Planets and Satellites: Kepler's Laws — Question 5

Section 13-6 · Physics pages 2000–2001

Question 5 An orbital measurement determines the central gravitational parameter A negligible satellite has semimajor axis a = 2a0 and period T = T0. A reference system has central mass M0, semimajor axis a0 and period T0, also with negligible satellite mass. a/a0 M/M0 (1, 1) (2, 8) At equal period, the inferred central mass scales as the cube of semimajor axis. (a) Infer the first central mass in units of M0. (b) If measured a is biased high by 1% and T is exact, find the exact fractional mass bias.
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Question 5 - Solution An orbital measurement determines the central gravitational parameter a/a0 M/M0 (1, 1) (2, 8) (a) Derivation and calculation Kepler’s law determines the gravitational parameter: µ = GM = 4π2a3 T 2 , M M0 = ( a a0 )3 (T0 T )2 . With a = 2a0, T = T0, M = 8M0 . Converting the directly inferred GM to mass uses a value for G. (b) Result and interpretation If ameas = 1.01atrue while T is exact, Mmeas Mtrue = (1.01)3 = 1 + 3(.01) + 3(.01)2 + (.01)3. ∆M M = .030301 = 3.0301% . The differential estimate dM/M = 3, da/a gives 3% and omits the positive higher-order terms. Physical check The cubic dependence amplifies a positive semimajor-axis bias into a larger positive mass bias.

Question 5

An orbital measurement determines the central gravitational parameter

A negligible satellite has semimajor axis a=2a0a=2a_0 and period T=T0T=T_0. A reference system has central mass M0M_0, semimajor axis a0a_0 and period T0T_0, also with negligible satellite mass.

Diagram shown in the original SVG worksheet.

  1. Infer the first central mass in units of M0M_0.

  2. If measured aa is biased high by 1%1\% and TT is exact, find the exact fractional mass bias.

Question 5 - Solution

An orbital measurement determines the central gravitational parameter

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Kepler’s law determines the gravitational parameter: μ=GM=4π2a3T2,MM0=(aa0)3(T0T)2.\mu=GM=\frac{4\pi^2a^3}{T^2},\qquad \frac M{M_0}=\left(\frac a{a_0}\right)^3\left(\frac{T_0}T\right)^2. With a=2a0a=2a_0, T=T0T=T_0, M=8M0.\boxed{M=8M_0}. Converting the directly inferred GMGM to mass uses a value for GG.

(b) Result and interpretation

If ameas=1.01atruea_{\mathrm{meas}}=1.01a_{\mathrm{true}} while TT is exact, MmeasMtrue=(1.01)3=1+3(.01)+3(.01)2+(.01)3.\frac{M_{\mathrm{meas}}}{M_{\mathrm{true}}}=(1.01)^3 =1+3(.01)+3(.01)^2+(.01)^3. ΔMM=.030301=3.0301%.\boxed{\frac{\Delta M}{M}=.030301=3.0301\%}. The differential estimate dM/M=3,da/adM/M=3,da/a gives 3%3\% and omits the positive higher-order terms.

Physical check

The cubic dependence amplifies a positive semimajor-axis bias into a larger positive mass bias.