K^2
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Yeah, for hovering, the equations are similar. Though, mass flow rate has to be factored in separately.rcgldr said:Still switch this case to a rocket "hovering" above the moon (no atmosphere), the rocket isn't moving, so no work done on the rocket, only on the propellent expelled from the rocket. This is a similar case to the hovering helicopter (the heli doesn't move, only the air). I think it's a reasonable comparason.
So let's see...
F = mg = -\dot{m} V_p
P = -\frac{1}{2} V_p^2 \dot{m}
\dot{m} = -\frac{mg}{V_p}
P = \frac{1}{2} mgV_p
m(t) = m_0 e^{-\frac{gt}{V_p}}
P(t) = \frac{1}{2} m_0 gV_p e^{-\frac{gt}{V_p}}
Ok, maybe not so similar, but the mg term is the same.