Answer:
[tex]T_{2}=\frac{535}{sin(\theta _{2})+cos(\theta _{2})tan(\theta _{1})}[/tex]
[tex]T_{1}=\frac{535}{sin(\theta _{1})+cos(\theta _{1})tan(\theta _{2})}[/tex]
Explanation:
Consider the general position of the climber as shown in the figure
we have for equilibrium along x and y directions we have
[tex]T_{1}cos(\theta _{1})=T_{2}cos(\theta _{2})\\\\T_{1}sin(\theta _{1})+T_{2}sin(\theta _{2})=W\\\\[/tex]
upon solving we get
[tex]T_{1}sin(\theta _{1})+\frac{T_{1}cos(\theta_{1})}{cos(\theta _{2})}sin(\theta _{2})=W\\\\T_{1}=\frac{W}{sin(\theta _{1})+cos(\theta _{1})tan(\theta _{2})}[/tex]
Similarly
[tex]T_{2}=\frac{W}{sin(\theta _{2})+cos(\theta _{2})tan(\theta _{1})}[/tex]