OSCILLATORY / ROLL & YAW
Dutch roll
Sideslip, roll and yaw oscillate together. The yaw damper targets this motion, but it also affects the coupled system.

All modules ↗DYNAMIC STABILITY / CHAPTER 02
One disturbance. Coupled motion. A different response with feedback.
OSCILLATORY / ROLL & YAW
Sideslip, roll and yaw oscillate together. The yaw damper targets this motion, but it also affects the coupled system.
FAST / ROTATION DIES AWAY
Wing roll damping removes roll rate quickly. Removing roll rate alone does not guarantee wings-level flight after a general disturbance.
SLOW / BANK DRIFT
The balance of dihedral and directional effects can make bank decay or grow. A yaw damper is not a bank-hold autopilot.
Mode metrics above describe the airframe with the damper off. Illustrations show characteristic behaviour; the curves below are computed. With feedback on, the same airframe initial state excites the closed-loop system.
03 / FOLLOW THE FEEDBACK · B
A washout filter rejects a sustained yaw rate once its transient has passed. It helps the damper avoid continually opposing a steady turn. This page simulates small disturbances about straight flight; the sketch illustrates the filter’s DC response.
04 / NOSE, VELOCITY & BANK · B
Top view: track direction χ ≈ ψ + β. Rear view: positive φ lowers the right wing. Diagrams retain actual angles when 3D exaggeration is enabled.
05 / GROUND TRACK
06 / ONE CLOCK, COUPLED EQUATIONS
Click a graph or use its arrow keys to scrub time.
A · dashed amber B · solid turquoise
07 / HOLD A, EXPLORE B
| Quantity | A · saved | B · live |
|---|
A remains fixed during this page session. Reloading clears it. Export includes settings, both spectra, inputs and response samples.
The fin, dihedral, damping and control derivatives act together. No longitudinal motion or second-order height loss is calculated.
Aircraft state: [β, p, r, φ]. β̇ = Y/(mV) − r + gφ/V; ṗ = L/Ixx; ṙ = N/Izz; φ̇ = p. The fin’s sideforce acts behind and above the CG. Wing dihedral, roll damping, yaw–roll coupling and aileron adverse yaw complete the model.
These are projections about straight, level flight, not finite-angle turn geometry.
Heading ψ̇ = r and lateral displacement ẏ = V(ψ + β) are first-order projections. Speed and altitude are frozen at trim. Products of inertia are set to zero; axes are aligned with the straight, level trim velocity. No second-order height loss is predicted.
Positive rudder produces a negative yaw moment under this page’s sign convention. The external rudder pulse is added after the damper output.
ẇ = (r − w)/3; δcmd = K(r − w); δ̇d = (δcmd − δd)/0.2. K has units of seconds. Positive rudder produces a negative yaw moment, so this feedback sign opposes yaw rate. The external rudder pulse is added to the damper output.
Airframe modes are eigenvectors of the four-state system. The controller adds two states. When switched on, it starts unexcited; it can change other modes as well as Dutch roll. A slowly growing spiral may remain.
Original illustrative aircraft: 1,800 kg; wing 22 m²; span 11 m; Ixx 3,000 and Izz 9,000 kg m². This shares teaching dimensions with the longitudinal lab, but is a separately scoped lateral approximation, not a validated combined aircraft.
Stop before |β| > 5°, |φ| > 10°, |ψ| > 15°, |p| or |r| > 15°/s, |δr| or |δcmd| > 10°, or actuator rate > 30°/s. Controls are not silently clipped. No stall, nonlinear spiral dive, turbulence, sustained-turn simulation or handling-quality certification.
Week 6, Equations of Motion, Part 2, 27 February 2026, slides 25–27: lateral modes. Week 13, 17 April 2026, slides 39–52: feedback and flight control.
MIT OCW · Aircraft Lateral Dynamics
MIT OCW · Basic Autopilot Design
Original diagrams and geometry; local Three.js under its existing MIT licence. Numerically checked teaching equations; no flight-test validation. Version .