When forces F1 , F2 , F3 are acting on a particle of mass m such that F2 and F3 are mutually perpendicular, then the particle remains stationary. If the force F1 is now removed then the acceleration of the particle is
(a) F1/m
(b) F2F3 /mF1
(c) (F2 – F3 )/m
(d) F2 /m.