The Hong Kong Polytechnic UniversityDepartment of Aeronautical and Aviation Engineering

THE AIRCRAFT AND THE INSTRUMENT CAN DISAGREE.

Air-data Faults & Control Response

Compare true motion with sensed motion. Introduce a pressure-source fault and watch it enter the feedback loop.

ONE CALCULATION · CONNECTED VIEWSA · AMBER   B · TURQUOISE

Drag to orbit · right-drag to pan · scroll to zoom. Flight-path angle is shown; body pitch is not resolved by this point-mass model. Height uses a relative scale. A is amber; B is turquoise.

Calculated state · choose a component below

The aircraft obeys force and kinematic equations. The controller receives the pressure-derived measurements.

Event timeline

Drag a B event · A stays fixed

Preparing calculation…

Whole-run summary · live values appear above

CAUSE → RESPONSE → COMPARISON

Follow the response

B · solid turquoise   A · dashed amber

Time plots share the playback cursor. Design sweeps and phase plots retain their own axes. A stopped run holds its final resolved state.

Compare A and B

Whole-run quantityA · savedB · liveB − AUnit

A snapshot includes parameter values and event times. Export retains both configurations and their calculated traces.

THE PHYSICS BEHIND THE RESPONSE

Read the model

Back to the experiment ↑

Follow each balance, then connect it to the response above. Open Symbols & units for the notation. A dot denotes a time derivative unless a non-dimensional time is stated.

01 / Follow the real aircraft

h˙=Vsin(γ)mV˙=T−D−mgsin(γ)L=m(Vγ˙+gcos(γ))

Actual motion follows force balance, even when a blocked pressure source gives the controller an incorrect indication.

Symbols & units
m
Aircraft mass · kg
V
True airspeed · m/s
γ
Flight-path angle; positive climbing · rad
T,D,L
Thrust, drag and lift · N
h
True altitude · m

02 / Convert pressure to speed

ptps=(1+κ−12M2)κκ−1V=MκRTair

The subsonic isentropic relation connects total and static pressure to Mach number. This model uses an independent true temperature to recover true airspeed.

Symbols & units
pt,ps
Total and static absolute pressure · Pa
M,κ
Mach number; specific-heat ratio 1.4
R,Tair
Gas constant · J/(kg K); temperature · K

03 / Close the feedback loop

γcmd=clamp(kh(hcmd−hsensed),−5°,5°)Tcmd=clamp(Ttrim+kV(Vcmd−Vsensed),0,Tmax)

Altitude error commands a flight-path angle. Airspeed error commands thrust. A plausible-looking but false indication can therefore produce a real control response.

Symbols & units
kh,kV
Height gain · rad/m; speed gain · N/(m/s)
Tmax
Maximum commanded thrust · 8000 N
clamp
Limit a demand to the stated lower and upper bounds

04 / Allow a finite response

γ˙=γcmd−γτγT˙=Tcmd−TτT

The aircraft path and thrust do not change instantaneously. Pressure-derived instrument values also have a 0.5 s first-order lag.

Symbols & units
τγ
Selected flight-path response time · s
τT
Thrust response time · 1.5 s
γ
Flight-path angle, not body pitch attitude · rad

Equations describe this bounded teaching model. Assumptions and source references are retained below. Internal calculations use SI units; controls and plots show their own labelled units.

Model limits & sources

Generic 3,000 kg aircraft; S = 24 m², CD = 0.026 + 0.055CL², |CL| ≤ 1.5, thrust 0–8 kN. Initial h = 1 km, TAS = 65 m/s. Pressure measurements use subsonic isentropic relations, independent true temperature and 0.5 s instrument lags. Thrust lag 1.5 s; path command ±5°. Blocked pressures are retained at the event. Invalid pressure reconstruction, excessive lift demand or speed below 30 m/s stops the trace. No sensor voting, detailed ADC, real flight-control law or post-stall model.

NASA · Pitot–static measurement ↗FAA · Aircraft systems ↗

Numerical checks test the stated equations. They do not establish aircraft certification or experimental accuracy. Schematic flow markers indicate direction; their speed is illustrative. No manufacturer geometry or performance data is reproduced. Version: coupled-labs-v1.1.

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