4  First-Order Circuits

4.1 Dynamic Analysis RC Circuit

Figure 4.1: Step response of a RC circuit.

The node analysis for the parallel RC circuit yields:

\[ i(t) = \frac{v_C}{R} + C \frac{dv_C}{dt} \]

Or, rewritten as:

\[ \frac{dv_C}{dt} + \frac{v_C}{RC} = \frac{i(t)}{C} \]

This is a linear differential equation with constant coefficients.

The complete solution consists of two parts:

  1. Homogeneous Solution
  2. Particular Solution

The overall solution is the sum of these two parts.

The homogeneous equation:

\[ \frac{dv_{CH}}{dt} + \frac{v_{CH}}{RC} = 0 \]

Assume \(v_{CH} = Ae^{st}\):

Substituting and solving gives:

\[ s = -\frac{1}{RC} \]

So,

\[ v_{CH} = A e^{-t/RC} \]

  • Product \(RC\) has dimension of time called time-constant .

Particular Solution

For a constant input current \(I_0\):

\[ I_0 = \frac{v_{cp}}{R} + C \frac{dv_{cp}}{dt} \]

Assume \(v_{CP} = K\):

Substitute into the equation:

\[ v_{CP} = I_0 R \]


Complete Solution

Combine both solutions:

\[ v_C = A e^{-t/RC} + I_0 R \]

Apply initial condition at \(t = 0\):

\[ A = -I_0 R \]

Thus,

\[ v_C = -I_0 R e^{-t/RC} + I_0 R \]

or

\[ v_C = I_0 R (1 - e^{-t/RC}) \]


Effect of RC Value

  • Small RC: Faster charging, steeper curve.
  • Large RC: Slower charging, gradual curve.

Discharge Transient

For the discharge case (homogeneous solution):

  • Initial condition: \(v_C = I_0 R\) at \(t = 0\)
  • Solution:

\[ v_C = I_0 R e^{-t/RC} \]


General Form

\[ v_C = v_C(0) e^{-t/RC} \]


Properties of the Exponential Decay

  • For \(x = A e^{-t/\tau}\), the initial slope at \(t = 0\):

\[ \left. \frac{dx}{dt} \right|_{t=0} = -\frac{A}{\tau} \]

  • At \(t = \tau\):

\[ x(\tau) = \frac{A}{e} \]

  • Time to go from 90% to 10%:

\[ t_{90\%} - t_{10\%} = RC \ln\left(\frac{0.9}{0.1}\right) = 2.2\tau \]


Summary Table

Parameter Formula Notes
Time Constant (\(\tau\)) \(RC\) Determines response speed
Charging Voltage \(I_0 R (1 - e^{-t/RC})\) Step input
Discharge Voltage \(v_C(0) e^{-t/RC}\) Initial voltage \(v_C(0)\)
Initial Slope \(-A/\tau\) At \(t = 0\)
90%-10% Time Span \(2.2\tau\) Exponential decay

Notes

  • The exponential response is a hallmark of first-order RC circuits.
  • The time constant \(RC\) is critical for determining how quickly the voltage changes in response to a step input or discharge.