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Orbital Energy Formula

Calculate the total mechanical energy of an orbiting satellite or planet.
Negative orbital energy means the object is gravitationally bound.

The Formula

E = −GMm / (2a)

The total mechanical energy of an orbiting body is the sum of its kinetic energy and gravitational potential energy. The result is always negative for a bound orbit — negative energy means the object is gravitationally captured. A positive total energy means the object has enough speed to escape to infinity (hyperbolic trajectory).

Variables

SymbolMeaningUnit
ETotal mechanical energy of the orbitJoules (J)
GGravitational constant = 6.674 × 10⁻¹¹ N·m²/kg²N·m²/kg²
MMass of the central body (planet, star, etc.)kg
mMass of the orbiting satellite or objectkg
aSemi-major axis of the orbit (radius for circular orbits)meters (m)

For a circular orbit, this simplifies because a = r and the orbital speed is v = √(GM/r):

E = −½mv²

The orbital energy depends only on the semi-major axis — not the eccentricity of the orbit. Two orbits with the same semi-major axis have the same energy, even if one is circular and the other is highly elliptical.

Example 1 — International Space Station

The ISS orbits at approximately 408 km altitude. Calculate its orbital energy per kilogram of spacecraft mass.

a = 6371 + 408 = 6779 km = 6.779 × 10⁶ m

G × M_Earth = 3.986 × 10¹⁴ m³/s² (standard gravitational parameter)

E/m = −GM/(2a) = −3.986 × 10¹⁴ / (2 × 6.779 × 10⁶)

E/m ≈ −29.4 MJ/kg. The ISS has 29.4 megajoules of negative orbital energy per kilogram of its mass.

Example 2 — Changing Orbits

A 1000 kg satellite moves from a circular orbit at 300 km altitude to 600 km altitude. How much energy must be added?

a₁ = 6371 + 300 = 6671 km = 6.671 × 10⁶ m

a₂ = 6371 + 600 = 6971 km = 6.971 × 10⁶ m

E₁ = −GM × m/(2a₁) = −3.986 × 10¹⁴ × 1000 / (2 × 6.671 × 10⁶) = −29.85 GJ

E₂ = −3.986 × 10¹⁴ × 1000 / (2 × 6.971 × 10⁶) = −28.58 GJ

ΔE = E₂ − E₁ = 1.27 GJ must be added by rocket thrust to raise the orbit

When to Use It

Use the orbital energy formula when:

  • Calculating the energy cost of launching satellites to different altitudes
  • Determining whether an orbit is bound (E < 0), parabolic (E = 0), or hyperbolic (E > 0)
  • Analyzing Hohmann transfers between circular orbits
  • Computing orbital periods using Kepler's third law (T² ∝ a³)

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