Weathercock Stability⚠ unverified
Aerospace / Stability · Return the weathercock (directional) stability metric
Parameters
| Input | Symbol | Unit | Default | Description |
|---|---|---|---|---|
| Cn_beta | Cn_β | — | 1.0 | Yawing-moment coefficient derivative with respect to sideslip angle (per radian, non-dimensional) |
| Output | Symbol | Unit | Description |
|---|---|---|---|
| result | metric | — | Weathercock stability metric, equal to ``Cn_beta`` (non-dimensional) |
The science & history
Understanding the Parameters
-
Sideslip angle $\beta$ — the angle between the aircraft's nose and the relative wind, measured in the horizontal plane. A gust or a rudder input can push the aircraft into sideslip; directional stability is the tendency to remove it.
-
The weathervane analogy — a weathervane has more area behind its pivot than in front, so the wind always swings the tail downwind and the point upwind. An aircraft's vertical tail plays the role of that trailing area: in a sideslip, the fin generates a side force behind the CG, yawing the nose back into the wind. More fin area or a longer tail arm means a larger positive $C_{n\beta}$.
-
Why positive means stable — with sideslip $\beta > 0$ (wind coming from the right of the nose), a stable aircraft must generate a positive (nose-right) yawing moment to reduce $\beta$ back toward zero. So $C_n$ must increase with $\beta$: $C_{n\beta} > 0$. (Note the sign convention is opposite to the pitch case, where stability needs $C_{m\alpha} < 0$ — a frequent source of confusion. The difference is just how the axes and positive senses are defined.)
-
What erodes it — the fuselage is destabilising in yaw (its side area ahead of the CG acts like the front of a badly-balanced weathervane), so the fin must overcome the fuselage's negative contribution. At high angle of attack the fin can be blanketed by the fuselage/wing wake, cutting $C_{n\beta}$ and risking directional divergence and departure/spin — a key limit on the flight envelope.
-
Coupled to roll — directional stability does not act alone: yaw and roll are aerodynamically coupled through sideslip. Weathercock stability ($C_{n\beta}$), dihedral effect (Dihedral Effect, $C_{l\beta}$), and the damping derivatives together govern the lateral-directional dynamic modes — the dutch roll, spiral, and roll modes. Their balance, not any one alone, sets good handling.
Derivation (Approaching a Proof)
The calculator is an identity, so the derivation is the meaning of directional static stability and the fin's contribution to it.
Directional static stability requires that a sideslip generate a restoring yawing moment — the moment must act to reduce the sideslip:
$$\frac{\partial C_n}{\partial \beta} = C_{n\beta} > 0 \quad\text{(stability condition)}.$$
The dominant stabilising contribution is the vertical tail. In a sideslip $\beta$, the fin sees an angle of attack $\approx \beta$ (modified by sidewash), generating a side force $Y_t \approx -\,\eta\,q\,S_v\,C_{L\alpha,v}\,\beta$ acting at the tail, a distance $\ell_v$ behind the CG. That side force makes a restoring yawing moment, giving a fin contribution
$$C_{n\beta,\,\text{fin}} = +\,\eta\,\frac{S_v\,\ell_v}{S\,b}\,C_{L\alpha,v} \;>\; 0,$$
where $S_v\ell_v/(S b)$ is the vertical-tail volume ratio. The fuselage contributes a negative (destabilising) term, so the net is
$$C_{n\beta} = C_{n\beta,\,\text{fin}} + C_{n\beta,\,\text{fuselage}} + \dots,$$
and the fin must be sized so the sum stays comfortably positive across the envelope. This is the directional analogue of building a positive Static Margin in pitch — the fin is the "tail" that does it.
Dimensional check. $C_n$ is a dimensionless moment coefficient and $\beta$ is in radians, so $C_{n\beta} = \partial C_n/\partial\beta$ is per radian ✓ — the natural units of a stability derivative.
History and Development
-
The vertical fin. Directional stability was one of the earliest practical necessities: without an adequate fin, an aircraft yaws and "fishtails" uncontrollably. The evolution of the vertical tail from the small rudders of early aircraft to the large fins of modern jets is largely the story of guaranteeing positive $C_{n\beta}$.
-
High-angle-of-attack departure. The loss of $C_{n\beta}$ at high $\alpha$ (fin blanketing) became a central concern with high-performance jets, producing directional departure, spin, and the need for ventral fins, strakes, and yaw-departure-limiting flight-control laws. The F-14 and many fighters carry twin canted fins partly to preserve directional stability at high $\alpha$.
-
Lateral-directional handling. Together with the dihedral effect $C_{l\beta}$, weathercock stability sets the character of the dutch-roll and spiral modes. The perennial trade — enough $C_{n\beta}$ for directional stability but not so much that it overwhelms dihedral and worsens dutch roll — is a staple of stability-and-control design (Etkin, Nelson).
Related Concepts: Dihedral Effect, Dutch Roll Wn, Spiral Mode Time Constant, Roll Mode Time Constant, Static Margin, Moment Coefficient
Notes: Pass-through — returns $C_{n\beta}$; content is its sign/meaning. $C_{n\beta}>0$ = directionally stable (nose weathervanes back into the wind); provided mainly by the vertical tail (fin volume ratio), opposed by the fuselage. Sign convention is opposite to pitch ($C_{m\alpha}<0$ for stable). Falls at high $\alpha$ (fin blanketing) → departure risk. With Dihedral Effect $C_{l\beta}$, sets the lateral-directional modes.