spaced-out said:
ghwellsjr said:
spaced-out said:
Well, the 1st post. does not pertain to simultaneity at all, it merely says that all inertial observers must find the same general laws. And the 2nd post. says that such observers must all get c for light's speed from Point A to Point B in their respective frames, but I fail to see this happening experimentally or even how it could happen.
The 2nd postulate does not say that observers must all get c for light's speed between two points, it
defines it.
Exactly how?
If you had read the article that I referenced in post #26, you'd already know the answer to your question. Here's the process:
1) Measure the distance between the two points with your ruler.
2) Place a mirror at the second point so that a flash of light emitted from the first point will reflect back to the first point.
3) Observe the time on a clock located at the first point when a flash of light is emitted from the first point and aimed at the mirror located at the second point.
4) Observe the time on the clock when the reflection of the flash off the mirror at the second point reaches back to the first point where the clock is located.
5) Double the distance measured in step 1 and divide it by the difference between the two observed clock times from steps 3 and 4. This is the measured value of c.
6) Divide the measured value of c from step 5 into the distance measured in step 1 to get the propagation time for light to go from the first point to the second point in order to fulfill the defined propagation speed of c.
7) Replace the mirror at the second point with a second clock.
8) Observe the time on the clock located at the first point when a flash of light is emitted from the first point and aimed at the second point.
9) Observe the time on the clock located at the second point when the flash of light reaches it.
10) Subtract the observed time on the first clock from the observed time on the second clock and compare the difference to the propagation time determined in step 6.
11) If the comparison is not zero, adjust the time on the second clock to get it closer to zero and repeat steps 8, 9 and 10 until the comparison is zero.
Is that exact enough for you?
spaced-out said:
ghwellsjr said:
spaced-out said:
OTOH, any pair of clocks in any inertial frame could possibly become absolutely synch'd by sheer accident (or by monkeys pushing buttons), and yet this would not in any way violate any physical law, so said clocks won't self-destuct or destroy the universe. They are not forbidden.
What is your definition of "absolutely synch'd"? Are you going to continue to keep it a secret? How can we respond if you won't give us your view?
My def is the same as E's:
"[In classical physics] [t]he simultaneity of two definite events with reference to one inertial system involves the simultaneity of these events in reference to all [other] inertial systems. This is what is meant when we say that the time of classical physics is absolute." [Einstein's book _Relativity_, p. 149]
Here's a link to your quote (it's about three quarters of the way down in the section entitled "The Field"):
http://www.relativitybook.com/resources/Einstein_space.html
And the very next sentence is:
According to the special theory of relativity it is otherwise.
And why is it otherwise? Because classical physics doesn't comport with reality. In post #26, I asked you for your definition of time that would comport with reality and you say it's the same as what classical physics defined. Your comment that "any pair of clocks in any inertial frame could possibly become absolutely synch'd by sheer accident" is not true as Einstein points out in this article. Don't you read the whole thing or do you like taking quotes out of context? Don't you understand that in classical physics, all clocks in all inertial frames can be absolutely synch'ed, no matter what their state of motion or acceleration?
But now that we know that classical physics does not comport with reality precisely because that concept is not true. At best you could define or assert the existence of a single inertial frame in which all stationary clocks are absolutely synch'd but those clocks would not be synch'd in another inertial frame moving with respect to the original one. Do you disagree with this statement?
So if your definition of "absolutely synch'd" is the same as Einstein's, then you must realize that his definition is for the purpose of showing that it is not adequate.
Do you want to try again?
spaced-out said:
ghwellsjr said:
spaced-out said:
If you read Einstein, you will see that he merely recommended *discarding* absolutely synch'd clocks, but never said that they cannot actually exist.
I don't recall Einstein ever saying that. Could you please provide an online link and either specify the exact location in the material where he said those words and/or provide an exact quote?
"Now before the advent of the theory of relativity it had always tacitly been assumed in physics that the statement of time had an absolute significance, i.e. that it is independent of the state of motion of the body of reference. But we have just seen that this assumption is incompatible with the most natural definition of simultaneity; if we discard this assumption, then the conflict between the law of the propagation of light in vacuo and the principle of relativity (developed in Section VII) disappears."
http://www.bartleby.com/173/9.html
This quote simply affirms the previous quote--that absolutely synch'd clocks are independent of motion in classical physics. But now we know this is not true. You cannot have all clocks absolutely synch'd. Do you disagree with this statement?