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
Admittance parameters (y-parameters)
Any linear two-port network is described by the following equations
$$\begin{equation}I_1=y_{11}V_1 + y_{12}V_2\end{equation}$$ $$\begin{equation}I_2=y_{21}V_1 + y_{22}V_2\end{equation}$$or, in matrix form,
$$\begin{bmatrix}I_1\\I_2\end{bmatrix} = \begin{bmatrix}y_{11} & y_{12}\\y_{21} & y_{22}\end{bmatrix} \begin{bmatrix}V_1\\V_2\end{bmatrix}$$The 4 parameters are called:
- $y_{11}$ - short-circuit input admittance
- $y_{12}$ - short-circuit transfer admittance
- $y_{21}$ - short-circuit transfer admittance (similar to $y_{12}$)
- $y_{22}$ - short-circuit output admittance
Measure the admittance parameters
Using the above definition, once can show that the admittance parameters can be computed by using the following equations
$$\begin{equation}y_{11}=\left.{\frac{I_1}{V_1}} \right|_{V_2=0}\end{equation}$$ $$\begin{equation}y_{12}=\left.{\frac{I_1}{V_2}} \right|_{V_1=0}\end{equation}$$ $$\begin{equation}y_{21}=\left.{\frac{I_2}{V_1}} \right|_{V_2=0}\end{equation}$$ $$\begin{equation}y_{22}=\left.{\frac{I_2}{V_2}} \right|_{V_1=0}\end{equation}$$The above formulas can be used to build the circuit that we need to solve to measure the y-parameters. For instance, if we want to measure the $y_{11}$ parameter, we need to:
- Short-circuit the output terminals (because the constraint requires $V_{2}=0$ V, which is equivalent to a short-circuit)
- We connect a voltage source of 1 V at the input terminals (because the denominator in the definition of $y_{11}$ contains a voltage and the subscript is $1$, which denotes the input)
- Compute current $I_{1}$ at the input terminals (because the numerator in the definition of $y_{11}$ 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