The dynamical system governed by the following time-varying ordinary differential equation

is a variation of the classic forced mass-spring-dashpot system with mass

, dashpot constant

, constant stiffness

, and forcing term

. Aging springs are characterized by a stiffness decaying with time. Here an exponential decay

from an initial value

at time zero to an asymptotic value

is considered.
Mathematica can integrate this equation exactly, but the solution in general is a huge expression involving
BesselJ and
Gamma functions, together with their integrals; it is very difficult to imagine their behavior as time advances.