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Library / Flight dynamics and control / FLT-02

Flight dynamics and control

Pitch-rate response to an elevator step

Pitch rate after a step elevator deflection, for a reduced first-order model of the aircraft near trim.

Ref
FLT-02
Rev
v1
Field
Flight dynamics and control
Result
q(t) [°/s]

The reduced model q̇ = −λqq + beδe describes the pitch rate near trim. λq = −aq is the rate at which the aircraft's own damping removes pitch rate, and be is the elevator control derivative. For a step elevator deflection the pitch rate rises exponentially to the steady value beδe/λq with time constant 1/λq. Angle-of-attack coupling is left out, so this is not the full short-period model.

Pitch rate after a step elevator deflection, for a reduced first-order model of the aircraft near trim. The model is q̇ = −λqq + beδe, where λq = −aq, and the rate rises exponentially to the steady value beδe/λq.

Calculator

Solve for
°/s
1/s
0.56
1/s²
220
°
0.55
s
05
  • Steady-state pitch rate, beδe/λq6 °/s
  • Time constant, 1/λq0.5 s
  • Time to reach 95 % of the steady rate, 3/λq1.5 s
  • Fraction of the steady rate reached at t86.47 %

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Pitch rate (°/s) current value 5.188 °/s
δeElevator deflectionKey driver
1.7317.3
beElevator effectiveness (nose-up positive)
1.313
λqPitch-rate damping rate (minus the rate derivative)
29.44
tTime since the step
06
  • The pitch rate heads for 6 °/s with a time constant of 0.5 s, so it has reached 86.5 % of that after 1 s.
  • Halving the damping to λq = 1 doubles the steady pitch rate to 12 °/s but doubles the time constant to 1 s. The pitch rate after 1 s is 7.585 °/s.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing (°/s)Local stepChange in result
δe Elevator deflection0.5 to 5 °1.72917.2915.56+10%+0.519 °/s
be Elevator effectiveness (nose-up positive)2 to 20 1/s²1.29712.9711.67+10%+0.519 °/s
λq Pitch-rate damping rate (minus the rate derivative)0.5 to 6 1/s1.9959.4437.448+10%−0.338 °/s
t Time since the step0 to 5 s066+10%+0.147 °/s

Sweep of Time since the step

Time since the step (s)Pitch rate (°/s)
00
0.6254.281
1.255.507
1.8755.859
2.55.96
3.1255.988
3.755.997
4.3755.999
56

Sweep one variable

Pitch rate (°/s)Hover, touch, or use the arrow keys on the chart
0123456 012345 Time since the step (s) now 5.188

Variables and how each one contributes

q(t)

Pitch rate

Result · °/s

What the equation gives you. Everything else feeds it.

λq

Pitch-rate damping rate (minus the rate derivative)

1/s · typical 0.5 to 6

The pitch-rate damping rate in 1/s: λq = −aq. Larger means more damping and a faster response. More damping both lowers the steady pitch rate and shortens the time constant. At a given time the rate can be higher or lower, since the two effects compete. Raising it by 10 % (to 2.2) moves the result by −6.51 %, from 5.188 to 4.85 °/s.

be

Elevator effectiveness (nose-up positive)

1/s² · typical 2 to 20

The elevator effectiveness be in 1/s², positive for a nose-up response to positive deflection. Directly proportional: a more effective elevator gives a proportionally larger pitch rate at every instant. Raising it by 10 % (to 8.8) moves the result by +10 %, from 5.188 to 5.707 °/s.

δe

Elevator deflection

° · typical 0.5 to 5

The elevator deflection in degrees, held constant after the step. Directly proportional, as long as the linear model holds. Raising it by 10 % (to 1.65) moves the result by +10 %, from 5.188 to 5.707 °/s.

t

Time since the step

s · typical 0 to 5

The time since the step, in s. The rate rises towards its steady value, gaining less each second. Raising it by 10 % (to 1.1) moves the result by +2.84 %, from 5.188 to 5.335 °/s.

Worked example with the values above

  1. Steady rate: beδe/λq = 8 × 1.5 / 2 = 6 °/s.
  2. Fraction reached: 1 − e−2 = 1 − 0.1353 = 0.8647.
  3. q(t) = 6 × 0.8647 = 5.188 °/s.

Assumptions and limits

  • A reduced linear model near trim: constant airspeed, small deflections, and no coupling to angle of attack.
  • A step input in elevator from rest, with the pitch rate zero at the start.

Common mistakes

  • Confusing the pitch rate q with the rate of change of pitch angle θ̇. They are equal only with the wings level.
  • Assuming the sign convention without checking it. The sign of the elevator effect depends on the axes and deflection convention.

Statistics and uncertainty

The steady pitch rate scales with be/λq, so independent errors of 10 % in each give about 14 % in the steady rate (√(10² + 10²)). Control derivatives are usually identified from flight test or a validated model, and they change with speed, altitude and centre of gravity, so a single value is valid only near one trim point.

Where it is used

  • Estimating how quickly an aircraft responds to an elevator command.
  • Sizing the inner pitch-rate loop and checking the model against a flight-test step.

Maths you need

  • First-order response: exponential approach with time constant 1/λ
  • Control derivative: the change in moment per unit deflection

Related formulas

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