Planets and Satellites: Kepler's Laws — Question 6

Section 13-6 · Physics pages 2002–2003

Question 6 A binary period measures total mass and a relative semimajor axis Two isolated stars have masses in ratio M1/M2 = 3. The semimajor axis of their relative separation is a = 1010 m and the period is T = 2 × 106 s. Use T 2 = 4π2a3/[G(M1 + M2)] and G = 6.67 × 10−11 SI. M1 M2 Circular illustration of the barycentric geometry; the semimajor-axis relations also hold for ellipses. (a) Find their total mass and individual masses. (b) Find the two semimajor axes about the common mass center.
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Question 6 - Solution A binary period measures total mass and a relative semimajor axis M1 M2 (a) Derivation and calculation The relative orbit measures total mass: Mtot = 4π2a3 GT 2 = 4π2(1010)3 (6.67 × 10−11)(2 × 106)2 = 1.47970 × 1029 kg. With mass ratio 3 : 1, M1 = 3 4Mtot = 1.10978 × 1029 kg , M2 = 1 4Mtot = 3.69925 × 1028 kg . (b) Result and interpretation The center-of-mass conditions are M1a1 = M2a2, a1 + a2 = a. Therefore a1 = M2 Mtot a = 2.5 × 109 m , a2 = M1 Mtot a = 7.5 × 109 m . The period formula uses the relative axis a = a1 + a2. Physical check The more massive star has the smaller orbit, and the two semimajor axes sum to the stated relative separation axis.

Question 6

A binary period measures total mass and a relative semimajor axis

Two isolated stars have masses in ratio M1/M2=3M_1/M_2=3. The semimajor axis of their relative separation is a=1010ma=10^{10}\,\mathrm m and the period is T=2×106sT=2\times10^6\,\mathrm s. Use T2=4π2a3/[G(M1+M2)]T^2=4\pi^2a^3/[G(M_1+M_2)] and G=6.67×10−11G=6.67\times10^{-11} SI.

Diagram shown in the original SVG worksheet.

  1. Find their total mass and individual masses.

  2. Find the two semimajor axes about the common mass center.

Question 6 - Solution

A binary period measures total mass and a relative semimajor axis

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The relative orbit measures total mass: Mtot=4π2a3GT2=4π2(1010)3(6.67×10−11)(2×106)2=1.47970×1029kg.M_{\mathrm{tot}}=\frac{4\pi^2a^3}{GT^2} =\frac{4\pi^2(10^{10})^3}{(6.67\times10^{-11})(2\times10^6)^2} =1.47970\times10^{29}\ \mathrm{kg}. With mass ratio 3:13:1, M1=34Mtot=1.10978×1029kg,\boxed{M_1=\tfrac34M_{\mathrm{tot}}=1.10978\times10^{29}\ \mathrm{kg}}, M2=14Mtot=3.69925×1028kg.\boxed{M_2=\tfrac14M_{\mathrm{tot}}=3.69925\times10^{28}\ \mathrm{kg}}.

(b) Result and interpretation

The center-of-mass conditions are M1a1=M2a2,a1+a2=a.M_1a_1=M_2a_2,\qquad a_1+a_2=a. Therefore a1=M2Mtota=2.5×109m,\boxed{a_1=\frac{M_2}{M_{\mathrm{tot}}}a=2.5\times10^9\ \mathrm m}, a2=M1Mtota=7.5×109m.\boxed{a_2=\frac{M_1}{M_{\mathrm{tot}}}a=7.5\times10^9\ \mathrm m}. The period formula uses the relative axis a=a1+a2a=a_1+a_2.

Physical check

The more massive star has the smaller orbit, and the two semimajor axes sum to the stated relative separation axis.