- #1
John O' Meara
- 330
- 0
A solid uniform disk of mass m and radius R is pivoted about a horizontal axis through its center, and a small body of mass m is attached to the rim of the disk. If the disk is released from rest with the small body at the end of a horizontal radius, find the angular velocity when the body is at the bottom.
Loss of P.E., = gain in K.E. Therefore
m*g*R = .5*I*w^2 + .5*m*v^2.
Where I = rotational inertia and w = angular velocity.
w=2*(g*R - 2*v)/R^2)^2.
Is this correct, if it isn't why or where? Thanks very much.
Loss of P.E., = gain in K.E. Therefore
m*g*R = .5*I*w^2 + .5*m*v^2.
Where I = rotational inertia and w = angular velocity.
w=2*(g*R - 2*v)/R^2)^2.
Is this correct, if it isn't why or where? Thanks very much.