Gravitation Potential Energy — Question 8

Section 13-5 · Physics pages 1986–1987

Question 8 Escape of two free bodies depends on relative energy Two isolated point masses M and m separate radially at distance r with relative speed vrel. Use reduced mass µ = Mm/(M + m) and internal energy Eint = µv2 rel/2 −GMm/r. M m r Point masses or spherical bodies; separation is measured between centers. (a) Find the threshold relative speed for unbounded separation. (b) Explain why giving both masses the same additional velocity cannot turn a bound relative motion into an escaping one.
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Question 8 - Solution Escape of two free bodies depends on relative energy M m r (a) Derivation and calculation For radial separation, unbounded escape requires Eint ≥0. At threshold, 1 2µv2 rel = GMm r , µ = Mm M + m. Therefore vrel,esc = √ 2G(M + m) r . (b) Result and interpretation Adding the same velocity⃗V to both bodies gives⃗ v′ rel = (⃗vm +⃗V ) −(⃗vM +⃗V ) =⃗vrel. The total kinetic energy separates as K = 1 2(M + m)V 2 CM + 1 2µv2 rel. Only the first term changes under a common boost; internal energy and the bound/escaping classification stay unchanged. Physical check When M ≫m, the relative escape speed approaches the usual fixed-source value √ 2GM/r.

Question 8

Escape of two free bodies depends on relative energy

Two isolated point masses MM and mm separate radially at distance rr with relative speed vrelv_{rel}. Use reduced mass μ=Mm/(M+m)\mu=Mm/(M+m) and internal energy Eint=μvrel2/2−GMm/rE_{int}=\mu v_{rel}^2/2-GMm/r.

Diagram shown in the original SVG worksheet.

  1. Find the threshold relative speed for unbounded separation.

  2. Explain why giving both masses the same additional velocity cannot turn a bound relative motion into an escaping one.

Question 8 - Solution

Escape of two free bodies depends on relative energy

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For radial separation, unbounded escape requires Eint≥0E_{\mathrm{int}}\ge0. At threshold, 12μvrel2=GMmr,μ=MmM+m.\frac12\mu v_{\mathrm{rel}}^2=\frac{GMm}r,\qquad \mu=\frac{Mm}{M+m}. Therefore vrel,esc=2G(M+m)r.\boxed{v_{\mathrm{rel,esc}}=\sqrt{\frac{2G(M+m)}r}}.

(b) Result and interpretation

Adding the same velocity V→\vec V to both bodies gives v→rel′=(v→m+V→)−(v→M+V→)=v→rel.\vec v'_{\mathrm{rel}}=(\vec v_m+\vec V)-(\vec v_M+\vec V)=\vec v_{\mathrm{rel}}. The total kinetic energy separates as K=12(M+m)VCM2+12μvrel2.K=\frac12(M+m)V_{\mathrm{CM}}^2+\frac12\mu v_{\mathrm{rel}}^2. Only the first term changes under a common boost; internal energy and the bound/escaping classification stay unchanged.

Physical check

When M≫mM\gg m, the relative escape speed approaches the usual fixed-source value 2GM/r\sqrt{2GM/r}.