Satellites: Orbits and Energy — Question 7

Section 13-7 · Physics pages 2024–2025

Question 7 Matching a rotation period is necessary but not sufficient for a stationary sky position A spherical planet has µ = 3.986 × 1014 m3/s2, radius R = 6.378 × 106 m, and rotation period T = 86164 s. Ignore perturbations. r v equatorial plane Equatorial prograde circular motion must share the planet's angular velocity. (a) Find the circular orbit radius and altitude for this period. (b) State the additional geometric and directional requirements for a satellite to remain above one fixed surface longitude and latitude.
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Question 7 - Solution Matching a rotation period is necessary but not sufficient for a stationary sky position r v equatorial plane (a) Derivation and calculation Match circular orbital angular speed to planetary rotation: µ r2 = (2π T )2 r, r = ( µT 2 4π2 )1/3 . r = [ (3.986 × 1014)(86164)2 4π2 ]1/3 ≃4.2164 × 107 m . h = r −R ≃3.5786 × 107 m . (b) Result and interpretation A fixed surface-relative position requires e = 0, i = 0, Ωorbit = Ωplanet > 0. The orbit is circular, equatorial, and prograde. Then d dt(ϕsatellite −ϕsurface) = 0, λsatellite = 0. Inclination produces latitude motion; eccentricity produces nonuniform angular motion; retrograde rotation cannot keep the longitude fixed. Physical check The calculated radius is measured from the center, while altitude subtracts the planetary radius.

Question 7

Matching a rotation period is necessary but not sufficient for a stationary sky position

A spherical planet has μ=3.986×1014m3/s2\mu=3.986\times10^{14}\,\mathrm{m^3/s^2}, radius R=6.378×106mR=6.378\times10^6\,\mathrm m, and rotation period T=86164sT=86164\,\mathrm s. Ignore perturbations.

Diagram shown in the original SVG worksheet.

  1. Find the circular orbit radius and altitude for this period.

  2. State the additional geometric and directional requirements for a satellite to remain above one fixed surface longitude and latitude.

Question 7 - Solution

Matching a rotation period is necessary but not sufficient for a stationary sky position

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Match circular orbital angular speed to planetary rotation: μr2=(2πT)2r,r=(μT24π2)1/3.\frac{\mu}{r^2}=\left(\frac{2\pi}{T}\right)^2r, \qquad r=\left(\frac{\mu T^2}{4\pi^2}\right)^{1/3}. r=[(3.986×1014)(86164)24π2]1/3≃4.2164×107m.\boxed{r=\left[\frac{(3.986\times10^{14})(86164)^2}{4\pi^2}\right]^{1/3} \simeq4.2164\times10^7\ \mathrm m}. h=r−R≃3.5786×107m.\boxed{h=r-R\simeq3.5786\times10^7\ \mathrm m}.

(b) Result and interpretation

A fixed surface-relative position requires e=0,i=0,Ωorbit=Ωplanet>0.e=0,\quad i=0,\quad \Omega_{\mathrm{orbit}}=\Omega_{\mathrm{planet}}>0. The orbit is circular, equatorial, and prograde. Then ddt(ϕsatellite−ϕsurface)=0,λsatellite=0.\frac{d}{dt}(\phi_{\mathrm{satellite}}-\phi_{\mathrm{surface}})=0,\qquad \lambda_{\mathrm{satellite}}=0. Inclination produces latitude motion; eccentricity produces nonuniform angular motion; retrograde rotation cannot keep the longitude fixed.

Physical check

The calculated radius is measured from the center, while altitude subtracts the planetary radius.