$$ct'=\gamma(ct-vt)$$ $$t'=\gamma\Bigg(t-\dfrac{\gamma^2-1}{\gamma^2v}x\Bigg)$$
I'm trying to understand how did the textbook derivate the Lorentz Factor just using these two equations.
$$ct'=\gamma(ct-vt)$$ $$t'=\gamma\Bigg(t-\dfrac{\gamma^2-1}{\gamma^2v}x\Bigg)$$
I'm trying to understand how did the textbook derivate the Lorentz Factor just using these two equations.
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We consider the transformations of Lorentz assuming that the lengths transverse to the direction of motion are the same.
\begin{cases} x'=\gamma ( x-\beta c t)\\ y'=y\\ z'=y\\ ct'=\gamma (c t-\beta x) \end{cases}
Being that $\beta=v/c$ (speed parameter) we have:
$1/\gamma^2=1-\beta^{2}$, equivalent to $$\beta^{2}=1-\frac{(\gamma^2-1)}{\gamma^2}=\frac{(\gamma-1)(\gamma+1)}{\gamma^2}$$ or $$\frac{\gamma-1}{\beta^{2}}=\frac{\gamma^2}{\gamma+1} \iff \beta^2=\frac{\gamma^2-1}{\gamma^2} \tag 1$$
After using the identity $(1)$ you have:
$$t'=\gamma t-\gamma\frac\beta c x= \gamma t-\gamma \frac{\beta}c\frac v v x=\gamma t-\frac{\gamma\beta^2}{v}x=\gamma t-\frac{\gamma \dfrac{\gamma^2-1}{\gamma^2}}{v}x=\gamma\Bigg(t-\dfrac{\gamma^2-1}{\gamma^2v}x\Bigg)$$