---
'outandbeyond2004' wrote:
"Put a one-meter stick on the table top. Put one unstarted clock at
one end and the other at the other end. Nah, won't do. We need to
start the clocks and make sure they are well synchronized. Then put
one clock at one end and the other clock at the other end. We can
design read-outs so that any observer standing in front of the table
and equidistant from the clocks can monitor them to ensure that they
are synchronized throughout the measurement process."
MM replies:
You did not tell us how the clocks are to be synchronized, and your
midpoint observer cannot verify correct synchronization unless he can
prove that he is not moving either toward or away from the light rays
from the clocks' readouts.
(To see that he may be moving wrt the light signals, simply add
a light source at each clock beside its readout, with the light
sources' frame moving wrt the clocks' frame, and let each source
emit light rays simultaneously with its nearby readout. This makes
it clear that only one frame out of an infinity of frames will
remain at rest relative to these sources, which in turn means that
only one frame out of an infinity of frames will remain at rest
in relation to the sources' light signals, which in turn means
that only one frame out of an infinity of them will remain at
rest in relation to the clock readouts' light signals. Bear in
mind that light's source independency guarantees us that the
light rays from a clock readout and a nearby light source will
travel together as if they were one ray.)
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'Hurkyl' noted:
"Sounds like you've already decided SR is wrong; I doubt any argument
or experiment, no matter how sound, could convince you otherwise."
MM replies:
Try me.
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'outandbeyond2004' noted:
"I have been trying to think of a reason why it is necessary to
specify that the clocks be unstarted. So far, i don't see that it
is necessary."
MM replies:
This was just an initial condition, not a final one. (I mentioned
it only to make sure that the experiment started from scratch;
the experimenter must of course start the clocks at some point,
but how and when are parts of the given problem.)
'outandbeyond2004' also noted:
"Perhaps this should be explained: Either two events are simultaneous as
seen by an observer, or they are not. Einstein's point is that events seen
as simultaneous by one observer are not necessarily seen as simultaneous by
any other observer. Is this what Martin Miller meant by mere "relative simultaneity"? If so, won't he please explain, contra Einstein, why all observers can see two events as simultaneous?"
MM replies:
Yes, that is exactly what I meant by "relative simultaneity," but I can
still see that a little more explanation is necessary here. The key
questions here are (a) Since events are observer-independent, why should
observers' mere _viewpoints_ of light rays from events be involved? and
(b) What is physical cause of Einstein's relative simultaneity?
To answer the last question first, the precise physical cause of the
relativity of simultaneity is simply different frame movements in
relation to the light rays from the events. No matter how two events
may actually occur, observers in different frames who view light rays
from the events _must_ see the rays arrive differently. For example,
Frame A's observer may move toward the light from Event 1 but away
from the light from Event 2, whereas Frame B's observer may move
away from the light from Event 1 but toward the light from Event 2.
(And it should be apparent that this answer also answers the first
question.)
Of course, simultaneity would not be relative if truly or absolutely
synchronous clocks were used to time events.
As I mentioned earlier, Einstein's clocks are not synchronous. In
fact, he explicitly admitted this in his book _Relativity_. Here is
how he put it:
quote from Einstein's _Relativity_:
" But an examination of this supposition would only be possible if
we already had at our disposal the means of measuring time."
[Ref.:
http://www.bartleby.com/173/8.html]
In this brief sentence, Einstein said a lot. Since the context was
light's one-way, two-clock speed, he was admitting that he could
not correctly measure this speed. Also, he was admitting that he
could not correctly measure any other one-way speed because, as
he said, he did not possesses the means of (correctly) measuring
time. Further, he was admitting that he could not correctly
measure any two-clock times. In short, he was admitting that the
clocks of special relativity are not truly synchronous.
We do _not_ need a theory whose clocks are asynchronous.
We _do_ need synchronous clocks.
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'wisp' noted:
"Good question Martin."
MM replies:
Thanks. And as soon as its full meaning has become apparent, you will
see that it is the most important question re flat space-time physics
that can be asked.
See the following to see why no rotating clocks can yield anisotropy:
http://www.geocities.com/antirelativity/Rotating_Clock_Analysis.html
The only real test of Einstein's light postulate is a direct and
simple measurement of light's one-way speed between two same-frame
clocks which are correctly related temporally. (No rotating clocks;
no transported clocks; no asynchronous {Einsteinian} clocks.)
---
'outandbeyond2004' further noted:
"People _are_ trying to see if light speed varies from place to place;
from time to time; from direction to direction (anti-isotropy)."
"See this "Living Review" article on experimental tests of GR:"
"relativity.livingreviews.experiments"
MM replies:
I saw nothing there about correctly synchronizing clocks or correctly
measuring any one-way speeds.
Here is what one must do to prove that one's two-clock time measurements
are correct:
[1] One must prove that one's clocks are correctly related.
[2] One must prove that one's clocks are not slowed.
[3] One must prove that the rod connecting the clocks is
not contracted.
So far, no one has presented a proof of any of the above; therefore,
no one has presented a proof that even mere _relative_ speeds can
be correctly measured, such as the speed of a bug relative to a log!