mechagouki":jbqhtcta said:
I'm not convinced - a wheel clearly has greater inertial weight whilst decelerating (than when stationary) or you wouldn't be able to ghost-ride bikes or do the old wheel as a gyroscope trick. and surely as the rotor is bolted to the wheel it's weight would increase proportionally.
I think we're at risk of getting lost in bad definitions.
A moving wheel has angular momentum, and angular momentum increases with angular velocity just as linear momentum increases with linear velocity. Inertial mass is the ratio between applied force and acceleration:
m=F/a
Because the wheel is rotating, you need to put more energy in to make it accelerate to a given speed that if it were simply sliding along on a frictionless surface. You can express that by making a correction to
m to take account of the rotational motion.
It's tricky to write out the equations on this forum, but if you write the total kinetic energy equation for the wheel with two terms, one linear and one rotational,
m becomes
m(1+(r/R)²) where
r is the radius of the rotor, and
R is the radius of the rim. You can see that the maximum possible value of the effective inertial mass is
2m, when
r=R, i.e. when the brake rotor is as big as the wheel.
I thought that it was accepted knowledge that the rotational weight of a wheel was the stationary weight multiplied by Pi?
I've no idea where you got that from. The effective "rotating weight" (moment of inertia) of a wheel depends on how the mass is distributed around the axis of rotation, and you can calculate that using the site you just posted:
http://easycalculation.com/physics/clas ... nertia.php
It's effectively the sum of
mr² for all the components of the wheel. That's why mass near the periphery is so much more important than mass near the axis. If all the mass is concentrated at the periphery of the wheel (the theoretical worst case) the maximum total effective inertial mass is
2m.