Re: SR cannot determine Contraction
- From: "rotchm@xxxxxxxxx" <rotchm@xxxxxxxxx>
- Date: Sun, 17 Feb 2008 07:44:10 -0800 (PST)
On Feb 17, 1:55 am, Peri of Pera <rie...@xxxxxxxxxxx> wrote:
SR cannot determine Contraction
Lorentz proposed contraction of moving objects in a paper 'The
relative motion of the earth and the ether', Versl.Kon.Akad.Wetensch.
1, 74 in 1892 and then published the Lorentz transformation formulas
in 1899 according to which objects moving through space contract
parallel to the direction of motion and in proportion to their speed
[L'=L/sqrt(1-v^2/c^2)].
Is it not L *times* sqrt(...) ?
Einstein accepted the formulas but writes in
1916 (Relativity: The Special and General Theory, Chapter 16): "The
contraction of moving bodies follows from the two fundamental
principles of the theory".
The real value of v in the formula is indeterminate i.e. the real
speed of a body is unknown.
Correct. The "v" in Lorentz work represents the "true" speed, the
speed relative to the ether (frame). As was well known since 1900,
this speed had (and has) no way to be determined and standard optical
and kinematical setups will not be able to detect it.
However, the speed relative to other
bodies may be known.
Do you mean "true" speed or *measured* speed? The true speed can not
be determined. The measured speed ( the now usual procedure-defined
speed) can be found (measured).
If body A moves relative to body B with a speed
of 200000km/sec,
You mean *measured* speed... ?
body A is seen by observers
Not "seen" but *measured* ?
on B to contract by L/sqrt(1-200000km/sec^2/c^2) and
Dont you mean L TIMES sqrt(...) ?
if body A moves at the same time
relative to body C with a speed of 100000km/sec it is seen
You mean *measured* ?
by observers on C to contract by L/sqrt(1-100000km/sec^2/c^2).
Dont you mean L TIMES sqrt(...) ?
Conclusion: SR is useless. It does not tell us anything about the
state and condition of A, B or C but gives in every instance an
incorrect amount of the contraction of body A.
Peter Riedt
Its calculations (predictions) correctly predict experiments; is that
not useful?
.
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