Three forces F2, F2 & F3 are acting on a particle of mass m such that F2 & F3 are mutually perpendicular, then the particle remains stationary. If the force F1 is now removed, then the acceleration of the particle is
\(\frac { { F }_{ 1 } }{ m } \)
\(\frac { { F }_{ 2 }{ F }_{ 3 } }{ mF } \)
\(\frac { { F }_{ 2 }-{ F }_{ 3 } }{ m } \)
\(\frac { { F }_{ 2 } }{ m } \)