Re: Principle of equivalence
- From: Eric Gisse <jowr.pi@xxxxxxxxx>
- Date: Fri, 18 Apr 2008 22:29:03 -0700 (PDT)
On Apr 18, 9:14 pm, Bryan Olson <fakeaddr...@xxxxxxxxxxx> wrote:
rbwinn wrote:
Well, in the first place, Bryan, there is no way to know for certain
what the Lorentz equations say with regard to where a clock thrown
from a moving frame of reference will hit just by saying it was thrown
from the frame of reference.
"In the first place" you posted wrong or nonsensical statements on
what the Lorentz transform predicts. In the second place, I did the
math you challenged me to do, and showed the result for which you
asked. We're not in the first place anymore, nor the second. Now you
are changing the question because the theory you do not like turned
out to work in the first place, contrary to your reporting.
So if I say that a clock is thrown from
the moving frame of reference in the opposite direction to the motion
of the frame of reference at half the velocity of the frame of
reference, then does that clock hit in S at x=0?
What a mess. I assume you mean it is thrown from the train such
that in our frame of reference S its velocity is v/2, or in S'
its velocity is -v/2.
No, I do not think so.
Did anyone say it would in that case? If so, who?
So how do you figure out where it hits in S using the Lorentz
equations?
The Lorentz transform expresses the S'coordinates of an event
as functions of the the S coordinates. In this case, we have
all the quantities relative to S, and you ask for "where it
hits in S". What's to transform?
If you want see the key bit of math showing that the Lorentz
transform supports the principle of equivalence, take the
transform's equations and solve them for x and t. The
transform expresses of x' and t' in terms of x and t; by
solving for x and t, you express them in terms of x' and t',
thus producing the inverse Lorentz transform.
--
--Bryan
No. The principle of equivalence states there is an equivalence
between uniform acceleration and gravitation - the principle you are
looking for is the principle of relativity.
.
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