Jack_
03-24-10, 04:59 PM
Assume we have two rigid body spheres of rest radius r in relative motion v along the x-axis. O is the stationary sphere and O' is the moving sphere. The moving sphere has a light source and clock at its origin.
The stationary sphere has a clock at its origin.
Assume when the origins of the two spheres are co-located, the two clocks are synched, and the light is flashed.
The following are the deductions from SR.
Light must proceed spherically from the center of the O sphere and strikes the rigid body sphere simultaneously.
Light must proceed spherically from the center of the O' sphere and strikes the rigid body sphere simultaneously.
O' does not believe O is struck simultaneously.
O does not believe O' is struck simultaneously.
For an observer sitting at O, when r/c elapses on its clock, all rigid body sphere points are struck simultaneously.
For an observer sitting at O', when r/c elapses on its clock, all rigid body sphere points are struck simultaneously.
Now, allow O to elapse a time of rγ/c since the flash of light occurred. This implies light has proceeded a distance rγ in all directions from O. In addition, by time dilation, the clock at O' elapsed r/c.
However, when the clock of O' elapses r/c, all of its sphere points are struck simultaneously. This implies light is a distance r in all directions from the center O'.
Now, only the positive x-axis light beam will be considered.
According to LT, x' = (x- vt)γ.Since t = rγ/c and x = rγ, then x' = (rγ- v(rγ/c))γ = rγ(γ - vγ/c).
But, since the clock of O elapsed rγ/c, then the clock of O' elapsed r/c and hence, x' = r since O' must meet is rigid body sphere simultaneity requirements when the clock at O' clock reads t/c.
Therefore, under the rules of SR, when the clock of O elapses rγ/c, the one light beam is located at both x' = r/c and x' = rγ(γ - vγ/c) which is a contradiction.
Alternatively, when the clock at O elapses rγ/c, light is a distance rγ in all directions as stated above.
In addition, the clock at O' must elapse r/c because of time dilation. Since the time elapsed r/c on the clock of O', then light must be a distance r from O' in all directions and in particular along the positive x-axis.
By LT, x = (x' + vt')γ. Since x' = r and t' = r/c, then x = (r + vr/c)γ = r(γ + vγ/c).
Hence, along the positive x-axis, light is a distance rγ/c from O, while at the same time, light is a distance r(γ + vγ/c) from O which is a contradiction.
The stationary sphere has a clock at its origin.
Assume when the origins of the two spheres are co-located, the two clocks are synched, and the light is flashed.
The following are the deductions from SR.
Light must proceed spherically from the center of the O sphere and strikes the rigid body sphere simultaneously.
Light must proceed spherically from the center of the O' sphere and strikes the rigid body sphere simultaneously.
O' does not believe O is struck simultaneously.
O does not believe O' is struck simultaneously.
For an observer sitting at O, when r/c elapses on its clock, all rigid body sphere points are struck simultaneously.
For an observer sitting at O', when r/c elapses on its clock, all rigid body sphere points are struck simultaneously.
Now, allow O to elapse a time of rγ/c since the flash of light occurred. This implies light has proceeded a distance rγ in all directions from O. In addition, by time dilation, the clock at O' elapsed r/c.
However, when the clock of O' elapses r/c, all of its sphere points are struck simultaneously. This implies light is a distance r in all directions from the center O'.
Now, only the positive x-axis light beam will be considered.
According to LT, x' = (x- vt)γ.Since t = rγ/c and x = rγ, then x' = (rγ- v(rγ/c))γ = rγ(γ - vγ/c).
But, since the clock of O elapsed rγ/c, then the clock of O' elapsed r/c and hence, x' = r since O' must meet is rigid body sphere simultaneity requirements when the clock at O' clock reads t/c.
Therefore, under the rules of SR, when the clock of O elapses rγ/c, the one light beam is located at both x' = r/c and x' = rγ(γ - vγ/c) which is a contradiction.
Alternatively, when the clock at O elapses rγ/c, light is a distance rγ in all directions as stated above.
In addition, the clock at O' must elapse r/c because of time dilation. Since the time elapsed r/c on the clock of O', then light must be a distance r from O' in all directions and in particular along the positive x-axis.
By LT, x = (x' + vt')γ. Since x' = r and t' = r/c, then x = (r + vr/c)γ = r(γ + vγ/c).
Hence, along the positive x-axis, light is a distance rγ/c from O, while at the same time, light is a distance r(γ + vγ/c) from O which is a contradiction.