Lorentz Transforms

once we get, \(x' = (x-vt)f(v)\) and \(t' = (t-vx)f(v)\)

we can prove that \(f(v)\) is \(\gamma\)

so our transformations are \(x' * \gamma\) and t'* gamma so,

\[ x' = \frac{(x-vt)}{\sqrt{1-v^2}} \] \[ t' = \frac{(t-vx)}{\sqrt{1-v^2}} \] and ect

---