Consider an expanding sphere of instantaneous radius R whose total mass remains constant. The expansion is such that the instantaneous density ρ remains uniform throughout the volume. The rate of fractional change in density (1ρdρdt) is constant. The velocity v of any point on the surface of the expanding sphere is proportional to
R
ρ=MassVolume
Mass=ρ×Volume=constant
Here total mass is given as constant
On differentiating,
Vdρdt+ρdVdt=0
43πR3×dρdt +ρ×ddt(43πR3)=0
1ρdρdt=−3RdRdt,