During a rescue operation, a 53oo-kg helicopter hovers about a fixed point. The helicopter blades send air downward with a speed of 62 m/s. What mass of air must pass through the blades every second to produce enough thrust for the helicopter to hover?
Remember that we can express change in momentum, the impulse as the integral of Force with respect to (wrt) time, \[ \Delta p = I = \int F \ dt \] That in turn means that we can also express Force as the derivative of p wrt time \[ F = \frac{dp}{dt} \] From this we can recover the usual expression, Newton's law, F=ma when mass is constant because \[ F = \frac{dp}{dt} = \frac{d \ }{dt} (mv) = m \frac{d \ }{dt} v = ma \] But in the case of the helicopter, what we are measuring is the impulse of the thrust from the air moved by the propeller, call it \( F_p \) and m is what is changing and v is constant, hence \[ F_p = \frac{d \ }{dt} (mv) = v \frac{dm}{dt} \] Now, if the aircraft is hovering, the force from the thrust of the propeller must exactly equal the gravitational force, \( F_g = Mg \), where M is the mass of the helicopter. Hence \( F_g = F_p \), i.e., \[ Mg = v \frac{dm}{dt} \] You now just need to solve for dm/dt.
[ Or to put it in simpler terms without derivatives, Force x time = Impulse = Change in momentum = Change in (mass x velocity): \[ F \Delta t = I = \Delta p = v \Delta m \] Hence \[ F = v \frac{\Delta m}{\Delta t} \]
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