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Lift

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Lift is the force of a fluid on a moving object perpendicular to the direction of motion. A plane stays up by pushing air down.

Why (momentum model, MacKay):

  • Newton 3: wings push air down ↔ air pushes wings up (= lift). Level flight (constant height): lift = MgMg
  • Newton 2: force = rate of change of momentum, F=Δ(mv)Δt=m˙ vF = \frac{\Delta(mv)}{\Delta t} = \dot m\, v → Mg=m˙air vliftMg = \dot m_{air}\, v_{lift} (like throwing 2 kg of balls down every second at 10 m/s → 20 N recoil upward)
  • Air deflected per second: the plane sweeps the area AliftA_{lift} at forward speed vv → m˙air=ρAliftv\dot m_{air} = \rho A_{lift} v vlift=MgρAliftvv_{lift} = \frac{Mg}{\rho A_{lift} v}
  • Power = kinetic energy given to that air per second: Plift=12m˙airvlift2=12(Mg)2Alift ρ vP_{lift} = \frac12 \dot m_{air} v_{lift}^2 = \frac12 \frac{(Mg)^2}{A_{lift}\,\rho\, v}

Why ∝1/v\propto 1/v: faster → more air per second → a smaller downward speed is enough → less energy (∝vlift2\propto v_{lift}^2).

Optimal speed: per distance, drag rises (∝v2\propto v^2) and lift cost falls (∝1/v2\propto 1/v^2) → there is a minimum: Ed=12cdragAdragρv2+12(Mg)2Aliftρv2\frac{E}{d} = \frac12 c_{drag} A_{drag} \rho v^2 + \frac12 \frac{(Mg)^2}{A_{lift}\rho v^2} ddv=0\frac{d}{dv} = 0 → at voptv_{opt} both terms are equal, and ρvopt2=MgcdragAdragAlift\rho v_{opt}^2 = \frac{Mg}{\sqrt{c_{drag} A_{drag} A_{lift}}}. Thinner air (high altitude) → higher voptv_{opt}, same minimum energy per distance.

Related: Drag, Buoyancy. Archimedes’ principle, Momentum and Force