Transforming differential equation to polar coordinates, example. 
... For example, if we write $\dfrac{\operatorname dy}{\operatorname dx} = \dfrac{-x}{y}$ in polar coordinates, we obtain the equation $\dfrac{\operatorname dr}{\operatorname d\theta} = 0$ whose solution is $r = C$.

Seems like a straightforward statement, but I don't seem to get there. I guess i'm doing something wrong... Could someone help?
If $x = r\cos \theta$, $y=r \sin \theta$ with the inverse transformation $r = \sqrt{x^2+y^2}$, $\theta = \arctan \dfrac{y}{x}$.
Then $\dfrac{-x}{y} = \dfrac{-\cos \theta}{\sin \theta}$
Next:
$$\dfrac{\operatorname dy}{\operatorname dx} \stackrel{\color{red}{(1)}}{=} \dfrac{\operatorname dy}{\operatorname dr}\cdot \dfrac{\operatorname dr}{\operatorname d\theta}\cdot \dfrac{\operatorname d\theta}{\operatorname dx} = \sin \theta \cdot  \dfrac{\operatorname dr}{\operatorname d\theta}\cdot \dfrac{-r\sin \theta}{r^2}$$
This results in:
$$\sin \theta \cdot  \dfrac{\operatorname dr}{\operatorname d\theta}\cdot \dfrac{-r\sin \theta}{r^2} = \dfrac{-\cos\theta}{\sin \theta}$$
or
$$\dfrac{\operatorname dr}{\operatorname d\theta}= \dfrac{r \cos\theta}{\sin^3 \theta}$$
Fault?
I suspect $\color{red}{(1)}$ is not right. Since $\dfrac{\operatorname dy}{\operatorname d r}$ doesn't make any sense. I should be using something like $\partial$, but how exactly?
 A: The fault is in: 
$\frac{dy}{dx}=\frac{dy}{d\theta}\frac{d\theta}{dx} + \frac{dy}{dr}\frac{dr}{dx} $
A: $$\frac{dy}{dx}=\frac{dy}{d\theta}\times\frac{d\theta}{dx}=\frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}}\tag{1}$$$$x=r\cos(\theta)$$$$\therefore\frac{dx}{d\theta}=\cos(\theta)\frac{dr}{d\theta}-r\sin(\theta)\tag{2}$$$$y=r\sin(\theta)$$$$\therefore\frac{dy}{d\theta}=\sin(\theta)\frac{dr}{d\theta}+r\cos(\theta)\tag{3}$$Substituting (2) and (3) into (1) then gives:$$\frac{dy}{dx}=\frac{\sin(\theta)\frac{dr}{d\theta}+r\cos(\theta)}{\cos(\theta)\frac{dr}{d\theta}-r\sin(\theta)}$$Hopefully you can proceed from here...

The mistakes you made were in the calculations of $\frac{dy}{dr}$ and $\frac{dx}{d\theta}$:$$\frac{dy}{dr}=\sin(\theta)+r\cos(\theta)\frac{d\theta}{dr}$$$$\frac{dx}{d\theta}=-r\sin(\theta)+\cos(\theta)\frac{dr}{d\theta}$$Using these in your approach would have led to the same result as I got above, i.e.:$$\frac{dy}{dx}=\frac{dy}{dr}\cdot\frac{dr}{d\theta}\cdot\frac{d\theta}{dx}$$$$=\left(\sin(\theta)+r\cos(\theta)\frac{d\theta}{dr}\right)\cdot\frac{dr}{d\theta}\cdot\left(\frac{1}{-r\sin(\theta)+\cos(\theta)\frac{dr}{d\theta}}\right)$$$$=\frac{\sin(\theta)\frac{dr}{d\theta}+r\cos(\theta)}{\cos(\theta)\frac{dr}{d\theta}-r\sin(\theta)}$$
A: You could also view your problem as an equality of differential forms: $x\mathbb{d}x + y\mathbb{d}y =0$. Since $\mathbb{d}x=\mathbb{d}(r\cos \theta)=\cos \theta \mathbb{d}r-r \sin \theta \mathbb{d}\theta$ and $\mathbb{d}y= \sin \theta \mathbb{d}r+ r \cos \theta \mathbb{d} \theta$, a simple substitution makes this is equivalent to $0= r \cos^2 \theta \mathbb{d} r - r^2 \sin \theta \cos \theta \mathbb{d}\theta + r \sin^2 \theta \mathbb{d}r + r^2 \sin \theta \cos \theta \mathbb{d}\theta = r \mathbb{d}r$, which means $\mathbb{d}r=0$ which gives $r=constant$.
