Gravitation Potential Energy — Question 3

Section 13-5 · Physics pages 1976–1977

Question 3 Falling from a finite radius releases less energy than falling from infinity A particle is released from rest at r = 3R outside a spherical body of mass M. It falls radially to the surface r = R. Neglect all non-gravitational forces. M r R 3R fall Release from rest at a finite radius; the particle accelerates inward to the surface. (a) Find its impact speed. (b) Compare with the speed acquired from rest at infinity and explain the difference.
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Question 3 - Solution Falling from a finite radius releases less energy than falling from infinity M r R 3R fall (a) Derivation and calculation Conservation between release and impact gives Ki + Ui = Kf + Uf, 0 −GMm 3R = 1 2mv2 −GMm R . Therefore 1 2v2 = 2GM 3R , v = √ 4GM 3R . (b) Result and interpretation For release from rest at infinity, 0 = 1 2mv2 ∞−GMm R , v∞= √ 2GM/R. v v∞ = √ 4/3 2 = √ 2/3 ≃.816497 . The finite release supplies only 2/3 of the kinetic energy available from infinity. Physical check The test mass cancels, and the finite-start impact speed is below the surface escape speed.

Question 3

Falling from a finite radius releases less energy than falling from infinity

A particle is released from rest at r=3Rr=3R outside a spherical body of mass MM. It falls radially to the surface r=Rr=R. Neglect all non-gravitational forces.

Diagram shown in the original SVG worksheet.

  1. Find its impact speed.

  2. Compare with the speed acquired from rest at infinity and explain the difference.

Question 3 - Solution

Falling from a finite radius releases less energy than falling from infinity

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Conservation between release and impact gives Ki+Ui=Kf+Uf,0−GMm3R=12mv2−GMmR.K_i+U_i=K_f+U_f,\qquad 0-\frac{GMm}{3R}=\frac12mv^2-\frac{GMm}{R}. Therefore 12v2=2GM3R,v=4GM3R.\frac12v^2=\frac{2GM}{3R},\qquad \boxed{v=\sqrt{\frac{4GM}{3R}}}.

(b) Result and interpretation

For release from rest at infinity, 0=12mv∞2−GMmR,v∞=2GM/R.0=\frac12mv_\infty^2-\frac{GMm}{R},\quad v_\infty=\sqrt{2GM/R}. vv∞=4/32=2/3≃.816497.\boxed{\frac v{v_\infty}=\sqrt{\frac{4/3}{2}}=\sqrt{2/3}\simeq.816497}. The finite release supplies only 2/32/3 of the kinetic energy available from infinity.

Physical check

The test mass cancels, and the finite-start impact speed is below the surface escape speed.