well this is a small problem in statics
u see force is applied such that it is moved slowly
=> At every instant it is in equillibrium
let the angle of the rod be theta
then as F is applied perpendicular to the rod, Fsinθ=f
for coefficient of friction to be minimum F should be minimum(as it will pass through all angles)
so to produce the maximum torque F should be applied at the end
at an instant
F*2L=mgcosθL
F=mgcosθ/2
further for horizontal and vertical equillibrium
Fsinθ=f
and Fcosθ+N=mg
as f<=μN
solving we get μ>cosθsinθ/(1+sin2θ)
now for no slipping μ should be greater than this value for all angles upto 90
If we make μ greater than the maximum possible value of the expression then it will take care of all angles ..
so maximum value of cosθsinθ/1+sin2θ
= sinθ/cosθ/(sec2θ+tan2θ)
=(1/((1/tanθ)+2tanθ))
applying A.M>=G.M to denominator
we get minimum value as 1/2√2 not 1/√3 as u mentioned in the question
I am very sure that this is the answer .. check your question
oherwise maybe i understood your problem wrongly - but that will be evident from my method above so please check ..