Control Power Moment⚠ unverified
Aerospace / Controls · Compute the pitching moment generated by a control-surface deflection
Parameters
| Input | Symbol | Unit | Default | Description |
|---|---|---|---|---|
| Cm_delta | Cm_δ | — | 1.0 | Pitching-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 | Wing reference area |
| c | c | m | 1.0 | Mean aerodynamic chord |
| Output | Symbol | Unit | Description |
|---|---|---|---|
| result | M | N*m | Pitching moment, in newton-metres (N*m) |
The science & history
Understanding the Parameters
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From coefficient to moment — aerodynamic moments are always written as a dimensionless coefficient times a dimensional scale. For pitch the scale is $q\,S\,c$: dynamic pressure sets the force per unit area, $S$ the area, and $c$ the moment arm (the chord). Multiplying the control-moment coefficient $C_{m\delta}\delta$ by $qSc$ turns "how much moment per unit dynamic pressure and size" into an actual newton-metre torque.
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Why $q$ makes controls "firm up" with speed — because $M \propto q = \tfrac12\rho V^2$ (Dynamic Pressure), the same elevator deflection produces four times the moment at twice the speed. This is why controls feel heavy and powerful at high speed and mushy near the stall, and why high-speed flight needs only tiny deflections (and why over-controlling at high $q$ can overstress the airframe — the origin of the manoeuvring-speed limit).
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The moment accelerates the aircraft in pitch — dividing $M$ by the pitch inertia $I_{yy}$ gives the pitch angular acceleration (Torque, $\ddot\theta = M/I_{yy}$). So this moment, set against the aircraft's inertia and opposed by pitch damping, drives the short-period pitch response.
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Sizing and authority — control power moment is what must overcome the airframe's natural moment to trim (Elevator Deflection trim) and to manoeuvre. A tail is sized so this moment stays adequate at the most demanding condition — typically low speed (small $q$) at forward CG, where the required moment is largest and the available $q$ smallest.
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Same form for all axes — the identical structure gives roll and yaw control moments (with $b$, the span, replacing $c$ for the lateral-directional axes). The elevator/pitch case shown here is the template.
Derivation (Approaching a Proof)
Aerodynamic moments are non-dimensionalised by convention. The pitching moment $M$ is written as a dimensionless moment coefficient $C_m$ times a reference dynamic pressure, area, and length:
$$M = C_m\,q\,S\,c,$$
where $q = \tfrac12\rho V^2$ is the dynamic pressure, $S$ the reference (wing) area, and $c$ the mean aerodynamic chord (the reference length for pitch). This is the definition of $C_m$, rearranged.
The contribution of the control surface to $C_m$ is, to first order, linear in its deflection through the control derivative $C_{m\delta}$:
$$\Delta C_m = C_{m\delta}\,\delta.$$
Substituting this control contribution into the dimensionalising relation gives the control-generated moment:
$$M = \Delta C_m\,q\,S\,c = C_{m\delta}\,\delta\,q\,S\,c. \qquad\blacksquare$$
So the calculator is simply the definition of a moment coefficient applied to the elevator's share of the pitching moment. The physics is entirely in $C_{m\delta}$ (how effectively the surface changes the flow's moment); the $qSc$ is bookkeeping that converts the coefficient to a torque.
Dimensional check. $C_{m\delta}$ is per radian and $\delta$ in radians, so $C_{m\delta}\delta$ is dimensionless; then $q\,S\,c = \text{Pa}\cdot\text{m}^2\cdot\text{m} = (\text{N}/\text{m}^2)\,\text{m}^3 = \text{N}\cdot\text{m}$ ✓ — a moment.
History and Development
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The coefficient convention. Non-dimensionalising forces and moments by $qS$ (and $qSc$, $qSb$) is one of the foundational moves of aerodynamics, letting wind-tunnel data at one scale and speed transfer to full-scale flight (the same similarity idea behind Reynolds number). Control derivatives like $C_{m\delta}$ are measured this way and stored in aircraft databases.
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Powered controls. As aircraft grew larger and faster, the moments — and the matching hinge moments the pilot felt (see Control Surface Hinge Moment) — outstripped human strength, driving hydraulically powered flight controls from the 1940s onward. Control power moment is what those actuators must deliver.
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Fly-by-wire and control allocation. Modern fly-by-wire aircraft with many surfaces (multiple elevons, spoilers, canards) distribute a commanded moment across surfaces by control allocation, each surface's contribution computed with exactly this $C_{m\delta}\,\delta\,qSc$ relation and summed — the moment budget that the flight-control law manages.
Related Concepts: Control Power Cm Delta, Elevator Deflection trim, Control Surface Hinge Moment, Pitch Rate Damping, Dynamic Pressure, Moment Coefficient, Pitching Moment, Torque
Notes: Dimensional pitching moment (N·m) = control coefficient $C_{m\delta}\delta$ × the normaliser $qSc$ (dynamic pressure × area × chord) — the dimensional companion of Control Power Cm Delta. $M\propto q\propto V^2$, so controls stiffen with speed (four-fold per doubling). $M/I_{yy}$ = pitch angular acceleration. Same form with span $b$ for roll/yaw. All coefficients per radian; defaults $1.0$.