The work done by →F1 is
W1=∫P2P1F1cosθds
From figure; s=R(π2−2θ)
or ds=(6m)d(−2θ)=−12dθ
and F1=20.
Hence, W1=−240∫0π/4cosθdθ
=240sinπ4=120√2J
The work done by →F3 is
W3=∫F3ds=∫6(π/2)0(15−10s)ds
=[15s−5s2]3π0=−302.8JJ
To calculate the work done by →F2 and by W, it is convenient to take the projection of the path in the direction of the force, instead of vice-versa. Thus,
W2=F2(¯¯¯¯¯¯¯¯OP2)=30(6)=180J
W=(−W)(¯¯¯¯¯¯¯¯¯¯P1O)=(−4)(6)=−24J
The total work done is W1+W3+W2+W=23J
Then, by the work-energy principle.
KP2−KP1=23J
=12(49.8)v22−12(49.8)(4)2=23
v2=11.3m/s