Dieter Britz <[email hidden]> wrote in message news:<[email hidden]>...
Quoted message said:Some years ago, I read that the force required to push the
bike forward goes up as the cube of the speed. Is this
correct, and if so, why? It can't be wind resistance, as
that gives a force (for a sphere {:] ) that goes up
proportionally with the speed. Can this be friction of the
bearings and tyres?
The force required is proportional to the square of
velocity. The power required is proportional to the cube of
velocity (power = force X velocity).
So the faster you cycle on level ground the more power is
required to overcome air resistance.
The next most important force required (assuming level
ground) is rolling resistance - this is related to the hub
bearings, tyres and road surface (mainly the latter two; in
other words normally adjusted hub bearing require a trivial
amount of power to overcome their resistance).
The next force required is to overcome the drivetrain - this
is the chain and derailleur.
As an example consider Chis Boardman's UCI legal world
record. On a smooth indoor velodrome using the highest
qaulity tubs available on single speed bike (without
derailleur) over 92% of his power output is required to
overcome air resistance when travelling @ 49.442 km/h.
*** "Chris Boardman (GBR) Athlete's Hour Record,
Manchester, 2000"
***
Input Parameters [Metric Format]
--------------------------------
Cyclist Velocity [km/h] ................ 49.442
Power Total [W] ........................ 401.2 Power Air
Resistance [W] ............... 372.8 92.91% Power Rolling
Resistance [W] ........... 20.4 5.09% Power Drive Train [W]
.................. 8.0 2.00%