Gravitation and the Principle of Superposition — Question 1

Section 13-2 · Physics pages 1912–1913

Question 1 The field cancellation point lies nearer the smaller source Fixed point sources M and 9M lie at x = 0 and x = d. A negligible test mass can be placed on their line. x M1 M2 0 d Sources lie on the horizontal axis; marked positions define the geometry. (a) Find every finite point on the line where the total gravitational field is zero. (b) Explain why adding field magnitudes instead of signed components would miss the cancellation.
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Question 1 - Solution The field cancellation point lies nearer the smaller source x M1 M2 0 d (a) Derivation and calculation For 0 < x < d, the left source attracts left and the right source attracts right: gx = −GM x2 + 9GM (d −x)2 . Setting gx = 0 and taking positive distances, d −x = 3x, x = d/4 . For x < 0 both fields point right; for x > d both point left. There are no other finite zeros. (b) Result and interpretation At the cancellation point, g1x = −16GM d2 , g2x = 9GM (3d/4)2 = 16GM d2 . g1x + g2x = 0, |g1x| + |g2x| = 32GM d2̸ = 0. Cancellation is a signed vector sum, not a sum of magnitudes. Physical check The zero lies nearer the smaller source, where its weaker mass is compensated by a shorter distance.

Question 1

The field cancellation point lies nearer the smaller source

Fixed point sources MM and 9M9M lie at x=0x=0 and x=dx=d. A negligible test mass can be placed on their line.

Diagram shown in the original SVG worksheet.

  1. Find every finite point on the line where the total gravitational field is zero.

  2. Explain why adding field magnitudes instead of signed components would miss the cancellation.

Question 1 - Solution

The field cancellation point lies nearer the smaller source

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For 0<x<d0<x<d, the left source attracts left and the right source attracts right: gx=−GMx2+9GM(d−x)2.g_x=-\frac{GM}{x^2}+\frac{9GM}{(d-x)^2}. Setting gx=0g_x=0 and taking positive distances, d−x=3x,x=d/4.d-x=3x,\qquad \boxed{x=d/4}. For x<0x<0 both fields point right; for x>dx>d both point left. There are no other finite zeros.

(b) Result and interpretation

At the cancellation point, g1x=−16GMd2,g2x=9GM(3d/4)2=16GMd2.g_{1x}=-\frac{16GM}{d^2},\quad g_{2x}=\frac{9GM}{(3d/4)^2}=\frac{16GM}{d^2}. g1x+g2x=0,|g1x|+|g2x|=32GMd2≠0.g_{1x}+g_{2x}=0,\qquad |g_{1x}|+|g_{2x}|=\frac{32GM}{d^2}\ne0. Cancellation is a signed vector sum, not a sum of magnitudes.

Physical check

The zero lies nearer the smaller source, where its weaker mass is compensated by a shorter distance.