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. Magnetically Coupled Circuits
8. Operational Amplifiers
9. Laplace Transforms
10. Time-Dependent Circuits
- Introduction
- First-order transients
- Nodal analysis
- Mesh analysis
- Laplace transforms
- Additional techniques
11. Two-port networks
Appendix
Voltage Source Combinations
Series
If two or more voltage sources $V_1$, $V_2$, ... $V_n$ are connected in series they can be replaced with a single voltage source with $$V_{eff}=\pm V_1 \pm V_2\pm...\pm V_n$$ where the terms in the right hand side are taken with $+$ sign if the corresponding voltage source $V_i$ is oriented in the same direction with $V_{eff}$ and with $-$ sign if $V_i$ is oriented in opposite direction with $V_{eff}$. Since the voltage sources are all connected in series, when we replace $V_i$ with $V_{eff}$, we need to replace the other voltage sources with short-circuits (wires).
For instance, considering the circuit in Fig. 1, voltage sources $V_1$ and $V_2$ are connected in series. Therefore, we can keep one the voltage sources, say $V_1$, replace its value with $V_{eff}=V_1-V_2$, and replace voltage source $V_2$ with a wire.
Parallel
Voltage sources should never be combined in parallel.
See also
Resistor combinations
Capacitor combinations
Inductor combinations
Current source combinations
Series and parallel connections
Current Source Combinations
Series
Current sources should never be combined in series.
Parallel
If two or more current sources $I_1$, $I_2$, ... $I_n$ are connected in parallel they can be replaced with a single current source with $$I_{eff}=\pm I_1 \pm I_2\pm...\pm I_n$$ where the terms in the right hand side are taken with $+$ sign if the corresponding current source $I_i$ is oriented in the same direction with $I_{eff}$ and with $-$ sign if $I_i$ is oriented in opposite direction with $I_{eff}$. Since all the current sources are connecte in parallel, when we replace $I_i$ with $I_{eff}$, we need to remove the other current sources.
For instance, considering the circuit in Fig. 2, current sources $I_1$, $I_2$, and $I_3$ are connected in parallel. Therefore, we can keep one the current sources, say $I_1$, replace its value with $I_{eff}=I_1-I_2+I_3$, and remove current sources $I_2$ and $I_3$ from the circuit.
See also
Resistor combinations
Capacitor combinations
Inductor combinations
Voltage source combinations
Series and parallel connections
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Combining voltage sources (analytical)
Circuit with 2 voltage sources, V0 (analytical)
Circuit with 3 voltage sources, V0 (analytical)
Circuit with 4 voltage sources, V0 (analytical)
Circuit with 5 voltage sources, V0 (analytical)
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Combining voltage sources (numerical)
Circuit with 2 voltage sources (numerical)
Circuit with 3 voltage sources (numerical)
Circuit with 4 voltage sources (numerical)
Circuit with 5 voltage sources (numerical)
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Combining current sources (analytical)
Circuit with 2 current sources, I0 (analytical)
Circuit with 3 current sources, I0 (analytical)
Circuit with 4 current sources, I0 (analytical)
Circuit with 5 current sources, I0 (analytical)
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Combining current sources (numerical)
Circuit with 2 current sources (numerical)
Circuit with 3 current sources (numerical)
Circuit with 4 current sources (numerical)
Circuit with 5 current sources (numerical)