Lesson 1 · 35 min

Airfoil Geometry and Families

Module 3 sized the business jet from a sketch, a few statistics and the Breguet equations. Before the sketch can become a drawing, the wing needs a shape: first its cross-section, the airfoil, and then its planform. This lesson describes airfoils the way designers do, by a few numbers that fix their shape, and introduces the families those numbers come from.

Learning objectives

The parts of an airfoil

An airfoil is the shape of a wing cut by a plane parallel to the flight direction. Four numbers describe most of it:

Camber mostly sets how much lift the airfoil gives at a given angle, and its pitching moment. Thickness mostly sets the structure and fuel the wing can hold, the maximum lift, and how early the flow becomes supersonic. The two are designed separately and then added: the upper and lower surfaces are the thickness distribution laid on either side of the camber line.

The NACA four-digit family

In the 1930s the National Advisory Committee for Aeronautics (NACA) built families of airfoils from simple formulas, so that one shape could be compared with another by changing one number at a time. The four-digit family is the simplest. In NACA 2412:

A symmetric airfoil has zeros for the first two digits: NACA 0012 is 12% thick with no camber.

NACA four-digit airfoil (\(x\) and \(y\) as fractions of the chord)

\[ y_c = \frac{m}{p^2}\left(2px - x^2\right) \quad (x \le p) \] \[ y_c = \frac{m}{(1-p)^2}\left[(1 - 2p) + 2px - x^2\right] \quad (x > p) \] \[ y_t = 5t\left(0.2969\sqrt{x} - 0.1260x - 0.3516x^2 + 0.2843x^3 - 0.1015x^4\right) \]

The camber line \(y_c\) is two parabolas that meet at \(x = p\). The half-thickness \(y_t\) is the same for every four-digit airfoil, scaled by \(t\); it is greatest at \(x = 0.30\), where it equals \(t/2\). The leading-edge radius is \(r = 1.1019\,t^2c\).

The surfaces are found by stepping \(y_t\) out on either side of the camber line, perpendicular to it. With \(\theta = \arctan(\dd y_c/\dd x)\), the slope angle of the camber line:

Upper and lower surfaces

\[ x_u = x - y_t\sin\theta, \qquad y_u = y_c + y_t\cos\theta \] \[ x_l = x + y_t\sin\theta, \qquad y_l = y_c - y_t\cos\theta \]

For thin, lightly cambered airfoils \(\theta\) is small, so \(y_u \approx y_c + y_t\) and \(y_l \approx y_c - y_t\).

Figure 1.1 A NACA four-digit airfoil drawn from its three numbers, to scale. The dashed line is the chord, the violet curve the mean camber line, with the maximum camber and the maximum thickness marked. Move the sliders, or pick a classic section: thickness changes the shape without changing the camber line, and camber bends the whole airfoil without changing its thickness.

Example 1.1 — A point on the NACA 2412

For the NACA 2412, find the camber, the half-thickness and the upper-surface point at \(x = 0.30\), and the leading-edge radius for a chord of \(2.0\ \text{m}\).

Show solution

Here \(m = 0.02\), \(p = 0.4\), \(t = 0.12\), and \(x = 0.30 < p\), so the forward parabola applies:

\[ y_c = \frac{0.02}{0.16}\left[2(0.4)(0.30) - 0.30^2\right] = 0.125(0.15) = 0.01875 \] \[ \frac{\dd y_c}{\dd x} = \frac{2m}{p^2}(p - x) = 0.25(0.10) = 0.025, \qquad \theta = 1.432^\circ \] \[ y_t = 5(0.12)(0.16262 - 0.03780 - 0.03164 + 0.00768 - 0.00082) = 0.06002 \] \[ x_u = 0.30 - 0.06002\sin 1.432^\circ = 0.2985 \] \[ y_u = 0.01875 + 0.06002\cos 1.432^\circ = 0.07875 \] \[ r = 1.1019(0.12)^2(2.0) = 0.0317\ \text{m} \]

The half-thickness at 30% of the chord is 6%: half of the 12% thickness, as it must be at the thickest point. On the 2.0 m chord the upper surface is 0.158 m above the chord line there.

Other families

Later families kept the idea of a designation that encodes the shape, but tuned the shape for a purpose:

How to read the main airfoil designations
FamilyExampleWhat the digits meanDesigned for
NACA four-digit (1930s)NACA 2412camber 2%, at 40% of the chord, 12% thicksimple, gentle stall; light aircraft, tails
NACA five-digit (1930s)NACA 23012design lift coefficient \(0.15 \times 2 = 0.3\); maximum camber at \(30/2 = 15\%\) of the chord; 12% thickmore lift, less pitching moment; maximum camber far forward
NACA six-series (1940s)NACA \(64_2\)-215six-series, minimum pressure at 40% of the chord; low drag for \(c_l\) within \(\pm 0.2\) of the design value; design \(c_l = 0.2\); 15% thicklaminar flow: a "drag bucket" of low drag around the design lift coefficient
Supercritical (1970s)NASA SC(2)-0410second-generation supercritical; design \(c_l = 0.4\); 10% thickhigh subsonic speed: a flat top delays and weakens the shock

Laminar-flow airfoils move the point of minimum pressure, and with it the start of turbulent flow, well aft. A boundary layer that stays laminar has much less skin friction, so within a narrow range of lift coefficients the drag drops sharply. Outside that range, or on a surface spoiled by rivets, insects or rain, the bucket disappears.

Supercritical airfoils address the problem of the jet age. At high subsonic speeds the flow over the upper surface becomes supersonic and ends in a shock wave, which adds drag. A supercritical airfoil has a flatter upper surface, so the supersonic region is weaker and the shock forms later, and its camber is concentrated near the trailing edge to recover the lift lost by the flat top. For the same speed it can be thicker, which saves weight and holds more fuel (Lesson 3).

Today most new aircraft use airfoils designed by computer for their own wing: the numbers are no longer standard, but the ideas are the same. The four-digit family remains the best way to learn what each feature does, which is why this module uses it.

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Key takeaways