When forces F1, F2 and 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
→F1+→F2+→F3=0∴→F1=−(→F2+→F3)
If F1 is removed, the resultiant of →F2 and →F3 is F1 in magnitude so acceleration =F1m