Transforming differentials to polar coordinates Consider the integral $$\iint\limits_R dxdy$$
in Cartesian coordinates. I know that we can use Jacobian to switch this integral to polar coordinates, which will give us
$$\iint\limits_S rdrd\theta$$
But how can we do this transformation without using Jacobians?
Is it true that if $r^2 = x^2 + y^2$ then $2rdr = 2xdx + 2ydy$? Then $xdx = rdr - ydy$ or $dx = rdr/x - ydy/x=\frac{dr}{\cos\theta}-\frac{\sin\theta dy}{\cos\theta}=\frac{dr}{\cos\theta}-\tan\theta dy$.
Also, $dy=rdr/y-xdx/y=\frac{dr}{\sin\theta}-\cot\theta dx$.
So how come $dxdy = rdrd\theta$? That is, what is it that I'm not doing right here?
 A: You can use the exterior derivative operator d to figure out this problem where for a function f $df = f_xdx+f_ydy+f_zdz$ We can use the other definitions of polar coordinates to solve for dx and dy in terms of r and $\theta$. Note that in this derivation we are using exterior products (Think cross product) of differentials not the usual point wise product and note: $dx\wedge dx = 0 $ and $dx\wedge dy = -dy \wedge dx$
$$
x = r\cos(\theta)
\\ y = r\sin(\theta)
\\ dx = \frac{\partial}{\partial r} r\cos(\theta)dr + \frac{\partial}{\partial \theta} r\cos(\theta)d\theta
\\ dx = \cos(\theta)dr - r\sin(\theta)d\theta
\\ dy = \frac{\partial}{\partial r} r\sin(\theta)dr + \frac{\partial}{\partial \theta} r\sin(\theta)d\theta
\\ dy = \sin(\theta)dr + r\cos(\theta)d\theta
\\ \text{Multiplication yields}
\\ dxdy = (\cos(\theta)dr - r\sin(\theta)d\theta) * (\sin(\theta)dr + r\cos(\theta)d\theta)
\\dxdy = \cos(\theta)dr*\sin(\theta)dr - r^2\sin(\theta)d\theta*\cos(\theta)d\theta-r\sin^2(\theta)d\theta dr+r\cos^2(\theta)drd\theta 
\\dxdy = 0 -0+r(\cos^2(\theta)drd\theta-\sin^2(\theta)d\theta dr)
\\dxdy = r(\cos^2(\theta)drd\theta+\sin^2(\theta)dr d\theta)
\\dxdy = rdrd\theta( \cos^2(\theta)+\sin^2(\theta))=rdrd\theta
\\\text{More accurately}
\\dx\wedge dy = rdr\wedge d\theta
\\\text{You can then integrate the differential 2-form}
\\ \int dx\wedge dy = \int rdr\wedge d\theta = \iint rdrd\theta
$$
Also when you differentiate both sides of an equation you have to differentiate with respect to a variable you cant differentiate each variable with a different variable. The exterior derivative is different however because it is a derivative with respect to every variable. 
$$
r^2 = x^2 + y^2 \equiv\frac{d}{dx}r^2 = \frac{d}{dx}(x^2 + y^2)
\\r^2 = x^2 + y^2 \not \equiv 2rdr = 2xdx + 2ydx
$$
A: It is important to understand that multiplication of differentials is "anti-commutative".  That is, dxdy= -dydx and, of course, dxdx= dydy= 0.  Given that $dx= cos(\theta)dr- rsin(\theta)d\theta$ and that $dy= sin(\theta)dr+ rcos(\theta)d\theta$, $dxdy= (cos(\theta)dr- rsin(\theta)d\theta)(sin(\theta)dr+ rcos(\theta)d\theta)= cos(\theta)sin(\theta)drdr- rsin^2(\theta)d\theta dr+ rcos^2(\theta)drd\theta- r^2 sin(\theta)cos(\theta)drdr$.
The first and last terms are 0 because drdr and $d\theta d\theta$ are both 0. And $- rsin^2(\theta)d\theta dr= rsin^2(\theta)drd\theta$ so the second and third terms sum to $r(sin^2(\theta)+ cos^2(\theta)) drd\theta= r drd\theta$.
