2.3 LTI Continuous-Time Systems 139
Remarks
n We will see that the impulse response is fundamental in the characterization of linear time-invariant
systems.
n Any system characterized by the convolution integral is linear and time invariant by the above construction.
The convolution integral is a general representation of LTI systems, given that it was obtained from a
generic representation of the input signal.
n We showed before that a system represented by a linear differential equation with constant coefficients and
no initial conditions, or input, before t= 0 is LTI. Thus, one should be able to represent that system by a
convolution integral after finding its impulse response h(t).
nExample 2.9
Obtain the impulse response of a capacitor and use it to find its unit-step response by means of
the convolution integral. LetC=1 F.
Solution
For a capacitor with a initial voltagevc( 0 )=0, we have that
vc(t)=
1
C
∫t
0
i(τ)dτ
The impulse response of a capacitor is found by letting the inputi(t)=δ(t)and the outputvc(t)=
h(t), which according to the above equation becomes
h(t)=
1
C
∫t
0
δ(τ)dτ=
1
C
t> 0
and zero ift<0, orh(t)=( 1 /C)u(t). ForC= 1 F, to compute the unit-step response of the
capacitor we let the inputi(t)=u(t), andvc( 0 )=0. The voltage across the capacitor is
vc(t)=
∫∞
−∞
h(t−τ)i(τ)dτ=
∫∞
−∞
1
C
u(t−τ)u(τ)dτ
and since, as a function ofτ,u(t−τ)u(τ)=1 for 0≤τ≤tand zero otherwise, we have that
vc(t)=
∫t
0
dτ=t
fort≥0 and zero otherwise (as the input is zero fort<0 and there are no initial conditions),
orvc(t)=r(t). The above result makes physical sense since the capacitor is accumulating charge
and the input is providing a constant charge, so that the result is a ramp function. Notice that the
impulse response is the derivative of the unit-step response.