Hohmann Transfer Orbit Calculator
Calculate the delta-v required for the most fuel-efficient transfer between two circular orbits.
How Hohmann Transfer Orbits Work
A Hohmann transfer orbit is the most fuel-efficient method to move a spacecraft between two circular orbits around the same central body. Proposed by German engineer Walter Hohmann in 1925, it uses an elliptical transfer orbit that is tangent to both the initial and final circular orbits, requiring exactly two engine burns.
The Two-Burn Maneuver
The first burn (perigee burn) at the lower orbit accelerates the spacecraft into an elliptical transfer orbit. The spacecraft then coasts along this ellipse for half an orbital period until it reaches the higher orbit altitude. A second burn (apogee burn) circularizes the orbit at the target altitude. The total velocity change, or delta-v, is the sum of both burns.
The Hohmann Transfer Formulas
The delta-v for each burn is calculated using the vis-viva equation and orbital mechanics:
Δv1 = √(μ/r1) × (√(2r2/(r1+r2)) - 1)
Δv2 = √(μ/r2) × (1 - √(2r1/(r1+r2)))
The transfer time is half the orbital period of the transfer ellipse:
T = π × √((r1+r2)3 / (8×μ))
Comparison to Direct Burns
A direct, impulsive transfer at an arbitrary point in the orbit would require significantly more delta-v because the spacecraft would need to change both speed and direction simultaneously. The Hohmann transfer takes advantage of orbital mechanics by performing burns only at the points where the transfer ellipse naturally aligns with the circular orbits, minimizing wasted energy.
Real-World Applications
Hohmann transfers are used extensively in spaceflight. The transfer from Low Earth Orbit (LEO) to Geostationary Earth Orbit (GEO) is one of the most common, taking about 5.3 hours and requiring approximately 3.94 km/s of delta-v. Mars transfer orbits from Earth use a similar principle around the Sun, with a transit time of about 8.5 months. The Apollo missions used modified Hohmann-like transfers to reach the Moon.
Limitations
Hohmann transfers assume circular, coplanar orbits and instantaneous impulse burns. Real orbits have eccentricity, inclination differences, and finite burn times that require corrections. For very large orbit ratios (greater than 11.94:1), a bi-elliptic transfer with three burns can actually be more fuel-efficient despite taking longer.