Satellite OrbitsJEE Main

Orbital & escape speed, Kepler's third law — interactive Physics simulation for IIT-JEE.

Concept

A satellite stays in orbit because gravity supplies exactly the centripetal force it needs. Balancing the two gives a unique orbital speed at each radius. Reaching escape speed (2\sqrt2 times larger) lets it leave the body entirely.

Key formula

vo=GMr,ve=2GMr=2vo,T=2πr3GMv_o = \sqrt{\frac{GM}{r}}, \quad v_e = \sqrt{\frac{2GM}{r}} = \sqrt2\,v_o, \quad T = 2\pi\sqrt{\frac{r^3}{GM}}

Derivation

Set gravity equal to the centripetal requirement: GMmr2=mvo2r\dfrac{GMm}{r^2} = \dfrac{mv_o^2}{r}, giving vo=GM/rv_o = \sqrt{GM/r}.

Escape speed comes from energy: 12mve2=GMmr\tfrac12 mv_e^2 = \dfrac{GMm}{r}, so ve=2GM/rv_e = \sqrt{2GM/r}.

The period follows from vo=2πr/Tv_o = 2\pi r/T, yielding Kepler's third law T2r3T^2 \propto r^3.

Scenarios to explore

  • Satellite Orbits — Orbital & escape speed, Kepler's third law.

Real-world applications

  • Geostationary communication satellites (T = 1 sidereal day).
  • Low-Earth-orbit imaging satellites (period ≈ 90 min).
  • Planning interplanetary launch windows.

JEE exam tips

  • vov_o at the surface (h=0h=0) for Earth ≈ 7.9 km/s; vev_e ≈ 11.2 km/s.
  • Total orbital energy E=GMm2rE = -\dfrac{GMm}{2r} — negative means bound.

Common mistakes

  • Using altitude instead of orbital radius r=R+hr = R + h from the centre.
  • Forgetting orbital speed decreases with altitude (higher = slower).
  • Mixing up ve=2vov_e = \sqrt2\,v_o direction — escape is the larger one.

Exam traps to avoid

  • Orbital speed is independent of the satellite's mass.
  • A higher orbit has more total energy (less negative) yet a smaller speed.