INGENIA

FLD-13

Lift force

L = ½ ρ v² S C_L. The aerodynamic lift equation.

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FluidsLift

Governing equation

L=12ρv2SCLL=\tfrac12\rho v^2 S C_L

where

\rho
Density (kg/m³)
v
Speed (m/s)
S
Area ()
C_L
Lift coefficient ()
L
Lift (kN)

Lecture brief

Historical brief

Bernoulli, Navier–Stokes, Reynolds (1883) and Stokes drag made continuum flow a dimensionless craft. The sheets compute head, drag, Re and a pedagogical NS snapshot. This sheet (FLD-13 — Lift force) is the form associated with Lift. Working symbols: ρ\rho, vv, SS, CLC_L \rightarrow LL. C_L grows with angle of attack until stall. Circulation theorem of Kutta–Joukowski.

Purpose

Purpose: compute LL from ρ\rho, vv, SS, CLC_L in Fluid physics via L=12ρv2SCLL=\tfrac12\rho v^2 S C_L L = ½ ρ v² S C_L. The aerodynamic lift equation. Use it when a real fluid physics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given ρ=1.225kg/m3\rho = 1.225\,\mathrm{kg/m^{3}}, v=60.000m/sv = 60.000\,\mathrm{m/s}, S=16.000m2S = 16.000\,\mathrm{m^{2}}, CL=0.800C_L = 0.800\,\mathrm{—}, the governing relation L=12ρv2SCLL=\tfrac12\rho v^2 S C_L yields L=28.22kNL = 28.22\,\mathrm{kN}. A wing, a circulation, an upward arrow. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Lift L28.22 kN
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FLD-13 · projectile
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Narration of this film

A wing, a circulation, an upward arrow.

C_L grows with angle of attack until stall. Circulation theorem of Kutta–Joukowski.

Reading speed

Watch on YouTube