The total energy of a solid body at the top of a plane is,
( TE ) 0 =mgh
Here, m is the mass of the solid body, g is the gravitational acceleration and h is the vertical height of the inclined plane.
The equation for the moment of inertia of the solid body is,
I=m k 2
Here, k is the radius of gyration of the body about its symmetrical axis.
The equation for the linear velocity of the solid body at the bottom of the plane is,
v=Rω
Here, ω is the angular speed of the solid body and R is the radius of the solid body.
Solving for ω the equation is rearranged as,.
ω= v R
The equation for the total kinetic energy of the solid body at the bottom of the plane is,
( TE ) f = 1 2 m v 2 + 1 2 I ω 2
Substituting the values of I and ω in the above equation, we get:
( TE ) f = 1 2 m v 2 + 1 2 ( m k 2 ) ( v R ) 2 = 1 2 m v 2 + 1 2 m( k 2 R 2 ) v 2 = 1 2 m v 2 ( 1+ k 2 R 2 )
The expression for the law of conservation of energy is,
( TE ) 0 = ( TE ) f
Substituting the calculated values in the above equation we get:
mgh= 1 2 m v 2 ( 1+ k 2 R 2 ) gh= 1 2 v 2 ( 1+ k 2 R 2 ) v 2 = 2gh ( 1+ k 2 R 2 )
Thus, the velocity of translation of a rolling body at the bottom of the inclined plane, v is given by the equation:
v 2 = 2gh ( 1+ k 2 / R 2 ) .