Control Surface Hinge Moment⚠ unverified
Aerospace / Controls · Compute the hinge moment acting on a control surface
Parameters
| Input | Symbol | Unit | Default | Description |
|---|---|---|---|---|
| Ch_alpha | Ch_α | — | 1.0 | Hinge-moment derivative with respect to angle of attack, per radian |
| alpha | α | rad | 1.0 | Angle of attack |
| Ch_delta | Ch_δ | — | 1.0 | Hinge-moment derivative with respect to control-surface deflection, per radian |
| delta | δ | rad | 1.0 | Control-surface deflection |
| q | q | Pa | 1.0 | Dynamic pressure |
| S | S | m^2 | 1.0 | Control-surface reference area |
| c | c | m | 1.0 | Control-surface reference chord |
| Output | Symbol | Unit | Description |
|---|---|---|---|
| result | H | N*m | Hinge moment, in newton-metres (N*m) |
The science & history
Understanding the Parameters
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Hinge moment is the "feel" of the controls — a deflected control surface has an aerodynamic load that acts at some distance behind its hinge, producing a moment that tries to return it to neutral. On a manual aircraft that moment is transmitted straight to the control column as stick force — the resistance the pilot feels. Good "control harmony" is largely a matter of designing these hinge moments so the forces feel right and scale sensibly with speed and manoeuvre.
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Two contributions, $\alpha$ and $\delta$ — the surface feels the flow both because the whole aircraft is at some angle of attack ($C_{h\alpha}\alpha$ — a floating tendency) and because the surface is itself deflected ($C_{h\delta}\delta$ — a restoring tendency). Their sum is the net hinge moment. Both are normally negative (nose-toward-neutral), so a deflected surface at positive $\alpha$ pushes back on the pilot.
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Scales with $q$, like all aerodynamic loads — $H \propto q \propto V^2$, so hinge moments — and stick forces — grow with the square of speed. At high speed an unpowered control could demand more force than a pilot can apply; this is precisely why hinge moments had to be managed as aircraft got faster.
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Aerodynamic balancing reduces it — designers deliberately shrink hinge moments (make $C_{h\alpha}$, $C_{h\delta}$ small) with aerodynamic balance: horn balances, set-back hinges, and balance tabs move the hinge line or add offset area so the aerodynamic load's moment arm is reduced. Too much balance, though, risks overbalance (controls that snatch or reverse) and flutter — a delicate compromise.
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The actuator sizing driver — for powered controls, the hinge moment sets how strong the hydraulic actuator must be. It is a primary structural and systems design number: the surface, its hinges, and its actuator are all sized by the worst-case $H$ across the flight envelope.
Derivation (Approaching a Proof)
Like every aerodynamic moment, the hinge moment is non-dimensionalised by $q\,S\,c$ (dynamic pressure × surface reference area × surface reference chord):
$$H = C_h\,q\,S\,c,$$
where $C_h$ is the dimensionless hinge-moment coefficient and $S, c$ here refer to the control surface's own area and chord (not the wing's). This is the definition of $C_h$, rearranged to give the moment.
The hinge-moment coefficient depends, to first order, linearly on the two angles that set the flow over the surface — the aircraft angle of attack $\alpha$ and the surface deflection $\delta$:
$$C_h = C_{h\alpha}\,\alpha + C_{h\delta}\,\delta,$$
with $C_{h\alpha} = \partial C_h/\partial\alpha$ and $C_{h\delta} = \partial C_h/\partial\delta$ the two hinge derivatives (a constant term is usually zero for a symmetric surface). Substituting:
$$H = q\,S\,c\,\big(C_{h\alpha}\,\alpha + C_{h\delta}\,\delta\big). \qquad\blacksquare$$
The physics lives in the two derivatives — how the pressure distribution over the surface, and hence its moment about the hinge, responds to angle of attack and deflection. Aerodynamic balancing is the art of shaping the surface so these derivatives (and thus the pilot's forces) come out at desired, usually small, values.
Dimensional check. $C_{h\alpha}\alpha$ and $C_{h\delta}\delta$ are each (1/rad)(rad) = dimensionless, so the bracket is dimensionless; then $q\,S\,c = \text{Pa}\cdot\text{m}^2\cdot\text{m} = \text{N}\cdot\text{m}$ ✓.
History and Development
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Stick force and the human pilot. Early aircraft had direct mechanical linkages, so hinge moments were the control forces. Handling-qualities research (e.g. Gilruth's 1943 criteria) tied acceptable flying to stick- force gradients — force per g, force per knot — all of which trace back to hinge moments.
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Aerodynamic balance and the tab. The horn balance, set-back hinge, and balance/servo tabs were developed to keep hinge moments within human strength as speeds rose. The servo tab (which uses aerodynamic force on a small tab to move the main surface) and spring tab were clever mechanical ways to reduce pilot effort — a whole sub-discipline built on managing this equation.
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Powered and fly-by-wire controls. When even balanced surfaces produced unmanageable hinge moments at high speed, hydraulically powered controls took over (from the 1940s–50s), with artificial feel systems synthesising a pleasant, $q$-scheduled stick force since the real hinge moment no longer reached the pilot. Fly-by-wire completed the separation — but the actuators still fight the physical hinge moment this formula gives.
Related Concepts: Control Power Moment, Elevator Deflection trim, Control Power Cm Delta, Dynamic Pressure, Moment Coefficient, Torque
Notes: Aerodynamic torque about the surface's hinge line — the load the pilot/actuator must overcome ("control feel"). Distinct from Control Power Moment (moment on the aircraft about the CG). $H\propto q\propto V^2$ → stick forces rise with speed; aerodynamic balancing (horn/set-back hinge/tabs) shrinks $C_{h\alpha},C_{h\delta}$ (usually negative/restoring) to keep forces manageable, at the risk of overbalance/ flutter. Sizes the actuator. $S,c$ are the surface's own; per radian; defaults $1.0$.