Let's say there is a solid cylinder floating in space and rotating about its axis of symmetry at rate $\omega$. At time t = 0 a force constant in magnitude is applied to the bottom of the cylinder. The force is parallel to the axis of symmetry and applied a distance r from it. From that moment forward, the force stays 'on' and its direction and point of application are fixed with respect to the cylinder. (In the second image below, the red vector represents the initial angular momentum, the blue vector represents the force, and the green vector represents the torque.)
Would the cylinder undergo precession (in addition to linear acceleration) or is the motion more complicated because the applied force is attached to the cylinder? I can see how for a precessing gyroscope always has the net torque perpendicular to $\frac{d\omega}{dt}$. I'm having trouble seeing if that would also be true here.

