Trans-lunar injection
A spacecraft performs a trans-lunar injection burn to leave its circular parking orbit around Earth. This large propulsive maneuver uses a chemical rocket engine to increase velocity significantly. The burn changes the path from a circle into a highly eccentric ellipse. As the craft coasts toward the Moon, it follows an elliptical orbit with an apogee near the lunar distance. Mission planners time this burn so the spacecraft reaches that far point just as the Moon arrives at the same location in space. The vehicle then enters the Moon's sphere of influence and executes a hyperbolic swingby. Typical transfers approximate Hohmann trajectories for short duration missions without external gravitational perturbations.
Engineers designed specific TLI burns to target free return trajectories during early human spaceflight programs. Such paths allow a spacecraft to loop behind the Moon and return to Earth without further propulsion. Apollos 8, 10, and 11 began on these safe arcs before later missions adopted hybrid trajectories requiring course corrections. These designs added critical margins of safety for crews traveling beyond low Earth orbit. A failure in the main engine would still guarantee a return home under gravity alone. The initial burn sets the entire mission architecture for potential emergency scenarios. Ground controllers monitored these parameters closely throughout the Apollo era.
Mission designers use patched conics to simplify lunar transfer calculations for rough studies. This method assumes acceleration occurs only under classical two-body dynamics dominated by Earth until reaching the Moon's sphere of influence. Motion within such systems remains deterministic and simple enough for back-of-the-envelope estimates. More realistic models treat the spacecraft as subject to restricted three-body problems involving both Earth and Moon. Henri Poincaré published foundational work on celestial mechanics methods between 1892 and 1899 that supports this approach. Numerical calculation becomes necessary since analytic solutions do not exist for complex gravitational interactions. Detailed simulations must account for solar radiation pressure and non-uniform gravity fields from both bodies.
The Soviet Union launched Luna 1 on the 2nd of January 1959 as the first probe attempting trans-lunar injection. That burn missed the target by more than three times the Moon's radius and sent the craft into heliocentric orbit instead. Luna 2 performed the same maneuver accurately on the 12th of September 1959 before crashing into the lunar surface two days later. The Soviets repeated these successes with twenty-two additional Luna missions and five Zond missions traveling to the Moon between 1959 and 1976. These early attempts established the technical foundation for future lunar exploration efforts worldwide. Ground teams analyzed telemetry data to refine trajectory calculations after each launch failure or success.
NASA used restartable J-2 engines in the S-IVB third stage of Saturn V rockets for Apollo TLI burns. Each burn lasted approximately 350 seconds while providing velocity changes between 3.05 and 3.25 kilometers per second. The spacecraft reached speeds near 10.4 kilometers per second relative to Earth after the engine cutoff. Observers from Hawaii saw the Apollo 8 firing in the pre-dawn sky south of Waikiki on the 21st of December 1968. Papers reported the next day that the burn was visible from the ground as a bright object moving across the horizon. Apollo 10's pre-dawn TLI appeared over Cloncurry, Australia in May 1969 like car headlights coming through fog. Witnesses described the craft as a bright comet with a greenish tinge against the dark sky.
Japan launched Hiten in 1990 to explore novel low delta-v transfer methods taking six months instead of three days. Clementine followed in 1994 using a three-week trajectory with two intermediate Earth flybys before lunar orbit insertion. Asiasat-3 became the first commercial satellite reaching the Moon's sphere of influence after a launch failure in 1997. It passed within 6200 kilometers of the surface during its swingby maneuvers. SMART-1 used solar-powered ion engines for propulsion starting in 2003 and took over thirteen months to reach lunar orbit. China placed Chang'e 1 into lunar orbit in 2007 using multiple burns to slowly raise apogee toward the target. Israel Aerospace Industries attempted a similar maneuver with Beresheet in 2019 though the lander crashed upon arrival.
Up Next
Continue Browsing
Common questions
What is trans-lunar injection and how does it work?
Trans-lunar injection is a large propulsive maneuver that uses a chemical rocket engine to increase velocity significantly. This burn changes the spacecraft path from a circular parking orbit into a highly eccentric ellipse with an apogee near lunar distance.
When did the Soviet Union first attempt trans-lunar injection?
The Soviet Union launched Luna 1 on the 2nd of January 1959 as the first probe attempting trans-lunar injection. That mission missed the target by more than three times the Moon's radius and sent the craft into heliocentric orbit instead.
How long did Apollo missions take to reach the Moon after trans-lunar injection?
Japan launched Hiten in 1990 to explore novel low delta-v transfer methods taking six months instead of three days. SMART-1 used solar-powered ion engines for propulsion starting in 2003 and took over thirteen months to reach lunar orbit.
Why do engineers design specific TLI burns for free return trajectories?
Engineers designed specific TLI burns to target free return trajectories during early human spaceflight programs such paths allow a spacecraft to loop behind the Moon and return to Earth without further propulsion. A failure in the main engine would still guarantee a return home under gravity alone.
What speed does a spacecraft achieve relative to Earth after trans-lunar injection?
Each burn lasted approximately 350 seconds while providing velocity changes between 3.05 and 3.25 kilometers per second. The spacecraft reached speeds near 10.4 kilometers per second relative to Earth after the engine cutoff.