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This is from Special Relativity, but it is not relevant to my question anyways.
I am trying to simplify this:
{\Delta}t = \frac{\ell}{c} \left[ \frac{1}{1- \beta^2} - \frac{1}{\sqrt{1 - \beta^2}} \right]
- TO -
{\Delta}t \approx \frac{\ell}{2c} \beta^2
For small x, (1 + x)^n \approx 1 + n x
NOTE: Problem SOLVED. Feel free to try this out yourself. Make x = -\beta^2, it makes it easier, or I think it does.
I am trying to simplify this:
{\Delta}t = \frac{\ell}{c} \left[ \frac{1}{1- \beta^2} - \frac{1}{\sqrt{1 - \beta^2}} \right]
- TO -
{\Delta}t \approx \frac{\ell}{2c} \beta^2
For small x, (1 + x)^n \approx 1 + n x
NOTE: Problem SOLVED. Feel free to try this out yourself. Make x = -\beta^2, it makes it easier, or I think it does.
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