So the Oberth effect is a little application of kinetic energy in classical mechanics. Essentially, since KE is proportional to $v^2$, at higher velocities a change in kinetic energy produces a greater change in velocity. This has applications in orbital mechanics, especially Hohmann transfers.
How does the derivation of the Oberth effect change in a relativistic setting? I know that one effect of relativity is an asymptote at $c$ where as you approach, more energy to further approach, but does the Oberth effect still hold in its entirety?