Potential Due to a Point Charge — Question 5

Section 24-5 · Physics pages 3880–3881

Question 5 Head-on repulsion fixes a closest-approach distance A positive particle q approaches a fixed positive point charge Q from infinity with speed v∞. Its mass is m, its angular momentum is zero, and only electrostatic work is relevant. Q q v Schematic; labels, not drawing lengths, specify the data. (a) Find its closest approach. (b) If it instead starts at radius R with inward speed vR, find the closest approach and its limiting value as vR →0.
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Question 5 - Solution Head-on repulsion fixes a closest-approach distance Q q v (a) Method and calculation E = 1 2mv2 ∞= kQq rmin (Kturn = 0). rmin = 2kQq mv2∞ . (b) Interpretation and further calculation 1 2mv2 R + kQq R = kQq rmin . rmin = ( 1 R + mv2 R 2kQq )−1 −→R. Physical check The zero-angular-momentum condition makes the turning-point kinetic energy zero; an oblique encounter retains tangential kinetic energy.

Question 5

Head-on repulsion fixes a closest-approach distance

A positive particle q approaches a fixed positive point charge Q from infinity with speed v∞v_\infty. Its mass is m, its angular momentum is zero, and only electrostatic work is relevant.

Diagram shown in the original SVG worksheet.

  1. Find its closest approach.

  2. If it instead starts at radius R with inward speed vRv_R, find the closest approach and its limiting value as vR→0v_R\to0.

Question 5 - Solution

Head-on repulsion fixes a closest-approach distance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ℰ=12mv∞2=kQqrmin(Kturn=0).\mathcal E=\tfrac12mv_\infty^2=\frac{kQq}{r_{\min}}\quad(K_{\mathrm{turn}}=0).rmin=2kQqmv∞2.r_{\min}=\frac{2kQq}{mv_\infty^2}.

(b) Interpretation and further calculation

12mvR2+kQqR=kQqrmin.\tfrac12mv_R^2+\frac{kQq}{R}=\frac{kQq}{r_{\min}}.rmin=(1R+mvR22kQq)−1→R.r_{\min}=\left(\frac1R+\frac{mv_R^2}{2kQq}\right)^{-1}\longrightarrow R.

Physical check

The zero-angular-momentum condition makes the turning-point kinetic energy zero; an oblique encounter retains tangential kinetic energy.