QUOTE(bondo @ Jul 18 2006, 10:34 AM)
Has anyone ever calculated the "theoretical benefit" as far as acceleration goes? It's an inertial effect, so it should be possible to roughly calculate an equivalent weight loss of non rotating mass. I.E. every 1 pound of mass removed from the flywheel is equivalent to lightening the body by x pounds. I'm guessing it would be something like 1.03.
This wouldn't takie into account the possible ability to shift faster, but you have to be pretty darn good to take advantage of that anyways.
There is some interesting numbers in
THIS THREADI found this quote from the thread interesting
"The lighter the rotating components the less energy needed to change their
rotational speed. The shape and radius also are important in this regard. lw
components let the drivtrain rev quicker(and shed revs quicker) and makes
clutch control more critical during street starts.
the biggest factor in the energy requirement equations is the angular velocity
which is a squared quantity it is analagous to v in the more familiar mv2
formulation
this means that the faster something rotates the more significant the loss of a
small quantity of mass is. Losing 2# from the clutch flywheel is far more
significant than losing 2# at the wheels.
I made a ss once that calculated compared the relative energy requirements
of the various components, both rotational and translational, during
acceleration. I'll have to see if I can dig it up, but from memory ~1# at the
flywheel is roughly comparable to ~10# at the wheels which is roughly 3hp"