THEVENIN-NORTON THEOREM

Slides:



Advertisements
Similar presentations
Advanced electronics.  EMF  Electromotive "force" is not considered a force measured in newtons, but a potential, or energy per unit of charge, measured.
Advertisements

1 ECE 3336 Introduction to Circuits & Electronics Note Set #6 Thévenin's and Norton’s Theorems Spring 2015, TUE&TH 5:30-7:00 pm Dr. Wanda Wosik.
10 Network Theorems Chapter Topics Covered in Chapter 10
Series-Parallel Circuits
Chapter 9 – Network Theorems
Chapter 9 – Network Theorems
1 ECE 3144 Lecture 21 Dr. Rose Q. Hu Electrical and Computer Engineering Department Mississippi State University.
Chapter 2 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Circuit Analysis III Section 06.
EE2003 Circuit Theory Chapter 2 Basic Laws
Network Theorems SUPERPOSITION THEOREM THÉVENIN’S THEOREM
Electrical Systems 100 Lecture 3 (Network Theorems) Dr Kelvin.
Thévenin’s and Norton’s Theorems
CHAPTER-2 NETWORK THEOREMS.
An Assignment Submitted for the fulfillment Of internal work in the subject Physics of B.Sc.I Semester Second (KINETIC THEORY, THERMODYNAMICS AND ELECTRIC.
ENE 103 Electrotechnology
Basic Electrical Engineering Lecture # 04 Simple Resistive Circuits Course Instructor: Engr. Sana Ziafat.
Chapter 8.
ELECTRICAL TECHNOLOGY EET 103/4
EMLAB 1 Chapter 5. Additional analysis techniques.
Chapter 9 Network Theorems.
10 Network Theorems Chapter 10-2: Thevenin’s Theorem
EENG 2610: Circuit Analysis Class 8: Thevenin’s and Norton’s Theorems Oluwayomi Adamo Department of Electrical Engineering College of Engineering, University.
Anuroop Gaddam. An ideal voltage source plots a vertical line on the VI characteristic as shown for the ideal 6.0 V source. Actual voltage sources include.
1 ECE 3144 Lecture 22 Dr. Rose Q. Hu Electrical and Computer Engineering Department Mississippi State University.
Chapter 8 Principles of Electric Circuits, Electron Flow, 9 th ed. Floyd © 2010 Pearson Higher Education, Upper Saddle River, NJ All Rights Reserved.
EE2010 Fundamentals of Electric Circuits Lecture 11 Network Theorems: Norton’s Theorem.
Block A Unit 3 outline One port network Two port network
Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Chapter 5 Handy Circuit Analysis Techniques.
CIRCUITS and SYSTEMS – part I Prof. dr hab. Stanisław Osowski Electrical Engineering (B.Sc.) Projekt współfinansowany przez Unię Europejską w ramach Europejskiego.
CIRCUIT ANALYSIS METHOD. TOPIC Node-Voltage Method Mesh-current Method Source of embodiment principle Thevenin’s Circuit Norton’s Circuit Maximum Power.
Chapter 1 Introduction to Electronics
Circuit Theorems. Quiz 1. The source resistance from a 1.50 V D-cell is 1.5 . The voltage that appears across a 75  load will be a V b V.
Grossman/Melkonian Chapter 3 Resistive Network Analysis.
Circuit Theory Chapter 2 Basic Laws
Tutorial 2 Review Ohms law, KVL and KCL The Wheatstone Bridge
Norton’s Theorem and Maximum Power Transfer Theorem Lecture No.7 By – Engr Sajid Hussain Qazi Lecturer Mehran University C.E.T Khairpur.
THEVENIN’S THEOREM ENGR. VIKRAM KUMAR B.E (ELECTRONICS)
MALVINO Electronic PRINCIPLES SIXTH EDITION. Chapter 1 Introduction.
Lesson 6: Current Sources Source Conversion
1 ECE 3144 Lecture 32 Dr. Rose Q. Hu Electrical and Computer Engineering Department Mississippi State University.
– Introduction  This chapter introduces important fundamental theorems of network analysis. They are the  Superposition theorem  Thévenin’s theorem.
Voltage Divider Circuits Input transducers Input transducers are devices that convert a change in physical conditions (for example, temperature) into a.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. MALVINO & BATES SEVENTH EDITION Electronic PRINCIPLES.
ABE425 Engineering Measurement Systems Circuit Analysis Dr. Tony E. Grift Dept. of Agricultural & Biological Engineering University of Illinois.
Objective of Lecture State Thévenin’s and Norton Theorems. Chapter 4.5 and 4.6 Fundamentals of Electric Circuits Demonstrate how Thévenin’s and Norton.
THEVENIN & NORTON THEOREMS. Basic Electric Circuits Thevenin’s and Norton’s Theorems.
SOURCE TRANSFORMATION
Dr inż. Agnieszka Wardzińska Room: 105 Polanka cygnus.et.put.poznan.pl/~award Advisor hours: Monday: Wednesday:
Chapter 1: Introduction and DC Circuit AZRALMUKMIN BIN AZMI.
Techniques of Circuit Analysis
Series-Parallel Circuits. Most practical circuits have both series and parallel components. Components that are connected in series will share a common.
Lecture Name: Dr. Mohammed Elmaleeh Office Location: Building No. D Office Contact Number: ELECTRICAL CIRCUITS (EE 270)
1 Fundamentals of Electric Circuits Chapter 2 Basic Laws Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Circuit Theorems 1.  Introduction  Linearity property  Superposition  Source transformations  Thevenin’s theorem  Norton’s theorem  Maximum power.
RESISTORS IN SERIES - In a series circuit, the current is the same
Supplement to Circuits Analysis
Lesson 7: Current Sources / Source Conversion
Techniques of Circuit Analysis
Norton’s Theorem. By: Engr.Irshad Raheem Memon
Thevenin Theorem Any combination of batteries and resistances with two terminals can be replaced by a single voltage source e and a single series resistor.
Chapter 2 Resistive Circuits
ECE 3301 General Electrical Engineering
The Theorems we will look at are:
Thévenin’s Theorem.
Network Theorems Presented by- Dr. Kakade K.P Rayat Shikshan Sanstha’s
Chapter 8.
Associate Professor, Dept. of Physics,
ECE 4991 Electrical and Electronic Circuits Chapter 3
Presentation transcript:

THEVENIN-NORTON THEOREM Title of the concept

Definitions and Keywords Thevenin Theorem : Any two terminals of a network composed of linear passive and active circuit elements may be replaced by an equivalent voltage source and an equivalent series resistance. The voltage source is equal to the potential difference between the two terminals connected to these terminals. The series resistance is the equivalent resistance looking into the two terminal ports with all the power sources within the terminal pair inactive. Norton Theorem : Any two terminals of a network composed of linear passive and active circuit elements may be replaced by an equivalent current source and a parallel resistance. The current of the source is the current measured in the short circuit placed across the terminal-pair. The parallel resistance is the equivalent resistance looking into the terminal-pair with all the independent power sources inactive.

CALCULATING THE THEVENIN EQUIVALENT To calculate the equivalent circuit, the resistance and voltage are needed, so two equations are required. These two equations are usually obtained by using the following steps, but any conditions placed on the terminals of the circuit should also work: 1. Calculate the output voltage, VAB, when in open circuit condition (no load resistor -meaning infinite resistance). This is VTh. 2.(a) Now replace voltage sources with short circuits and current sources with open circuits. (b) Replace the load circuit with an imaginary ohmmeter and measure the total resistance, R, "looking back" into the circuit. This is RTh.

CALCULATING THE NORTON EQUIVALENT To calculate the equivalent circuit, the resistance and voltage are needed, so two equations are required. These two equations are usually obtained by using the following steps, but any conditions placed on the terminals of the circuit should also work: 1. Find the Norton current INo. Calculate the output current, IAB, with a short circuit as the load (meaning 0 resistance between A and B). This is INo. 2. Find the Norton resistance RNo. When there are no dependent sources (i.e., all current and voltage sources are independent), there are two methods of determining the Norton impedance RNo. Calculate the output voltage, VAB, when in open circuit condition (i.e., no load resistor — meaning infinite load resistance). RNo equals this VAB divided by INo. or Replace independent voltage sources with short circuits and independent current sources with open circuits. The total resistance across the output port is the Norton impedance Rno .

Concept details The circuit consists of resistors and a voltage source. Terminals A and B are the terminals across which Thevenin equivalent circuit is to be determined. The diagram will be morphed into the next equivalent circuit diagram which is the circuit for calculating the equivalent output voltage. A typical Circuit diagram. 1 Current, using an arrow tip, will be circulated across the loop as well as voltage drop across each resistor will be displayed in parallelism. After 1 complete circulation it’s value will be determined and from there the voltage across terminals A and B. Equivalent circuit for determining equivalent output voltage. 2 Equivalent circuit for determining equivalent resistance. Req=R1+[(R2+R3)||R4] The previous circuit will be morphed into the circuit for determining equivalent resistance. Next the voltage source will be converted into a short. And, equivalent resistance will be calculated using the formula provided. 3

The previous circuit will be morphed into original circuit The previous circuit will be morphed into original circuit . Next, all the resistances will be combined together and the equivalent resistance will be displayed in parallelism of changing the value of 15V to 7.5V . The final equivalent circuit of the original circuit. The Thevenin equivalent circuit. 4 The circuit consists of resistors and a voltage source. Terminals A and B are the terminals across which Norton equivalent circuit is to be determined. The diagram will be morphed into the next equivalent circuit diagram which is the circuit for calculating the equivalent output voltage. A typical Circuit diagram. 5 Itotal =V1/[R4+{R1||(R2+R3)}] Itotal will be calculated using Kirchhoff's laws . And, finally using the current divider rule I will be calculated. Equivalent circuit for determining equivalent output voltage. 6 Using current divider rule: I=[(R2+R3)/(R1+R2+R3)]* Itotal

Req= R1+R4||(R2+R3) The previous circuit will be morphed into the circuit for determining equivalent resistance. Next the voltage source will be converted into a short. And, equivalent resistance will be calculated using the formula provided. 7 Equivalent circuit for determining equivalent resistance. The previous circuit will be morphed into original circuit . Next, all the resistances will be combined together and the equivalent resistance will be displayed in parallelism of changing the value of voltage source from 15V to current source of 3.75mA . The Norton equivalent circuit. 8 The final equivalent circuit of the original circuit.

Interactivity and Boundary limits While determining the Thevenin equivalent of a given circuit the user can alter the value of resistances and sources and observe the changes. Changing the values of the inputs changes the equivalent outputs. None of the resistances or sources should be zero or infinity. While determining the Thevenin equivalent of a given circuit the user can alter the value of resistances and sources and observe the changes. Changing the values of the inputs changes the equivalent outputs. None of the resistances or sources should be zero or infinity.

Questionnaire 1. The relation between Thevenin equivalent resistance(RTH) and that of Norton’s (RN) is given by: Answers: a) RTH>RN b) RTH=RN c)RTH<RN d)RTH>>RN

2.In the Thevenin equivalent circuit, the equivalent voltage source is _______ with the equivalent Thevenin resistance. Answer: a)in Parallel b)not connected. c)in series. d)None of them.

3.In the Norton equivalent circuit, the equivalent Norton resistance is _______ with the equivalent Norton current source. Answer: a)in Parallel b)not connected. c)in series. d)None of them.

4. A network has the configuration shown in the figure 4.A network has the configuration shown in the figure. All resistance values are expressed in ohms. Find the current through RL when it takes on values of 10, 50 and 200 ohms. Answer: a)0.324A, 0.481A and 0.146A respectively b)0.481A, 0.146A and 0.324A respectively c)0.481A, 0.324A and 0.146A respectively d)None of these.

5.The small signal equivalent of a vacuum-tube amplifier has the configuration depicted in the figure. The indicated circuit parameters have the following values: µ=99, R1=147,000 ohms ,rp =66,000 ohms and R2 =100,000 ohms. Find the value of the voltage for Eg=0.4 volt. Answer: a)1.872V b)18.72V c)11.42V d)15.78V

Links for further reading [1] “Electrical Engineering Fundamentals”, by Vincent Del Toro, Prentice-hall Of India Pvt. Ltd. [2] “Basic Electrical Engineering”, by D.P. Kothari and I.J. Nagrath, Tata McGraw-Hill Publishing Pvt. Ltd.

Thank you Made by:- Rutesh Chavda