Exercise 3 (Resistive Network Analysis)
|
|
- Meghan Riley
- 7 years ago
- Views:
Transcription
1 Circuit Analysis Exercise 0/0/08 Problem. (Hambley.49) Exercise (Resistive Network Analysis) Problem. (Hambley.5)
2 Circuit Analysis Exercise 0/0/08 Problem. (Hambley.59) Problem 4. (Hambley.68)
3 Circuit Analysis Exercise 0/0/08 Problem 5. (Hambley.75)
4 Circuit Analysis Exercise 0/0/08 Problem 6. (Hambley.8) 4
5 Circuit Analysis Exercise 0/0/08 Problem 7. (Hambley.84) Problem 8. (Hambley.88) 5
6 Circuit Analysis Exercise 0/0/08 Problem 9. (Hambley.94) 6
7 Circuit Analysis Exercise 0/0/08 Problem 0. (Rizzoni.0) Using node voltage analysis in the circuit of Figure, find the three indicated node voltages. Let I 0.A; R 00 ; R 75 ; R 5 ; R 50 ; R 00 ; Known quantities: Figure The current source value, the voltage source value and the resistance values for the circuit shown in Figure P.0. The three node voltages indicated in Figure P.0 using node voltage analysis. At node : v 00 v v A At node : v v 75 v 5 v v 50 At node : v v v i i 0 For the voltage source we have: v 0 v olving the system, we obtain: v 4.4, v 4.58, v 5.4 and, finally, i 54 ma. Problem. (Rizzoni.0) For the circuit of Figure P.0, use mesh current analysis to find the matrices required to solve the circuit, and solve for the unknown currents. Hint:You may find source transformations useful. 7
8 Circuit Analysis Exercise 0/0/08 Circuit shown in Figure P.0. Mesh equation in matrix form and solve for currents. after source transformation, we can have the equivalent circuit shown in the right hand side. We can write down the following matrix I, 0 I 4 I4 5 olve the equation, we can have I, A.66 I I A I A I A Problem. (Rizzoni.0) Using mesh current analysis, find the current i in the circuit of FigureP.0. 8
9 Circuit Analysis Exercise 0/0/08 Known quantities: The values of the resistors in the circuit of Figure P.0. The current in the circuit of Figure P.0 using mesh current analysis. ince I is unknown, the problem will be solved in terms of this current. For mesh #, it is obvious that: i I For mesh #: For mesh #: olving, i 0.645I i 0.48I i i 5 i 5 0 i 4 i 5 i Then, i i i and i0.48i0.645i0.6i Problem. (Rizzoni.56) Find the Thevenin equivalet resistance seen by the load resistor R L in the circuit of Figure P.56. Problem.56 Known quantities: Circuit shown in Figure P.56. 9
10 Circuit Analysis Exercise 0/0/08 Thevenin equivalent circuit To find R T, we need to make the current source an open circuit and voltage sources short circuits, as follows: Note that this circuit has only three nodes. Thus, we can re-draw circuit as shown: and combine the two parallel resistors to obtain: the the Thus, R T 50 (50.) 00.8 Problem 4. (Rizzoni.58) Find the Thevenin equivalent of the circuit connected to R L in the Figure, where R 0 ; R 0 ; R 0., and R ; g p Figure Known quantities: Circuit shown in Figure P.58. Thevenin equivalent circuit To find RT, we short circuit the source tarting from the left side, ( 0.) 00.99, ( ) 0.89 Therefore, we have R T Ω.. 0
11 Circuit Analysis Exercise 0/0/08 To find, we apply mesh analysis: v oc Two resistors are omitted because no current flows through them and they, therefore, do not affect voc i -0i i -0i 0 = + olving for i, i 06. A we obtain, vt voc 0i 4. Problem 5. (Rizzoni.59) The Wheatstone bridge circuit shown in Figure is used in a number of practical applications. One traditional use is in determining the value of an unknown resistor R x. Find the value of the voltage ab = a - b in terms of R, R x, and s. If R k, s and ab =m, what is the value of R x? Figure Known quantities: Circuit shown in Figure P.59. alue of resistance R x R R+R R R+Rx a) We have x ab a-b - ab = R - x R + R x b) For kw R, s, ab m, R x R x 996 Ω 000 +R x
12 Circuit Analysis Exercise 0/0/08 Problem 6. (Rizzoni.4) With reference to Figure 4, using superposition, determine the component of the current through R that is due to s. 450 ; R 7; R 5; R 0 R 4 R 5 Figure 4 Known quantities: The values of the voltage sources and of the resistors in the circuit of Figure P.4: 450 R 7 R 5 R 0 R 4 R 5 The component of the current through R that is due to, using superposition. uppress by replacing it with a short circuit. Redraw the circuit. A solution using equivalent resistances looks reasonable. R and R 4 are in parallel: R 4 R R 4 7 R R R4is in series with R : R 4 R 4 R R eq R 5 R R 4 R 5 R R 4 5 R R OL: CD: I R eq A 5 I R I R R R A
13 Circuit Analysis Exercise 0/0/08 Problem 7. (Rizzoni.) In the circuit the Figure 5, assume the source voltage and source current and all resistances are known. a. Write the node equations required to determine the node voltages. b. Write the matrix solution for each node voltage in terms of the known parameters. Known quantities: Circuit of Figure P. with voltage source, Figure 5, current source, I, and all resistances. a. The node equations required to determine the node voltages. b. The matrix solution for each node voltage in terms of the known parameters. a) pecify the nodes (e.g., A on the upper left corner of the circuit in Figure P.0, and B on the right corner). Choose one node as the reference or ground node. If possible, ground one of the sources in the circuit. Note that this is possible here. When using KCL, assume all unknown current flow out of the node. The direction of the current supplied by the current source is specified and must flow into node A. KCL: I a R a R R a b R 0 b I R R KCL: b a R a R b R b 0 R 4 0 b R R R 4 R b) Matrix solution:
14 Circuit Analysis Exercise 0/0/08 a I R R R R R R 4 R R R R R R R 4 I R R R R 4 R R R R R R R 4 R R b R R I R R R R R R R R R R 4 R R R R I R R R R R R 4 R R Notes:. The denominators are the same for both solutions.. The main diagonal of a matrix is the one that goes to the right and down.. The denominator matrix is the "conductance" matrix and has certain properties: a) The elements on the main diagonal [i(row) = j(column)] include all the conductance connected to node i=j. b) The off-diagonal elements are all negative. c) The off-diagonal elements are all symmetric, i.e., the i j-th element = j i-th element. This is true only because there are no controlled (dependent) sources in this circuit. d) The off-diagonal elements include all the conductance connected between node i [row] and node j [column]. Problem 8. (Rizzoni.4) Using KCL, perform node analysis on the circuit shown in Figure 6, and determine the voltage across R 4. Note that one source is a controlled voltage source! Let 5 ; A 70; R.k; R.8k; R 6.8k; 0 R4 Figure 6 4
15 Circuit Analysis Exercise 0/0/08 Known quantities: Circuit shown in Figure P.4 5 A 70 R. k R.8 k R 6.8 k R 4 0 The voltage across R 4 using KCL and node voltage analysis. Node analysis is not a method of choice because the dependent source is [] a voltage source and [] a floating source. Both factors cause difficulties in a node analysis. A ground is specified. There are three unknown node voltages, one of which is the voltage across R 4. The dependent source will introduce two additional unknowns, the current through the source and the controlling voltage (across R ) that is not a node voltage. Therefore 5 equations are required: KCL 0 KCL IC 0 R R R R KCL I C 04KL R 0R R R4 5KL A 0 A A R R ubstitute using Equation [5] into Equations [], [] and [] and eliminate (because it only appears twice in these equations). Collect terms: A R R R R R R I C 0 A R R A I C A R R R R I C 0 R R R 4 R R R R R R A 70 R R A R R R R A (5)70 R mA A 5 R.0 (5) mA olving, we have: Notes: R R4 5. m. This solution was not difficult in terms of theory, but was terribly long and arithmetically cumbersome. This was because the wrong method was used. There are only mesh currents in the circuit; the sources were voltage sources; therefore, a mesh analysis is the method of choice. 5
16 Circuit Analysis Exercise 0/0/08. In general, a node analysis will have fewer unknowns (because one node is the ground or reference node) and will, in such cases, be preferable. 6
Circuit Analysis using the Node and Mesh Methods
Circuit Analysis using the Node and Mesh Methods We have seen that using Kirchhoff s laws and Ohm s law we can analyze any circuit to determine the operating conditions (the currents and voltages). The
More informationExample: Determine the power supplied by each of the sources, independent and dependent, in this circuit:
Example: Determine the power supplied by each of the sources, independent and dependent, in this circuit: Solution: We ll begin by choosing the bottom node to be the reference node. Next we ll label the
More informationThevenin Equivalent Circuits
hevenin Equivalent Circuits Introduction In each of these problems, we are shown a circuit and its hevenin or Norton equivalent circuit. he hevenin and Norton equivalent circuits are described using three
More informationHow To Find The Current Of A Circuit
The node voltage method Equivalent resistance Voltage / current dividers Source transformations Node voltages Mesh currents Superposition Not every circuit lends itself to short-cut methods. Sometimes
More informationSeries-Parallel Circuits. Objectives
Series-Parallel Circuits Objectives Identify series-parallel configuration Analyze series-parallel circuits Apply KVL and KCL to the series-parallel circuits Analyze loaded voltage dividers Determine the
More informationPreamble. Kirchoff Voltage Law (KVL) Series Resistors. In this section of my lectures we will be. resistor arrangements; series and
Preamble Series and Parallel Circuits Physics, 8th Edition Custom Edition Cutnell & Johnson Chapter 0.6-0.8, 0.0 Pages 60-68, 69-6 n this section of my lectures we will be developing the two common types
More informationKirchhoff's Current Law (KCL)
Kirchhoff's Current Law (KCL) I. Charge (current flow) conservation law (the Kirchhoff s Current law) Pipe Pipe Pipe 3 Total volume of water per second flowing through pipe = total volume of water per
More informationBasic Laws Circuit Theorems Methods of Network Analysis Non-Linear Devices and Simulation Models
EE Modul 1: Electric Circuits Theory Basic Laws Circuit Theorems Methods of Network Analysis Non-Linear Devices and Simulation Models EE Modul 1: Electric Circuits Theory Current, Voltage, Impedance Ohm
More informationTristan s Guide to: Solving Parallel Circuits. Version: 1.0 Written in 2006. Written By: Tristan Miller Tristan@CatherineNorth.com
Tristan s Guide to: Solving Parallel Circuits. Version: 1.0 Written in 2006 Written By: Tristan Miller Tristan@CatherineNorth.com Parallel Circuits. Parallel Circuits are a little bit more complicated
More informationLecture 7 Circuit analysis via Laplace transform
S. Boyd EE12 Lecture 7 Circuit analysis via Laplace transform analysis of general LRC circuits impedance and admittance descriptions natural and forced response circuit analysis with impedances natural
More informationCHAPTER 28 ELECTRIC CIRCUITS
CHAPTER 8 ELECTRIC CIRCUITS 1. Sketch a circuit diagram for a circuit that includes a resistor R 1 connected to the positive terminal of a battery, a pair of parallel resistors R and R connected to the
More informationLecture 2 Linear functions and examples
EE263 Autumn 2007-08 Stephen Boyd Lecture 2 Linear functions and examples linear equations and functions engineering examples interpretations 2 1 Linear equations consider system of linear equations y
More informationMATRIX ALGEBRA AND SYSTEMS OF EQUATIONS. + + x 2. x n. a 11 a 12 a 1n b 1 a 21 a 22 a 2n b 2 a 31 a 32 a 3n b 3. a m1 a m2 a mn b m
MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS 1. SYSTEMS OF EQUATIONS AND MATRICES 1.1. Representation of a linear system. The general system of m equations in n unknowns can be written a 11 x 1 + a 12 x 2 +
More informationMesh-Current Method (Loop Analysis)
Mesh-Current Method (Loop Analysis) Nodal analysis was developed by applying KCL at each non-reference node. Mesh-Current method is developed by applying KVL around meshes in the circuit. A mesh is a loop
More informationDependent Sources: Introduction and analysis of circuits containing dependent sources.
Dependent Sources: Introduction and analysis of circuits containing dependent sources. So far we have explored timeindependent (resistive) elements that are also linear. We have seen that two terminal
More information13.10: How Series and Parallel Circuits Differ pg. 571
13.10: How Series and Parallel Circuits Differ pg. 571 Key Concepts: 5. Connecting loads in series and parallel affects the current, potential difference, and total resistance. - Using your knowledge of
More information12.4 UNDRIVEN, PARALLEL RLC CIRCUIT*
+ v C C R L - v i L FIGURE 12.24 The parallel second-order RLC circuit shown in Figure 2.14a. 12.4 UNDRIVEN, PARALLEL RLC CIRCUIT* We will now analyze the undriven parallel RLC circuit shown in Figure
More information2.1 Introduction. 2.2 Terms and definitions
.1 Introduction An important step in the procedure for solving any circuit problem consists first in selecting a number of independent branch currents as (known as loop currents or mesh currents) variables,
More informationCircuits. The light bulbs in the circuits below are identical. Which configuration produces more light? (a) circuit I (b) circuit II (c) both the same
Circuits The light bulbs in the circuits below are identical. Which configuration produces more light? (a) circuit I (b) circuit II (c) both the same Circuit II has ½ current of each branch of circuit
More informationLecture Notes: ECS 203 Basic Electrical Engineering Semester 1/2010. Dr.Prapun Suksompong 1 June 16, 2010
Sirindhorn International Institute of Technology Thammasat University School of Information, Computer and Communication Technology Lecture Notes: ECS 203 Basic Electrical Engineering Semester 1/2010 Dr.Prapun
More informationEquivalent Circuits and Transfer Functions
R eq isc Equialent Circuits and Transfer Functions Samantha R Summerson 14 September, 009 1 Equialent Circuits eq ± Figure 1: Théenin equialent circuit. i sc R eq oc Figure : Mayer-Norton equialent circuit.
More informationMATRIX ALGEBRA AND SYSTEMS OF EQUATIONS
MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS Systems of Equations and Matrices Representation of a linear system The general system of m equations in n unknowns can be written a x + a 2 x 2 + + a n x n b a
More informationChapter 6. Orthogonality
6.3 Orthogonal Matrices 1 Chapter 6. Orthogonality 6.3 Orthogonal Matrices Definition 6.4. An n n matrix A is orthogonal if A T A = I. Note. We will see that the columns of an orthogonal matrix must be
More informationW03 Analysis of DC Circuits. Yrd. Doç. Dr. Aytaç Gören
W03 Analysis of DC Circuits Yrd. Doç. Dr. Aytaç Gören ELK 2018 - Contents W01 Basic Concepts in Electronics W02 AC to DC Conversion W03 Analysis of DC Circuits (self and condenser) W04 Transistors and
More informationMatrix Differentiation
1 Introduction Matrix Differentiation ( and some other stuff ) Randal J. Barnes Department of Civil Engineering, University of Minnesota Minneapolis, Minnesota, USA Throughout this presentation I have
More informationa 11 x 1 + a 12 x 2 + + a 1n x n = b 1 a 21 x 1 + a 22 x 2 + + a 2n x n = b 2.
Chapter 1 LINEAR EQUATIONS 1.1 Introduction to linear equations A linear equation in n unknowns x 1, x,, x n is an equation of the form a 1 x 1 + a x + + a n x n = b, where a 1, a,..., a n, b are given
More informationEDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 67 - FURTHER ELECTRICAL PRINCIPLES NQF LEVEL 3 OUTCOME 1 TUTORIAL 1 - DIRECT CURRENT CIRCUIT THEOREMS
EDEXCE NATIONA CERTIFICATE/DIPOMA UNIT 67 - FURTHER EECTRICA PRINCIPES NQF EVE 3 OUTCOME 1 TUTORIA 1 - DIRECT CURRENT CIRCUIT THEOREMS Unit content 1 Be able to apply direct current (DC) circuit analysis
More informationChapter 5. Parallel Circuits ISU EE. C.Y. Lee
Chapter 5 Parallel Circuits Objectives Identify a parallel circuit Determine the voltage across each parallel branch Apply Kirchhoff s current law Determine total parallel resistance Apply Ohm s law in
More informationES250: Electrical Science. HW7: Energy Storage Elements
ES250: Electrical Science HW7: Energy Storage Elements Introduction This chapter introduces two more circuit elements, the capacitor and the inductor whose elements laws involve integration or differentiation;
More informationVer 3537 E1.1 Analysis of Circuits (2014) E1.1 Circuit Analysis. Problem Sheet 1 (Lectures 1 & 2)
Ver 3537 E. Analysis of Circuits () Key: [A]= easy... [E]=hard E. Circuit Analysis Problem Sheet (Lectures & ). [A] One of the following circuits is a series circuit and the other is a parallel circuit.
More informationAbstract: We describe the beautiful LU factorization of a square matrix (or how to write Gaussian elimination in terms of matrix multiplication).
MAT 2 (Badger, Spring 202) LU Factorization Selected Notes September 2, 202 Abstract: We describe the beautiful LU factorization of a square matrix (or how to write Gaussian elimination in terms of matrix
More informationCornerstone Electronics Technology and Robotics I Week 15 Combination Circuits (Series-Parallel Circuits)
Cornerstone Electronics Technology and Robotics I Week 15 Combination Circuits (Series-Parallel Circuits) Administration: o Prayer o Turn in quiz Electricity and Electronics, Chapter 8, Introduction: o
More information= (0.400 A) (4.80 V) = 1.92 W = (0.400 A) (7.20 V) = 2.88 W
Physics 2220 Module 06 Homework 0. What are the magnitude and direction of the current in the 8 Ω resister in the figure? Assume the current is moving clockwise. Then use Kirchhoff's second rule: 3.00
More informationModule 2. DC Circuit. Version 2 EE IIT, Kharagpur
Module DC Circuit Lesson 4 Loop Analysis of resistive circuit in the context of dc voltages and currents Objectives Meaning of circuit analysis; distinguish between the terms mesh and loop. To provide
More informationFirst Order Circuits. EENG223 Circuit Theory I
First Order Circuits EENG223 Circuit Theory I First Order Circuits A first-order circuit can only contain one energy storage element (a capacitor or an inductor). The circuit will also contain resistance.
More informationTristan s Guide to: Solving Series Circuits. Version: 1.0 Written in 2006. Written By: Tristan Miller Tristan@CatherineNorth.com
Tristan s Guide to: Solving Series Circuits. Version: 1.0 Written in 2006 Written By: Tristan Miller Tristan@CatherineNorth.com Series Circuits. A Series circuit, in my opinion, is the simplest circuit
More information120 CHAPTER 3 NODAL AND LOOP ANALYSIS TECHNIQUES SUMMARY PROBLEMS SECTION 3.1
IRWI03_082132v3 8/26/04 9:41 AM Page 120 120 CHAPTER 3 NODAL AND LOOP ANALYSIS TECHNIQUES SUMMARY Nodal analysis for an Nnode circuit Select one node in the Nnode circuit as the reference node. Assume
More informationCircuits 1 M H Miller
Introduction to Graph Theory Introduction These notes are primarily a digression to provide general background remarks. The subject is an efficient procedure for the determination of voltages and currents
More informationDATA ANALYSIS II. Matrix Algorithms
DATA ANALYSIS II Matrix Algorithms Similarity Matrix Given a dataset D = {x i }, i=1,..,n consisting of n points in R d, let A denote the n n symmetric similarity matrix between the points, given as where
More informationSimilar matrices and Jordan form
Similar matrices and Jordan form We ve nearly covered the entire heart of linear algebra once we ve finished singular value decompositions we ll have seen all the most central topics. A T A is positive
More informationAfter completing this chapter, the student should be able to:
DC Circuits OBJECTIVES After completing this chapter, the student should be able to: Solve for all unknown values (current, voltage, resistance, and power) in a series, parallel, or series-parallel circuit.
More information1 2 3 1 1 2 x = + x 2 + x 4 1 0 1
(d) If the vector b is the sum of the four columns of A, write down the complete solution to Ax = b. 1 2 3 1 1 2 x = + x 2 + x 4 1 0 0 1 0 1 2. (11 points) This problem finds the curve y = C + D 2 t which
More informationSeries and Parallel Circuits
Series and Parallel Circuits Components in a circuit can be connected in series or parallel. A series arrangement of components is where they are inline with each other, i.e. connected end-to-end. A parallel
More informationExperiment 4: Sensor Bridge Circuits (tbc 1/11/2007, revised 2/20/2007, 2/28/2007) I. Introduction. From Voltage Dividers to Wheatstone Bridges
Experiment 4: Sensor Bridge Circuits (tbc //2007, revised 2/20/2007, 2/28/2007) Objective: To implement Wheatstone bridge circuits for temperature measurements using thermistors. I. Introduction. From
More informationDC mesh current analysis
DC mesh current analysis This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,
More informationUsing row reduction to calculate the inverse and the determinant of a square matrix
Using row reduction to calculate the inverse and the determinant of a square matrix Notes for MATH 0290 Honors by Prof. Anna Vainchtein 1 Inverse of a square matrix An n n square matrix A is called invertible
More informationSolution of Linear Systems
Chapter 3 Solution of Linear Systems In this chapter we study algorithms for possibly the most commonly occurring problem in scientific computing, the solution of linear systems of equations. We start
More information6 Series Parallel Circuits
6 Series Parallel Circuits This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit http://creativecommons.org/licenses/by/3.0/. Air Washington
More informationLecture 20: Transmission (ABCD) Matrix.
Whites, EE 48/58 Lecture 0 Page of 7 Lecture 0: Transmission (ABC) Matrix. Concerning the equivalent port representations of networks we ve seen in this course:. Z parameters are useful for series connected
More informationFB-DC3 Electric Circuits: Series and Parallel Circuits
CREST Foundation Electrical Engineering: DC Electric Circuits Kuphaldt FB-DC3 Electric Circuits: Series and Parallel Circuits Contents 1. What are "series" and "parallel"? 2. Simple series circuits 3.
More informationNodal and Loop Analysis
Nodal and Loop Analysis The process of analyzing circuits can sometimes be a difficult task to do. Examining a circuit with the node or loop methods can reduce the amount of time required to get important
More informationResistors. Some substances are insulators. A battery will not make detectible current flow through them.
Resistors Some substances are insulators. A battery will not make detectible current flow through them. Many substances (lead, iron, graphite, etc.) will let current flow. For most substances that are
More informationLecture 2 Matrix Operations
Lecture 2 Matrix Operations transpose, sum & difference, scalar multiplication matrix multiplication, matrix-vector product matrix inverse 2 1 Matrix transpose transpose of m n matrix A, denoted A T or
More informationIntroduction to Matrix Algebra
Psychology 7291: Multivariate Statistics (Carey) 8/27/98 Matrix Algebra - 1 Introduction to Matrix Algebra Definitions: A matrix is a collection of numbers ordered by rows and columns. It is customary
More informationExperiment NO.3 Series and parallel connection
Experiment NO.3 Series and parallel connection Object To study the properties of series and parallel connection. Apparatus 1. DC circuit training system 2. Set of wires. 3. DC Power supply 4. Digital A.V.O.
More informationDecember 4, 2013 MATH 171 BASIC LINEAR ALGEBRA B. KITCHENS
December 4, 2013 MATH 171 BASIC LINEAR ALGEBRA B KITCHENS The equation 1 Lines in two-dimensional space (1) 2x y = 3 describes a line in two-dimensional space The coefficients of x and y in the equation
More informationSERIES-PARALLEL DC CIRCUITS
Name: Date: Course and Section: Instructor: EXPERIMENT 1 SERIES-PARALLEL DC CIRCUITS OBJECTIVES 1. Test the theoretical analysis of series-parallel networks through direct measurements. 2. Improve skills
More informationVector and Matrix Norms
Chapter 1 Vector and Matrix Norms 11 Vector Spaces Let F be a field (such as the real numbers, R, or complex numbers, C) with elements called scalars A Vector Space, V, over the field F is a non-empty
More informationSeries and Parallel Resistive Circuits
Series and Parallel Resistive Circuits The configuration of circuit elements clearly affects the behaviour of a circuit. Resistors connected in series or in parallel are very common in a circuit and act
More informationExperiment 8 Series-Parallel Circuits
Experiment 8 Series-Parallel Circuits EL 111 - DC Fundamentals By: Walter Banzhaf, E.K. Smith, and Winfield Young University of Hartford Ward College of Technology Objectives: 1. For the student to measure
More informationBJT AC Analysis. by Kenneth A. Kuhn Oct. 20, 2001, rev Aug. 31, 2008
by Kenneth A. Kuhn Oct. 20, 2001, rev Aug. 31, 2008 Introduction This note will discuss AC analysis using the beta, re transistor model shown in Figure 1 for the three types of amplifiers: common-emitter,
More informationBJT Amplifier Circuits
JT Amplifier ircuits As we have developed different models for D signals (simple large-signal model) and A signals (small-signal model), analysis of JT circuits follows these steps: D biasing analysis:
More informationBJT Amplifier Circuits
JT Amplifier ircuits As we have developed different models for D signals (simple large-signal model) and A signals (small-signal model), analysis of JT circuits follows these steps: D biasing analysis:
More informationSection 1.7 22 Continued
Section 1.5 23 A homogeneous equation is always consistent. TRUE - The trivial solution is always a solution. The equation Ax = 0 gives an explicit descriptions of its solution set. FALSE - The equation
More informationSmall Signal Analysis of a PMOS transistor Consider the following PMOS transistor to be in saturation. Then, 1 2
Small Signal Analysis of a PMOS transistor Consider the following PMOS transistor to be in saturation. Then, 1 I SD = µ pcox( VSG Vtp)^2(1 + VSDλ) 2 From this equation it is evident that I SD is a function
More informationField-Effect (FET) transistors
Field-Effect (FET) transistors References: Hayes & Horowitz (pp 142-162 and 244-266), Rizzoni (chapters 8 & 9) In a field-effect transistor (FET), the width of a conducting channel in a semiconductor and,
More informationLab #4 Thevenin s Theorem
In this experiment you will become familiar with one of the most important theorems in circuit analysis, Thevenin s Theorem. Thevenin s Theorem can be used for two purposes: 1. To calculate the current
More informationSeries and Parallel Circuits
Pre-Laboratory Assignment Series and Parallel Circuits ECE 2100 Circuit Analysis Laboratory updated 16 May 2011 1. Consider the following series circuit. Derive a formula to calculate voltages V 1, V 2,
More informationUsing the Impedance Method
Using the Impedance Method The impedance method allows us to completely eliminate the differential equation approach for the determination of the response of circuits. In fact the impedance method even
More informationAnalysis of a single-loop circuit using the KVL method
Analysis of a single-loop circuit using the KVL method Figure 1 is our circuit to analyze. We shall attempt to determine the current through each element, the voltage across each element, and the power
More informationHomework Assignment 03
Question 1 (2 points each unless noted otherwise) Homework Assignment 03 1. A 9-V dc power supply generates 10 W in a resistor. What peak-to-peak amplitude should an ac source have to generate the same
More informationTECH TIP # 37 SOLVING SERIES/PARALLEL CIRCUITS THREE LAWS --- SERIES CIRCUITS LAW # 1 --- THE SAME CURRENT FLOWS THROUGH ALL PARTS OF THE CIRCUIT
TECH TIP # 37 SOLVING SERIES/PARALLEL CIRCUITS Please study this Tech Tip along with assignment 4 in Basic Electricity. Parallel circuits differ from series circuits in that the current divides into a
More informationTransistor Biasing. The basic function of transistor is to do amplification. Principles of Electronics
192 9 Principles of Electronics Transistor Biasing 91 Faithful Amplification 92 Transistor Biasing 93 Inherent Variations of Transistor Parameters 94 Stabilisation 95 Essentials of a Transistor Biasing
More information8.2. Solution by Inverse Matrix Method. Introduction. Prerequisites. Learning Outcomes
Solution by Inverse Matrix Method 8.2 Introduction The power of matrix algebra is seen in the representation of a system of simultaneous linear equations as a matrix equation. Matrix algebra allows us
More information9.2 Summation Notation
9. Summation Notation 66 9. Summation Notation In the previous section, we introduced sequences and now we shall present notation and theorems concerning the sum of terms of a sequence. We begin with a
More informationExperiment #5, Series and Parallel Circuits, Kirchhoff s Laws
Physics 182 Summer 2013 Experiment #5 1 Experiment #5, Series and Parallel Circuits, Kirchhoff s Laws 1 Purpose Our purpose is to explore and validate Kirchhoff s laws as a way to better understanding
More informationLINEAR ALGEBRA. September 23, 2010
LINEAR ALGEBRA September 3, 00 Contents 0. LU-decomposition.................................... 0. Inverses and Transposes................................. 0.3 Column Spaces and NullSpaces.............................
More informationA Primer on Index Notation
A Primer on John Crimaldi August 28, 2006 1. Index versus Index notation (a.k.a. Cartesian notation) is a powerful tool for manipulating multidimensional equations. However, there are times when the more
More informationApplication of Linear Algebra in. Electrical Circuits
Application of Linear Algebra in Electrical Circuits Seamleng Taing Math 308 Autumn 2001 December 2, 2001 Table of Contents Abstract..3 Applications of Linear Algebra in Electrical Circuits Explanation..
More informationEnvironmental Monitoring with Sensors: Hands-on Exercise
Environmental Monitoring with Sensors: Hands-on Exercise Now that you ve seen a few types of sensors, along with some circuits that can be developed to condition their responses, let s spend a bit of time
More information[1] Diagonal factorization
8.03 LA.6: Diagonalization and Orthogonal Matrices [ Diagonal factorization [2 Solving systems of first order differential equations [3 Symmetric and Orthonormal Matrices [ Diagonal factorization Recall:
More information1 Determinants and the Solvability of Linear Systems
1 Determinants and the Solvability of Linear Systems In the last section we learned how to use Gaussian elimination to solve linear systems of n equations in n unknowns The section completely side-stepped
More informationSolution to Homework 2
Solution to Homework 2 Olena Bormashenko September 23, 2011 Section 1.4: 1(a)(b)(i)(k), 4, 5, 14; Section 1.5: 1(a)(b)(c)(d)(e)(n), 2(a)(c), 13, 16, 17, 18, 27 Section 1.4 1. Compute the following, if
More informationThe BJT Differential Amplifier. Basic Circuit. DC Solution
c Copyright 010. W. Marshall Leach, Jr., Professor, Georgia Institute of Technology, School of Electrical and Computer Engineering. The BJT Differential Amplifier Basic Circuit Figure 1 shows the circuit
More informationSection 3. Sensor to ADC Design Example
Section 3 Sensor to ADC Design Example 3-1 This section describes the design of a sensor to ADC system. The sensor measures temperature, and the measurement is interfaced into an ADC selected by the systems
More informationChapter 19. General Matrices. An n m matrix is an array. a 11 a 12 a 1m a 21 a 22 a 2m A = a n1 a n2 a nm. The matrix A has n row vectors
Chapter 9. General Matrices An n m matrix is an array a a a m a a a m... = [a ij]. a n a n a nm The matrix A has n row vectors and m column vectors row i (A) = [a i, a i,..., a im ] R m a j a j a nj col
More informationTransistor Characteristics and Single Transistor Amplifier Sept. 8, 1997
Physics 623 Transistor Characteristics and Single Transistor Amplifier Sept. 8, 1997 1 Purpose To measure and understand the common emitter transistor characteristic curves. To use the base current gain
More informationMAT188H1S Lec0101 Burbulla
Winter 206 Linear Transformations A linear transformation T : R m R n is a function that takes vectors in R m to vectors in R n such that and T (u + v) T (u) + T (v) T (k v) k T (v), for all vectors u
More informationOperating Manual Ver.1.1
Class B Amplifier (Push-Pull Emitter Follower) Operating Manual Ver.1.1 An ISO 9001 : 2000 company 94-101, Electronic Complex Pardesipura, Indore- 452010, India Tel : 91-731- 2570301/02, 4211100 Fax: 91-731-
More informationExperiment 4 ~ Resistors in Series & Parallel
Experiment 4 ~ Resistors in Series & Parallel Objective: In this experiment you will set up three circuits: one with resistors in series, one with resistors in parallel, and one with some of each. You
More information7 Gaussian Elimination and LU Factorization
7 Gaussian Elimination and LU Factorization In this final section on matrix factorization methods for solving Ax = b we want to take a closer look at Gaussian elimination (probably the best known method
More information3: Nodal Analysis. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 1 / 12. 3: Nodal Analysis
Current Floating Voltage Dependent E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 1 / 12 Aim of Nodal Analysis Current Floating Voltage Dependent The aim of nodal analysis is to determine the
More information1 Introduction to Matrices
1 Introduction to Matrices In this section, important definitions and results from matrix algebra that are useful in regression analysis are introduced. While all statements below regarding the columns
More informationFundamentals of Electrical Engineering 2 Grundlagen der Elektrotechnik 2
Fundamentals of Electrical Engineering 2 Grundlagen der Elektrotechnik 2 Chapter: Sinusoidal Steady State Analysis / Netzwerkanalyse bei harmonischer Erregung Michael E. Auer Source of figures: Alexander/Sadiku:
More informationChapter 9 Balanced Faults
Chapter 9 alanced Faults 9.1 Introduction The most common types of fault are (in order) single-line-to-ground fault, line-to-line fault, and double-line-to-ground fault. All of these are unbalanced faults.
More informationTECHNIQUES OF. C.T. Pan 1. C.T. Pan
TECHNIQUES OF CIRCUIT ANALYSIS C.T. Pan 1 4.1 Introduction 4.2 The Node-Voltage Method ( Nodal Analysis ) 4.3 The Mesh-Current Method ( Mesh Analysis ) 4.4 Fundamental Loop Analysis 4.5 Fundamental Cutset
More informationLecture 3: Finding integer solutions to systems of linear equations
Lecture 3: Finding integer solutions to systems of linear equations Algorithmic Number Theory (Fall 2014) Rutgers University Swastik Kopparty Scribe: Abhishek Bhrushundi 1 Overview The goal of this lecture
More informationAP Physics Electricity and Magnetism #4 Electrical Circuits, Kirchoff s Rules
Name Period AP Physics Electricity and Magnetism #4 Electrical Circuits, Kirchoff s Rules Dr. Campbell 1. Four 240 Ω light bulbs are connected in series. What is the total resistance of the circuit? What
More informationJ.L. Kirtley Jr. Electric network theory deals with two primitive quantities, which we will refer to as: 1. Potential (or voltage), and
Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.061 Introduction to Power Systems Class Notes Chapter 1: eiew of Network Theory J.L. Kirtley Jr. 1 Introduction
More informationSignal Conditioning Wheatstone Resistive Bridge Sensors
Application Report SLOA034 - September 1999 Signal Conditioning Wheatstone Resistive Bridge Sensors James Karki Mixed Signal Products ABSTRACT Resistive elements configured as Wheatstone bridge circuits
More information