In solving the above second-order equation, it is common to rewrite it in terms of two coupled first-order equations with the velocity
v(t)=\frac{dx}{dt},and the acceleration
\frac{dv}{dt}=F(t)-\eta v(t)-x(t).With the initial conditions v_0=v(t_0) and x_0=x(t_0) defined, we can integrate these equations and find their respective solutions.