Let the volume of the steel ball be V, and let the volume o fits 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
ρstV=ρmerV0,
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 baal, the buoyant force exerted on it by water is ρw(V−V1)g, where ρw is the density of water, while the buoyancy of mercury is ρmerV1g. The condition of floating for the ball now becomes
ρstV=ρmerV1+ρw(V−V1)
whence
V1=ρst−ρwρmer−ρwV
Thus, the ratio of the volumes of the parts of the ball submerged in mercury in the former and latter cases is
V0V1=ρstρmerρmer−ρwρst−ρw=1−ρw/ρmer1−ρw/ρst
Since ρmer>ρst,V0>V1 i.e. the volume of the parts of the ball immersed in mercury will becomes smaller when water is poured.