Control Power Cm Delta⚠ unverified
Aerospace / Stability · Compute the pitch control power
Parameters
| Input | Symbol | Unit | Default | Description |
|---|---|---|---|---|
| Cm_delta | Cm_δ | — | 1.0 | Pitching-moment coefficient derivative with respect to elevator deflection (per radian, non-dimensional) |
| Output | Symbol | Unit | Description |
|---|---|---|---|
| result | controlpower | — | Pitch control power magnitude (non-dimensional) |
The science & history
Understanding the Parameters
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The control derivative $C_{m\delta}$ — how much the aircraft's pitching-moment coefficient changes for each radian of elevator deflection. A large magnitude means a small elevator movement produces a big pitching moment: lots of authority. It is set by the tail area, the elevator's chord fraction, the tail moment arm, and the dynamic pressure.
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Why the magnitude — the sign of $C_{m\delta}$ just encodes the convention (trailing-edge-down elevator gives nose-down or nose-up moment depending on sign definitions); what matters for "how much authority do I have" is the size. Hence the absolute value.
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Control power vs stability — the balance — these two derivatives must be matched. To trim a stable aircraft, the elevator must generate enough moment to cancel the aircraft's natural moment at the target angle of attack: roughly, the required deflection is $\delta_e \sim -C_{m\alpha}\,\alpha_{trim}/C_{m\delta}$. A large static margin (large $|C_{m\alpha}|$) demands large control power to trim and manoeuvre. Too little control power and the aircraft cannot reach high angle of attack (e.g. cannot flare to land or rotate for takeoff); this sets the forward CG limit, the mirror of the aft limit that the static margin sets.
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Manoeuvre authority — beyond trimming, control power determines the pitch acceleration available: the elevator moment divided by pitch inertia sets how fast the nose can be commanded to move, feeding directly into the short-period response and the load factor a pilot can pull. A "responsive" aircraft has ample $C_{m\delta}$ relative to its inertia and stability.
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The elevator can run out — control power is finite: at large deflections the elevator stalls or hits its travel limit, and effectiveness $C_{m\delta}$ itself drops. Designers size the tail and elevator so that full authority remains available at the most demanding condition — typically the forward CG, low-speed, flare or rotation case.
Derivation (Approaching a Proof)
The calculator is an identity ($|C_{m\delta}|$), so the content is what the derivative is and why its magnitude governs authority.
The total pitching-moment coefficient depends on both angle of attack and elevator deflection. Expanding linearly about a reference:
$$C_m = C_{m0} + C_{m\alpha}\,\alpha + C_{m\delta}\,\delta_e,$$
where $C_{m\delta} = \partial C_m/\partial\delta_e$ is the elevator control power. The elevator changes the tail's lift, which acts through the tail moment arm; a first-principles estimate is
$$C_{m\delta} = -\,\eta\,\frac{S_t\,\ell_t}{S\,\bar c}\,C_{L\alpha,t}\,\tau,$$
with $\eta$ the tail efficiency, $S_t\ell_t/(S\bar c)$ the tail volume ratio, $C_{L\alpha,t}$ the tail lift-curve slope, and $\tau$ the elevator effectiveness factor (how much of a full angle-of-attack change the flap deflection is worth). Every term is a design choice — larger tail, longer arm, bigger elevator → more control power.
Using it to trim. Set $C_m = 0$ (trim, see Longitudinal Trim Moment) and solve for the required elevator:
$$\delta_{e,\,trim} = -\frac{C_{m0} + C_{m\alpha}\,\alpha_{trim}}{C_{m\delta}}.$$
The elevator deflection needed is inversely proportional to $C_{m\delta}$ — small control power means large deflections, and eventually not enough travel to trim. Taking the magnitude, $|C_{m\delta}|$, gives the authority figure the calculator reports.
Dimensional check. $C_m$ is dimensionless and $\delta_e$ is in radians, so $C_{m\delta} = \partial C_m/\partial\delta_e$ is per radian; its absolute value carries the same units ✓.
History and Development
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Sizing the tail. Control power is one of the two pillars (with static stability) of tail design. The tail volume ratio $V_H = S_t\ell_t/(S\bar c)$, which appears directly in $C_{m\delta}$ and in the neutral point, has been the governing parameter of empennage sizing since the earliest systematic stability studies of the 1910s–20s.
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Control at the CG limits. The realisation that the forward CG limit is set by control power (can the elevator still raise the nose to land?) while the aft limit is set by stability (static margin) is a cornerstone of the CG-envelope concept, formalised in mid-century handling-qualities work and every aircraft flight manual since.
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Powered and relaxed-stability controls. As aircraft grew faster and larger, hinge moments outstripped pilot strength, driving hydraulically powered controls; and relaxed-stability fly-by-wire designs deliberately reduced static stability so that less control power is spent fighting the airframe and more is available for manoeuvring — a direct exploitation of the stability-vs-control-power balance this quantity expresses.
Related Concepts: Longitudinal Trim Moment, Static Margin, Moment Coefficient, Pitching Moment, Lift Curve Slope, Weathercock Stability
Notes: Pass-through — returns $|C_{m\delta}|$ unchanged; the content is why it is the pitch-authority figure of merit. $C_{m\delta}=\partial C_m/\partial\delta_e$ (per rad), set by tail volume ratio × elevator effectiveness. In balance with the Static Margin: high stability demands high control power to trim/manoeuvre. Sets the forward CG limit (mirror of the static margin's aft limit). Required trim deflection $\propto 1/C_{m\delta}$.