Gravitation Potential Energy — Question 6

Section 13-5 · Physics pages 1982–1983

Question 6 Assembly energy counts each gravitational pair exactly once Three point masses m, 2m and 3m are placed at the vertices of an equilateral triangle of side a. They are assembled quasistatically from infinite separation and then held fixed. m 2m 3m a Schematic; labels, not drawing lengths, specify the data. (a) Find total gravitational potential energy. (b) Find the external work needed to remove only the 3m mass to infinity while the other two stay fixed.
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Question 6 - Solution Assembly energy counts each gravitational pair exactly once m 2m 3m a (a) Derivation and calculation Sum unordered pairs exactly once: U = −G ∑ i<j mimj rij = −G a [(m)(2m) + (m)(3m) + (2m)(3m)]. U = −11Gm2 a . Equivalently, U = 1 2 ∑ i miΦothers(⃗ri); the half prevents double counting. (b) Result and interpretation After removing only 3m, the remaining energy is Uf = −G(m)(2m) a = −2Gm2 a . Quasistatic external work is Wext = Uf −Ui = (−2 + 11)Gm2 a = 9Gm2 a . Only the pair energies −3Gm2/a and −6Gm2/a disappear. Physical check The remaining pair stays bound, so removing one mass does not raise the system energy all the way to zero.

Question 6

Assembly energy counts each gravitational pair exactly once

Three point masses mm, 2m2m and 3m3m are placed at the vertices of an equilateral triangle of side aa. They are assembled quasistatically from infinite separation and then held fixed.

Diagram shown in the original SVG worksheet.

  1. Find total gravitational potential energy.

  2. Find the external work needed to remove only the 3m3m mass to infinity while the other two stay fixed.

Question 6 - Solution

Assembly energy counts each gravitational pair exactly once

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Sum unordered pairs exactly once: U=−G∑i<jmimjrij=−Ga[(m)(2m)+(m)(3m)+(2m)(3m)].U=-G\sum_{i<j}\frac{m_im_j}{r_{ij}} =-\frac G a[(m)(2m)+(m)(3m)+(2m)(3m)]. U=−11Gm2a.\boxed{U=-\frac{11Gm^2}{a}}. Equivalently, U=12∑imiΦothers(r→i)U=\tfrac12\sum_i m_i\Phi_{\mathrm{others}}(\vec r_i); the half prevents double counting.

(b) Result and interpretation

After removing only 3m3m, the remaining energy is Uf=−G(m)(2m)a=−2Gm2a.U_f=-\frac{G(m)(2m)}a=-\frac{2Gm^2}a. Quasistatic external work is Wext=Uf−Ui=(−2+11)Gm2a=9Gm2a.\boxed{W_{\mathrm{ext}}=U_f-U_i=(-2+11)\frac{Gm^2}a=\frac{9Gm^2}a}. Only the pair energies −3Gm2/a-3Gm^2/a and −6Gm2/a-6Gm^2/a disappear.

Physical check

The remaining pair stays bound, so removing one mass does not raise the system energy all the way to zero.