Prove that, in the forced vortex motion (fluids subjected to rotation externally) of a liquid, the rate of increase of the pressure, $p$, with respect to the radius, r , at a point in liquid is given by $\mathrm{dp} / \mathrm{dr}=\rho \omega^2 \mathrm{r}$, in which $\omega$ is the angular velocity of the liquid and $\rho$ is its mass density. Hence calculate the thrust of the liquid on the top of a closed vertical cylinder of 450 mm diameter, completely filled with water under a pressure of $10 \mathrm{~N} / \mathrm{cm}^2$, when the cylinder rotates about its axis at 240 rpm .