See what the air is doing to the airplane
Change power, elevator, flap setting, weight, wind, and turbulence. Indicated airspeed and altitude emerge from those inputs, while the diagram resolves the major forces, shows the approach to a stall, and models the consequences of prolonged high-altitude flight without supplemental oxygen.
GROUND SPEED
Groundspeed
Vertical speed
See where each gallon’s energy goes
This is no longer a weighted teaching score. The powered index comes directly from modeled lift-to-drag ratio × propeller efficiency ÷ brake-specific fuel consumption, normalized to this model’s clean best-range condition. With the engine stopped it reports aerodynamic glide efficiency.
EFFICIENCY
Adjust one control at a time and watch what changes.
The index is a direct relative result from the simulation’s aerodynamic, propeller, and fuel-flow model—not a weighted opinion score. Wind changes range over the ground but does not change the airplane’s own energy conversion, so the index uses airspeed. It is not a POH range prediction or fuel-planning value.
One force picture, several different limits
Lift and load factor
Dynamic pressure, wing area, actual intermediate flap position, and angle of attack determine the modeled lift. The tracked single-slot flaps take time to move, so lift, drag, stall speed, and pitching moment change continuously during extension or retraction rather than jumping when a button is selected. Lift divided by weight produces load factor. A 2 G pull requires roughly twice the lift and raises stall speed. The elevator control uses the 172N’s published 28° up and 23° down surface travel; wing angle of attack is a separate calculated result, not the elevator angle.
Two kinds of drag
Parasite drag rises rapidly with airspeed and exposed landing gear or flap extension. Induced drag is the lift-related cost of producing lift and becomes most important at low speed and high lift coefficient.
Approach to the stall
The displayed stall speed is a 1-G reference, not a stall switch. Lower speed reduces dynamic pressure, so maintaining altitude requires progressively more angle of attack. The warning begins only as the wing approaches the modeled 16° critical angle. At the break, airflow separates, lift drops rapidly—but not to zero—and the trainer pitches nose-down into a continuing descent. Recovery begins only after the pilot lowers angle of attack below the critical angle long enough for airflow to reattach; raising the nose too soon can cause a secondary stall.
Power, propwash, pitch, and airspeed
Pitch is no longer a hand-set visual offset. The model sums the 172N’s angle-of-attack stability, elevator control power, pitch-rate damping, thrust-line moment, and pitch inertia. Changing RPM changes thrust and its pitching moment; NASA actuator-disk momentum theory then calculates the propeller’s induced airflow from thrust, propeller diameter, air density, and present airspeed. That added dynamic pressure is applied only to the root-wing area and tail inside the slipstream—not to the complete wing—so powered local lift, induced drag, and elevator authority change together. Published Cessna 172N performance anchors and the shared propeller momentum model drive thrust, propwash, pitch response, airspeed, and altitude.
Turbulence and buffet
The turbulence selector now drives a Dryden-style colored-gust field instead of arbitrary motion. Longitudinal, lateral, and vertical gust velocities use RMS intensity, altitude-dependent scale length, and the airplane's speed through the air mass. Vertical gust velocity changes angle of attack and load; lateral gust velocity drives the roll and control response. Stall buffet uses a separate short-scale filtered component, so the shaking is irregular but does not create imaginary lift or altitude.
Forward slip
The slip control no longer assigns a fixed angle or minimum descent rate. Published 172N lateral stability and control derivatives solve the crossed rudder and opposite-aileron balance. The resulting sideslip creates a calculated side force, which sets the wing-low bank needed to hold the original ground track. Exposed side area and dynamic pressure determine the added drag; that drag’s power then removes altitude energy from the same flight model. More airspeed, more crossed control, and aircraft weight therefore change the result naturally.
Altitude, oxygen, and hypoxia
Without supplemental oxygen, the panel follows the FAA operating thresholds: required crew must use oxygen after 30 minutes from 12,500 through 14,000 feet pressure altitude, and continuously above 14,000 feet. Impairment is progressive—not an instant boundary—and varies widely. To make that progression observable, one real second represents one minute on the physiology demonstration clock. Severe exposure causes modeled pilot incapacitation, a time-compressed uncontrolled descent, and ground impact. The extreme-altitude range exists to teach physiology; it does not imply that this normally aspirated 172N can climb to those altitudes.
Useful for concepts—not aircraft operation
The geometry and limits represent a legacy Cessna 172N-style landplane: 174 ft² of wing area, 2,300 lb maximum weight, 160 hp at 2,700 RPM, 40° maximum landing flap deflection, and a red line near 160 KIAS. Performance anchors come from its POH: 50-knot clean and 44-knot full-flap power-off stalls, 65 KIAS best glide, 770 ft/min maximum sea-level climb at 73 KIAS, and the published 2,000-foot cruise table. A 172N has fixed landing gear; the gear selector is an explicitly hypothetical comparison. This remains an educational approximation—not a POH, performance calculator, or substitute for instruction.
Model basis: Published Cessna and FAA operating data anchor the envelope and performance. Published UIUC/NASA derivatives and standard equations supply the dynamic model. Explicit training thresholds remain educational methodology rather than aircraft certification data.