Gravitation Near Earth's Surface — Question 1

Section 13-3 · Physics pages 1932–1933

Question 1 Half of surface gravity occurs well above a nearby mountaintop Treat Earth as a nonrotating sphere of radius R. Outside it, g(r) = GM/r2 and g0 = GM/R2. R r Spherical central body; radii are measured from its center. (a) Find the altitude h where g = g0/2. (b) For h = .01R, find the exact gravity ratio and compare with the linear approximation.
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Question 1 - Solution Half of surface gravity occurs well above a nearby mountaintop R r (a) Derivation and calculation For x = h/R, the exterior inverse-square law gives g(h) g0 = ( R R + h )2 = (1 + x)−2. For half gravity, (1 + x)2 = 2, h = ( √ 2 −1)R ≃.414214R . (b) Result and interpretation At h = .01R, g/g0 = 1/1.012 = 0.98029605 . The small-altitude expansion is (1 + x)−2 = 1 −2x + 3x2 + O(x3). First order gives 0.980000; its difference from the exact ratio is 2.9605 × 10−4. Physical check The expansion parameter is h/R; the half-gravity altitude is too large for a first-order estimate.

Question 1

Half of surface gravity occurs well above a nearby mountaintop

Treat Earth as a nonrotating sphere of radius RR. Outside it, g(r)=GM/r2g(r)=GM/r^2 and g0=GM/R2g_0=GM/R^2.

Diagram shown in the original SVG worksheet.

  1. Find the altitude hh where g=g0/2g=g_0/2.

  2. For h=.01Rh=.01R, find the exact gravity ratio and compare with the linear approximation.

Question 1 - Solution

Half of surface gravity occurs well above a nearby mountaintop

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For x=h/Rx=h/R, the exterior inverse-square law gives g(h)g0=(RR+h)2=(1+x)−2.\frac{g(h)}{g_0}=\left(\frac R{R+h}\right)^2=(1+x)^{-2}. For half gravity, (1+x)2=2,h=(2−1)R≃.414214R.(1+x)^2=2,\qquad\boxed{h=(\sqrt2-1)R\simeq.414214R}.

(b) Result and interpretation

At h=.01Rh=.01R, g/g0=1/1.012=0.98029605.\boxed{g/g_0=1/1.01^2=0.98029605}. The small-altitude expansion is (1+x)−2=1−2x+3x2+O(x3).(1+x)^{-2}=1-2x+3x^2+O(x^3). First order gives 0.9800000.980000; its difference from the exact ratio is 2.9605×10−42.9605\times10^{-4}.

Physical check

The expansion parameter is h/Rh/R; the half-gravity altitude is too large for a first-order estimate.