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Simultaneity
in Special Relativity - 2
by
Ardeshir
Mehta
Ottawa, Canada
Thursday, October
25, 2001
Relativity claims
that if two events are simultaneous in an inertial frame of reference,
then they cannot be simultaneous in another inertial frame of reference
which is moving uniformly and rectilinearly at a velocity v relative
to the first inertial frame of reference.
But if the Lorentz
transformation equations are correct, this claim results in a clear contradiction,
as follows:
-
Let there be an inertial
frame of reference -- which we shall designate as I -- in which
there are two clocks C1 and C2, separated
from one another spatially, and synchronised: so that whenever the
clock C1 indicates a moment in time t1,
the other indicates a moment in time t2 such that t1
= t2 = t.
-
Let there be another
inertial frame of reference -- which we shall designate as I' --
also moving rectilinearly and uniformly at a velocity v relative
to I, in which there are two more spatially separated clocks C'1
and C'2, which are also synchronised: that is,
whenever the clock C'1 indicates a moment t' coinciding
with the moment t indicated by the clock C1, the
clock C'2 also indicates the same moment t'
indicated by the clock C'1.
-
Now when the clock C1
indicates any particular moment t1, the moment t1
must be related to the moment t'1 indicated by the clock
C'1
by the Lorentz transformation equation
t'1
= (t-vx/c2)/(1-v2/c2)0.5
... where x
is the distance, as measured by an observer in I, between clock
C1
and clock C'1, and the moment t = t1
is that indicated by the clock C1 ... and c is
of course the speed of light.
-
So when C1
and C2 both indicate a particular moment t = t1
= t2, C'1 indicates a particular moment
t'1.
-
And when the clock C2
indicates the same moment t2 = t = t1 as is
indicated by Clock C1, the moment t2
must be related to the moment t'2 indicated by the clock
C'2
by the Lorentz transformation equation
t'2
= (t-vy/c2)/(1-v2/c2)0.5
... where y
is the distance, as measured by an observer in I, between clock
C2
and clock C'2, and the moment t is, again,
that indicated by the clock C2 ... and c is again
the speed of light.
-
So when the clocks C1
and C2 both simultaneously indicate a particular
moment t = t1 = t2, the clock C'2
indicates a particular moment t'2.
-
Now unless x = y
above -- which is highly unlikely, though of course not impossible -- it
is clear that t'1 will not be equal to t'2
above: both of them being indicated, of course, when both the clocks C1
and C2 indicate the single moment in time t
= t1 = t2.
-
But this contradicts
Point No. 2. above, according to which whenever C'1 indicates
any particular moment t', C'2 must also
indicate the same moment t', since both C'1
and C'2 are synchronised.
Or expressed
in table form:
According to Point
No. 2, when:
|
C1
indicates
|
C2
indicates
|
C'1
indicates
|
C'2
indicates
|
Such that
|
|
t1
= t2 = t
|
t2
= t1 = t
|
t'1
|
t'2
|
t'1
= t'2
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According to Points
Nos. 3, 5 and 7, when:
|
C1
indicates
|
C2
indicates
|
C'1
indicates
|
C'2
indicates
|
Such that
|
|
t1
= t2 = t
|
t2
= t1 = t
|
t'1
|
t'2
|
t'1
=/= t'2 *
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It is of course abundantly
clear that the above two tables contradict one another in their fifth columns.
Any comments? e-mail
me.
* At
least, not necessarily.
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