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
R
R2/3
R3
1/R
Solution:
ρ = Mass/Volume Mass = ρ × Volume = constant On differentiating, Vdρ/dt + ρdV/dt = 0 (4/3)πR³ × dρ/dt + ρ × d/dt((4/3)πR³) = 0 (1/ρ)dρ/dt = -3(dR/dt)/R dR/dt = v (velocity of any point on the surface) Therefore, v ∝ R