Lift Coefficient vs Angle of Attack (CL-α curve)
The CL-α curve (often "lift curve") shows how the lift coefficient CL varies with the angle of attack α. It is the most important characteristic of an airfoil.
Typical course
CL
| *
| * ← α_stall
| * \
| * \
| * \___ ← stall region
|*
+-------------- α
α_0 α_stall
Regions
1. Linear region (small to medium α)
- Slope: dCL/dα ≈ 2π per radian (theoretical, thin airfoil in ideal fluid) or ≈ 0.1 per degree in practice.
- CL = CL₀ + a · α (a ≈ 0.1 /°).
- Symmetric airfoil: CL₀ = 0, so CL = 0 at α = 0°.
- Cambered airfoil: CL₀ > 0, so CL > 0 at α = 0°. NACA 2412 typically CL₀ ≈ 0.2.
2. Near stall (α near α_stall)
- Curve flattens → CL_max reached.
- CL_max for typical GA airfoils: 1.2 to 1.8 (no flaps); with flaps 1.8–2.4.
3. Stall region (α > α_stall)
- CL drops abruptly.
- Boundary layer separates, flow stall.
- Recovery: reduce angle of attack.
Typical values
| Parameter | Value (typical GA) | Source |
|---|---|---|
| α_zero-lift α₀ (cambered) | −1° to −3° | NACA Reports |
| dCL/dα (slope) | 0.1 per degree | Anderson Ch. 4 |
| α_stall | 14°–18° (airfoil); 10°–12° (wing) | FAA AFH |
| CL_max | 1.2–1.8 without flaps, up to 2.5 with flaps | NACA 2412 |
Why does CL drop after stall?
At small α: flow follows the profile cleanly (laminar/turbulent boundary layer attached).
At critical α (α_stall): adverse pressure gradient on upper surface becomes too large → boundary layer separates.
At α > α_stall: massive separation → large vortex region above airfoil → CL drops dramatically, CD rises sharply.
Wing stall vs airfoil stall
Airfoil (2D): α_stall typically 14–18°. Wing (3D): α_stall typically 10–12°, because wingtip vortices and downwash reduce the effective α at the tips — root stalls first (in a normally designed wing with washout).
Flap influence
Flaps raise CL_max and shift the CL-α curve up and left:
- CL_max can rise from 1.4 to 2.4.
- α_stall can drop from 16° to 12° (flaps "increase" effective airfoil AoA).
- CL₀ becomes more negative (flaps add camber).
Source: FAA AFH Chapter 5.
Practical consequences
- CL_max sets stall speed: higher CL_max → lower Vs.
- Flaps for approach/landing: lower Vapp possible.
- Manoeuvring speed Va: at CL_max the maximum g-factor is also limited.
- Spin: asymmetric stall (one wing earlier) → autorotation.
What happens exactly in stall? (see lesson "Stall / Flow Separation")
- Nose drops (no lift despite high α).
- Speed falls (at constant pitch).
- Recovery: yoke forward (reduce α), increase power, then pitch up.