2.1 The Convolution Integral
So now we have examined several simple properties that the differential equation satisfies
linearity and time-invariance. We have also seen that the complex exponential has the special
property that it passes through changed only by a complex numer the differential equation. Also,
we have discussed the roll of tansforms, as representing arbitrary inputs via the superpositions of
complex exponentials. This discussion is often called a ”frequency domain analysis”. Frequency
domain analysis studyies the outputs of linear and time-invariant systems via their response to
complex exponentials. Now we turn our focus to a pure time domain analysis, understanding the
response of the differential equation directly in terms of its time domain inputs. For this we
explore the ”convolution integral”. We do this by solving the first-order differential equation
directly using integrating factors. For this, examine the differential equation and introduce the
integrating factor f(t) which has the property that it makes one side of the equation into a total
differential. Define
which implies
This implies the integrating factor is
, and using the boundary condition y(−∞) = 0 the
total differential is solved giving
We have almost arrived at our convolution formula. For this introduce the unit step function, and
the definition of the convolution formulation. The unit-step function is zero to the left of the
origin, and 1 elsewhere:
1, 0
0, 0
Definition 2.2. Given time signals f(t), g(t), then their convolution is defined as
Proposition 2.1. The output of this first order differential equation with input x(t) is given
according to
To see this, simply use the property of the unit step to rewrite the solution of Eqn. 13 according to
