Chassis & Dynamics
Aero Drag & Top Speed
Drag force, power demand and the speed where power runs out.
Inputsdrag · tap · type
m²
kW
kg
km/h
Fig. 16Airflow and power demand
Total demandAeroRolling
Theoretical top speed251km/hwhere demand meets available power
Power needed at 130 km/h25.4kW
Aero drag force527N
Rolling resistance177N
Drag area CdA0.66m²
Aero share of load75%
§ How it works
At steady speed on a level road the engine fights two forces: the air it has to shove aside, and the tires flexing as they roll.
Aerodynamic drag
- : air density, 1.225 kg/m³ at sea level and 15 °C.
- : drag coefficient, a measure of shape. : frontal area. Their product is what the air actually "sees".
- : speed through the air in m/s. Drag force grows with its square.
Rolling resistance
Roughly constant with speed, so it dominates in town and fades into the background on the motorway.
Power demand
Power is force times speed, which adds one more factor of :
That cubic term is why top speed is so expensive. Going 10 % faster needs about 33 % more power; doubling top speed needs roughly eight times as much. Top speed is found where the demand curve crosses the power the car can put to the road.
References
- Modern Drag Equation — NASA Glenn Research Centerthe D = ½·Cd·ρ·V²·A form used above