Question:
A great amount of oil is spilled in the ocean. After a brief turbolence, the oil spreads forming a disk of radius $r$ and thickness $h$. The radius of the disk is increasing and the thickness is decreasing. Knowing that $h=\frac {c}{\sqrt t}$, prove that the $\frac {dr}{dt} $ is inversely proportional to $t^{3/4} $.
Attempted solution: We know that the volume of oil spilled ($V$) remains unchanged. Therefore: $$\frac {dV}{dt} = \pi(r^2\frac{dh}{dt}+2rh\frac{dr}{dt}) = 0$$ $$\frac {dh}{dt} = \frac {-1}{2} \frac{c}{t^{3/2}}$$ Symplifying and substing: $$ \frac {-1}{2} \frac{c}{t^{3/2}}r^2+2r\frac {c}{\sqrt t}\frac{dr}{dt} = 0 $$
Isolating the request: $$ \frac{dr}{dt} = \frac {1}{2} \frac{c}{t^{3/2}}r^2 * \frac {t^{1/2}}{c *2r}$$ $$ \frac{dr}{dt} = \frac {1}{4} \frac{r}{t} $$
I think that the $r$ at the top is the problem, but I don't know how to go on. I've also tried with implicit differentiation and I get the same result.
Ps. Sorry for my bad English, which is obviously not my first language!
Everything you've done is fine. But you haven't used $V_0 = \pi r^2 h$ to get $r$ as a function of $t$.