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I was wondering if there is a way to prove the length contraction without using the time dilation? because every time I see a derivation to length contraction it comes with the time dilation and start based on it.

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It depends on your postulates: on what premisses are you going to build your theory. If you take the Lorentz transforms as your premisses then you don't really use time dilation to establish length contraction. But you still need to consider time in order to understand length contraction. In particular you need to realise that in a frame, S, in which a body is moving (in the +$x$ direction, you must make simultaneous measurements of the positions of $x_A$ and $x_B$ of A and B on the body in order to measure the distance ($x_B-x_A$) in your frame. In the S' frame, in which the body is stationary there is no need for simultaneous measurement of $x'_A$ and $x'_B$. Using the Lorentz transform for displacements parallel to the relative velocity between frames, and the simultaneity of measuring $x_A$ and $x_B$ we have: $$x'_A = \gamma(x_A-vt)\ \ \ \ \text{and}\ \ \ \ x'_B = \gamma(x_B-vt)\ \ \ \ \text{so}\ \ \ \ x'_B-x'_A=\gamma(x_A-x_B) $$ Since $\gamma > 1$ we have $x_A-x_B<x'_B-x'_A.$

Philip Wood
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