Quick Recap — Fields, Potential & Satellites

  • Variation of gg: with height gh=g(1−2hR)g_h = g\left(1 - \dfrac{2h}{R}\right) (for h≪Rh\ll R); with depth gd=g(1−dR)g_d = g\left(1 - \dfrac{d}{R}\right).
  • Gravitational potential V=−GMrV = -\dfrac{GM}{r} (a scalar); potential energy U=−GMmrU = -\dfrac{GMm}{r}; both are taken as zero at infinity.
  • Orbital velocity vo=GMrv_o = \sqrt{\dfrac{GM}{r}}, and ve=2 vov_e = \sqrt2\, v_o at the same radius.
  • Satellite energy: total E=−GMm2rE = -\dfrac{GMm}{2r}, with KE=∣E∣KE = |E| and PE=2EPE = 2E.
  • Geostationary satellite: period 24 h, orbiting over the equator at a height of about 36000 km.