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Power for an Orbital Maneuver

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A satellite of mass mm is in a stable circular orbit of radius rr around a planet of mass MM. The orbital radius is slowly increased at a rate of dr/dtdr/dt, such that the orbit remains nearly circular. Which of the following expressions represents the power required to sustain this change in orbital radius?

A

P=−GMm2r2drdtP = -\frac{GMm}{2r^2} \frac{dr}{dt}

B

P=GMm2r2drdtP = \frac{GMm}{2r^2} \frac{dr}{dt}

C

P=GMm4r2drdtP = \frac{GMm}{4r^2} \frac{dr}{dt}

D

P=GMm2r2drdtP = \frac{GMm}{2r^2} \frac{dr}{dt}

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