stated. In reality light traces out null geodesics in curved space-time. No changes in speed anywhere. Yes, the light does indeed go at the same speed. You will find no experiment and no observation which will ever show light to be propagating at anything else but c. You only find curved null geodesics in curved space-time.
The Shapiro delay is the experiment. If light passes between two massive bodies it travels in a straight line, and reaches the detector later than when the bodies aren't there. All local observations will of course show light moving at the speed of light, but the coordinate speed of light varies in a non-inertial reference frame.
OnlyMe: your post #225 noted. Good stuff IMHO.
OnlyMe: your post #225 noted. Good stuff IMHO.
I am przyk. What I don't show much willingness about is stuff like "nonsense" and "meaningless" salted with ad-hominems in lieu of sincere discussion of the physics.I am disappointed that you seem reluctant to show much willingness to consider the points of view of others. One has to wonder why you find this so difficult, since merely acknowledging that someone has a certain opinion is in no way an entrapment for you.
OK.Here are my responses (again) to the three points I summarised in [POST=3067397]post #200[/POST]. Many of them I made, in even more detail, in [THREAD=105796]this[/THREAD] (starting around page 5) and subsequent threads, as well as in a PM discussion about six months ago. If you think they are unfair representations of your end conclusions, or that I have misunderstood something, then now is your opportunity to say so.
Apart from Markus. Like you said, I'm right, but Markus reacts very badly to it.Of course, this is a reference to the first few sentences in [POST=3066616]post #158[/POST]:This is the least interesting point to deal with because most physicists would see it as vacuous. To the extent you are right, you are not saying anything that anyone needs to be educated about.Farsight said:Spacetime is an abstract mathematical space in which motion does not occur because it models space at all times. You can draw world-lines in it, and you can draw them curved, but that worldline represents the motion of a body through space over time. The body doesn't actually move through spacetime. People tend to talk of "the spacetime around the Earth" and suggest that light moves through it, but that's wrong.
I beg to differ. I can hold up my hands and say look przyk, there's a space between them. In this respect space is empirical. I can also waggle my hands and say look przyk, this is motion. So motion is empirical too. These things aren't abstract. You can't show me spacetime in any similar way.Your argument "spacetime is an abstract mathematical space" is pointless because the same could be said of any mathematical notation or formalism used in physics.
Come off it, przyk. Go out into the garden later and look up at the night sky. You're gazing up at space, not spacetime. You see a shooting star, something moving through space. You don't see world-lines and light-cones. The difference is utterly testable.There is no testable difference between the "spacetime" view and the "space + time" view, and consequently no meaningful distinction as far as most physicists are concerned.
I reject that, and counter with it's simply a question of which accurately reflects the world we see. Talking of which, sit down in your chair, and take a look at your watch. See the second hand going round? You can see it moving, that's empirical. Your watch clocks up some kind of regular cyclic motion, probably that of a quartz crystal, and shows you a cumulative result that you call the time. It isn't actually measuring "the flow of time", and nor is it actually measuring "your motion along your worldline". You're just sitting in your chair.It is simply a question of which notation is the most practical or useful, and in relativistic physics the "spacetime" view and notation just better reflects certain symmetries in relativistic theories. In some cases, the difference is as minor as writing something like $$\phi(x^{\mu})$$ as opposed to $$\phi(\bar{x};\,t)$$.
Try not to use words like "silly".The next part, "[...] in which motion does not occur" is silly.
The whole point of our conversation is that they aren't. They're talking about "motion through spacetime" instead of "motion through space". They confuse spacetime with space.When a physicist talks about "motion" in the context of spacetime without further qualification, they are almost certainly referring to exactly the same type of "motion" you might in space: changing position over time.
No problem with that. We represent motion through space with a slanting worldline drawn in spacetime. Like the red streak in the stack of film frames represents the motion of the thrown ball.You even explain exactly how to describe that in the language of spacetime (with worldlines and so on). Same thing, different notation and language. That's it. A Minkowski diagram of a worldline is essentially the same thing as the distance-time graphs we make kids draw in highschool physics, except with the space and time axes inverted.
I don't. I'm just alert for people conflating space and spacetime and suggesting that light moves through the latter.The response to the rest of that passage is pretty much the same: when you read someone say something with the word "spacetime" in it, don't simply invent the stupidest interpretation you can come up with and attribute it to that person. That's an instant strawman that serves only to derail the discussion.
You're rather putting words into my mouth with this. General relativity is laden with curvature, so the word "flat" goes against the grain. The point ought to concern that cause of curvilinear motion, which Einstein made clear. Light doesn't curve because spacetime is curved.Next point:
2) General relativity is, or can be interpreted as, a theory about flat but inhomogeneous space.
As the person claiming this, the burden of proof of course falls on you to adequately support it.
This is a straw-man, przyk. I'm not saying GR should be reformulated, I'm saying it should be understood.Specifically, you have to successfully show that general relativity can be formulated this way and, most importantly, that it actually works. However, what you offer up in support falls far short of this.
Whilst I quote Einstein, what he said isn't as important as hard scientific empirical evidence. Which we have. Optical clocks go slower where gravitational potential is lower. And those clocks don't literally measure the flow of time.Note that merely finding an instance where someone says something is not proof that the idea actually works. That pretty much disqualifies any nontechnical source you might try to use, since the point of nontechnical expositions is just that -- exposition -- and not proofs or derivations.
There's no problem with any of that. But how do we measure a distance? With a metre rod, wherein the metre is the distance travelled by light in 1/299,792,458th of a second. How do we measure a time? With our light clock.First, we get the elephant out of the way. Einstein's 1916 paper was the first complete and general formulation of Einstein's theory that was developed to the point that it could make arbitrary predictions. For some reason you cite it as supporting your case in post #158, despite the fact it is 3+1 dimensional pseudo-Riemannian geometry from beginning to end. The 3+1 dimensional "spacetime" bit is spelled out in the introductory sections that set the stage and define notations for the rest of the paper. For instance, there's a sort of preface on the first page which includes:
The generalization of the theory of relativity has been facilitated considerably by Minkowski, a mathematician who was the first one to recognize the formal equivalence of space coordinates and the time coordinate.
So there already, apparently we're getting from Einstein that Minkowski's spacetime language and formalism is really helpful for understanding and generalising relativity. The very next sentence is:
The mathematical tools that are necessary for general relativity were readily available in the "absolute differential calculus," which is based upon the research on non-Euclidean manifolds by Gauss, Riemann, and Christoffel, and which has been systematized by Ricci and Levi-Civita and has already been applied to problems of theoretical physics
Unsurprisingly, the content of Einstein's paper is pretty much what you would expect from this preface. In fact, the first several section can be read as an abridged recap of special relativity in Minkowski's notation followed by a tutorial on the methods of (pseudo) Riemannian geometry in 3+1 dimensional spacetime. Note the references to "space-time", "four-dimensional", and such language, including definitions of four-vectors, tensors, and so on. Of course, pointing out specific instances like this just amounts to a bit of quote mining, and there is no substitute for actually reading Einstein's paper and understanding why he's doing things that way (which anyone following so far is of course encouraged to do).
No problem with that. A geodesic in spacetime is a static curved worldline which relates to motion through space.That's not to say that Einstein uses the Minkowski "spacetime" language exclusively throughout the whole paper and never uses the "space + time" language, but the general pattern that emerges is that Einstein uses the "spacetime" language when he's speaking in generalities (i.e. developing the general theoretical framework), and reserves the "space + time" language for far more specific and restricted problems in the latter part of the paper, e.g. low velocity and weak field approximations that make the correspondence with Newtonian physics.
Note that the general "equation of motion" that Einstein (re)derives in this paper, which you refer to in post #158, is the geodesic equation in 3+1 dimensional spacetime given as equation (20d) in section 9 on page 168. (In Minkowski notation, Greek indices run over the four spacetime coordinates. This is more or less explicitly stated toward the end of page 155 in section 4). In [POST=2727436]this post[/POST], I also showed that the time component part of the geodesic equation was vital for the recovery of Newtonian gravity in the weak field approximation. As I also pointed out back then, a more detailed discussion of this approximation is given by Einstein in section 21 around pages 194--195.
What do you mean also? And it definitely isn't false. Go and look at the etymology: that by which anything is measured. When Einstein refers to the metrical qualities of the continuum of space-time he's talking about measurements of distance and time.Your statement that "metric is to do with measurement" is also false.
Absolutely not so. Einstein says "and is ascertainable by measurements of space and time". Lower down he says "ds² is a quantity measurable by rod-clock measurement". See the Simple Derivation of the Lorentz Transformation where Einstein says things like we suppose a light-signal sent out from the origin of K at the time t = 0.The metric components are basically the coefficients that appear in a generalised differential version of Pythagoras' theorem, and are defined and discussed on page 155. They are not defined as being measurable.
You've said nothing! In special relativity ds² is invariant because whether you sit in your chair or go on a fast out-and-back trip, the light-path-length in your parallel-mirror light clock is the same. Subtract one from the other and you get zero. And don't forget "According to this theory the metrical qualities of the continuum of space-time differ in the environment of different points of space-time, and are partly conditioned by the matter existing outside of the territory under consideration. This space-time variability of the reciprocal relations of the standards of space and time, or, perhaps, the recognition of the fact that 'empty space' in its physical relation is neither homogeneous nor isotropic, compelling us to describe its state by ten functions (the gravitation potentials gμν)..." Take your out-and-back trip through space where gμν is not constant, and I can pan with my gendaken telescope watching your parallel-mirror light clock, and plot a curvature that you don't detect locally.It is clear from the definition in equation (3) and surrounding discussion that they are coordinate-dependent: pick an arbitrary coordinate system, then $$\mathrm{d}s^{2}$$ is an invariant and the $$g_{\mu\nu}$$s are just whatever they need to be in that coordinate system such that $$\mathrm{d}s^{2} \,=\, g_{\mu\nu} \mathrm{d}x^{\mu} \mathrm{d}x^{\nu}$$. In particular, this implies that the metric components transform according to
$$g'_{\alpha\beta} \,=\, \frac{\partial x^{\mu}}{\partial x'^{\alpha}} \, \frac{\partial x^{\nu}}{\partial x'^{\beta}} \, g_{\mu\nu} \,.$$
This is a special case of the (covariant) rank 2 tensor component transformation rule given in equation (11) on page 159.
So then what? Honestly as far as your case goes, that's pretty much it, really.
Not good enough. He wrote material both before and after, and you haven't made anything like a convincing case to refute my post #158.Of the various sources you cited, Einstein's 1916 paper is by far the most important for two reasons: 1) it is the only one that defines general relativity formally and precisely enough that predictions can be derived from it (which he does for certain specific circumstances in all the gory details), and 2) being a technical paper it is addressed primarily at physicists who needed to fully understand his work. This is how Einstein wanted his scientific peers to understand his theory.
That's a weak argument. It's saying you must be wrong because we can't be, and it's saying "die Ausbreitungs-geschwindigkeit des Lichtes mit dem Orte variiert must be wrong because we can't be." Or more succinctly "Einstein was wrong because we can't be". He said what he said. He referred to the variable speed of light time and time again. The underlying problem is the "paradigm shift" that occurred in the "Golden Age" of general relativity which threw away Einstein's variable speed of light and his inhomogeneous space. It comes with Einstein didn't mean what he said, he meant what we say he meant.Your case is undermined by the absence of any paper by Einstein or anyone else establishing a formal equivalence between the 3+1 dimensional Riemannian geometry and an alternative formulation that is based around some idea of inhomogeneous space. The best evidence you have is that some Chinese researchers had a shot at it in 2008. (!) I thought I already made this point as clearly as possible at the conclusion of [POST=3051334]this post[/POST]:
If there is an alternative version of GR, why isn't there a complete treatise on it in the literature, say something analogous to Einstein's 1916 paper?
You said In this theory, curvature of space-time is not synonymous with inhomogeneity of space, as shown by the FRW solutions. The FLRW metric starts with the assumption of homogeneity and isotropy of space, which absolutely contradicts Einstein. Again it's Einstein was wrong because we can't be, and nothing else.(I [POST=2707463]previously responded[/POST] with regard to the Chinese Physics Letters paper too, by the way.)
I do. Extension of the postulate. Observable fact of experience. Law of causality. Laws of motion conditioned by distant masses. Not laws of curved spacetime conditioned by distant masses. Take a look at the bottom of page 150. It will also be obvious that the principle of the constancy of the velocity of light in vacuo must be modified. The word was Geschwindigkeit. And the principle, the postulate, was the constant speed of light.przyk said:Of course, you're thinking about the Leyden address, which finally brings us to the last point:
3) Albert Einstein was personally a proponent of point #2.
As explained above, and many times to you before, you won't find anything to back this up in Einstein's 1916 paper.
It does. As does A curvature of light can only occur when the speed of light varies with position. It veers, przyk. It doesn't curve because it moves through curved spacetime. lt moves through space, and space isn't curved. It's inhomogeneous. Read what the guy said.przyk said:Instead, you offer what seems to be one of your all-time favourite Einstein quotes, from the 1920 Leyden address:
According to this theory the metrical qualities of the continuum of space-time differ in the environment of different points of space-time, and are partly conditioned by the matter existing outside of the territory under consideration. This space-time variability of the reciprocal relations of the standards of space and time, or, perhaps, the recognition of the fact that "empty space" in its physical relation is neither homogeneous nor isotropic, compelling us to describe its state by ten functions (the gravitation potentials gμν), has, I think, finally disposed of the view that space is physically empty.
from which you somehow jump to "Space is inhomogeneous, not curved." But the part you bolded doesn't support that.
No! He said spacetime in the previous sentence. Now he says space. Not spacetime. Spot the difference!przyk said:First, it merely states that "empty space" is inhomogeneous, which is not controversial (e.g. the geometry or curvature of spacetime within the solar system is inhomogeneous).
What dichotomy? Inhomogeneous space is (nearly) equivalent to curved spacetime. Light moves through the former, and its motion is modelled using the latter.przyk said:You don't explain where you get this dichotomy between inhomogeneity and curvature -- that's not in your quote.
Yes. Did you notice metrical qualities? That's measurement qualities. You measure seconds and metres via the motion of light. And did you notice space as opposed to space-time?przyk said:And since we're happily quote mining, did you notice the bits I highlighted in red for you?
Noooooooo! The whole passage amounts to spacetime being n abstract "continuum" of measurements made using light moving through inhomogeneous space. The motion of light defines the standards of space and time, and gμν describes the state of space. The space that light moves through.przyk said:The whole passage basically amounts to arguing that spacetime should be viewed as having properties.
I've got more than that pryzk. I've got Shapiro, and GPS, and optical clocks, and the parallel-mirror gif. And all this:przyk said:That is entirely consistent with Einstein's 1916 paper, and there is no indication that Einstein is recanting anything from his original formulation of the theory. Once again, I point out that there is no article by Einstein formally establishing a version or interpretation of general relativity specifically based around inhomogeneity of space. All you have are a few isolated quotes mined from various places.