Farsight versus Einstein, part 2
...Let's use
the metric form posted by sol invictus. In that coordinate system, the four nonzero components of the covariant metric tensor are
[latex]
\[
\begin{align*}
g_{00} &= - (x^1 - r_0) \\
g_{11} &= \frac{1}{x^1 - r_0} \\
g_{22} &= 1 \\
g_{33} &= 1
\end{align*}
\]
[/latex]
You lost me, and everybody else.
I didn't lose anybody who understands general relativity. Not at that point, anyway.
But I lost you.
That means you never understood Einstein's equation (3), in the most important paper he ever wrote on general relativity (Die Grundlage der allgemeinen Relativitätstheorie). There are 75 numbered equations in that paper, and you got lost at equation (3).
How can that be?
You said you understood this stuff.
That means you never even came close to understanding what Einstein called "the fundamental tensor g
μν". How can that be?
You said you understood this stuff.
That means you never had a clue concerning Einstein's "ten functions" that
you've been yammering about for years. How can that be?
What does sol's metric represent again?
Flat spacetime. That question has been answered at least a dozen times now, including several answers within the past 24 hours.
All I've managed to squeeze out of him is "flat spacetime", and more recently "constant proper acceleration".
The first of those answers took me less than five minutes to prove (using a far simpler technique than calculating the Riemann tensor).
You said this is a class, but you're teaching us. Why is this stuff so much harder for you than for your students?
Look, go back to what Einstein said and think it through then contribute sensibly to the discussion instead of hiding behind mathematics.
I'm using Einstein's math. To be more specific, my
previous post used Einstein's equations (21), (23), (43), and (45), although I combined (21), (23), and (45) into a single equation and used more modern notation for both.
Why do you think Einstein's equations aren't sensible? Why do you think Einstein was hiding behind all that math?
"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".
Do you get it yet? Space isn't nothing. And you don't change space by moving through it.
I get it, all right. You must have had no idea of what Einstein meant by "ten functions (the gravitation potentials g
μν)". Here's a hint:
You got lost when I wrote four of those functions down and said the other six were zero.
You've been quoting that passage
for at least two years. Why do you continue to quote passages you don't understand?
Clinger's dollop of Emperor's New Clothes doesn't change that one bit. Care to list the terms, explain what they mean, and talk us through that maths? Never seems to happen does it?
You never seem to tell us which terms you don't understand. You don't appear to understand the terms used in
differential calculus, but it would be silly to explain freshman-level concepts to "
a cage-fighter working out toddlers". At the same time, we don't want to waste time explaining PhD-level material only to find you're still struggling with calculus.
To make it easier for us to know what kind of help you need, I'm going to ask you to answer each of the following questions. (I'm asking for the textbooks you used because some of us may own copies of those same textbooks and can refer you to the relevant sections.)
Questions for
Farsight to answer if he honestly wants us to explain the terms he doesn't understand:
- Have you taken a course in differential calculus? If so, please name the textbook you used.
- Have you taken a course in integral calculus? If so, please name the textbook you used.
- Have you taken a course in vector calculus? If so, please name the textbook you used.
- Have you taken a course in differential equations? If so, please name the textbook you used.
- Have you taken a course in linear algebra? If so, please name the textbook you used.
- Have you taken a course in general topology? If so, please name the textbook you used.
- Have you taken a course in differential geometry? If so, please name the textbook you used.
- Have you taken a course in Newtonian mechanics? If so, please name the textbook you used.
- Have you taken a course in electromagnetism that covers Maxwell's equations? If so, please name the textbook you used.
And yet he presented it as a fait accompli without explanation, and there's still no explanation of what [latex]$ds^2 = -(r-r_0) dt^2 + dr^2/(r-r_0) + dy^2 + dz^2$[/latex] represents. This is getting laughable. It's like priests in a corner desperately spouting Latin.
No, it's like physicists speaking the language Einstein spoke fluently: math.
I related the standard coordinates of flat space time to sol's. And sol is still fighting shy of explaining why his expression relates to [latex]$ds^2 = -dt^2 + dx^2 + dy^2 + dz^2$[/latex]. Talk about smoke and mirrors. Do you really think you can ignore the hard scientific evidence and what Einstein said, and get away with it by use of a mathematical smokescreen?
It is not possible to participate in a scientific discussion of what Einstein said about general relativity without discussing his math. Charlatans may pretend otherwise, but they're charlatans.
A spacetime metric that represents what, exactly? Here it is, it's like Pythagoras's theorem, we've got a spacetime interval and the usual y and z terms, but we've now got r terms. What do they represent exactly, and what real-world scenario does the overall expression describe?
It's a concrete example of Einstein's equation (3). It's a very nice example of what Einstein was talking about in his § 13, where he presents equations (45) and (46) as examples of a nonzero gravitational field in flat spacetime, and goes on to say he's going to assume those equations hold also for curved spacetime. Einstein's § 13 is one of the high points of one of the high points of 20th century physics, but you aren't going to understand what Einstein was saying until you understand equation (3).
[latex]$ds^2 = -(r-r_0) dt^2 + dr^2/(r-r_0) + dy^2 + dz^2$[/latex]
I know what a metric is.
But we still don't know what Clinger is computing the curvature of now do we? It's been weeks now, you've got nothing, and you're still trying to dismiss Einstein and scientific evidence
Yes, we've been telling you for weeks now that the metric form you wrote above describes flat spacetime. You may not know that I computed the curvature of that flat spacetime, but those of us who have some basic understanding of general relativity know that.
and defend your waterfall neverland fantasies with mathematics that you will not relate to a real-world scenario.
How can you dismiss the waterfall analogy and its real-world implications when you so obviously don't understand the mathematics? You're beginning to look a wee bit arrogant.
Who said you did? The metric is just a representation. Space is the same regardless of what metric you use. Nobody is contesting that. But that is rather the point: you have mistaken features of the metric for features of the space. And so when Sol presents you with a metric for flat spacetime which has these strange features, you can't grasp that they are only features of the metric, and of the space itself.
I think
Ziggurat meant to say "and
not of the space itself", but he's being a mite sloppy here. The metric tensor really is a feature of spacetime itself, and is independent of the coordinate system. What
Ziggurat meant to say is that the metric
form is
not a feature of spacetime itself, but depends upon the coordinate system.
With that minor terminological correction, what
Ziggurat said is entirely consistent with what Einstein wrote.
Farsight disagrees, but he's arguing with Einstein.
I don't think so Edd. One of the big problems here is that people confuse spacetime with space and think of "the metric" as space.
Nonsense. The metric tensor itself is a feature of spacetime, and is independent of coordinate systems, but what counts as space depends on the coordinate system, as does the metric form.
As can be seen from the preceding paragraph, terminology is important. Before we try to explain that terminology, we need to know more of
Farsight's mathematical background.
To conclude this part 2, I urge
Farsight to follow the advice given by
sol invictus:
Stop pretending to understand when you don't, drop the attitude, start over, and ask some basic questions, nicely. We'll help you.