✈️ NACA Airfoil — Lift, Drag & Pressure Distribution

Generate any NACA 4-digit wing profile and compute aerodynamic coefficients from thin airfoil theory. Adjust camber, camber position, thickness and angle of attack. Watch streamlines shift as lift changes.

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Airfoil cross-section with flow (blue = low pressure, red = high pressure)
Pressure coefficient Cp(x/c) — upper surface (blue) / lower (red)

NACA 4-Digit Profile

NACA 2412

Flight Conditions

⚠ STALL

Aerodynamics

Cl (lift coeff.)
Cd (total)
L/D ratio
Zero-lift α_L0
Stall angle
Cm (moment)
Thin airfoil theory:
Cl = 2π(α − αL0)
Cd = Cd0 + Cl²/(πARe)
e ≈ 0.85 (Oswald efficiency)

How the Simulation Works

The NACA 4-digit designation encodes the wing geometry: the first digit is max camber as a percentage of chord, the second is its chordwise position in tenths, and the last two are the thickness ratio in percent. Coordinates are generated using the standard thickness distribution formula, and the camber line is computed analytically. Lift is calculated from thin airfoil theory: Cl = 2π(α − αL0), where αL0 is the zero-lift angle determined numerically from the camber distribution. Drag& uses the sum of profile drag (empirical, dependent on T) and induced drag Cdi = Cl²/(πARe). The flow visualisation uses a point vortex at the quarter-chord point (Kutta–Joukowski): Γ = ClVc/2, producing circulation that deflects the streamlines.

About the NACA Airfoil Simulator

This simulation generates any NACA 4-digit wing profile and computes its aerodynamic behaviour in real time. The four digits encode geometry: maximum camber (% of chord), camber position (tenths of chord) and thickness (% of chord). Coordinates use the standard thickness distribution with cosine spacing, and lift follows thin airfoil theory, Cl = 2π(α − αL0), where the zero-lift angle is integrated numerically from the camber slope.

The sliders set max camber M, camber position P, thickness T, angle of attack α and aspect ratio AR. From these the panel reports Cl, total Cd, lift-to-drag ratio, zero-lift angle, stall angle and the quarter-chord moment Cm. Animated streamlines, driven by a point vortex with circulation Γ = ClVc/2, show how lift bends the flow. The same theory underpins real wing, propeller and turbine-blade design.

Frequently Asked Questions

What does a NACA 4-digit number such as 2412 mean?

The first digit is maximum camber as a percentage of the chord (2%), the second is the chordwise position of that camber in tenths of the chord (0.4c), and the final two digits are the maximum thickness as a percentage of the chord (12%). The simulator builds the exact section from these three numbers using the sliders M, P and T.

How is the lift coefficient calculated?

Lift comes from thin airfoil theory: Cl = 2π(α − αL0), where α is the angle of attack and αL0 is the zero-lift angle. The lift-curve slope is therefore 2π per radian. The simulator finds αL0 by numerically integrating the camber-line slope, so cambered sections lift at zero degrees.

What do the camber and thickness sliders actually change?

Camber M and its position P bend the mean line, shifting the zero-lift angle more negative and adding loading near the front of the section. Thickness T fattens the profile, which raises profile drag and slightly delays stall. You can watch the airfoil outline, the Cp curve and the coefficient readouts respond instantly to each change.

How is drag computed in this model?

Total drag is the sum of profile drag and induced drag: Cd = Cd0 + Cl²/(πARe). The profile term Cd0 rises with thickness, while the induced term grows with the square of lift and falls with aspect ratio AR. The Oswald efficiency factor e is fixed at about 0.85, a typical value for a real wing.

Why does a higher aspect ratio reduce drag?

Induced drag is Cl²/(πARe), so it is inversely proportional to aspect ratio. A long, slender wing has weaker tip vortices and loses less energy to the downwash trailing behind it. That is why gliders and high-altitude aircraft use very high aspect ratios, and why raising the AR slider lowers Cd and improves the L/D ratio.

What is the zero-lift angle and why is it negative for cambered wings?

The zero-lift angle αL0 is the angle of attack at which the section produces no lift. A cambered aerofoil is curved so that it still deflects air even when its chord line points slightly downward, so it must be pitched to a negative angle before lift disappears. The simulator computes it from the camber distribution, giving a small negative value for any non-symmetric section.

What happens at the stall angle?

Thin airfoil theory predicts lift growing without limit, which is unphysical. The simulator adds an empirical stall angle that increases with camber and thickness, and beyond it the lift coefficient decays exponentially rather than rising. A red STALL badge appears, mirroring how real flow separates from the upper surface once the angle of attack becomes too steep.

What does the pressure-coefficient plot show?

The lower chart plots the pressure coefficient Cp against chordwise position x/c for the upper surface (blue) and lower surface (red). Strong negative Cp on the upper surface marks the low-pressure suction region that produces most of the lift, with a peak near the leading edge that grows as the angle of attack increases.

How accurate is this simulator?

It is a teaching tool, not a CFD solver. The geometry equations are exact, and thin airfoil theory is genuinely accurate for thin sections at small angles in attached flow. However, the drag, stall and flow-visualisation models are simplified and empirical, so absolute numbers should be treated as indicative rather than wind-tunnel precise.

What is the quarter-chord moment Cm?

Cm is the pitching-moment coefficient taken about the quarter-chord point, which thin airfoil theory identifies as the aerodynamic centre where the moment stays roughly constant with angle of attack. A symmetric section gives zero, while camber produces a steady nose-down moment that an aircraft must trim out with its tailplane.

Where are NACA airfoils used in the real world?

The NACA 4-digit family was developed in the 1930s and is still used on light aircraft wings, tail surfaces, propellers, wind-turbine blades and model aeroplanes. Sections like the NACA 2412 appear on classic general-aviation aircraft, and the same parametric approach underlies modern aerofoil design and the layout of this very simulator.