Electric Circuits. Overview. Hani Mehrpouyan,

Similar documents
Mesh-Current Method (Loop Analysis)

Example: Determine the power supplied by each of the sources, independent and dependent, in this circuit:

120 CHAPTER 3 NODAL AND LOOP ANALYSIS TECHNIQUES SUMMARY PROBLEMS SECTION 3.1

Nodal and Loop Analysis

Circuit Analysis using the Node and Mesh Methods

Lecture Notes: ECS 203 Basic Electrical Engineering Semester 1/2010. Dr.Prapun Suksompong 1 June 16, 2010

Series and Parallel Resistive Circuits

TECHNIQUES OF. C.T. Pan 1. C.T. Pan

Module 2. DC Circuit. Version 2 EE IIT, Kharagpur

= (0.400 A) (4.80 V) = 1.92 W = (0.400 A) (7.20 V) = 2.88 W

Basic Laws Circuit Theorems Methods of Network Analysis Non-Linear Devices and Simulation Models

Bipolar Junction Transistor Basics

OPERATIONAL AMPLIFIERS

W03 Analysis of DC Circuits. Yrd. Doç. Dr. Aytaç Gören

DC mesh current analysis

Preamble. Kirchoff Voltage Law (KVL) Series Resistors. In this section of my lectures we will be. resistor arrangements; series and

Lab 7: Operational Amplifiers Part I

How To Find The Current Of A Circuit

Thevenin Equivalent Circuits

LAB VIII. BIPOLAR JUNCTION TRANSISTOR CHARACTERISTICS

Chapter 5. Parallel Circuits ISU EE. C.Y. Lee

Voltage Divider Bias

Unit/Standard Number. High School Graduation Years 2010, 2011 and 2012

Chapter 1. Fundamental Electrical Concepts

Superposition Examples

Series-Parallel Circuits. Objectives

LAB VII. BIPOLAR JUNCTION TRANSISTOR CHARACTERISTICS

Department of Electrical and Electronic Engineering, California State University, Sacramento

Chapter 19 Operational Amplifiers

Circuits 1 M H Miller

Series and Parallel Circuits

LAB2 Resistors, Simple Resistive Circuits in Series and Parallel Objective:

Series and Parallel Circuits

BJT Characteristics and Amplifiers

Transistor Characteristics and Single Transistor Amplifier Sept. 8, 1997

Lab 5 Operational Amplifiers

Experiment 4 ~ Resistors in Series & Parallel

3: Nodal Analysis. E1.1 Analysis of Circuits ( ) Nodal Analysis: 3 1 / 12. 3: Nodal Analysis

Kirchhoff's Current Law (KCL)

Bipolar Junction Transistors

BJT Amplifier Circuits

Analysis of a single-loop circuit using the KVL method

BJT AC Analysis. by Kenneth A. Kuhn Oct. 20, 2001, rev Aug. 31, 2008

6 Series Parallel Circuits

2.1 Introduction. 2.2 Terms and definitions

Electronics. Discrete assembly of an operational amplifier as a transistor circuit. LD Physics Leaflets P

BJT Amplifier Circuits

1. Introduction and Chapter Objectives

PROCEDURE: 1. Measure and record the actual values of the four resistors listed in Table 10-1.

Basic Electronics Prof. Dr. Chitralekha Mahanta Department of Electronics and Communication Engineering Indian Institute of Technology, Guwahati

13.10: How Series and Parallel Circuits Differ pg. 571

The 2N3393 Bipolar Junction Transistor

ES250: Electrical Science. HW7: Energy Storage Elements

Physics 623 Transistor Characteristics and Single Transistor Amplifier Sept. 13, 2006

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

Lecture 3: DC Analysis of Diode Circuits.

Parallel and Series Resistors, Kirchoff s Law

1Meg. 11.A. Resistive Circuit Nodal Analysis

Tristan s Guide to: Solving Parallel Circuits. Version: 1.0 Written in Written By: Tristan Miller Tristan@CatherineNorth.com

DC Circuits (Combination of resistances)

POWER SUPPLY MODEL XP-15. Instruction Manual ELENCO

Chapter 7 Direct-Current Circuits

ET - Electronics for Telecommunications

8.2. Solution by Inverse Matrix Method. Introduction. Prerequisites. Learning Outcomes

Dependent Sources: Introduction and analysis of circuits containing dependent sources.

Lecture 7 Circuit analysis via Laplace transform

Laboratory 4: Feedback and Compensation

Lecture 12: DC Analysis of BJT Circuits.

Field-Effect (FET) transistors

The BJT Differential Amplifier. Basic Circuit. DC Solution

How To Calculate The Power Gain Of An Opamp

Fundamentals of Electrical Engineering 2 Grundlagen der Elektrotechnik 2

Experiment 8 Series-Parallel Circuits

V out. Figure 1: A voltage divider on the left, and potentiometer on the right.

School of Engineering Department of Electrical and Computer Engineering

J.L. Kirtley Jr. Electric network theory deals with two primitive quantities, which we will refer to as: 1. Potential (or voltage), and

Transistor Amplifiers

Bipolar Transistor Amplifiers

People s Physics Book

The basic cascode amplifier consists of an input common-emitter (CE) configuration driving an output common-base (CB), as shown above.

Content Map For Career & Technology

Experiment #5, Series and Parallel Circuits, Kirchhoff s Laws

Electrical Fundamentals Module 3: Parallel Circuits

Common-Emitter Amplifier

Experiment NO.3 Series and parallel connection

Table 1 Comparison of DC, Uni-Polar and Bi-polar Stepper Motors

Current vs. Voltage Feedback Amplifiers

Differential Amplifier Offset. Causes of dc voltage and current offset Modeling dc offset R C

Scaling and Biasing Analog Signals

ARRL Morse Code Oscillator, How It Works By: Mark Spencer, WA8SME

SIMULATIONS OF PARALLEL RESONANT CIRCUIT POWER ELECTRONICS COLORADO STATE UNIVERSITY

Lesson Plan. Parallel Resistive Circuits Part 1 Electronics

LM 358 Op Amp. If you have small signals and need a more useful reading we could amplify it using the op amp, this is commonly used in sensors.

Figure 1. Diode circuit model

Diode Circuits. Operating in the Reverse Breakdown region. (Zener Diode)

CONSTRUCTING A VARIABLE POWER SUPPLY UNIT

Lab #9: AC Steady State Analysis

LABORATORY 2 THE DIFFERENTIAL AMPLIFIER

AP Physics Electricity and Magnetism #4 Electrical Circuits, Kirchoff s Rules

Fig6-22 CB configuration. Z i [6-54] Z o [6-55] A v [6-56] Assuming R E >> r e. A i [6-57]

Transcription:

Electric Circuits Hani Mehrpouyan, Department of Electrical and Computer Engineering, Lecture 5 (Mesh Analysis) Sep 8 th, 205 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 Overview With Ohm s and Kirchhoff s law established, they may now be applied to circuit analysis. Two techniques will be presented in this chapter: Nodal analysis, which is based on Kichhoff current law (KCL) Mesh analysis, which is based on Kichhoff voltage law (KVL) Any linear circuit can be analyzed using these two techniques. The analysis will result in a set of simultaneous equations which may be solved by Cramer s rule or computationally (using MATLAB for example) Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 2

Mesh Analysis Another general procedure for analyzing circuits is to use the mesh currents as the circuit variables. Recall: A loop is a closed path with no node passed more than once A mesh is a loop that does not contain any other loop within it Mesh analysis uses KVL to find unknown currents Mesh analysis is limited in one aspect: It can only apply to circuits that can be rendered planar. A planar circuit can be drawn such that there are no crossing branches. Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 3 Planar vs Nonpalanar The figure on the left is a nonplanar circuit: The branch with the 3Ω resistor prevents the circuit from being drawn without crossing branches The figure on the right is a planar circuit: It can be redrawn to avoid crossing branches Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 4

Mesh Analysis Steps Mesh analysis follows these steps:.assign mesh currents i,i 2, i n to the n meshes 2.Apply KVL to each of the n mesh currents. 3.Solve the resulting n simultaneous equations to get the mesh currents Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 5 Mesh Analysis Example The above circuit has two paths that are meshes (abefa and bcdeb) The outer loop (abcdefa) is a loop, but not a mesh First, mesh currents i and i 2 are assigned to the two meshes. Applying KVL to the meshes: V ( R + R ) i ( i i ) 3 ( i i ) + Ri + R3 2 = 0 R2i2 + V2 + R3 2 = 0 3 R i = V 3 2 R i + ( R2 + R3) i2 = V2 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 6

Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 7 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 8

Mesh Analysis with Current Sources The presence of a current source makes the mesh analysis simpler in that it reduces the number of equations. If the current source is located on only one mesh, the current for that mesh is defined by the source. For example: Here, the current i 2 is equal to -5A Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 9 Supermesh Similar to the case of nodal analysis where a voltage source shared two non-reference nodes, current sources (dependent or independent) that are shared by more than one mesh need special treatment The two meshes must be joined together, resulting in a supermesh. The supermesh is constructed by merging the two meshes and excluding the shared source and any elements in series with it A supermesh is required because mesh analysis uses KVL But the voltage across a current source cannot be known in advance. Intersecting supermeshes in a circuit must be combined to for a larger supermesh. Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 0

Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 2

Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 3 Selecting an Appropriate Approach In principle both the nodal analysis and mesh analysis are useful for any given circuit. What then determines if one is going to be more efficient for solving a circuit problem? There are two factors that dictate the best choice: The nature of the particular network is the first factor The second factor is the information required Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 4

Mesh analysis when If the network contains: Many series connected elements Voltage sources Supermeshes A circuit with fewer meshes than nodes If branch or mesh currents are what is being solved for. Mesh analysis is the only suitable analysis for transistor circuits It is not appropriate for operational amplifiers because there is no direct way to obtain the voltage across an op-amp. Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 5 Nodal analysis if If the network contains: Many parallel connected elements Current sources Supernodes Circuits with fewer nodes than meshes If node voltages are what are being solved for Non-planar circuits can only be solved using nodal analysis This format is easier to solve by computer Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 24 6

Circuit Analysis with PSpice PSpice is a common program used for circuit analysis. It is capable of determining all of the branch voltages and currents if the numerical values for all circuit components are known. Analysis using PSpice begins with drawing a schematic view of the circuit. The node voltages of interest can be indicated during the schematic setup using VIEWPOINTS The values are obtained by running Analysis/ Simulate Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 25 7 Rendering a circuit in PSpice Converting a standard schematic (top) to a PSpice schematic (bottom) is fairly straightforward. Note the explicit definition of the reference node by using the ground symbol labeled with a 0 and the nodal voltages of interest displayed with the viewpoints Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 26 8

Application: DC transistor circuit In general, there are two types of transistors commonly used: Field Effect (FET) and Bipolar Junction (BJT). A BJT is a three terminal device, where the input current into one terminal (the base) affects the current flowing out of a second terminal (the collector). The third terminal (the emitter) is the common terminal for both currents Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 27 9 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 20

Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 2 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 22

Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 23 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 24

Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 205 25