3: Nodal Analysis. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 1 / 12. 3: Nodal Analysis



Similar documents
Circuit Analysis using the Node and Mesh Methods

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

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

Nodal and Loop Analysis

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

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

Mesh-Current Method (Loop Analysis)

How To Find The Current Of A Circuit

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

Series and Parallel Resistive Circuits

School of Engineering Department of Electrical and Computer Engineering

1Meg. 11.A. Resistive Circuit Nodal Analysis

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

Kirchhoff's Current Law (KCL)

Thevenin Equivalent Circuits

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

Resistors. Some substances are insulators. A battery will not make detectible current flow through them.

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

Student Exploration: Circuits

Ver 3537 E1.1 Analysis of Circuits (2014) E1.1 Circuit Analysis. Problem Sheet 1 (Lectures 1 & 2)

Welcome to this presentation on Driving LEDs Resistors and Linear Drivers, part of OSRAM Opto Semiconductors LED Fundamentals series.

DC mesh current analysis

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

Conversion Between Analog and Digital Signals

OPERATIONAL AMPLIFIERS

A Short Discussion on Summing Busses and Summing Amplifiers By Fred Forssell Copyright 2001, by Forssell Technologies All Rights Reserved

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

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

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

Experiment NO.3 Series and parallel connection

Chapter 11. Inductors ISU EE. C.Y. Lee

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

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

Chapter 19 Operational Amplifiers

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

Energy, Work, and Power

Analysis of a single-loop circuit using the KVL method

ELECTRICAL CIRCUITS. Electrical Circuits

DIGITAL-TO-ANALOGUE AND ANALOGUE-TO-DIGITAL CONVERSION

Series and Parallel Circuits

Lab 7: Operational Amplifiers Part I

Electrical Fundamentals Module 3: Parallel Circuits

Parallel and Series Resistors, Kirchoff s Law

Operational Amplifier - IC 741

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

Parallel DC circuits

THE BREADBOARD; DC POWER SUPPLY; RESISTANCE OF METERS; NODE VOLTAGES AND EQUIVALENT RESISTANCE; THÉVENIN EQUIVALENT CIRCUIT

1. Introduction and Chapter Objectives

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

MAS.836 HOW TO BIAS AN OP-AMP

Superposition Examples

Pre-Algebra Lecture 6

Use and Application of Output Limiting Amplifiers (HFA1115, HFA1130, HFA1135)

Series and Parallel Circuits

On the Application of Superposition to Dependent Sources in Circuit Analysis

ES250: Electrical Science. HW7: Energy Storage Elements

1. True or False? A voltage level in the range 0 to 2 volts is interpreted as a binary 1.

RMS Power. The Meaning of Average

The BJT Differential Amplifier. Basic Circuit. DC Solution

Rectifier circuits & DC power supplies

Tutorial 12 Solutions

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

OHM S LAW AND RESISTANCE

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.

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

Experiment 4 ~ Resistors in Series & Parallel

Kirchhoff s Laws Physics Lab IX

Direct-Current Circuits

Chapter 1. Fundamental Electrical Concepts

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

Lab 5 Operational Amplifiers

S-Parameters and Related Quantities Sam Wetterlin 10/20/09

Reading assignment: All students should read the Appendix about using oscilloscopes.

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

DC Circuits (Combination of resistances)

Lecture 7 Circuit analysis via Laplace transform

Digital to Analog and Analog to Digital Conversion

Measuring Electric Phenomena: the Ammeter and Voltmeter

Resistors in Series and Parallel Circuits

MATHEMATICS FOR ENGINEERING BASIC ALGEBRA

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

Chapter 10 Advanced CMOS Circuits

Chapter 13: Electric Circuits

Resistors in Series and Parallel

Application of Linear Algebra in. Electrical Circuits

Fig. 1 Analogue Multimeter Fig.2 Digital Multimeter

How To Calculate The Power Gain Of An Opamp

Output Ripple and Noise Measurement Methods for Ericsson Power Modules

Solutions to Bulb questions

CHECKING AND TESTING ELECTRICAL INSTALLING WORK

Ohm s Law. George Simon Ohm

Light Bulbs in Parallel Circuits

Transistor Characteristics and Single Transistor Amplifier Sept. 8, 1997

Algebra: Real World Applications and Problems

Basic Op Amp Circuits

Field-Effect (FET) transistors

OPERATIONAL AMPLIFIERS. o/p

The 2N3393 Bipolar Junction Transistor

2 A bank account for electricity II: flows and taxes

PS-6.2 Explain the factors that determine potential and kinetic energy and the transformation of one to the other.

Transcription:

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 voltage at each node relative to the reference node (or ground). Once you have done this you can easily work out anything else you need. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 2 / 12

Aim of Nodal Analysis Current Floating Voltage Dependent The aim of nodal analysis is to determine the voltage at each node relative to the reference node (or ground). Once you have done this you can easily work out anything else you need. There are two ways to do this: (1) Nodal Analysis - systematic; always works (2) Circuit Manipulation - ad hoc; but can be less work and clearer E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 2 / 12

Aim of Nodal Analysis Current Floating Voltage Dependent The aim of nodal analysis is to determine the voltage at each node relative to the reference node (or ground). Once you have done this you can easily work out anything else you need. There are two ways to do this: (1) Nodal Analysis - systematic; always works (2) Circuit Manipulation - ad hoc; but can be less work and clearer Reminders: A node is all the points in a circuit that are directly interconnected. We assume the interconnections have zero resistance so all points within a node have the same voltage. Five nodes: A,,E. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 2 / 12

Aim of Nodal Analysis Current Floating Voltage Dependent The aim of nodal analysis is to determine the voltage at each node relative to the reference node (or ground). Once you have done this you can easily work out anything else you need. There are two ways to do this: (1) Nodal Analysis - systematic; always works (2) Circuit Manipulation - ad hoc; but can be less work and clearer Reminders: A node is all the points in a circuit that are directly interconnected. We assume the interconnections have zero resistance so all points within a node have the same voltage. Five nodes: A,,E. Ohm s Law: V BD = IR 5 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 2 / 12

Aim of Nodal Analysis Current Floating Voltage Dependent The aim of nodal analysis is to determine the voltage at each node relative to the reference node (or ground). Once you have done this you can easily work out anything else you need. There are two ways to do this: (1) Nodal Analysis - systematic; always works (2) Circuit Manipulation - ad hoc; but can be less work and clearer Reminders: A node is all the points in a circuit that are directly interconnected. We assume the interconnections have zero resistance so all points within a node have the same voltage. Five nodes: A,,E. Ohm s Law: V BD = IR 5 KVL:V BD = V B V D E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 2 / 12

Aim of Nodal Analysis Current Floating Voltage Dependent The aim of nodal analysis is to determine the voltage at each node relative to the reference node (or ground). Once you have done this you can easily work out anything else you need. There are two ways to do this: (1) Nodal Analysis - systematic; always works (2) Circuit Manipulation - ad hoc; but can be less work and clearer Reminders: A node is all the points in a circuit that are directly interconnected. We assume the interconnections have zero resistance so all points within a node have the same voltage. Five nodes: A,,E. Ohm s Law: V BD = IR 5 KVL:V BD = V B V D KCL: Total current exiting any closed region is zero. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 2 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 1: Current Floating Voltage Dependent To find the voltage at each node, the first step is to label each node with its voltage as follows (1) Pick any node as the voltage reference. Label its voltage as0v. (2) If any fixed voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then go back to step (2) until all nodes are labelled. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 3 / 12

Nodal Analysis Stage 2: Current Floating Voltage Dependent The second step is to write down a KCL equation for each node labelled with a variable by setting the total current flowing out of the node to zero. For a circuit withn nodes ands voltage sources you will haven S 1 simultaneous equations to solve. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 4 / 12

Nodal Analysis Stage 2: Current Floating Voltage Dependent The second step is to write down a KCL equation for each node labelled with a variable by setting the total current flowing out of the node to zero. For a circuit withn nodes ands voltage sources you will haven S 1 simultaneous equations to solve. We only have one variable: X 8 1 k + X 0 2 k + X ( 2) 3 k = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 4 / 12

Nodal Analysis Stage 2: Current Floating Voltage Dependent The second step is to write down a KCL equation for each node labelled with a variable by setting the total current flowing out of the node to zero. For a circuit withn nodes ands voltage sources you will haven S 1 simultaneous equations to solve. We only have one variable: X 8 1 k + X 0 2 k + X ( 2) 3 k = 0 Numerator for a resistor is always of the formx V N wherev N is the voltage on the other side of the resistor. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 4 / 12

Nodal Analysis Stage 2: Current Floating Voltage Dependent The second step is to write down a KCL equation for each node labelled with a variable by setting the total current flowing out of the node to zero. For a circuit withn nodes ands voltage sources you will haven S 1 simultaneous equations to solve. We only have one variable: X 8 1 k + X 0 2 k + X ( 2) 3 k = 0 (6X 48)+3X +(2X +4) = 0 Numerator for a resistor is always of the formx V N wherev N is the voltage on the other side of the resistor. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 4 / 12

Nodal Analysis Stage 2: Current Floating Voltage Dependent The second step is to write down a KCL equation for each node labelled with a variable by setting the total current flowing out of the node to zero. For a circuit withn nodes ands voltage sources you will haven S 1 simultaneous equations to solve. We only have one variable: X 8 1 k + X 0 2 k + X ( 2) 3 k = 0 (6X 48)+3X +(2X +4) = 0 11X = 44 X = 4 Numerator for a resistor is always of the formx V N wherev N is the voltage on the other side of the resistor. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 4 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8,X E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8,X andy. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8,X andy. (3) Write equations X 8 1 + X 2 + X Y 3 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8,X andy. (3) Write equations X 8 1 + X 2 + X Y 3 = 0 Y X 3 +( 1) = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8,X andy. (3) Write equations X 8 1 + X 2 + X Y 3 = 0 Y X 3 +( 1) = 0 Ohm s law works OK if all resistors are inkω and all currents inma. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Current Current Floating Voltage Dependent Current sources cause no problems. (1) Pick reference node. (2) Label nodes: 8,X andy. (3) Write equations X 8 1 + X 2 + X Y 3 = 0 Y X 3 +( 1) = 0 Ohm s law works OK if all resistors are inkω and all currents inma. (4) Solve the equations: X = 6, Y = 9 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 5 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. (2) Label nodes: 8 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. (2) Label nodes: 8,X E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. (2) Label nodes: 8,X andx +2since it is joined tox via a voltage source. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. (2) Label nodes: 8,X andx +2since it is joined tox via a voltage source. (3) Write KCL equations but count all the nodes connected via floating voltage sources as a single super-node giving one equation X 8 1 + X 2 + (X+2) 0 3 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. (2) Label nodes: 8,X andx +2since it is joined tox via a voltage source. (3) Write KCL equations but count all the nodes connected via floating voltage sources as a single super-node giving one equation X 8 1 + X 2 + (X+2) 0 3 = 0 Ohm s law always involves the difference between the voltages at either end of a resistor. (Obvious but easily forgotten) E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Floating Voltage Current Floating Voltage Dependent Floating voltage sources have neither end connected to a known fixed voltage. We have to change how we form the KCL equations slightly. (1) Pick reference node. (2) Label nodes: 8,X andx +2since it is joined tox via a voltage source. (3) Write KCL equations but count all the nodes connected via floating voltage sources as a single super-node giving one equation X 8 1 + X 2 + (X+2) 0 3 = 0 (4) Solve the equations: X = 4 Ohm s law always involves the difference between the voltages at either end of a resistor. (Obvious but easily forgotten) E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 6 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. KCL equation for nodex: X V 1 R 1 + X V 2 R 2 + X V 3 R 3 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. KCL equation for nodex: X V 1 R 1 + X V 2 R 2 + X V 3 R 3 = 0 Or using conductances: (X V 1 )G 1 +(X V 2 )G 2 +(X V 3 )G 3 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. KCL equation for nodex: X V 1 R 1 + X V 2 R 2 + X V 3 R 3 = 0 Or using conductances: (X V 1 )G 1 +(X V 2 )G 2 +(X V 3 )G 3 = 0 X(G 1 +G 2 +G 3 ) = V 1 G 1 +V 2 G 2 +V 3 G 3 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. KCL equation for nodex: X V 1 R 1 + X V 2 R 2 + X V 3 R 3 = 0 Or using conductances: (X V 1 )G 1 +(X V 2 )G 2 +(X V 3 )G 3 = 0 X(G 1 +G 2 +G 3 ) = V 1 G 1 +V 2 G 2 +V 3 G 3 X = V 1G 1 +V 2 G 2 +V 3 G 3 G 1 +G 2 +G 3 = Vi G i Gi E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. KCL equation for nodex: X V 1 R 1 + X V 2 R 2 + X V 3 R 3 = 0 Or using conductances: (X V 1 )G 1 +(X V 2 )G 2 +(X V 3 )G 3 = 0 X(G 1 +G 2 +G 3 ) = V 1 G 1 +V 2 G 2 +V 3 G 3 X = V 1G 1 +V 2 G 2 +V 3 G 3 G 1 +G 2 +G 3 = Vi G i Gi VoltageX is the average ofv 1, V 2, V 3 weighted by the conductances. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Weighted Average Circuit Current Floating Voltage Dependent A very useful sub-circuit that calculates the weighted average of any number of voltages. KCL equation for nodex: X V 1 R 1 + X V 2 R 2 + X V 3 R 3 = 0 Still works ifv 3 = 0. Or using conductances: (X V 1 )G 1 +(X V 2 )G 2 +(X V 3 )G 3 = 0 X(G 1 +G 2 +G 3 ) = V 1 G 1 +V 2 G 2 +V 3 G 3 X = V 1G 1 +V 2 G 2 +V 3 G 3 G 1 +G 2 +G 3 = Vi G i Gi VoltageX is the average ofv 1, V 2, V 3 weighted by the conductances. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 7 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value 6 in decimal. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. We useb 2 b 1 b 0 to control the switches which determine whetherv i = 5V orv i = 0V. ThusV i = 5b i. Switches shown forb = 6. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. We useb 2 b 1 b 0 to control the switches which determine whetherv i = 5V orv i = 0V. ThusV i = 5b i. Switches shown forb = 6. X = 1 2 V 2+ 1 4 V 1+ 1 8 V 0 1 2 +1 4 +1 8 G 2 = 1 R 2 = 1 2k = 1 2 ms,... E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. We useb 2 b 1 b 0 to control the switches which determine whetherv i = 5V orv i = 0V. ThusV i = 5b i. Switches shown forb = 6. X = 1 2 V 2+ 1 4 V 1+ 1 8 V 0 1 2 +1 4 +1 8 = 1 7 (4V 2 +2V 1 +V 0 ) G 2 = 1 R 2 = 1 2k = 1 2 ms,... E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. We useb 2 b 1 b 0 to control the switches which determine whetherv i = 5V orv i = 0V. ThusV i = 5b i. Switches shown forb = 6. X = 1 2 V 2+ 1 4 V 1+ 1 8 V 0 1 2 +1 4 +1 8 = 1 7 (4V 2 +2V 1 +V 0 ) butv i = 5 b i since it connects to either0 V or5 V G 2 = 1 R 2 = 1 2k = 1 2 ms,... E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. We useb 2 b 1 b 0 to control the switches which determine whetherv i = 5V orv i = 0V. ThusV i = 5b i. Switches shown forb = 6. X = 1 2 V 2+ 1 4 V 1+ 1 8 V 0 1 2 +1 4 +1 8 = 1 7 (4V 2 +2V 1 +V 0 ) butv i = 5 b i since it connects to either0 V or5 V = 5 7 (4b 2 +2b 1 +b 0 ) = 5 7 b G 2 = 1 R 2 = 1 2k = 1 2 ms,... E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Digital-to-Analog Current Floating Voltage Dependent A 3-bit binary number,b, has bit-weights of4,2and1. Thus110 has a value6in decimal. If we label the bitsb 2 b 1 b 0, thenb = 4b 2 +2b 1 +b 0. We useb 2 b 1 b 0 to control the switches which determine whetherv i = 5V orv i = 0V. ThusV i = 5b i. Switches shown forb = 6. X = 1 2 V 2+ 1 4 V 1+ 1 8 V 0 1 2 +1 4 +1 8 = 1 7 (4V 2 +2V 1 +V 0 ) butv i = 5 b i since it connects to either0 V or5 V = 5 7 (4b 2 +2b 1 +b 0 ) = 5 7 b G 2 = 1 R 2 = 1 2k = 1 2 ms,... So we have made a circuit in whichx is proportional to a binary numberb. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 8 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. (3) Write equation for the dependent source,i S, in terms of node voltages: I S = 0.2(U X) E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. (3) Write equation for the dependent source,i S, in terms of node voltages: I S = 0.2(U X) (4) Write KCL equations: X U 10 + X 10 + X Y 20 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. (3) Write equation for the dependent source,i S, in terms of node voltages: I S = 0.2(U X) (4) Write KCL equations: X U 10 + X 10 + X Y 20 = 0 Y X 20 +I S + Y 15 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. (3) Write equation for the dependent source,i S, in terms of node voltages: I S = 0.2(U X) (4) Write KCL equations: X U 10 + X 10 + X Y 20 = 0 Y X 20 +I S + Y 15 = 0 (5) Solve all three equations to findx,y andi S in terms ofu: E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. (3) Write equation for the dependent source,i S, in terms of node voltages: I S = 0.2(U X) (4) Write KCL equations: X U 10 + X 10 + X Y 20 = 0 Y X 20 +I S + Y 15 = 0 (5) Solve all three equations to findx,y andi S in terms ofu: X = 0.1U, Y = 1.5U, I S = 0.18U E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Current Floating Voltage Dependent A dependent voltage or current source is one whose value is determined by voltages or currents elsewhere in the circuit. These are most commonly used when modelling the behaviour of transistors or op-amps. Each dependent source has a defining equation. In this circuit: I S = 0.2W ma wherew is in volts. (1) Pick reference node. (2) Label nodes: 0, U,X andy. (3) Write equation for the dependent source,i S, in terms of node voltages: I S = 0.2(U X) (4) Write KCL equations: X U 10 + X 10 + X Y 20 = 0 Y X 20 +I S + Y 15 = 0 (5) Solve all three equations to findx,y andi S in terms ofu: X = 0.1U, Y = 1.5U, I S = 0.18U Note that the value ofu is assumed to be known. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 9 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. (2) Label nodes: 0, 5 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. (2) Label nodes: 0, 5,X, X +3 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. (2) Label nodes: 0, 5,X, X +3and X +V S. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. (2) Label nodes: 0, 5,X, X +3and X +V S. (3) Write equation for the dependent source,v S, in terms of node voltages: V S = 10J = 10 X+V S 5 40 3V S = X 5 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. (2) Label nodes: 0, 5,X, X +3and X +V S. (3) Write equation for the dependent source,v S, in terms of node voltages: V S = 10J = 10 X+V S 5 40 3V S = X 5 (4) Write KCL equations: all nodes connected by floating voltage sources and all components connecting these nodes are in the same super-node X+V S 5 40 + X 5 + X+3 5 = 0 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Dependent Voltage Current Floating Voltage Dependent The value of the highlighted dependent voltage source isv S = 10J Volts wherej is the indicated current inma. (1) Pick reference node. (2) Label nodes: 0, 5,X, X +3and X +V S. (3) Write equation for the dependent source,v S, in terms of node voltages: V S = 10J = 10 X+V S 5 40 3V S = X 5 (4) Write KCL equations: all nodes connected by floating voltage sources and all components connecting these nodes are in the same super-node X+V S 5 40 + X 5 + X+3 5 = 0 (5) Solve the two equations: X = 1 andv S = 2 E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 10 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Universal Nodal Analysis Current Floating Voltage Dependent (1) Pick any node as the voltage reference. Label its voltage as0v. Label any dependent sources withv S, I S,... (2) If any voltage sources are connected to a labelled node, label their other ends by adding the value of the source onto the voltage of the labelled end. (3) Pick an unlabelled node and label it withx, Y,..., then loop back to step (2) until all nodes are labelled. (4) For each dependent source, write down an equation that expresses its value in terms of other node voltages. (5) Write down a KCL equation for each normal node (i.e. one that is not connected to a floating voltage source). (6) Write down a KCL equation for each super-node. A super-node consists of a set of nodes that are joined by floating voltage sources and includes any other components joining these nodes. (7) Solve the set of simultaneous equations that you have written down. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 11 / 12

Summary Current Floating Voltage Dependent Nodal Analysis Simple Circuits (no floating or dependent voltage sources) E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 12 / 12

Summary Current Floating Voltage Dependent Nodal Analysis Simple Circuits (no floating or dependent voltage sources) Floating Voltage use supernodes: all the nodes connected by floating voltage sources (independent or dependent) E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 12 / 12

Summary Current Floating Voltage Dependent Nodal Analysis Simple Circuits (no floating or dependent voltage sources) Floating Voltage use supernodes: all the nodes connected by floating voltage sources (independent or dependent) Dependent Voltage and Current Label each source with a variable Write extra equations expressing the source values in terms of node voltages Write down the KCL equations as before E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 12 / 12

Summary Current Floating Voltage Dependent Nodal Analysis Simple Circuits (no floating or dependent voltage sources) Floating Voltage use supernodes: all the nodes connected by floating voltage sources (independent or dependent) Dependent Voltage and Current Label each source with a variable Write extra equations expressing the source values in terms of node voltages Write down the KCL equations as before Mesh Analysis (in most textbooks) Alternative to nodal analysis but doesn t work for all circuits No significant benefits ignore it E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 12 / 12

Summary Current Floating Voltage Dependent Nodal Analysis Simple Circuits (no floating or dependent voltage sources) Floating Voltage use supernodes: all the nodes connected by floating voltage sources (independent or dependent) Dependent Voltage and Current Label each source with a variable Write extra equations expressing the source values in terms of node voltages Write down the KCL equations as before Mesh Analysis (in most textbooks) Alternative to nodal analysis but doesn t work for all circuits No significant benefits ignore it For further details see Hayt et al. Chapter 4. E1.1 Analysis of Circuits (2015-7020) Nodal Analysis: 3 12 / 12