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Theory of relativity (view source)
Revision as of 13:25, September 30, 2016
, 13:25, September 30, 2016Maths formatting
Length contraction may be derived using the [[Lorentz transformation]]s as with time dilation. This time we use the equation for <math>x</math>. In this case, the time in the undashed frame must be the '''same'''. Following the same procedure as above we find that:
Length contraction may be derived using the [[Lorentz transformation]]s as with time dilation. This time we use the equation for <math>x</math>. In this case, the time in the undashed frame must be the '''same'''. Following the same procedure as above we find that:
<math>x'_2 -x'_1 = \frac{x_2 - x_1}{\gamma}
<math>x'_2 -x'_1 = \frac{x_2 - x_1}{\gamma}</math>
This is the same as above with <math>x_2 - x_1</math> and <math>x'_2 - x'_1</math> being the lengths in the undashed and dashed frames respectively. Again, geometrical arguments may be used to achieve the same result.
This is the same as above with <math>x_2 - x_1</math> and <math>x'_2 - x'_1</math> being the lengths in the undashed and dashed frames respectively. Again, geometrical arguments may be used to achieve the same result.
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