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Question: Fan of a remote operated model helicopter of mass $m$ has diameter $d$. Denoting density of air by $...

Fan of a remote operated model helicopter of mass mm has diameter dd. Denoting density of air by ρ\rho and acceleration of free fall by gg, deduce expression for the minimum power required for take-off.

Answer

2(mg)3/2dρπ\frac{2(mg)^{3/2}}{d\sqrt{\rho \pi}}

Explanation

Solution

  1. For take-off, the upward lift force must equal the helicopter's weight mgmg.

  2. The lift force is generated by pushing air downwards. Using a simplified model where the force exerted by the fan on the air is F=ρAv2F = \rho A v^2, where AA is the fan area and vv is the speed of the air pushed downwards.

  3. The fan area is A=π(d/2)2=πd2/4A = \pi (d/2)^2 = \pi d^2/4.

  4. Setting lift equal to weight: ρ(πd2/4)vmin2=mg\rho (\pi d^2/4) v_{min}^2 = mg.

  5. Solve for the minimum air speed vmin=4mgρπd2=2dmgρπv_{min} = \sqrt{\frac{4mg}{\rho \pi d^2}} = \frac{2}{d}\sqrt{\frac{mg}{\rho \pi}}.

  6. The power required to push the air downwards is P=Fv=(ρAv2)v=ρAv3P = F v = (\rho A v^2) v = \rho A v^3.

  7. The minimum power is Pmin=ρAvmin3P_{min} = \rho A v_{min}^3.

  8. Substitute AA and vminv_{min}: Pmin=ρ(πd2/4)(2dmgρπ)3=ρπd248d3(mgρπ)3/2=2πd(mg)3/2(ρπ)3/2=2πd(mg)3/2ρ3/2π3/2=2d(mg)3/2ρ1/2π1/2=2(mg)3/2dρπP_{min} = \rho (\pi d^2/4) \left(\frac{2}{d}\sqrt{\frac{mg}{\rho \pi}}\right)^3 = \rho \frac{\pi d^2}{4} \frac{8}{d^3} \left(\frac{mg}{\rho \pi}\right)^{3/2} = \frac{2\pi}{d} \frac{(mg)^{3/2}}{(\rho \pi)^{3/2}} = \frac{2\pi}{d} \frac{(mg)^{3/2}}{\rho^{3/2} \pi^{3/2}} = \frac{2}{d} \frac{(mg)^{3/2}}{\rho^{1/2} \pi^{1/2}} = \frac{2(mg)^{3/2}}{d\sqrt{\rho \pi}}.

Answer: The expression for the minimum power required for take-off is 2(mg)3/2dρπ\frac{2(mg)^{3/2}}{d\sqrt{\rho \pi}}.