On Jan 4, rotchm wrote:
> Again, your description is very ambiguous to me. I have no idea
> what you are talking about. I will assume you mean:
<<snip 1983 definition of length>>
Here is what I'm talking about:
======================================
It simply is not possible to separate OWLS
from the method of clock synchronization.
Different methods of synchronization can yield
different values of OWLS, but the standard
methods of synchronization all yield OWLS = TWLS.
Tom Roberts
The above is an excerpt from the thread
"A Proposed Experiment to test OWLS"
======================================
Einstein said that observers using the absolutely
synchronous clocks of classical physics will get
a variable one-way light speed.
[Quoting Einstein:]
"w is the required velocity of light with respect to
the carriage, and we have
w = c - v.
The velocity of propagation of a ray of light relative
to the carriage thus comes out smaller than c.
But this result comes into conflict with the principle
of relativity.... For, like every other general law of
nature, the law of the transmission of light in vacuo
must, according to the principle of relativity, be the
same for the railway carriage as reference-body as when
the rails are the body of reference."
http://www.bartleby.com/173/7.html
This is not a closing velocity because Einstein claims
that it conflicts with the principle of relativity, and
a closing velocity would not do this.
Also, no mere closing velocity could have given Einstein
a headache.
And no mere closing velocity could have caused the creation
of the theory of special relativity.
The only way to get c and c - v prior to special relativity
would be by using classical physics' absolute synchronization.
======================================
Clearly, the one-way light speed is experimentally independent of the
two-way speed.
But let's begin again using your stuff.
Observers in Inertial Frame A time a light ray's round-trip using one
clock at the origin and a mirror at the end of the trip. The round-
trip time = 2 years per the origin clock. Out of sheer desperation
(due to their lack of absolute clock synchronization), they are forced
to force the distant clock to read the time 1 year when the light ray
makes a one-way trip to it from the origin clock (which read zero when
the light ray left it).
Now let the observers in another frame (B) do the same thing.
Now let both observers compare their coordinate systems experimentally
using a single light source S, as follows:
Frame A
origin clocks start but both right-hand clocks are unstarted
[0]------------------x------------------[1yr]-->
S~>light emitted
[0]------------------x------------------[1yr]--->
Frame B
Note: A moves to the right relative to S, and B moves to the right
relative to A.
Note: It is not critical that the two distant clocks be perfectly
aligned as shown; all that matters is that the observers in each frame
have separately measured their own distance between their own clocks
to be x, as was given. (For example, x in each frame could be 1 light-
year.)
Related note: In no case does any observer in either frame measure any
distance that is not in his own frame. (No "cross-measurements" are
involved.)
Frame A A's right-hand clock starts now
--------[?]-----------x-----------[1yr]-->
S----------------------------------->light
--------------------[?]-----------x-----------[1yr]--->
Frame B B's right-hand clock still unstarted
If one wishes to have *correct* time measurements, then one must
acknowledge the simple fact that clock synchronization is not subject
to mere definition. This is because there is only ONE way to relate
clocks that will yield *correct* measurement, and that way is absolute
synchronization.
Therefore, any other clock-setting method must *conflict* with
experiment, as did Einstein's as shown by the above simple diagrams.
These diagrams show that Einstein's defined "c-invariance" directly
conflicts with experiment by invalidly having the distant clocks read
the same start time when they were in fact started at absolutely
different times. (We know that they were started at absolutely
different times because the two clock-starting events are light-like,
and such events have an absolute before and after. We are not
invoking absolute time here, only an absolute time difference between
two events.)
Both Einstein's second postulate and his definition of clock
"synchronization" are flawed because they attempt to define
synchronization. Man cannot do this. Synchronization (or
simultaneity) exists independently of man and his mere definitions.
All that man can do is attempt to correctly measure simultaneous
events (or any other events). For example, if two stars explode, then
the only way to correctly determine if they exploded simultaneously or
not is by placing two truly synchronous clocks at the clocks prior to
the explosions. This cannot be done by mere definition. The clocks
must be correctly related experimentally. No definition!