For continuous A,fA,f, the solution of y′=A(t)y+f(t)y'=A(t)y+f(t), y(s)=ysy(s)=y_s, is

y(t)=Φ(t,s)ys+∫stΦ(t,τ)f(τ) dτ,y(t)=\Phi(t,s)y_s+\int_s^t\Phi(t,\tau)f(\tau)\,d\tau,

where Φ\Phi is the of the homogeneous system. This is Duhamel's formula, also called variation of constants.

Verification

Differentiate the integral: its moving endpoint contributes f(t)f(t), and differentiating the propagator contributes A(t)A(t) times the integral. The initial condition follows at t=st=s. Equivalently, differentiating X(t)−1y(t)X(t)^{-1}y(t) gives X(t)−1f(t)X(t)^{-1}f(t). Bounds on Φ\Phi therefore turn source bounds into solution bounds.