Gravitation Potential Energy — Question 5

Section 13-5 · Physics pages 1980–1981

Question 5 The interior potential of a uniform planet must match the exterior value A uniform spherical planet has mass M and radius R. Its interior field magnitude is g(r) = GMr/R3. Use dΦ/dr = g(r) and Φ(R) = −GM/R. r/R Φ/(GM/R) −3/2 −1 1 Potential is continuous at the surface and approaches zero from below. (a) Derive Φ(r) inside the planet. (b) Find the work to move a test mass from the center to the surface and then from the surface to infinity.
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Question 5 - Solution The interior potential of a uniform planet must match the exterior value r/R Φ/(GM/R) −3/2 −1 1 (a) Derivation and calculation Integrate the specified radial derivative using the surface boundary value: Φ(r) −Φ(R) = ∫r R GMs R3 ds = GM 2R3 (r2 −R2). Since Φ(R) = −GM/R, Φ(r) = −GM 2R3 (3R2 −r2) . (b) Result and interpretation The endpoint potentials are Φ(0) = −3GM 2R , Φ(R) = −GM R , Φ(∞) = 0. Thus W0→R = m[Φ(R) −Φ(0)] = GMm 2R , WR→∞= GMm R = 2W0→R. Physical check Differentiating the result recovers dΦ/dr = GMr/R3; the potential and its slope match the exterior at R.

Question 5

The interior potential of a uniform planet must match the exterior value

A uniform spherical planet has mass MM and radius RR. Its interior field magnitude is g(r)=GMr/R3g(r)=GMr/R^3. Use dΦ/dr=g(r)d\Phi/dr=g(r) and Φ(R)=−GM/R\Phi(R)=-GM/R.

Diagram shown in the original SVG worksheet.

  1. Derive Φ(r)\Phi(r) inside the planet.

  2. Find the work to move a test mass from the center to the surface and then from the surface to infinity.

Question 5 - Solution

The interior potential of a uniform planet must match the exterior value

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Integrate the specified radial derivative using the surface boundary value: Φ(r)−Φ(R)=∫RrGMsR3ds=GM2R3(r2−R2).\Phi(r)-\Phi(R)=\int_R^r\frac{GMs}{R^3}\,ds =\frac{GM}{2R^3}(r^2-R^2). Since Φ(R)=−GM/R\Phi(R)=-GM/R, Φ(r)=−GM2R3(3R2−r2).\boxed{\Phi(r)=-\frac{GM}{2R^3}(3R^2-r^2)}.

(b) Result and interpretation

The endpoint potentials are Φ(0)=−3GM2R,Φ(R)=−GMR,Φ(∞)=0.\Phi(0)=-\frac{3GM}{2R},\quad \Phi(R)=-\frac{GM}{R},\quad\Phi(\infty)=0. Thus W0→R=m[Φ(R)−Φ(0)]=GMm2R,\boxed{W_{0\to R}=m[\Phi(R)-\Phi(0)]=\frac{GMm}{2R}}, WR→∞=GMmR=2W0→R.\boxed{W_{R\to\infty}=\frac{GMm}{R}}=2W_{0\to R}.

Physical check

Differentiating the result recovers dΦ/dr=GMr/R3d\Phi/dr=GMr/R^3; the potential and its slope match the exterior at RR.