Hi Arun!
A board swinging about its end is what is called a "physical pendulum." In a simple pendulum, the mass is all concentrated at the end of the support, and the rest of the support is considered to have insignificant mass. In a physical pendulum, though, the mass is spread all along the support (which I assume to be uniform; otherwise, we would need to have some kind of mass distribution function). In this case, the period of the pendulum is given by:
T = 2π(√(I/mgLcm))
where
I = moment of inertia of the object around the support axis
m = mass of object
Lcm = distance from the support point to the center of mass
For a uniform rod (or board) swinging around one end, we can look up the moment of inertia in a table (or online). It is:
I = (1/3)mL2
where
L = full length of the board
So we get, for the period:
T = 2π(√(((1/3)mL2)/(mgLcm))
with, in this case:
L = 3 m
Lcm = 1.5 m (since the center of mas should be halfway down the board from the support point)
Note that the mass of the board cancels out here, so it does not matter (which is why it is not given).
Using g = 9.8 m/s2, I get T = 2.84 s.
I hope this helps! Just let me know if you have any questions at all about this.