Answer:

Explanation:
From the free body diagram attached below; we will see that
T₃ = Fg ------ (1)
Thus; as the system is in equilibrium, the net force in the x and y direction shows to be zero
Then;


Also;

---- (3)
From equation (2):

Replacing the above value for T₂ into equation 3; we have


---- (4)
Using trigonometric identity Sin (A+B) = SIn A cos B + Cos A sin B
So ; equation 4 can now be:
--- (5)
replacing equation (1) into equation (5) ; we have:

Hence; the tension in the string is:
