Gravitation Near Earth's Surface — Question 8

Section 13-3 · Physics pages 1946–1947

Question 8 Two altitude readings can separate planetary radius from mass For a spherical nonrotating planet, gravity is measured at the surface and at known altitude h. Their ratio is q = g(h)/g(0), with 0 < q < 1. M r g(0) g(h) h R Two gravity measurements share one radial baseline h; schematic dimensions. (a) Infer R and then GM from these measurements. (b) For q = 100/121 and h = 100 km, find R and explain the sensitivity when q is near one.
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Question 8 - Solution Two altitude readings can separate planetary radius from mass M r g(0) g(h) h R (a) Derivation and calculation The field ratio eliminates GM: q = GM/(R + h)2 GM/R2 = ( R R + h )2 . Solving √q(R + h) = R gives R = h√q 1 −√q , GM = g(0)R2 . (b) Result and interpretation For q = 100/121, √q = 10/11, so R = 10h = 1000 km . At fixed h, differentiation quantifies sensitivity: d ln R d ln q = 1 2(1 −√q), δR R ≃ 1 2(1 −√q) δq q . The amplification is 5.5 here and diverges as q →1. Physical check A ratio close to one corresponds to a short baseline compared with the inferred radius.

Question 8

Two altitude readings can separate planetary radius from mass

For a spherical nonrotating planet, gravity is measured at the surface and at known altitude hh. Their ratio is q=g(h)/g(0)q=g(h)/g(0), with 0<q<10<q<1.

Diagram shown in the original SVG worksheet.

  1. Infer RR and then GMGM from these measurements.

  2. For q=100/121q=100/121 and h=100kmh=100\,\mathrm{km}, find RR and explain the sensitivity when qq is near one.

Question 8 - Solution

Two altitude readings can separate planetary radius from mass

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The field ratio eliminates GMGM: q=GM/(R+h)2GM/R2=(RR+h)2.q=\frac{GM/(R+h)^2}{GM/R^2}=\left(\frac R{R+h}\right)^2. Solving q(R+h)=R\sqrt q(R+h)=R gives R=hq1−q,GM=g(0)R2.\boxed{R=\frac{h\sqrt q}{1-\sqrt q}},\qquad \boxed{GM=g(0)R^2}.

(b) Result and interpretation

For q=100/121q=100/121, q=10/11\sqrt q=10/11, so R=10h=1000km.\boxed{R=10h=1000\ \mathrm{km}}. At fixed hh, differentiation quantifies sensitivity: dln⁡Rdln⁡q=12(1−q),δRR≃12(1−q)δqq.\frac{d\ln R}{d\ln q}=\frac1{2(1-\sqrt q)},\qquad \frac{\delta R}{R}\simeq\frac{1}{2(1-\sqrt q)}\frac{\delta q}{q}. The amplification is 5.55.5 here and diverges as q→1q\to1.

Physical check

A ratio close to one corresponds to a short baseline compared with the inferred radius.