Let us consider the conditions of equilibrium for the mass of water contained between cross sections separated by x and x + Δx from the rotational axis relative to the tube. This part of the liquid, whose mass is ρwS Δx, uniformly rotates at an angular velocity ω under the action of the forces of pressure on its lateral surfaces. Denoting the pressure in the section x by p (x), we obtain

Making Δx tend to zero, we obtain the following equation:

Using the conditions of the problem

we obtain the angular velocity of the tube:
