Gravitation Potential Energy — Question 7

Section 13-5 · Physics pages 1984–1985

Question 7 A midpoint with zero field is still gravitationally bound Two equal fixed point masses M lie at x = ±a. A test particle starts at their midpoint and is launched along the positive y axis. The source masses remain fixed; the particle follows the symmetry axis. M M y v0 Schematic; labels, not drawing lengths, specify the data. (a) Find its potential energy along that axis and the minimum launch speed to reach infinity. (b) Explain how the midpoint can have zero field but a nonzero escape speed.
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Question 7 - Solution A midpoint with zero field is still gravitationally bound M M y v0 (a) Derivation and calculation On the symmetry axis both source distances are s = √ a2 + y2: U(y) = −2GMm √ a2 + y2 , U(0) = −2GMm a . Marginal escape has E = U(∞) = 0, giving 1 2mv2 esc −2GMm a = 0, vesc = √ 4GM/a . (b) Result and interpretation Differentiation gives Fy = −dU dy = −2GMmy (a2 + y2)3/2 , Fy(0) = 0. For y > 0, dU/dy > 0: the potential increases monotonically to zero. The required increase is ∆U = 0 −U(0) = 2GMm a > 0. Vector fields cancel at the midpoint while scalar potentials add. Physical check The zero-energy launch can climb the entire axis without an intervening potential barrier.

Question 7

A midpoint with zero field is still gravitationally bound

Two equal fixed point masses MM lie at x=±ax=\pm a. A test particle starts at their midpoint and is launched along the positive yy axis. The source masses remain fixed; the particle follows the symmetry axis.

Diagram shown in the original SVG worksheet.

  1. Find its potential energy along that axis and the minimum launch speed to reach infinity.

  2. Explain how the midpoint can have zero field but a nonzero escape speed.

Question 7 - Solution

A midpoint with zero field is still gravitationally bound

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

On the symmetry axis both source distances are s=a2+y2s=\sqrt{a^2+y^2}: U(y)=−2GMma2+y2,U(0)=−2GMma.\boxed{U(y)=-\frac{2GMm}{\sqrt{a^2+y^2}}},\qquad U(0)=-\frac{2GMm}a. Marginal escape has E=U(∞)=0E=U(\infty)=0, giving 12mvesc2−2GMma=0,vesc=4GM/a.\frac12mv_{\mathrm{esc}}^2-\frac{2GMm}a=0, \qquad\boxed{v_{\mathrm{esc}}=\sqrt{4GM/a}}.

(b) Result and interpretation

Differentiation gives Fy=−dUdy=−2GMmy(a2+y2)3/2,Fy(0)=0.F_y=-\frac{dU}{dy}=-\frac{2GMmy}{(a^2+y^2)^{3/2}},\qquad F_y(0)=0. For y>0y>0, dU/dy>0dU/dy>0: the potential increases monotonically to zero. The required increase is ΔU=0−U(0)=2GMma>0.\Delta U=0-U(0)=\frac{2GMm}a>0. Vector fields cancel at the midpoint while scalar potentials add.

Physical check

The zero-energy launch can climb the entire axis without an intervening potential barrier.