Concept:
An ideal solenoid generates a uniform magnetic field inside it, oriented along its axis. A magnetic field can exert a force on a charged particle only when the particle’s velocity has a component perpendicular to the magnetic field direction.
The magnetic force on a moving charge is given by:
\[
\vec{F}_B = q\,\vec{v} \times \vec{B}
\]
Step 1: Directions of magnetic field and particle velocity
Inside the ideal solenoid, the magnetic field $\vec{B}$ is directed along the axis of the solenoid.
Since the axis of the solenoid is vertical, the magnetic field is also vertical.
The charged particle is projected vertically downward, so its velocity $\vec{v}$ is vertical as well.
Step 2: Magnetic force on the charged particle
\[
\vec{F}_B = q\,\vec{v} \times \vec{B}
\]
As the velocity $\vec{v}$ is parallel to the magnetic field $\vec{B}$,
\[
\vec{v} \times \vec{B} = 0
\]
Thus, no magnetic force acts on the charged particle.
Step 3: Resultant force and acceleration
With zero magnetic force, the only force acting on the particle is its weight:
\[
F = mg
\]
Hence, the acceleration of the particle is:
\[
a = g
\]
Conclusion:
The charged particle continues to accelerate solely due to gravity.
\[
\boxed{a = g}
\]