Given that \( F_1 \) and \( F_2 \) are perpendicular, the particle is under the influence of two forces. When \( F_1 \) is removed, the only force acting on the particle is \( F_2 \). The acceleration of the particle due to the force \( F_2 \) is given by Newton's second law:
\[
a = \frac{F_2}{m}
\]
Where:
- \( F_2 \) is the remaining force acting on the particle,
- \( m \) is the mass of the particle.
Thus, the acceleration of the particle is \( \frac{F_2}{m} \).