Consider a transformation between the coordinates given by $x^{a}$ to another system given by coordinates $x^{'a}$. So a transformation of the type: $x^{a} \rightarrow x^{'a}$.
With that I can construct the Jacobian matrix:
$\bigg[ \frac{\partial x^{'a}}{\partial x^{b}} \bigg]$
The determinant of this matrix is called the Jacobian determinant, hereafter J. I want to prove that:
$dx^{'1}dx^{'2}...dx^{'N} = Jdx^{1}dx^{2}...dx^{N}$
where primed system is cartesian and the unprimed one is a general set of coordinates. How can I do that?
I remembered that in transformation of coordinate is valid to write (using the summation convention) that:
$dx^{'a} = \frac{\partial x^{'a}}{\partial x^{b}}dx^{b}$
And tried to apply that to proof that I need, but, I was not abble to go anywhere because of lot of terms shows up. Actually, in the case we considerer just 2 dimensions I ended up with something like that:
$dx^{'1}dx^{'2} = \bigg( \frac{\partial x^{'1}}{\partial x^{1}} \frac{\partial x^{'2}}{\partial x^{1}} \bigg)(dx^{1})^{2}+ \bigg( \frac{\partial x^{'1}}{\partial x^{2}} \frac{\partial x^{'2}}{\partial x^{2}} \bigg)(dx^{2})^{2} + \bigg[\bigg( \frac{\partial x^{'1}}{\partial x^{1}} \frac{\partial x^{'2}}{\partial x^{2}} \bigg) + \bigg( \frac{\partial x^{'1}}{\partial x^{2}} \frac{\partial x^{'2}}{\partial x^{1}} \bigg)\bigg]dx^{1}dx^{2} $
As is possible to see, the last two therms inside the brackets are almost the Jacobian determinant. So my question is: what is wrong in this approach?
I did found this article with a different ideia of the proof. But why should I use that instead of the mine? And also: how could I generalize the ideia of this article for N-dimensions?
Following the tip given by @Neal and @Ted Shifrin I looked up more in the subject and I believe that I found a better (and more convincing) proof for the problem. Here in the Math Stackexchange.
The link for the (probable) answer is here!