Figure shows the situation wn the load (body `P`) desceneds due to the stretch in the wires. The new positions of wires `PQ` and `PS` are shown by the dotted lines. Let `T_(1)` and `T_(2), T_(3)` be teloads (tensions) carried by the three wires `PQ, PR` and `PS`, respectively, with the wires `PQ` and `PS` making angle `theta` with the vertical.
Considering the horizontal equilibrium of point `P`
`T_(1)sintheta=T_(3)sinthetaimpliesT_(1)=T_(3)=T` (say)
Considering vertical equilibrium of point `P`
`T_(2)+2Tcostheta=Mg`..........i
If `delta_(1)` and `delta_(2)` be the elongations in the wires `PR` and `PQ` (or `PS`), respectively then
`deltal_(2)=deltal_(1)costheta` (from geometry)
If `A` and `Y` be the cross sectional area and Young's modulus of each of the wires, then
`T/(AY)(Asectheta)=(T_(2))/(AY)Acosthetaimplies T=T_(2)cos^(2)theta`........ii
Solving eqn i and ii `T_(2)=(Mg)/(1+2cos^(3)theta)`
and `T_(1)=T_(3)=T=(Mgcos^(2)theta)/(1+2cos^(3)theta)`