Orbits
A short lesson with diagrams, a worked example, a problem to try, and a quick check. Then quiz yourself on 5 practice questions.
Gravity provides the centripetal force for a circular orbit, giving v = √(GM/r). In any orbit, gravity points at the planet’s center, so it makes no torque about it: angular momentum is conserved. Total energy E = K + U is conserved too.
1. Circular orbits
A higher orbit is slower (smaller K) but has more total energy (E is less negative). Moving up takes energy from the rockets.
Escape speed: E = 0, so ½mv² = GMm/R and vesc = √(2GM/R), √2 times the circular orbital speed at that radius.
2. Elliptical orbits
At the two ends of the ellipse, v ⊥ r, so conserving L gives r1v1 = r2v2.
Energy is also conserved: ½mv1² − GMm/r1 = ½mv2² − GMm/r2. Together these two equations solve most orbit problems.
3. Example, then try it
A satellite orbits Earth (GM = 4.0 × 10¹⁴ m³/s²) at r = 6.8 × 10⁶ m. Find its speed and period.
v = √(4.0 × 10¹⁴ ÷ 6.8 × 10⁶) ≈ 7.7 × 10³ m/s.
T = 2πr/v = 2π(6.8 × 10⁶) ÷ 7.7 × 10³ ≈ 5.6 × 10³ s, about 93 minutes.
A 500 kg satellite moves from a circular orbit of radius 7.0 × 10⁶ m to one twice as large. Using GM = 4.0 × 10¹⁴ m³/s², find its kinetic and total energy in each orbit, the energy its rockets must supply, and how its period changes.
Lower orbit: K = GMm/(2r) = (4.0 × 10¹⁴)(500) ÷ (1.4 × 10⁷) ≈ 1.43 × 10¹⁰ J; E = −K ≈ −1.43 × 10¹⁰ J.
Higher orbit (2r): K ≈ 7.1 × 10⁹ J; E ≈ −7.1 × 10⁹ J. Slower, but more total energy.
Energy needed: ΔE ≈ −7.1 × 10⁹ − (−1.43 × 10¹⁰) ≈ +7.1 × 10⁹ J.
Period: T ∝ r3/2, so it grows by 23/2 ≈ 2.8 times.
Answer: K halves, E rises by 7.1 × 10⁹ J, and the period grows 2.8×.
4. Common mistakes
At which point of an elliptical orbit is a satellite moving fastest?
Angular momentum is conserved, and at the ends of the ellipse L = mvr. The smallest r gives the largest v.
Ready to practice?
5 questions on Orbits, each with a hint and an explanation for every wrong answer.
