Linear Circuit Analysis
1. Introduction
2. Basic Concepts
- Currents and voltages
- Linear circuits
- Linear components
- Loops and nodes
- Series and parallel
- R, L & C combinations
- V & I combinations
- Power and energy
3. Simple Circuits
- Ohm's law
- Kirchhoff's current law
- Kirchhoff's voltage law
- Single loop circuits
- Single node-pair circuits
- Voltage division
- Current division
4. Nodal and Mesh Analysis
5. Additional Analysis Techniques
- Superposition
- Source transformation
- The $V_{test}/I_{test}$ method
- Norton equivalent
- Thévenin equivalent
- Max power transfer
6. AC Analysis
7. Operational Amplifiers
8. Laplace Transforms
9. Time-Dependent Circuits
- Introduction
- First-order transients
- Nodal analysis
- Mesh analysis
- Laplace transforms
- Additional techniques
10. Two-port networks
Inverse transmission parameters (A'B'C'D'-parameters also called t'-parameters)
Any linear two-port network is described by the following equations
$$\begin{equation}V_2=A' V_1 - B' I_1\end{equation}$$ $$\begin{equation}I_2=C' V_1 - D' I_1\end{equation}$$or, in matrix form,
$$\begin{bmatrix}V_2\\I_2\end{bmatrix} = \begin{bmatrix}A & B\\C & B\end{bmatrix} \begin{bmatrix}V_1\\-I_1\end{bmatrix}$$Measure the y-parameters
Using the above definitiion, once can show that the admittance parameters can be computed by using the following equations
$$\begin{equation}A'=\left.{\frac{V_2}{V_1}} \right|_{I_1=0}\end{equation}$$ $$\begin{equation}B'=-\left.{\frac{V_2}{I_1}} \right|_{V_1=0}\end{equation}$$ $$\begin{equation}C'=\left.{\frac{I_2}{V_1}} \right|_{I_1=0}\end{equation}$$ $$\begin{equation}D'=-\left.{\frac{I_2}{I_1}} \right|_{V_1=0}\end{equation}$$The above formulas can be used to build the circuit that we need to solve to measure the transmission parameters. For instance, if we want to measure the $A'$ parameter, we need to:
- Open-circuit the input terminals (because the constraint requires $I_{1}=0$ A, which is equivalent to an open-circuit)
- Since we open-circuited the input terminals, we can connect a voltage source of 1 V at the output terminals (because the numerator in the definition of $A'$ contains a voltage and the subscript is $2$, which denotes the output), and
- Compute voltage $V_{1}$ at the input terminals (because the numerator in the definition of $A'$ contains a current and the subscript is $1$, which denotes the input)
- Short-circuit the input terminals (because the constraint requires $V_{1}=0$ V, which is equivalent to a short-circuit)
- Since we short-circuited the input terminals, we can connect a voltage source of 1 A at the output terminals (because the numerator in the definition of $B'$ contains a voltage and the subscript is $2$, which denotes the output), and
- Compute current $I_{1}$ at the input terminals (because the numerator in the definition of $B'$ contains a current and the subscript is $1$, which denotes the input)
Sample Solved Problems
The examples below are randomly generated.
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DC two-port networks
2 loops and 3 R
2 loops and 3 R (analytical)
3 loops and 6 R
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AC two-port networks
2 loops and 1 R, 1 L, 1 C
3 loops, 4 R, 1 L, 1 C, 1 dependent source
5 loops, 4 R, 1 L, 1 C, 1 dependent source