look ill give u the soln. to a general case....
the free body diagram is as posted below.......let the mass be 'm' the length be 'l'........let 'N' be the normal force which the rod experiences from the bottom..............."
" be the coeff of friction..............
analysing rotational motion abt the pt rotation....ie the pt of contact with ground............
mgcos
*l/2 =ml2/3 *
...........................1) Torque abt pt P
so we have
=3gcos
/2l.......................2)
analysing accleration of centre of mass in horizontal direction.....
max=
N..............3)
analysing acceleration in vertical dirn....
mg-N= may........................4)
but we know that ay is nothing but component of accn of c.m in vertical dirn........and as no slipping.....
accn of c.m=
*l/2........
thus ax=
*l/2cos
................................5)
and ay=
*l/2sin
..................................6)
so using 1, 2, 3, 4, 5 and 6 and solving for 
we get....
=
here u can substitute theta as pi/3 to get the reqd. result....
from the above eqn.s solve for
and the 2 accns wud be
l/2 and
l respectively...(interms of g)
ill try to post the free body diagram...
hope it helps...
rate if useful....