Linear Circuit Analysis
1. Introduction
2. Basic Concepts
- Charge, current, and voltage
- Power and energy
- Linear circuits
- Linear components
- Nodes and loops
- Series and parallel
- R, L & C combinations
- V & I combinations
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 (DC)
5. Additional Analysis Techniques (DC)
- Superposition
- Source transformation
- The $V_{test}/I_{test}$ method
- Norton equivalent
- Thévenin equivalent
- Max power transfer
- DC analysis of L & C
6. AC Analysis
7. Magnetically Coupled Circuits
8. Polyphase Systems
9. Operational Amplifiers
10. Laplace Transforms
11. Time-Dependent Circuits
- Introduction
- Inductors and capacitors
- First-order transients
- Second-order transients
-
Parallel RLC circuits
Series RLC circuits - Nodal analysis
- Mesh analysis
- Laplace transforms
- Additional techniques
12. Two-Port Networks
Appendix
The Inverse Laplace Transform
The inverse Laplace transform is defined as $$\begin{equation}ℒ^{-1}\left[F(s)\right]=\frac{1}{2\pi j}\int_{\sigma_1-j\infty}^{\sigma_1+j\infty}F(s)e^{st} ds\end{equation}$$
Although it is possible to apply the above formula to compute the $ℒ^{-1}\left[F(s)\right]$, in electric circuits we usually compute the inverse Laplace transform using the method of partial fraction decomposition.
Properties of Inverse Laplace Transform
| $F(s)$ | $f(t)=ℒ^{-1}\left[F(s)\right]$ | |
|---|---|---|
| Addition/subtraction | $F_1(\class{mjblue}{s}) \pm F_2(s)$ | $f_1(t) \pm f_2(t)$ |
| Linearity | $C_1 F_1(\class{mjblue}{s}) \pm C_2 F_2(\class{mjblue}{s})$ | $C_1 f_1(t) \pm C_2 f_2(t)$ |
| Frequency scaling | $F(c \class{mjblue}{s})$ | $\dfrac{1}{c} f\left(\dfrac{t}{c}\right)$ |
| Frequency shifting | $F(\class{mjblue}{s}-a)$ | $e^{a t} f(t)$ |
| Time shifting | $e^{-a@s}F(s)$ | $f(t-a)u(t-a)$ |
| Division by $s$ | $\dfrac{F(\class{mjblue}{s})}{\class{mjblue}{s}}$ | $\int_{0}^{t} f(x) \,dx$ |
Partial Fractions Decomposition
A partial fraction is a fraction in which the numerator is a constant (real or complex) and the denominator is a linear polynomial raised to a positive power. Partial fractions have the form $$\frac{A}{(\class{mjblue}{s}+a)^n}$$ where $A$ and $a$ are real or complex numbers and $n$ is a positive integer.
Any proper rational function (where the degree of the numerator is less than the degree of the denominator) can be expressed as a sum of partial fractions using the method of partial fraction decomposition.
Inverse Laplace transforms of partial fractions
| $F(\class{mjblue}{s})$ | $f(t)=ℒ^{-1}\left[F(\class{mjblue}{s})\right]$ |
|---|---|
| $\dfrac{1}{\class{mjblue}{s}}$ | $1$ |
| $\dfrac{1}{\class{mjblue}{s}+a}$ | $e^{-at}$ |
| $\dfrac{1}{\class{mjblue}{s}^{n}}$ | $\dfrac{t^{n-1}}{(n-1)!}$ |
| $\dfrac{1}{(\class{mjblue}{s}+a)^{n}}$ | $\dfrac{t^{n-1} e^{-at}}{(n-1)!}$ |
Examples of Solved Problems
-
Inverse Laplace transforms
Inverse Laplace transform of K/(R1*R1)
Inverse Laplace transform of R1/(R1*R1
Inverse Laplace transform of R1/R2
Inverse Laplace transform of Exp/(R1*R1)
Inverse Laplace transform of R1/C2
Inverse Laplace transform of R1/R1^2
Inverse Laplace transform of R1/R1^3
Inverse Laplace transform of R2/R1^3
Inverse Laplace transform of R1/(R1*R2)
Inverse Laplace transform of R1/(R1*C2)
Inverse Laplace transform of Exp*R1/(R1*R1)
Inverse Laplace transform of Exp*R1/R2
Inverse Laplace transform of Exp*R1/C2
Inverse Laplace transform of Exp*R1/R1^2
Inverse Laplace transform of Exp*R1/R1^3
Inverse Laplace transform of Exp*R2/R1^3
Inverse Laplace transform of Exp*R1/(R1*R2)
Inverse Laplace transform of Exp*R1/(R1*C2)
See also
Read more
Inverse Laplace transform
Euler's formula
Pierre-Simon Laplace
Leonhard Euler