Re: Why TWLS=OWLS=c in any ONE Frame.
- From: "Paul B. Andersen" <paul.b.andersen@xxxxxxxxxxxxxxxx>
- Date: Tue, 31 Jan 2006 23:28:05 +0100
Henri Wilson wrote:
A____________L______________B
A and B are two observers equipped with light sources and clocks, at each end
of a long rigid rod of length L. Because the clocks are at mutually at rest,
the clock rates can be absolutely synched.
When A's clock reads 0.000000000000, A sends a light pulse towards B. Its speed is 'c' relative to A, and therefore also 'c' relative to B. Its travel time is L/c (but at this stage we don't know the value of c).
When the pulse arrives, B instantly adjusts his own clock to 0.0000000000000 and immediately sends a return pulse towards A. It travels at 'c' wrt B and therefore also 'c' wrt A. Its travel time is also L/c (but at this stage we still don't know the value of c).
This is sufficient to demonstrate that tAB=tBA. They are both numerically equal to L/c. Only an aethrist would disagree.
Next, A reads his clock when B's pulse arrives. It reads x.yxyeycjfmflfldfdgdkg.
This reading, 't', is light's total travel time from A to B and back again to A. From this A calculates c as being 2L/t.
Note: A can replace B with a mirror and do the same thing, knowing that the travel times in each direction must be the same.
To synch the clocks A and B according to Einstein, B simply adjusts his current clock reading upwards by (x.yxyeycjfmflfldfdgdkg)/2.
Now, if A sends a pulse to B at time To, B receives it at (To+L/c), at which instant A's clock must also read exactly (To+L/c).
If B sends a pulse towards A at time T1, A receives it at (T1+L/c), at which instant B's clock must also read exactly (T1+L/c)
The clocks are now 'absolutely' synched.
Where did the 'absolute' come from? What does it mean?
Paul .
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