In his 1905 paper, Einstein derives the Lorentz transformation using the two postulates of SR;constancy of $c$ for all inertial frames and the Invariance of the laws of physics for all inertial frames.
I'll summarize his mathematical derivation and then ask one specific question about it.
So we consider two frames $(x,y,z,t)$ and $(\xi,η, ζ,\tau)$ in relative motion along the x-axis with velocity $v$, and we're interested in finding a spacetime transformation that relates thier coordinates.
We consider some arbitrary point $x'=x-vt$. This point is at rest in $(\xi,η, ζ,\tau)$ since it's moving with $v$, Therefore this point has $x',y,z$ coordinates that is independent of time, in other words the distance between that point and the origin of $(\xi,η, ζ,\tau)$ is constant.
We consider the following scenario: hit a beam of light from the origin of $(\xi,η, ζ,\tau)$ at $\tau_0$ arriving at the point $x'$ at $\tau_1$ and then being reflected and arrive at the origin of $(\xi,η, ζ,\tau)$ at $\tau_2$.
So that we have: $1/2(\tau_0+\tau_2)=\tau_1$. Since $\tau$ is a function of $(x,y,z,t)$ we have:
$\dfrac{1}{2}[\tau(0,0,0,t)+\tau(0,0,0,t+\dfrac{x'}{c-v}+\dfrac{x'}{c+v})]=\tau(x',0,0,t+\dfrac{x'}{c-v})$
Assuming that $x'$ is infinitely small then taylor expanding this equation and approximating it to first order we get:
$\dfrac{\partial \tau}{\partial x'}+\dfrac{v}{c^2-v^2}\dfrac{\partial\tau}{\partial t}=0$
Solving it then we have:
$\tau=a(t-\dfrac{v}{c^2-v^2}x')$
where $a$ is some unkown function of $v$ (in fact $a=1$).
Finally consider a beam of light emitted from $(\xi,η, ζ,\tau)$ at the origin, it's $\xi$ coordinate is given by $\xi=c\tau=ca(t-\dfrac{v}{c^2-v^2}x')$
It's given by $\dfrac{x'}{c-v}=t$ in $(x,y,z,t)$, plugging in for $t$ we get:
$\xi=a\dfrac{c^2}{c^2-v^2}x'$
He then states:
Substituting for $x'$ its value, we obtain $\xi=a\dfrac{1}{\sqrt{1-v^2/c^2}}(x-vt)$ ...
My question is:
1) the three equations $\tau=a(t-\dfrac{v}{c^2-v^2}x')$ and $\xi=c\tau$ and $x'=x-vt$ when combined together gives :
$\xi=c\tau=ca(t-\dfrac{v}{c^2-v^2}x')=a\dfrac{c^2}{c^2-v^2}x'$, since $x'=x-vt$ by plugging in we get:
$\xi=a\dfrac{c^2}{c^2-v^2}(x-vt)=a\dfrac{1}{1-v^2/c^2}(x-vt)$ not $a\dfrac{1}{\sqrt{1-v^2/c^2}}(x-vt)$ .
But He says
Substituting for $x'$ its value, we obtain $\xi=a\dfrac{1}{\sqrt{1-v^2/c^2}}(x-vt)$ ...
All these equations are copied from Einstein's original paper, So what is wrong with my calculations that does not make it match up with that of Einstein?