Figure shows a rod of length L pivoted near an end and which is made to rotate in a horizontal plane with a constant angular speed. A ball of mass ma is suspended by a string also of length L from the other end of the rod. If θ is the angle made by sting with the vertical, then
(A) T sinθ = mω2 L( 1 + sinθ)
(B) T cosθ mg
(C) tan θ = \(\frac{\omega^2L(1+ sin \theta)}{g}\)
(D) None of above