For the op amp circuit in Fig. 7.55(a), find v_{o} for t > 0 given that v(0)= 3 V . Let R_{f} = 80 kΩ, R_{1} = 20 kΩ, and C = 5 μF.
This problem can be solved in two ways:
■ METHOD 1 Consider the circuit in Fig. 7.55(a). Let us derive the appropriate differential equation using nodal analysis. If v_{1} is the voltage at node 1, at that node, KCL gives
\frac{0 – v_{1}}{R_{1}} = C \frac{dv}{dt} (7.14.1)
Since nodes 2 and 3 must be at the same potential, the potential at node 2 is zero. Thus, v_{1} – 0 = v or v_{1} = v and Eq. (7.14.1) becomes
\frac{dv}{dt} + \frac{v}{CR_{1}} = 0 (7.14.2)
This is similar to Eq. (7.4b) so that the solution is obtained the same way as in Section 7.2, i.e.,
\frac{dv}{dt} + \frac{v}{RC} = 0 (7.4b)
v(t) = V_{0} e^{-t/\tau} , \tau = R_{1} C (7.14.3)
where V_{0} is the initial voltage across the capacitor. But v(0) = 3 = V_{0} and \tau = 20 × 10^{3} × 5 × 10^{-6} = 0.1 Hence,
v(t) = 3e^{-10t} (7.14.4)
Applying KCL at node 2 gives
C \frac{dv}{dt} = \frac{0 – v_{o}}{R_{f}}
or
v_{o} = – R_{f} C\frac{dv}{dt} (7.14.5)
Now we can find v_{0} as
v_{o} = -80 × 10^{3} × 5 × 10^{-6} (-30 e^{-10t} ) = 12 e^{-10t} V , t > 0
■ METHOD 2 Let us apply the short-cut method from Eq. (7.53). We need to find v_{o}(0^{+}), v_{o}(∞), and \tau . Since v(0^{+}) = v(0^{-}) = 3 V we apply KCL at node 2 in the circuit of Fig. 7.55(b) to obtain
v(t) = v(∞) + [ v(0) – v(∞) ] e^{t/\tau} (7.53)
\frac{3}{20,000} + \frac{0 – v_{o}(0^{+})}{80,000} = 0
or v_{o} (0^{+}) = 12 V . Since the circuit is source free,v(∞)= 0 V To find \tau we need the equivalent resistance R_{eq} across the capacitor terminals. If we remove the capacitor and replace it by a 1-A current source, we have the circuit shown in Fig. 7.55(c). Applying KVL to the input loop yield
20,000(1) – v = 0 ⇒ v = 20kV
Then
R_{eq} = \frac{v}{1} = 20 k Ω
and \tau = R_{eq}C = 0.1 . Thus,
v_{o} (t) = v_{o} (∞) + [v_{o}(0) – v_{o} (∞)] e^{-t/ \tau}
= 0 + ( 12 – 0 ) e^{-10t} = 12 e^{-10t} V , t > 0
as before.