Abstract

An obvious strategy to escape from a stable circular orbit in the Schwarzschild spacetime is to employ a tangential instantaneous acceleration. Using the theory of optimal rocket trajectories in general relativity, recently developed in Henriques and Natário (J Optim Theory Appl 154:500–552; 2011), we show that this manoeuvre satisfies the optimality conditions for maximizing the rocket’s final energy (given a fixed amount of fuel) if and only if the magnitude of the acceleration is smaller than a certain bound. This is the general relativistic version of a result by Lawden (J Brit Interplan Soc 12:68–71; 1953).

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