Let the volume of the steel ball be V, and let the volume of its part immersed in mercury be V0 before water is poured and V1 after water covers the ball completely. The value of V0 can be found from the condition

where ρst and ρmer are the densities of steel and mercury. Since the pressure of water is transmitted through mercury to the lower part of the ball, the buoyant force exerted on it by water is ρw (V - V1) g, where p, is the density of water, while the buoyancy of mercury is ρmer V1g. The condition of floating for the ball now becomes

Thus, the ratio of the volumes of the parts of the ball submerged in mercury in the former and latter cases is


i.e. the volume of the part of the ball immersed in mercury will become smaller when water is poured.