The work done on an object moving from position (x1, y1) to (x2, y2) under an applied force F is given by the work integral:
W = ∫ F ⋅ dr
where dr is the displacement vector from position (x1, y1) to (x2, y2).
For the given scenario, the applied force is F = (x^2 + y^2)i + (x^2 + y^2)^(1/2)j, and the displacement is from (4,0) to (0,4), which is given by dr = (-4, 4)i + (0, 4)j.
So, the work done is:
W = ∫ F ⋅ dr = ∫ ((x^2 + y^2)i + (x^2 + y^2)^(1/2)j) ⋅ ((-4)i + (4)j)
= ∫ -4x^2 - 4y^2 + 4(x^2 + y^2)^(1/2) dx
This work integral cannot be solved in closed form and will require numerical methods to evaluate the definite integral.