There are two forces which are acting on the body tension on the string and the weight mg
T=mv2+mgcosθ
By substituting the velocity as follows,
v2=u2−2ag(1−cosθ)
We get the tension as
T=mu2a−mg(2−3cosθ)
At θ=60∘the tension in the string becomes negligible.
Hence we get
u=√ag2
The tension at the initial point of the projection is at θ=0∘
T=3mg2