Here, α = 36.9°, β = 53.1°
If T1, T2 are tensions in the string. Then for equilibrium along the horizontal
T1 sin α = T2 sin β
or, T1/T2 = sin β/sin α = sin 53.1°/sin 36.9°
= 0.747/0.5477 = 1.3523
d is the distance of the centre of gravity G of the bar from the left end.
For rotational equilibrium about c.
T1 cos α x d = T2 cos β(2 - d)
or, T1 cos 36.9° x d = T2 cos 53.1°(2 - d)
or, T1 0.8366 d = T2 x 0.6718(2 - d)
Putting T1 = 1.3523 T2
We get d = 0.745 m = 74.5 cm