A thin disc rotates about an axis passing through its centre and perpendicular to its plane with a constant angular velocity ' ω' I is the moment of inertia of that disc and 'L' is its angular momentum about the given axis. Then rotational kinetic energy of the disc 'E' is
A) E L2 B) E L-2 C) E l D)E l-1
(KE)r = 1/2 IW2 = 1/2 ( (IW)2 / I )
⇒ (KE)r = L2 / 2I
.: E = 1/2 IW2 and E = L2 / 2I
Also , L = I W
Since W is constant ,
E α i and L α I only (c) is correct.