Three controls, three different aerodynamic effects
Shape of the mean line
Camber is the curvature of an airfoil. A positively cambered airfoil can produce positive lift even at zero geometric angle of attack because its zero-lift angle is shifted negative.
Controls dynamic pressure
Dynamic pressure is q = ½ρV². If every other quantity remains unchanged, doubling speed produces four times the dynamic pressure and therefore four times the lift.
Changes lift coefficient
Angle of attack is the angle between the wing chord line and the relative wind. Before stall, increasing α usually increases CL approximately linearly.
L = q S CL, q = ½ρV², CL ≈ a(α − α₀) before stallWhy airflow changes direction
For positive lift, the wing turns the surrounding airflow downward. The air exerts an equal and opposite aerodynamic force on the wing. Pressure differences around the airfoil and the momentum change in the airflow are two consistent ways of describing the same fluid-dynamic interaction.
What this tutorial is modeling
This page uses an educational, quasi-steady aerodynamic model. The attached-flow region follows a typical lift-curve slope, camber shifts the zero-lift angle, and a simple post-stall decay represents flow separation. It is not a CFD solver and should not be used for aircraft design, certification, or flight planning.
Change the wing and flight condition
The three large controls are the ones to explore first. Advanced values are supplied so the page can turn the dimensionless lift coefficient into an actual force.
Advanced aircraft and atmosphere inputs
Airfoil and relative airflow
Attached flowWhat the forces mean for the aircraft
Force balanceWhy more angle of attack eventually gives less lift
Attached-flow region
At modest angle of attack, the boundary layer largely remains attached to the upper surface. Lift coefficient increases approximately linearly with α.
Adverse pressure gradient strengthens
As the flow moves toward the trailing edge, it must recover toward ambient pressure. At high α, this pressure recovery becomes difficult for the slower boundary-layer air.
Flow separates
The boundary layer can reverse locally and separate from the surface. A broad turbulent wake forms over part of the upper surface.
Lift falls and drag rises
Once significantly stalled, increasing α no longer produces the pre-stall lift increase. The lift coefficient drops from its peak while drag grows strongly.
Lift curve for the current camber
The curve is generated from the same simplified educational model used by the simulator. The current angle of attack is marked on the curve.
Use the simulator like a small wind tunnel
Choose a preset, observe the visual and force outputs, then change only one control at a time.
Experiment A · Camber
Compare presets 1 and 2. The geometric angle of attack stays at 0°, but positive camber moves the zero-lift angle negative, so the cambered wing develops positive lift.
Experiment B · Speed squared
Compare presets 3 and 4. The aerodynamic coefficients stay approximately the same because α and camber are unchanged, but increasing speed from 25 to 50 m/s multiplies dynamic pressure and aerodynamic forces by about four.
Experiment C · Stall
Compare presets 5 and 6. The larger angle does not guarantee more lift. After the critical angle, the separated-flow model reduces CL and raises drag.
Useful values and relationships
| Quantity | Typical educational value or range | Why it matters |
|---|---|---|
| Sea-level standard air density | about 1.225 kg/m³ | Lift is directly proportional to density. |
| Dynamic pressure | q = ½ρV² | Contains the speed-squared effect. This is why speed changes aerodynamic force so strongly. |
| Airfoil camber | 0–6% of chord is a useful classroom exploration range | Positive camber typically shifts the zero-lift angle to a negative value and changes maximum lift behavior. |
| Pre-stall lift-curve slope | often roughly 0.08–0.11 per degree for many subsonic wing/airfoil examples | Explains the near-linear increase of CL with α before nonlinear effects dominate. |
| Critical angle of attack | often roughly 12–18° for conventional subsonic airfoils, but highly configuration-dependent | Beyond this angle, significant separation can cause stall. |
| Reynolds number | Re = ρVc/μ | Changes boundary-layer behavior, transition, drag, and stall characteristics. Real stall cannot be predicted from α alone. |