Volume element in different coordinate system

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The discussion focuses on transforming the volume element from Cartesian to polar coordinates, highlighting the importance of the Jacobian in this process. The initial calculation leads to a discrepancy between the volume elements in Cartesian and polar coordinates, prompting a search for the error. Participants emphasize the necessity of applying the formal rules for differentials, including the skew product, to correctly compute the volume element. The transformation is clarified through vector representation, demonstrating how the cross product of differential vectors yields the correct volume element. Ultimately, the conversation underscores the complexities involved in coordinate transformations and the proper treatment of differentials.
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Very simple question:

Let x^0,x^1,...,x^n be some fixed coordinate system, so that the infinitesimal volume element is dV=dx^0dx^1...dx^n.
Then any change to a new (primed) coordinate system x^{0'},x^{1'},...,x^{n'} transforms the volume to dV=\frac{\partial (x^0,x^1,...,x^n)}{\partial (x^{0'},x^{1'},...,x^{n'})}dx^{0'}dx^{1'}...dx^{n'} where \frac{\partial (x^0,x^1,...,x^n)}{\partial (x^{0'},x^{1'},...,x^{n'})} is the determinat of the jacobian of the transformation.

So let's try to do this in a concrete example: the transformation from cartesian x,y to polar r,\theta coordinates.
The Jacobian is simply r and so i get to dV=dxdy=rdrd\theta.

Doing the math i get dV^{pol.}=r(\cos\theta dx+\sin\theta dy)(-\frac{1}{r}\sin\theta dx+\frac{1}{r}\cos\theta dy)since dr=\cos\theta dx+\sin\theta dy and d\theta=-\frac{1}{r}\sin\theta dx+\frac{1}{r}\cos\theta dy.
But then:dV^{pol.}=-\cos\theta\sin\theta dx^2+\cos^2\theta dxdy-\sin^2\theta dxdy + \cos\theta\sin\theta dy^2 and is clear that dV^{cart.}\neq dV^{pol.} !
Where is my mistake?? Thanks for your help guys!
 
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You can't just multiply differentials.

Try using the formal rules

dx dx = dy dy = 0

and

dx dy = -dy dx
 
x= r cos(\theta) y= r sin(\theta)

dx= cos(\theta)dr- r sin(\theta)d\theta

dy= sin(\theta)dr+ r cos(\theta)d\theta

But when you multiply differentials, you have to use "skew product" Petr Mugver mentions.

A good way of thinking about it is as vectors
dx= cos(\theta)dr\vec{i}- r sin(\theta)d\theta\vec{j}
dy= sin(\theta)dr\vec{i}+ r sin(\theta)d\theta\vec{j}

Now the product is the cross product of the two "vectors".

\left|\begin{array}{ccc}\vec{i} & \vec{j} & \vec{k} \\ cos(\theta) & - rsin(\theta) & 0 \\ sin(\theta) & rcos(\theta) & 0 \end{array}\right|= (rcos^2(\theta)+ rsin^2(\theta))drd\theta\vec{k}= r drd\theta \vec{k}
 

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