
Chapter 7
Returning to the RC network, we can ask — how did we actually arrive at the transfer
function stated above? For that, we first use Kirchhoff’s voltage law to generate the
following differential equation:
v
i
= v
res
(t ) + v
cap
(t ) = i(t)R +
q(t)
C
where i(t) is the charging current, q(t) is the charge on the capacitor, v
res
(t) is the voltage
across the resistor, and v
cap
(t) is the voltage across the capacitor (i.e. v
o
(t), the output).
Further, since charge is related to current by dq(t)/dt = i(t), we can write the preceding
equation as
v
i
= R ×
dq(t)
dt
+
q(t)
C
or
dq(t)
dt
+
1
RC
q(t) =
v
i
R
At this point we actually “cheat” a little. Knowing the properties of ...