Set a flare event and compare the same approach with and without the ground. Follow height, speed and lift together.
ONE CALCULATION · CONNECTED VIEWSA · AMBER B · TURQUOISE
Drag to orbit · right-drag to pan · scroll to zoom. Body pitch = path angle + incidence. Height is exaggerated ×10 relative to distance. A is amber; B is turquoise.
Calculated state · choose a component below
A fair ground-effect comparison keeps mass, speed, height and control inputs identical.
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 quantity
A · saved
B · live
B − A
Unit
A snapshot includes parameter values and event times. Export retains both configurations and their calculated traces.
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 / Resolve the flight-path forces
The flare changes lift and path curvature; weight still acts vertically. Contact occurs when wheel height reaches zero.
Symbols & units
Aircraft mass · kg
True airspeed · m/s
Flight-path angle; positive climbing · rad
Thrust, drag and lift · N
Wheel height above the runway · m
02 / Scale the ground influence
This smooth teaching fit reduces induced drag as the wing approaches the surface. With ground effect switched off, φ is set to 1.
Symbols & units
Ground-effect factor · dimensionless
Wing height above the runway · m
Span · 13 m
03 / Update lift and drag together
The same ground factor changes both the lift slope and the induced-drag term. The profile-drag coefficient remains 0.04.
Symbols & units
Incidence; lift offset 2° · rad internally
Span efficiency 0.8; aspect ratio b²/S
Lift and drag coefficients · dimensionless
04 / Apply the flare command
The selected incidence step is followed with a finite response time. This is a prescribed-incidence point-mass model, not a solved pitch-control or landing-gear model.
Symbols & units
Initial incidence plus the selected step after the event
Incidence response time · s
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 point mass; S = 24 m², span 13 m, e = 0.8, sea-level density 1.225 kg/m³. Wing is 2 m above wheel contact height. The smooth ground-effect factor is an illustrative fit to the FAA approximate induced-drag reductions at h/b = 0.1 and 0.25; it is not a CFD solution or a particular wing measurement. Initial path −3°. Incidence follows a first-order command; body pitch dynamics are excluded. Integration stops at touchdown, CL > 1.6, TAS < 25 m/s, |γ| > 20°, or 60 s. No tyre, strut, crosswind or autopilot flare model.
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.