here's the solution
Using conservation of energy between the initial position n at the position at angle Q, we have
( Mp w2 / 2) = [mg (1-cosQ)] (l/2)
where Mp is the moment of inertia wrt axis passing thru P , having value
Mp = [m(l/2)2 ] /3
frome this we have w2 = 3g(1-cosQ)/l ............(1)
Also Mp (alpha) = mg(l/2) sin Q
where alpha is the angular acceleration,
so, alpha = (3gsinQ) / 2l ...........(2)
Now as in the given figure, Fy = mg + mar cosQ + mat sinQ
and Fx = mat cos Q- mar sinQ
Where ar = radial acceleration
= w2 (l/2)
and at = tangential acceleration
= alpha (l/2)
thus using equation 1 and 2, we can solve for Fx and Fy