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 (1/ρ dρ/dt) is constant. The velocity v of any point on the surface of the expanding sphere is proportional to
(A) R
(B) R3
(C)1/R
(D) R2/3