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Hohmann Transfer Orbit

Quick answer

A Hohmann transfer is the classic two-burn route between circular orbits: one burn stretches the orbit into an ellipse touching the destination altitude, a second circularises on arrival. For most orbit pairs it is the minimum-fuel transfer — the default path from LEO toward GEO.

📘 Full definition✓ Reviewed 2026-09-07
The Hohmann transfer, published by Walter Hohmann in 1925, moves a spacecraft between two circular, coplanar orbits using two engine burns and an elliptical bridge. Burn one, at the departure orbit, adds velocity to raise the far side of the orbit — apogee — to the destination altitude, creating a transfer ellipse that just kisses both circles. The spacecraft coasts half a revolution, then burn two at apogee adds the velocity needed to circularise. For destination radii less than about 11.9 times the starting radius it is the most delta-v-efficient two-impulse transfer, which made it the backbone of practical astronautics: the geostationary transfer orbit is precisely a Hohmann first leg, and interplanetary trajectories generalise the idea to orbits around the Sun, complete with the launch windows that arise from waiting for planets to align. The economy has a cost — time (the transfer takes half the ellipse's period, months to Mars) — and the pattern breaks where three-body dynamics, low-thrust spirals or gravity assists offer cheaper if slower routes.
Burns Required
2
LEO→GEO Total ΔV
3.9 km/s
Transfer Time (LEO→GEO)
5 hours
Invented
1925 (Walter Hohmann)

Understanding Hohmann Transfer

The numbers for LEO to GEO

From a 300 km parking orbit, burn one adds about 2.4 km/s, stretching apogee to 35,786 km; after a five-and-a-quarter-hour coast, burn two at apogee adds roughly 1.5 km/s (bundled, in practice, with the plane change to zero inclination). Around 3.9 km/s total — the sum every GEO mission budget is built on, whether spent by an upper stage in hours or an electric thruster over months of spiralling.

Phasing: arriving where the target is

Transfers to a destination — a station, a rendezvous — must arrive at an occupied point, not just an altitude. Because lower orbits move faster, a chaser adjusts its altitude to drift relative to the target, then times the Hohmann legs so both bodies reach the meeting point together. Rendezvous choreography, from cargo craft to interceptors, is Hohmann arithmetic plus patience.

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Frequently Asked Questions

Both burns fire along the velocity vector at the points of maximum leverage — the Oberth logic. Any transfer that leaves and arrives tangentially wastes nothing steering; the Hohmann ellipse is the unique orbit tangent to both circles, so all propellant goes into changing energy, none into changing direction.
At extreme ratios — beyond roughly 11.9:1 in radius — a bi-elliptic transfer (flying far out, adjusting there where velocity is tiny, then falling back) beats it despite three burns. Continuous low-thrust spirals also abandon Hohmann geometry entirely, trading months of thrusting for chemical stages saved.
The transfer ellipse takes a fixed ~8.5 months to cross from Earth's orbit to Mars's, so Mars must be positioned to arrive at the meeting point when the spacecraft does. That geometry recurs roughly every 26 months — the synodic rhythm that clusters Mars launches into famous windows.

Sources & References

Definitions are reviewed against primary sources. Last reviewed: 2026-09-07.