To escape the Solar system in the single-Sun approximation, the heliocentric specific orbital energy must reach zero. At Earth's orbital radius, the required heliocentric escape speed is . The smallest change from Earth's initial velocity is prograde, parallel to its motion:
Combining the terrestrial and solar energy requirements gives
The asymptotic heliocentric trajectory is a parabolic Kepler orbit; larger launch speeds can give positive solar orbital energy.

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