The following equations take into account all of the relevant resistance components:
Rolling friction including the dynamic (speed-dependent) rolling friction, air drag including the influence of wind speed, mechanical losses, and uphill/downhill forces.
|
P |
Rider's power |
V |
Velocity of the bicycle |
W |
Wind speed |
Hnn |
Height above sea level (influences air density) |
T |
Air temperature, in ° Kelvin (influences air density) |
grade |
Inclination (grade) of road, in percent |
β |
("beta") Inclination angle, = arctan(grade/100) |
mbike |
Mass of the bicycle (influences rolling friction, slope pulling force, and normal force) |
mrider |
Mass of the rider (influences rolling friction, slope pulling force, and the rider's frontal area via body volume) |
Cd |
Air drag coefficient |
A |
Total frontal area (bicycle + rider) |
Cr |
Rolling resistance coefficient |
CrV |
Coefficient for velocity-dependent dynamic rolling resistance, here approximated with 0.1 |
CrVn |
Coefficient for the dynamic rolling resistance, normalized to road inclination; CrVn = CrV*cos(β) |
Cm |
Coefficient for power transmission losses and losses due to tire slippage (the latter can be heard while pedaling powerfully at low speeds) |
ρ |
("rho") Air density |
ρ0 |
Air density on sea level at 0° Celsius (32°F) |
p0 |
Air pressure on sea level at 0° Celsius (32°F) |
g |
Gravitational acceleration |
Frg |
Rolling friction (normalized on inclined plane) plus slope pulling force on inclined plane |