Let us consider the system in a frame rotating with the rod. In this frame, the rod is at rest and experiences not only the gravitational force m vector g and the reaction force vector R, but also the centrifugal force vector Fcf.
In the considered frame, from the condition of equilibrium i.e. Noz=0

or, Ncf=mg l/2sinθ .......(1)
where Ncf is the moment of centrifugal force about O. To calculate Ncf, let us consider an element of length dx, situated at a distance x from the point O. This element is subjected to a horizontal pseudo force (m/l) dxω2xsinθ.
The moment of this pseudo force about the axis of rotation through the point O is
