espen180
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I present here an alternative derivation of the result found in the wiki article. Hopefully the fact that different approaches lead to the same result will convince you that the result is not erroneous.
The Minkowski metric, which really is fundamental to SR, gives a very short derivation of the formula you are critiquing. This metric illustrates a very fundamental aspect of Relativity, namely the invariance of the spacetime element ds between frames. We have that
ds^2=c^2dt^2-dx^2-dy^2-dz^2 (Note that I am using a convention different from, but physically equivalent to, the one used by JesseM. (This can also be interpreted as "The norms of all vectors (ct,x,y,z) in Minkowski spacetime are equal.")
For our purposes we may assume dy=dz=0 and let the x-axes of all frames point in the direction the clock is moving. We will now derive from this the relationship between the relevant frames.
1) The rest frame of the observer. This frame is stationary relative to the observer (Note that ALL measurements MUST have an observer).
2) The rest frame of the clock, moving with velocity v with respect respect to the observer.
The question we want to answer is: As the clock moves past the observer (we assume it does), at what rate does the observer measure the passing clock to tick relative to his own wristwatch, assuming they tick at the same rate when stationary with respect to one another? (This problem statement was a mouthful, be sure you got everything).
Of course, the clock is at rest with respect to its own rest frame, so ds^2=c^2d\tau^2, where d\tau is an infinitesimal interval of time. By convention, we call this the proper time of the clock along its trajectory.
However, the clock is moving with constant velocity v=\frac{dx}{dt} in the observer's rest frame, and by the invariance of the spacetime element we therefore have
c^2d\tau^2=c^2dt^2-dx^2
\left(\frac{d\tau}{dt}\right)^2=1-\frac{v^2}{c^2}
Giving us the time dilation formula
\frac{dt}{d\tau}=\frac{1}{\sqrt{1-\frac{v^2}{c^2}}}=\gamma
or
dt=\gamma d\tau
And I restate my convention that dt is an infinitesimal time interval in the observer's rest frame, where the clock is moving, and d\tau is an infinitesimal time interval in the clock's rest frame.
The Minkowski metric, which really is fundamental to SR, gives a very short derivation of the formula you are critiquing. This metric illustrates a very fundamental aspect of Relativity, namely the invariance of the spacetime element ds between frames. We have that
ds^2=c^2dt^2-dx^2-dy^2-dz^2 (Note that I am using a convention different from, but physically equivalent to, the one used by JesseM. (This can also be interpreted as "The norms of all vectors (ct,x,y,z) in Minkowski spacetime are equal.")
For our purposes we may assume dy=dz=0 and let the x-axes of all frames point in the direction the clock is moving. We will now derive from this the relationship between the relevant frames.
1) The rest frame of the observer. This frame is stationary relative to the observer (Note that ALL measurements MUST have an observer).
2) The rest frame of the clock, moving with velocity v with respect respect to the observer.
The question we want to answer is: As the clock moves past the observer (we assume it does), at what rate does the observer measure the passing clock to tick relative to his own wristwatch, assuming they tick at the same rate when stationary with respect to one another? (This problem statement was a mouthful, be sure you got everything).
Of course, the clock is at rest with respect to its own rest frame, so ds^2=c^2d\tau^2, where d\tau is an infinitesimal interval of time. By convention, we call this the proper time of the clock along its trajectory.
However, the clock is moving with constant velocity v=\frac{dx}{dt} in the observer's rest frame, and by the invariance of the spacetime element we therefore have
c^2d\tau^2=c^2dt^2-dx^2
\left(\frac{d\tau}{dt}\right)^2=1-\frac{v^2}{c^2}
Giving us the time dilation formula
\frac{dt}{d\tau}=\frac{1}{\sqrt{1-\frac{v^2}{c^2}}}=\gamma
or
dt=\gamma d\tau
And I restate my convention that dt is an infinitesimal time interval in the observer's rest frame, where the clock is moving, and d\tau is an infinitesimal time interval in the clock's rest frame.