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Sideslip Due To Rudder⚠ unverified

Aerospace / Controls · Compute the sideslip angle produced by a rudder deflection

Parameters

InputSymbolUnitDefaultDescription
Cy_delta_rCydeltar1.0Side-force derivative with respect to rudder deflection, per radian
delta_rΔrrad1.0Rudder deflection
Cy_betaCy_β1.0Side-force derivative with respect to sideslip angle, per radian
OutputSymbolUnitDescription
resultβradSideslip angle, in radians (rad). Returns 0.0 when ``Cy_beta`` is zero

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

Consider the aircraft's side-force (y-axis) equilibrium in a steady, straight sideslip. The total side-force coefficient is the sum of the sideslip contribution and the rudder contribution (to first order, linear):

$$C_y = C_{y\beta}\,\beta + C_{y\delta_r}\,\delta_r.$$

In a steady straight-line sideslip with no net lateral acceleration, the side forces must balance, so the net side-force coefficient is zero:

$$C_y = 0 \quad\Longrightarrow\quad C_{y\beta}\,\beta + C_{y\delta_r}\,\delta_r = 0.$$

Solve for the sideslip angle:

$$\beta = -\frac{C_{y\delta_r}\,\delta_r}{C_{y\beta}}. \qquad\blacksquare$$

The reading is intuitive: the sideslip grows until the airframe's weathervane side force ($C_{y\beta}\beta$) exactly opposes the rudder-induced side force ($C_{y\delta_r}\delta_r$). A stronger directional response (larger $|C_{y\beta}|$) yields less sideslip for the same rudder — a stiff weathervane resists being pushed off the wind. Returning 0 when $C_{y\beta}=0$ reflects the degenerate case of no restoring side force (no equilibrium).

Dimensional check. $C_{y\delta_r}\delta_r$ is (1/rad)(rad) = dimensionless, and dividing by $C_{y\beta}$ (1/rad) gives radians ✓ — a sideslip angle.

History and Development

Related Concepts: Rudder Yaw Rate Coeff, Weathercock Stability, Dihedral Effect, Dutch Roll Damping, Aileron Roll Rate

Notes: Steady side-force balance — sideslip grows until the airframe's weathervane side force $C_{y\beta}\beta$ cancels the rudder side force $C_{y\delta_r}\delta_r$. Stiffer directional response (larger $|C_{y\beta}|$) ⇒ less sideslip per rudder. This is the steady-heading (crosswind) sideslip. Only the side-force part — a full trim also balances yaw (Rudder Yaw Rate Coeff) and roll (Dihedral Effect) moments (needs aileron). Per radian; returns 0 if $C_{y\beta}=0$.

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