A particle of mass
m moves along the quarter section of the circular path whose centre is at the origin. The radius of the circular path is
a. A force
→F=y^i−x^j newton acts on the particle, where
x,y denote the coordinates of position of the particle. The work done by this force in taking the particle from point A (
a,0) to point B (
0,a) along the circular path is