Airfoil Lift & Drag: The Physics of Flight

simulator intermediate ~10 min
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Cl = 0.548 — generating 1821 N of lift at 60 m/s

A 1.5m chord airfoil at 5° angle of attack in standard sea-level air at 60 m/s generates a lift coefficient of 0.548 and a lift force of about 1821 N per meter of wingspan.

Formula

Lift: L = ½ × ρ × V² × S × Cl
Thin airfoil Cl: Cl = 2π × sin(α)
Drag polar: Cd = Cd0 + Cl² / (π × e × AR)

Why Wings Fly

The airfoil — a carefully shaped cross-section — is the fundamental element of flight. By curving the upper surface and angling the wing into the oncoming air, an airfoil creates a pressure difference: lower pressure above, higher pressure below. This pressure imbalance produces lift. The thin airfoil theory, derived by Max Munk in the 1920s, predicts that the lift coefficient grows linearly with angle of attack at a rate of 2π per radian — a remarkably accurate approximation for small angles.

The Drag Budget

Every aircraft designer fights drag. Parasitic drag — the friction and pressure drag from the aircraft's shape — grows with the square of airspeed. Induced drag — the unavoidable penalty of creating lift — actually decreases with speed. The total drag curve has a minimum at some optimum speed, and the corresponding maximum L/D ratio defines the aircraft's best glide performance. This simulation plots both force vectors so you can see how they change with angle and speed.

Stall: The Lift Cliff

As angle of attack increases, a point is reached where the airflow can no longer follow the curved upper surface. The boundary layer separates, turbulence engulfs the wing, and lift collapses while drag spikes. This is stall — the most critical flight condition pilots must understand. The simulation shows the approach to stall by modeling the nonlinear lift curve beyond the critical angle.

From Biplanes to Supercritical Wings

Airfoil design has evolved dramatically. The Wright brothers used thin, cambered profiles based on wind tunnel tests. NACA systematically cataloged airfoil families in the 1930s-40s. Modern supercritical airfoils, designed by Richard Whitcomb at NASA, flatten the upper surface to delay shock wave formation at transonic speeds — enabling jets to cruise faster with less wave drag. Each advance came from deeper understanding of the pressure distributions this simulation helps you explore.

FAQ

How does an airfoil generate lift?

An airfoil generates lift by deflecting airflow downward. The curved upper surface accelerates air (lowering pressure via Bernoulli's principle) while the angled lower surface pushes air downward (Newton's third law). Both mechanisms contribute — the net pressure difference across the wing creates an upward lift force proportional to speed squared.

What is angle of attack?

Angle of attack (AoA) is the angle between the wing chord line and the incoming airflow direction. Increasing AoA increases lift up to a critical angle (typically 12-18°), beyond which the airflow separates from the upper surface and the wing stalls — lift drops and drag surges.

What causes aerodynamic drag?

Drag has two main components: parasitic drag (skin friction and form drag from the body's shape) and induced drag (a byproduct of generating lift — the wingtip vortices create a downwash that tilts the lift vector backward). Induced drag decreases with speed while parasitic drag increases with speed squared.

What is the lift-to-drag ratio?

The lift-to-drag ratio (L/D) measures aerodynamic efficiency — how much lift a wing produces per unit of drag. A higher L/D means the aircraft can glide farther per unit altitude lost. Commercial jets achieve L/D of 15-20, while high-performance sailplanes exceed 50.

Sources

Embed

<iframe src="https://homo-deus.com/lab/aerospace/lift-drag/embed" width="100%" height="400" frameborder="0"></iframe>
View source on GitHub