You get linear equations of motion for the important case of harmonic oscillators. The EoM reads
$$m \ddot{x}+2 m \gamma \dot{x}+m\omega^2 x=F,$$
where ##F=F(t)## is an external force, ##\gamma## the damping, and ##\omega## the eigenfrequency of the (undamped) oscillator.
It's among the most simple equations of state, and you should carefully study its solutions. It's often a good approximation for the bound motion around the minimum of a more complicated potential, if the deviation from this stable fix point doesn't become too large (small amplitudes of oscillations).