--- title: "Impulse response" sort_title: "Impulse response" date: 2021-03-09 categories: - Mathematics - Physics layout: "concept" --- The **impulse response** $$u_p(t)$$ of a system whose behaviour is described by a linear operator $$\hat{L}$$, is defined as the reponse of the system when forced by the [Dirac delta function](/know/concept/dirac-delta-function/) $$\delta(t)$$: $$\begin{aligned} \boxed{ \hat{L} \{ u_p(t) \} = \delta(t) } \end{aligned}$$ This can be used to find the response $$u(t)$$ of $$\hat{L}$$ to *any* forcing function $$f(t)$$, i.e. not only $$\delta(t)$$, by simply taking the convolution with $$u_p(t)$$: $$\begin{aligned} \hat{L} \{ u(t) \} = f(t) \quad \implies \quad \boxed{ u(t) = (f * u_p)(t) } \end{aligned}$$ {% include proof/start.html id="proof-theorem" -%} Starting from the definition of $$u_p(t)$$, we shift the argument by some constant $$\tau$$, and multiply both sides by the constant $$f(\tau)$$: $$\begin{aligned} \hat{L} \{ u_p(t - \tau) \} &= \delta(t - \tau) \\ \hat{L} \{ f(\tau) \: u_p(t - \tau) \} &= f(\tau) \: \delta(t - \tau) \end{aligned}$$ Where $$f(\tau)$$ can be moved inside using the linearity of $$\hat{L}$$. Integrating over $$\tau$$ then gives us: $$\begin{aligned} \int_0^\infty \hat{L} \{ f(\tau) \: u_p(t - \tau) \} \dd{\tau} &= \int_0^\infty f(\tau) \: \delta(t - \tau) \dd{\tau} = f(t) \end{aligned}$$ The integral and $$\hat{L}$$ are operators of different variables, so we reorder them: $$\begin{aligned} \hat{L} \int_0^\infty f(\tau) \: u_p(t - \tau) \dd{\tau} &= (f * u_p)(t) = \hat{L}\{ u(t) \} = f(t) \end{aligned}$$ {% include proof/end.html id="proof-theorem" %} This is useful for solving initial value problems, because any initial condition can be satisfied due to the linearity of $$\hat{L}$$, by choosing the initial values of the homogeneous solution $$\hat{L}\{ u_h(t) \} = 0$$ such that the total solution $$(f * u_p)(t) + u_h(t)$$ has the desired values. Meanwhile, for boundary value problems, the related [fundamental solution](/know/concept/fundamental-solution/) is preferable. ## References 1. O. Bang, *Applied mathematics for physicists: lecture notes*, 2019, unpublished.