Gravitation Potential Energy — Question 10

Section 13-5 · Physics pages 1990–1991

Question 10 Building a uniform sphere reveals its gravitational self-energy Build a uniform sphere of final mass M and radius R by bringing thin shells from infinity. At assembly radius r, use M(r) = M(r/R)3 and dM = 3Mr2dr/R3. A shell contributes dU = −GM(r)dM/r. r dM A thin shell is added around the already assembled interior mass. (a) Integrate the total self-energy. (b) If a fixed mass contracts between uniform states of radii R and R/2, find the released gravitational energy.
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Question 10 - Solution Building a uniform sphere reveals its gravitational self-energy r dM (a) Derivation and calculation A new shell interacts with the mass already assembled: dU = −GM(r) r dM = −G r Mr3 R3 3Mr2 R3 dr = −3GM2 R6 r4 dr. Integrating, U = −3GM2 R6 [ r5 5 ]R 0 = −3GM2 5R . (b) Result and interpretation For fixed mass contracting to Rf = R/2, Ui = −3GM2 5R , Uf = −6GM2 5R . ∆U = −3GM2 5R , Ereleased = −∆U = 3GM2 5R . Energy partition among heat, radiation, and motion needs additional physics. Physical check The negative self-energy becomes more negative during contraction; assembly by shells counts each interaction once.

Question 10

Building a uniform sphere reveals its gravitational self-energy

Build a uniform sphere of final mass MM and radius RR by bringing thin shells from infinity. At assembly radius rr, use M(r)=M(r/R)3M(r)=M(r/R)^3 and dM=3Mr2dr/R3dM=3Mr^2dr/R^3. A shell contributes dU=−GM(r)dM/rdU=-GM(r)dM/r.

Diagram shown in the original SVG worksheet.

  1. Integrate the total self-energy.

  2. If a fixed mass contracts between uniform states of radii RR and R/2R/2, find the released gravitational energy.

Question 10 - Solution

Building a uniform sphere reveals its gravitational self-energy

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

A new shell interacts with the mass already assembled: dU=−GM(r)rdM=−GrMr3R33Mr2R3dr=−3GM2R6r4dr.dU=-\frac{GM(r)}r\,dM =-\frac G r\frac{Mr^3}{R^3}\frac{3Mr^2}{R^3}\,dr =-\frac{3GM^2}{R^6}r^4\,dr. Integrating, U=−3GM2R6[r55]0R=−3GM25R.\boxed{U=-\frac{3GM^2}{R^6}\left[\frac{r^5}5\right]_0^R =-\frac{3GM^2}{5R}}.

(b) Result and interpretation

For fixed mass contracting to Rf=R/2R_f=R/2, Ui=−3GM25R,Uf=−6GM25R.U_i=-\frac{3GM^2}{5R},\qquad U_f=-\frac{6GM^2}{5R}. ΔU=−3GM25R,Ereleased=−ΔU=3GM25R.\Delta U=-\frac{3GM^2}{5R},\qquad \boxed{E_{\mathrm{released}}=-\Delta U=\frac{3GM^2}{5R}}. Energy partition among heat, radiation, and motion needs additional physics.

Physical check

The negative self-energy becomes more negative during contraction; assembly by shells counts each interaction once.