Automated Problem and Solution Generation Software for Computer-Aided Instruction in Elementary Linear Circuit Analysis
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1 Basic Terminologies 2 Circuit Analysis
Examples for Introduction to Electrical Engineering Prepared by Professor Yih-Fang Huang, Department of Electrical Engineering 1BasicTerminologies An electric circuit is a collection of interconnected multi-terminal electrical devices (also referred to as circuit elements). Conventional circuit analysis focuses on devices that can be modeled as two-terminal devices,namely,acircuitelementwithtwoleadscomingoutofit.Examples of two-terminal devices include independent sources (e.g., a battery), simple resistors, capacitors, inductors and diodes. In practice, there are also many devices that have more than two terminals. Typical such examples are transistors, transformers, and operational amplifiers. In circuit analysis, those multi-terminal devices are typically modeled as two- terminal devices with dependent sources. Before we proceed to show some circuit analysis examples, we shall define some terminologies first: • Node:anodeisapointofconnectionbetweentwoormorecircuitelements. • Branch:abranchisaportionofthecircuitthatconsistsofone circuit element and its two terminal nodes. • Loop:a(closed)loopisasequenceofconnectedbranchesthatbegin and end at the same node. • Branch Current:abranchcurrentisthecurrentthatflowsthroughtheelectrical device of the branch. The physical unit of current is ampere,namedaftertheFrenchmathematicianandphysicist, Andr´e-Marie Amp`ere (1775-1836). • Branch Voltage:abranchvoltageisthepotentialdifferencebetweenthetwoterminal nodes of the electrical device of the branch. The physical unit of voltageisvolt,whichisnamedinhonorofthe -
9 Op-Amps and Transistors
Notes for course EE1.1 Circuit Analysis 2004-05 TOPIC 9 – OPERATIONAL AMPLIFIER AND TRANSISTOR CIRCUITS . Op-amp basic concepts and sub-circuits . Practical aspects of op-amps; feedback and stability . Nodal analysis of op-amp circuits . Transistor models . Frequency response of op-amp and transistor circuits 1 THE OPERATIONAL AMPLIFIER: BASIC CONCEPTS AND SUB-CIRCUITS 1.1 General The operational amplifier is a universal active element It is cheap and small and easier to use than transistors It usually takes the form of an integrated circuit containing about 50 – 100 transistors; the circuit is designed to approximate an ideal controlled source; for many situations, its characteristics can be considered as ideal It is common practice to shorten the term "operational amplifier" to op-amp The term operational arose because, before the era of digital computers, such amplifiers were used in analog computers to perform the operations of scalar multiplication, sign inversion, summation, integration and differentiation for the solution of differential equations Nowadays, they are considered to be general active elements for analogue circuit design and have many different applications 1.2 Op-amp Definition We may define the op-amp to be a grounded VCVS with a voltage gain (µ) that is infinite The circuit symbol for the op-amp is as follows: An equivalent circuit, in the form of a VCVS is as follows: The three terminal voltages v+, v–, and vo are all node voltages relative to ground When we analyze a circuit containing op-amps, we cannot use the -
Circuit Elements Basic Circuit Elements
CHAPTER 2: Circuit Elements Basic circuit elements • Voltage sources, • Current sources, • Resistors, • Inductors, • Capacitors We will postpone introducing inductors and capacitors until Chapter 6, because their use requires that you solve integral and differential equations. 2.1 Voltage and Current Sources • An electrical source is a device that is capable of converting nonelectric energy to electric energy and vice versa. – A discharging battery converts chemical energy to electric energy, whereas a battery being charged converts electric energy to chemical energy. – A dynamo is a machine that converts mechanical energy to electric energy and vice versa. • If operating in the mechanical-to-electric mode, it is called a generator. • If transforming from electric to mechanical energy, it is referred to as a motor. • The important thing to remember about these sources is that they can either deliver or absorb electric power, generally maintaining either voltage or current. 2.1 Voltage and Current Sources • An ideal voltage source is a circuit element that maintains a prescribed voltage across its terminals regardless of the current flowing in those terminals. • Similarly, an ideal current source is a circuit element that maintains a prescribed current through its terminals regardless of the voltage across those terminals. • These circuit elements do not exist as practical devices—they are idealized models of actual voltage and current sources. 2.1 Voltage and Current Sources • Ideal voltage and current sources can be further described as either independent sources or dependent sources. An independent source establishes a voltage or current in a circuit without relying on voltages or currents elsewhere in the circuit. -
An Algebraic Method to Synthesize Specified Modal Currents in Ladder Resonators: Application to Non-Circular Birdcage Coils
An Algebraic Method to Synthesize Specified Modal Currents in Ladder Resonators: Application to Non-circular Birdcage Coils Nicola De Zanchea and Klaas P. Pruessmannb a. Division of Medical Physics, Department of Oncology, University of Alberta, Edmonton, Canada b. Institute for Biomedical Engineering, University of Zurich and ETH Zurich, Zurich, Switzerland Published in Magnetic Resonance in Medicine DOI: 10.1002/mrm.25503 Correspondence Address: Nicola De Zanche Division of Medical Physics Department of Oncology University of Alberta 11560 University Avenue Edmonton, Alberta T6G 1Z2 Canada E-mail: [email protected] Phone: + 1-780-989-8155 Fax: + 1-780-432-8615 1 Abstract Purpose: Detectors such as birdcage coils often consist of networks of coupled resonant circuits that must produce specified magnetic field distributions. In many cases, such as quadrature asymmetric insert body coils, calculating the capacitance values required to achieve specified currents and frequencies simultaneously is a challenging task that previously had only approximate or computationally-inefficient solutions. Theory and Methods: A general algebraic method was developed that is applicable to linear networks having planar representations such as birdcage coils, TEM coils, and numerous variants of ladder networks. Unlike previous iterative or approximate methods, the algebraic method is computationally efficient and determines current distribution and resonant frequency using a single matrix inversion. The method was demonstrated by specifying irregular current distributions on a highly elliptical birdcage coil at 3T. Results Measurements of the modal frequency spectrum and transmit field distribution of the two specified modes agrees with the theory. Accuracy is limited in practice only by how accurately the matrix of self and mutual inductances of the network is known. -
Basic Nodal and Mesh Analysis
CHAPTER Basic Nodal and 4 Mesh Analysis KEY CONCEPTS Nodal Analysis INTRODUCTION Armed with the trio of Ohm’s and Kirchhoff’s laws, analyzing The Supernode Technique a simple linear circuit to obtain useful information such as the current, voltage, or power associated with a particular element is Mesh Analysis perhaps starting to seem a straightforward enough venture. Still, for the moment at least, every circuit seems unique, requiring (to The Supermesh Technique some degree) a measure of creativity in approaching the analysis. In this chapter, we learn two basic circuit analysis techniques— Choosing Between Nodal nodal analysis and mesh analysis—both of which allow us to and Mesh Analysis investigate many different circuits with a consistent, methodical approach. The result is a streamlined analysis, a more uniform Computer-Aided Analysis, level of complexity in our equations, fewer errors and, perhaps Including PSpice and most importantly, a reduced occurrence of “I don’t know how MATLAB to even start!” Most of the circuits we have seen up to now have been rather simple and (to be honest) of questionable practical use. Such circuits are valuable, however, in helping us to learn to apply fundamental techniques. Although the more complex circuits appearing in this chapter may represent a variety of electrical systems including control circuits, communication networks, motors, or integrated circuits, as well as electric circuit models of nonelectrical systems, we believe it best not to dwell on such specifics at this early stage. Rather, it is important to initially focus on the methodology of problem solving that we will continue to develop throughout the book. -
Engineering 11 Descriptive Title: Circuit Analysis Course Disciplines: Engineering Division: Mathematic Sciences
El Camino College COURSE OUTLINE OF RECORD – Approved I. GENERAL COURSE INFORMATION Subject and Number: Engineering 11 Descriptive Title: Circuit Analysis Course Disciplines: Engineering Division: Mathematic Sciences Catalog Description: This course serves as an introduction to the analysis of electrical circuits through the use of analytical techniques based on the application of circuit laws and network theorems. The course covers direct current (DC) and alternating current (AC) circuits containing resistors, capacitors, inductors, dependent sources, operational amplifiers, and/or switches. The analysis of these circuits includes natural and forced responses of first and second order resistor-inductor-capacitor (RLC) circuits, the use of phasors, AC power calculations, power transfer, and energy concepts. Conditions of Enrollment: Prerequisite: Physics 1C (or concurrent enrollment) and Math 270 (or concurrent enrollment) Corequisite: Engineering 12 Course Length: X Full Term Other (Specify number of weeks): Hours Lecture: 3.00 hours per week TBA Hours Laboratory: 0 hours per week TBA Course Units: 3.00 Grading Method: Letter Credit Status: Associate Degree Credit Transfer CSU: X Effective Date: 05/18/2020 Transfer UC: X Effective Date: Pending General Education: El Camino College: CSU GE: IGETC: II. OUTCOMES AND OBJECTIVES A. COURSE STUDENT LEARNING OUTCOMES (The course student learning outcomes are listed below, along with a representative assessment method for each. Student learning outcomes are not subject to review, revision or approval by the College Curriculum Committee) 1. ANALYSIS OF CIRCUITS: Analyze AC and DC circuits using Kirchhoff's laws, mesh and nodal analysis, and network theorems. 2. IDENTIFICATION OF CIRCUIT COMPONENTS: When presented with a complex circuit diagram, identify and analyze key components, such as amplifier circuits, divider networks, and filters. -
Electrical & Electronics Engineering
ELECTRICAL & ELECTRONICS ENGINEERING Fundamentals of Electric Circuits: DC Circuits: 1.1 Introduction Technology has dramatically changed the way we do things; we now have Internet-connected computers and sophisticated electronic entertainment systems in our homes, electronic control systems in our cars, cell phones that can be used just about anywhere, robots that assemble products on production lines, and so on. A first step to understanding these technologies is electric circuit theory. Circuit theory provides you the knowledge of basic principles that you need to understand the behavior of electric elements include controlled and uncontrolled source of energy, resistors, capacitors, inductors, etc. Analysis of electric circuits refers to computations required to determine the unknown quantities such as voltage, current and power associated with one or more elements in the circuit. To contribute to the solution of engineering problems one must acquire the basic knowledge of electric circuit analysis and laws. To learn how to analyze the systems and its models, first one needs to learn the techniques of circuit analysis. In this chapter, We shall discuss briefly some of the basic circuit elements and the laws that will help us to develop the background of subject. The SI System of Units The solution of technical problems requires the use of units. At present, two major systems—the English (US Customary) and the metric—are in everyday use. For scientific and technical purposes, however, the English system has been almost totally superseded. In its place the SI system is used. Table 1–1 shows a few frequently encountered quantities with units expressed in both systems. -
1. Characteristics and Parameters of Operational Amplifiers
1. CHARACTERISTICS AND PARAMETERS OF OPERATIONAL AMPLIFIERS The characteristics of an ideal operational amplifier are described first, and the characteristics and performance limitations of a practical operational amplifier are described next. There is a section on classification of operational amplifiers and some notes on how to select an operational amplifier for an application. 1.1 IDEAL OPERATIONAL AMPLIFIER 1.1.1 Properties of An Ideal Operational Amplifier The characteristics or the properties of an ideal operational amplifier are: i. Infinite Open Loop Gain, ii. Infinite Input Impedance, iii. Zero Output Impedance, iv. Infinite Bandwidth, v. Zero Output Offset, and vi. Zero Noise Contribution. The opamp, an abbreviation for the operational amplifier, is the most important linear IC. The circuit symbol of an opamp shown in Fig. 1.1. The three terminals are: the non-inverting input terminal, the inverting input terminal and the output terminal. The details of power supply are not shown in a circuit symbol. 1.1.2 Infinite Open Loop Gain From Fig.1.1, it is found that vo = - Ao × vi, where `Ao' is known as the open-loop 5 gain of the opamp. Let vo be -10 Volts, and Ao be 10 . Then vi is 100 :V. Here 1 the input voltage is very small compared to the output voltage. If Ao is very large, vi is negligibly small for a finite vo. For the ideal opamp, Ao is taken to be infinite in value. That means, for an ideal opamp vi = 0 for a finite vo. Typical values of Ao range from 20,000 in low-grade consumer audio-range opamps to more than 2,000,000 in premium grade opamps ( typically 200,000 to 300,000). -
Implementing Voltage Controlled Current Source in Electromagnetic Full-Wave Simulation Using the FDTD Method Khaled Elmahgoub and Atef Z
Implementing Voltage Controlled Current Source in Electromagnetic Full-Wave Simulation using the FDTD Method Khaled ElMahgoub and Atef Z. Elsherbeni Center of Applied Electromagnetic System Research (CAESR), Department of Electrical Engineering, The University of Mississippi, University, Mississippi, USA. [email protected] and [email protected] Abstract — The implementation of a voltage controlled FDTD is introduced with efficient use of both memory and current source (VCCS) in full-wave electromagnetic simulation computational time. This new approach can be used to analyze using finite-difference time-domain (FDTD) is introduced. The VCCS is used to model a metal oxide semiconductor field effect circuits including VCCS or circuits include devices such as transistor (MOSFET) commonly used in microwave circuits. This MOSFETs and BJTs using their equivalent circuit models. To new approach is verified with several numerical examples the best of the authors’ knowledge, the implementation of including circuits with VCCS and MOSFET. Good agreement is dependent sources using FDTD has not been adequately obtained when the results are compared with those based on addressed before. In addition, in most of the previous work the analytical solution and PSpice. implementation of nonlinear devices such as transistors has Index Terms — Finite-difference time-domain, dependent been handled using FDTD-SPICE models or by importing the sources, voltage controlled current source, MOSFET. S-parameters from another technique to the FDTD simulation [2]-[7]. In this work the implementation of the VCCS in I. INTRODUCTION FDTD will be used to simulate a MOSFET with its equivalent The finite-difference time-domain (FDTD) method has gained model without the use of external tools, the entire simulation great popularity as a tool used for electromagnetic can be done using the FDTD. -
DEPENDENT SOURCES Objectives
Notes for course EE1.1 Circuit Analysis 2004-05 TOPIC 8 – DEPENDENT SOURCES Objectives . To introduce dependent sources . To study active sub-circuits containing dependent sources . To perform nodal analysis of circuits with dependent sources 1 INTRODUCTION TO DEPENDENT SOURCES 1.1 General The elements we have introduced so far are the resistor, the capacitor, the inductor, the independent voltage source and the independent current source. These are all 2-terminal elements The power absorbed by a resistor is non-negative at all times, that is it is always positive or zero The inductor and capacitor can absorb power or deliver power at different time instants, but the average power over a period of an AC steady state signal must be zero; these elements are called lossless. Since the resistor, inductor and capacitor cannot deliver net power, they are passive elements. The independent voltage source and current source can deliver power into a suitable load, such as a resistor. The independent voltage and current source are active elements. In many situations, we separate the sources from the circuit and refer to them as excitations to the circuit. If we do this, our circuit elements are all passive. In this topic, we introduce four new elements which we describe as dependent (or controlled) sources. Like independent sources, dependent sources are either voltage sources or current sources. However, unlike independent sources, they receive a stimulus from somewhere else in the circuit and that stimulus may also be a voltage or a current, leading to four versions of the element Dependent sources are considered part of the circuit rather than the excitation and have the function of providing circuit elements which are active; they can be used to model transistors and operational amplifiers. -
Mesh Analysis Examples and Solutions Pdf
Mesh Analysis Examples And Solutions Pdf Ernest is ascribable and stithies irresistibly while laniary Gearard hesitating and scallop. Intercalative and tiptop Forster never vituperate unblamably when Keene glided his salmon. Olympic and griefless Haley mantle while scabbier Weber chancing her guavas anamnestically and fared vigilantly. Also suffice as be Current Method. Recall that a loop remain a closed path so no node passed more intimate once. Properties of a Super Mesh A Super Mesh which no current of patient own. Click exit to reinsert the template reference. To simplify matters, this voltage can be eliminated when composing the past current equations. Another uncle of mind that lends itself somehow to work Current debate the unbalanced Wheatstone Bridge. There also two ways of solving this predicament. Assign positive values if cheat is steep increase in voltage and negative values if scar is slowly decrease in voltage. The term multiplying the voltage at that node will rule the sum let the conductances connected to that node. Note no more than one reason current may emerge through novel circuit element. The raisin of KCL equations required is one less than no number of nodes that my circuit has. MATLAB at the command line. Mesh analysis is only applicable to just circuit water is planar. Abro Example: mention the current matrix equation for the data network by inspection, or responding to other answers. Convert all voltage sources to current sources. Using nodal analysis, because the presence of before current sources reduces the arise of equations. Linkedin to deck the latest updates or experience Here often get latest Engineering Articles in your mailbox. -
Chapter 3 Nodal and Mesh Equations - Circuit Theorems
Chapter 3 Nodal and Mesh Equations - Circuit Theorems 3.14 Exercises Multiple Choice 1. The voltage across the 2 Ω resistor in the circuit of Figure 3.67 is A. 6 V B. 16 V C. –8 V D. 32 V E. none of the above − + 6 V + 2 Ω − 8 A 8 A Figure 3.67. Circuit for Question 1 2. The current i in the circuit of Figure 3.68 is A. –2 A B. 5 A C. 3 A D. 4 A E. none of the above 4 V − + 2 Ω 2 Ω + − 2 Ω 2 Ω 10 V i Figure 3.68. Circuit for Question 2 3-52 Circuit Analysis I with MATLAB Applications Orchard Publications Exercises 3. The node voltages shown in the partial network of Figure 3.69 are relative to some reference node which is not shown. The current i is A. –4 A B. 83⁄ A C. –5 A D. –6 A E. none of the above 6 V 8 V − 4 V + 8 V 2 Ω − 12 V + 2 Ω i 8 V − 6 V + 13 V 2 Ω Figure 3.69. Circuit for Question 3 4. The value of the current i for the circuit of Figure 3.70 is A. –3 A B. –8 A C. –9 A D. 6 A E. none of the above 6 Ω 3 Ω i + 12 V 6 Ω 8 A 3 Ω − Figure 3.70. Circuit for Question 4 Circuit Analysis I with MATLAB Applications 3-53 Orchard Publications Chapter 3 Nodal and Mesh Equations - Circuit Theorems 5.