Difference between revisions of "EGR 224/Concept List/S22"
Jump to navigation
Jump to search
(Created page with "The notes below are not meant to be comprehensive but rather to capture the general topics of any particular class. These note are in no way a replacement for actively attend...") |
|||
Line 1: | Line 1: | ||
− | The notes below are not meant to be comprehensive but rather to capture the general topics of | + | The notes below are not meant to be comprehensive but rather to capture the general topics of covered during lectures in [[EGR 224/Spring 2022|EGR 224 for Spring 2022]]. These note are in no way a replacement for actively attending class. |
== Lecture 1 - 1/5 - No Class == | == Lecture 1 - 1/5 - No Class == |
Revision as of 03:57, 12 February 2022
The notes below are not meant to be comprehensive but rather to capture the general topics of covered during lectures in EGR 224 for Spring 2022. These note are in no way a replacement for actively attending class.
Contents
- 1 Lecture 1 - 1/5 - No Class
- 2 Lecture 2 - 1/7 - Course Introduction, Nomenclature
- 3 Lecture 3 - 1/10- Voltage and Current; Power and Energy
- 4 Lecture 4 - 1/14 - Equivalents
- 5 Lecture 5 - 1/21 - Voltage Division and Current Division
- 6 Lecture 6 - 1/24 - Node Voltage Method
- 7 Lecture 7 - 1/28 - Mesh and Branch Current Method
- 8 Lecture 8 - 1/31 - Linearity and Superposition
- 9 Lecture 9 - 2/4 - Thévenin and Norton Equivalent Circuits
- 10 Lecture 10 - 2/7 - Capacitors and Inductors
- 11 Lecture 11 - 2/11 - First-Order Circuits (constant forcing functions)
Lecture 1 - 1/5 - No Class
Lecture 2 - 1/7 - Course Introduction, Nomenclature
- Circuit terms (Element, Circuit, Path, Branch and Essential Branch, Node and Essential Node, Loop and Mesh).
- Circuit topology (parallel, series)
- Electrical quantities (charge, current, voltage, power)
Lecture 3 - 1/10- Voltage and Current; Power and Energy
- Power redux
- Passive Sign Convention and Active Sign Convention and relation to calculating power absorbed and/or power delivered.
- Example of how to find $$i$$, $$v$$, and $$p_{\mathrm{abs}}$$
- $$i$$-$$v$$ characteristics of various elements (ideal independent voltage source, ideal independent current source, short circuit, open circuit, switch, resistor)
- Kirchhoff's Laws
Lecture 4 - 1/14 - Equivalents
- Combining voltage sources in series; ability to move series items
- Combining current sources in parallel; ability to move parallel items
- Equivalent resistances
- series, parallel, and other (Delta-Wye)
- Examples/Req
Lecture 5 - 1/21 - Voltage Division and Current Division
- Voltage division (actually covered during Lab 2)
- Current Division
- Beginning of Node Voltage Method and label techniques
Lecture 6 - 1/24 - Node Voltage Method
- More NVM
- Start of Mesh Current Method
Lecture 7 - 1/28 - Mesh and Branch Current Method
- More MCM
- Branch Current Method
Lecture 8 - 1/31 - Linearity and Superposition
- Definition of a linear system
- Examples of nonlinear systems and linear systems
- Nonlinear system examples (additive constants, powers other than 1, trig):
- $$\begin{align*} y(t)&=x(t)+1\\ y(t)&=(x(t))^n, n\neq 1\\ y(t)&=\cos(x(t)) \end{align*} $$
- Linear system examples (multiplicative constants, derivatives, integrals):
- $$\begin{align*} y(t)&=ax(t)\\ y(t)&=\frac{d^nx(t)}{dt^n}\\ y(t)&=\int x(\tau)~d\tau \end{align*} $$
- Superposition
- Redraw the circuit as many times as needed to focus on each independent source individually
- If there are dependent sources, you must keep them activated and solve for measurements each time
Lecture 9 - 2/4 - Thévenin and Norton Equivalent Circuits
- Thévenin and Norton Equivalents
- Circuits with independent sources, dependent sources, and resistances can be reduced to a single source and resistance from the perspective of any two nodes
- Equivalents are electrically indistinguishable from one another
- Several ways to solve:
- If there are only independent sources, turn independent sources off and find $$R_{eq}$$ between terminals of interest to get $$R_{T}$$. Then find $$v_{oc}=v_{T}$$ and recall that $$v_T=R_Ti_N$$
- If there are both independent sources and dependent sources, solve for $$v_{oc}=v_T$$ first, then put a shirt circuit between the terminals and solve for $$i_{sc}=i_N$$. Recall that $$v_T=R_Ti_N$$
- If there are only dependent sources, you have to activate the circuit with an external source.
Lecture 10 - 2/7 - Capacitors and Inductors
- Intro to capacitors and inductors
- Basic physical models
- Basic electrical models
- Energy storage
- Continuity requirements
- DCSS equivalents
Lecture 11 - 2/11 - First-Order Circuits (constant forcing functions)
- First-order switched circuits with constant forcing functions
- Sketching basic exponential decays
- Using Node Voltage Method to get model equation