Difference between revisions of "ECE 110/Concept List/S25"
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** Number of independent KVL equations = meshes | ** Number of independent KVL equations = meshes | ||
* Example of how to find $$i$$, $$v$$, and $$p_{\mathrm{abs}}$$ using conservation equations and how to check using extra conservation equations | * Example of how to find $$i$$, $$v$$, and $$p_{\mathrm{abs}}$$ using conservation equations and how to check using extra conservation equations | ||
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== Lecture 3 - 1/15 - Sources and Resistors == | == Lecture 3 - 1/15 - Sources and Resistors == | ||
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** Write KCL at nodes not touching a voltage source; if there are voltage sources, look at nodes on either side or source to make a supernode | ** Write KCL at nodes not touching a voltage source; if there are voltage sources, look at nodes on either side or source to make a supernode | ||
− | + | == Lecture 7 - 2/3 - Current Methods == | |
− | |||
− | |||
− | |||
− | == Lecture 7 - 2/ | ||
* Examples on Canvas | * Examples on Canvas | ||
* BCM | * BCM | ||
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*** Label each mesh current, understanding that current sources, current measurements, and voltage measurements will require additional equations. | *** Label each mesh current, understanding that current sources, current measurements, and voltage measurements will require additional equations. | ||
− | == Lecture 8 - 2/ | + | == Lecture 8 - 2/5 - Computational Methods == |
+ | * Using Maple to set up and solve simultaneous equations | ||
+ | |||
+ | == Lecture 9 - 2/10 - Linearity and Superposition == | ||
* Definition of a linear system | * Definition of a linear system | ||
* Examples of nonlinear systems and linear systems | * Examples of nonlinear systems and linear systems | ||
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** If there are dependent sources, you must keep them activated and solve for measurements each time - this likely means that superposition may not actually make solving things easier. | ** If there are dependent sources, you must keep them activated and solve for measurements each time - this likely means that superposition may not actually make solving things easier. | ||
− | == Lecture | + | == Lecture 10 - 2/12 - Thévenin and Norton Equivalent Circuits == |
* Thévenin and Norton Equivalents | * 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 | * Circuits with independent sources, dependent sources, and resistances can be reduced to a single source and resistance from the perspective of any two nodes | ||
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** If there are both independent sources and dependent sources, solve for $$v_{oc}=v_T$$ first, then put a short circuit between the terminals and solve for $$i_{sc}=i_N$$. 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 short 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. | ** If there are '''only''' dependent sources, you have to activate the circuit with an external source. | ||
+ | * Side note: MCM by inspection | ||
+ | |||
+ | == Lecture 11 - 2/17 - Operational Amplifiers == | ||
+ | * Model using two resistors and a VCVS | ||
+ | * Without feedback, only really good as a comparator | ||
+ | * Feedback from output to inverting input makes circuit more useful | ||
+ | * Ideal op-amp assumptions are about the op-amp, not the circuit: $$A\rightarrow\infty$$, $$r_i\rightarrow\infty$$, $$r_o\rightarrow 0$$ | ||
+ | * Using ideal op-amp with a circuit with feedback from output to inverting input leads to a very useful circuit with implications of: | ||
+ | ** No voltage drop between the input terminals | ||
+ | ** No current entering the input terminals | ||
+ | ** Still possible to have current at the output terminal! | ||
+ | |||
+ | == Lecture 12 - 2/19 - More Op-Amp Circuits == | ||
+ | * Various configurations that are directly or nearly-directly from the circuit developed in Lecture 11: | ||
+ | ** Inverting | ||
+ | ** Non-inverting | ||
+ | *** Buffer / Voltage follower as a specific instance | ||
+ | ** Inverting summation | ||
+ | *** Mixing board | ||
+ | ** Difference | ||
+ | * Creating a circuit to produce a proscribed linear combination of input voltages | ||
+ | * Analyzing op-amp circuits that are not directly based on circuit developed in Lecture 11 | ||
+ | |||
+ | == Lecture 13 - 2/24 - Test 1 == | ||
− | == Lecture | + | == Lecture 14 - 2/26 - Capacitors and Inductors == |
* Intro to capacitors and inductors | * Intro to capacitors and inductors | ||
* Basic physical models | * Basic physical models | ||
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* DCSS equivalents | * DCSS equivalents | ||
− | == Lecture | + | == Lecture 15 - 3/3 - Initial Conditions and Finding Equations == |
* DCSS equivalents | * DCSS equivalents | ||
* Finding values just before and just after circuit changes | * Finding values just before and just after circuit changes | ||
** For $$t=0^+$$, can model inductor as independent current source and capacitor as independent voltage source | ** For $$t=0^+$$, can model inductor as independent current source and capacitor as independent voltage source | ||
− | * | + | * First-order switched circuits with constant forcing functions |
+ | * Sketching basic exponential decays | ||
− | == Lecture | + | == Lecture 16 - 3/5 - First-Order Circuits == |
− | + | * Using methods (NVM, MCM, BCM) to get model equations | |
+ | * Setting up and solving with Maple | ||
− | == Lecture | + | == Lecture 17 - 3/17 - Sinusoids and Complex Numbers == |
− | * | + | * Solving even a simple differential equation with a sinusoidal input is somewhat complicated |
− | + | * At the heart of complex analysis is an understanding of [[Complex Numbers]] | |
− | * | ||
+ | <!-- | ||
== Lecture 14 - 2/27 - ACSS and Phasors == | == Lecture 14 - 2/27 - ACSS and Phasors == | ||
* Overview of [[Calculator Tips]] | * Overview of [[Calculator Tips]] | ||
− | + | ||
* Solving ACSS using just trig gets complex very quickly - we will use complex analysis to simplify the process - this is a motivation for phasors | * Solving ACSS using just trig gets complex very quickly - we will use complex analysis to simplify the process - this is a motivation for phasors | ||
* A phasor is a complex number whose magnitude represents the amplitude of a single-frequency sinusoid and whose angle represents the phase of a single-frequency sinusoid | * A phasor is a complex number whose magnitude represents the amplitude of a single-frequency sinusoid and whose angle represents the phase of a single-frequency sinusoid | ||
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* General second-order equation | * General second-order equation | ||
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== Lecture 23 - 4/4 - Analyzing Circuits with Op-Amps == | == Lecture 23 - 4/4 - Analyzing Circuits with Op-Amps == |
Latest revision as of 21:43, 17 March 2025
Contents
- 1 Lecture 1 - 1/8 - Course Introduction, Nomenclature
- 2 Lecture 2 - 1/13 - Electrical Quantities
- 3 Lecture 3 - 1/15 - Sources and Resistors
- 4 Lecture 4 - 1/22 - Equivalent Circuits
- 5 Lecture 5 - 1/27 - Division
- 6 Lecture 6 - 1/29 - Node Voltage Method
- 7 Lecture 7 - 2/3 - Current Methods
- 8 Lecture 8 - 2/5 - Computational Methods
- 9 Lecture 9 - 2/10 - Linearity and Superposition
- 10 Lecture 10 - 2/12 - Thévenin and Norton Equivalent Circuits
- 11 Lecture 11 - 2/17 - Operational Amplifiers
- 12 Lecture 12 - 2/19 - More Op-Amp Circuits
- 13 Lecture 13 - 2/24 - Test 1
- 14 Lecture 14 - 2/26 - Capacitors and Inductors
- 15 Lecture 15 - 3/3 - Initial Conditions and Finding Equations
- 16 Lecture 16 - 3/5 - First-Order Circuits
- 17 Lecture 17 - 3/17 - Sinusoids and Complex Numbers
Lecture 1 - 1/8 - Course Introduction, Nomenclature
- Circuit terms (Element, Circuit, Path, Branch and Essential Branch, Node and Essential Node, Loop and Mesh).
- Accounting:
- # of Elements * 2 = total number of voltages and currents that need to be found using brute force method
- # of Essential Branches = number of possibly-different currents that can be measured
- # of Meshes = number of independent currents in the circuit (or generally Elements - Nodes + 1 for planar and non-planar circuits)
- # of Nodes - 1 = number of independent voltage drops in the circuit
Lecture 2 - 1/13 - Electrical Quantities
- Electrical quantities (charge, current, voltage, power)
- Passive Sign Convention and Active Sign Convention and relation to calculating power absorbed and/or power delivered.
- Power conservation
- Kirchhoff's Laws
- Number of independent KCL equations = nodes-1
- Number of independent KVL equations = meshes
- Example of how to find $$i$$, $$v$$, and $$p_{\mathrm{abs}}$$ using conservation equations and how to check using extra conservation equations
Lecture 3 - 1/15 - Sources and Resistors
- $$i$$-$$v$$ relationships of various elements (ideal independent voltage source, ideal independent current source, short circuit, open circuit, switch)
- Resistor symbol (and spring symbol)
- Resistance as $$R=\frac{\rho L}{A}$$
- $$i$$-$$v$$ relationship for resistors; resistance [$$\Omega$$] and conductance $$G=1/R$$ $$[S]$$
- $$i$$-$$v$$ for dependent (controlled) sources (VCVS, VCCS, CCVS, CCCS)
Lecture 4 - 1/22 - Equivalent Circuits
- Combining voltage sources in series; ability to move series items and put together
- Combining current sources in parallel; ability to move parallel items and put together
- Equivalent resistances
- series and parallel
- Examples/Req
- Delta-Wye equivalencies (mainly refer to book)
Lecture 5 - 1/27 - Division
- Voltage Division and Re-division
- Current Division and Re-Division
Lecture 6 - 1/29 - Node Voltage Method
- Basics of NVM
- NVM
- Labels:
- Really Lazy: label ground, then make every other node a new unknown. Voltage sources, voltage measurements, and current measurements will provide additional equations.
- Lazy: label ground, then label any node connected to ground if it has a voltage source or voltage measurement. Make every other node a new unknown. Voltage sources not connected to ground, voltage measurements not connected to ground, and current measurements will provide additional equations.
- Smart: label ground; once a node gets labeled, if there is a voltage source or a voltage measurement anchored at that node, use the source or measurement to label the other node it is attached to. Current measurements will provide additional equations.
- Really Smart: same as smart, only also use voltage drops across resistors with current measurements to relate node voltages.
- #KCL = #nodes - 1 - #v. sources
- Write KCL at nodes not touching a voltage source; if there are voltage sources, look at nodes on either side or source to make a supernode
- Labels:
Lecture 7 - 2/3 - Current Methods
- Examples on Canvas
- BCM
- Labels:
- Label each (essential) branch current, using as few unknowns as possible by incorporating current source and current measurement labels
- Labels:
- MCM
- Labels:
- Label each mesh current, understanding that current sources, current measurements, and voltage measurements will require additional equations.
- Labels:
Lecture 8 - 2/5 - Computational Methods
- Using Maple to set up and solve simultaneous equations
Lecture 9 - 2/10 - 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
- Use combinations of Phm's Law, Voltaeg Division, and Current Division, rather than setting up and solving multiple equations
- If there are dependent sources, you must keep them activated and solve for measurements each time - this likely means that superposition may not actually make solving things easier.
Lecture 10 - 2/12 - 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 short 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.
- Side note: MCM by inspection
Lecture 11 - 2/17 - Operational Amplifiers
- Model using two resistors and a VCVS
- Without feedback, only really good as a comparator
- Feedback from output to inverting input makes circuit more useful
- Ideal op-amp assumptions are about the op-amp, not the circuit: $$A\rightarrow\infty$$, $$r_i\rightarrow\infty$$, $$r_o\rightarrow 0$$
- Using ideal op-amp with a circuit with feedback from output to inverting input leads to a very useful circuit with implications of:
- No voltage drop between the input terminals
- No current entering the input terminals
- Still possible to have current at the output terminal!
Lecture 12 - 2/19 - More Op-Amp Circuits
- Various configurations that are directly or nearly-directly from the circuit developed in Lecture 11:
- Inverting
- Non-inverting
- Buffer / Voltage follower as a specific instance
- Inverting summation
- Mixing board
- Difference
- Creating a circuit to produce a proscribed linear combination of input voltages
- Analyzing op-amp circuits that are not directly based on circuit developed in Lecture 11
Lecture 13 - 2/24 - Test 1
Lecture 14 - 2/26 - Capacitors and Inductors
- Intro to capacitors and inductors
- Basic physical models
- Basic electrical models
- Energy storage
- Continuity requirements
- Finding circuit equation models
- DCSS equivalents
Lecture 15 - 3/3 - Initial Conditions and Finding Equations
- DCSS equivalents
- Finding values just before and just after circuit changes
- For $$t=0^+$$, can model inductor as independent current source and capacitor as independent voltage source
- First-order switched circuits with constant forcing functions
- Sketching basic exponential decays
Lecture 16 - 3/5 - First-Order Circuits
- Using methods (NVM, MCM, BCM) to get model equations
- Setting up and solving with Maple
Lecture 17 - 3/17 - Sinusoids and Complex Numbers
- Solving even a simple differential equation with a sinusoidal input is somewhat complicated
- At the heart of complex analysis is an understanding of Complex Numbers