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Consider an expanding sphere of instantaneous radius R whose total mass remains constant. The expansion is such that the instantaneous density p remains uniform throughout the volume. The rate of fractional change in density \((\frac{1}{p}\frac{dp}{dt})\) 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

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