to-tee) Equivalent Circuits

Similar documents
Series-Parallel Circuits. Objectives

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

HOW TO USE MULTIMETER. COMPILE BY: Dzulautotech

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

Method 1: 30x Method 2: 15

Series and Parallel Resistive Circuits Physics Lab VIII

Mesh-Current Method (Loop Analysis)

DC Circuits (Combination of resistances)

Lab 1: DC Circuits. Student 1, Partner : Student 2, student2@ufl.edu

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

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

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

Chapter 7 Direct-Current Circuits

Tutorial 12 Solutions

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

Lab 3 - DC Circuits and Ohm s Law

BSNL TTA Question Paper-Instruments and Measurement Specialization 2007

Experiment 4: Sensor Bridge Circuits (tbc 1/11/2007, revised 2/20/2007, 2/28/2007) I. Introduction. From Voltage Dividers to Wheatstone Bridges

Experiment NO.3 Series and parallel connection

Series and Parallel Resistive Circuits

Environmental Monitoring with Sensors: Hands-on Exercise

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

Nodal and Loop Analysis

Kirchhoff's Current Law (KCL)

Basic Principles of. Electricity. Basic Principles of Electricity. by Prof. Dr. Osman SEVAİOĞLU Electrical and Electronics Engineering Department

1. Introduction and Chapter Objectives

Circuit Analysis using the Node and Mesh Methods

People s Physics Book

Series and Parallel Circuits

Circuit Analyses. Laboration 1 how to measure Current and Voltage and Resistance

ES250: Electrical Science. HW7: Energy Storage Elements

STUDY MATERIAL FOR CLASS Physics- CURRENT ELECTRICITY. The flow of electric charges in a particular direction constitutes electric current.

Fig. 1 Analogue Multimeter Fig.2 Digital Multimeter

Electronics. Basic Concepts. Yrd. Doç. Dr. Aytaç GÖREN Yrd. Doç. Dr. Levent ÇETİN

Current and Voltage Measurements. Current measurement

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

EXPERIMENT 7 OHM S LAW, RESISTORS IN SERIES AND PARALLEL

CURRENT ELECTRICITY - I

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

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

OHM S LAW AND RESISTANCE

How To Find The Current Of A Circuit

CHAPTER 28 ELECTRIC CIRCUITS

Ammeter design. Resources and methods for learning about these subjects (list a few here, in preparation for your research):

Experiment 8 Series-Parallel Circuits

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

PHYSICS 111 LABORATORY Experiment #3 Current, Voltage and Resistance in Series and Parallel Circuits

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

13.10: How Series and Parallel Circuits Differ pg. 571

First Year (Electrical & Electronics Engineering)

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

Student Exploration: Circuits

OPERATIONAL AMPLIFIERS

Experiment 4 ~ Resistors in Series & Parallel

Resistance, Ohm s Law, and the Temperature of a Light Bulb Filament

Thevenin Equivalent Circuits

Lab 2: Resistance, Current, and Voltage

Lesson Plan. Parallel Resistive Circuits Part 1 Electronics

Experiment: Series and Parallel Circuits

Chapter 7. DC Circuits

After completing this chapter, the student should be able to:

Chapter 28B - EMF and Terminal P.D. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University

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

Electrical Fundamentals Module 3: Parallel Circuits

Physics 3330 Experiment #2 Fall DC techniques, dividers, and bridges R 2 =(1-S)R P R 1 =SR P. R P =10kΩ 10-turn pot.

Making Accurate Voltage Noise and Current Noise Measurements on Operational Amplifiers Down to 0.1Hz

Using Ohm s Law to Build a Voltage Divider

ANALOG AND DIGITAL METERS ANALOG VS. DIGITAL METERS VOLTMETERS ANALOG AND DIGITAL

Maximum value. resistance. 1. Connect the Current Probe to Channel 1 and the Differential Voltage Probe to Channel 2 of the interface.

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

Last time : energy storage elements capacitor.

Series and Parallel Circuits

How To Use Multiisim On A Computer Or A Circuit Design Suite 10.0 (Aero)

ES 154 Electronic Devices and Circuits

Collection of Solved Feedback Amplifier Problems

Measurement of Capacitance

Cornerstone Electronics Technology and Robotics I Week 15 Combination Circuits (Series-Parallel Circuits)

Using Ohm s Law to Build a Voltage Divider

Kirchhoff s Laws Physics Lab IX

Current, Resistance and Electromotive Force. Young and Freedman Chapter 25

Ohm's Law and Circuits

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

Physics, Chapter 27: Direct-Current Circuits

Lab 7: Operational Amplifiers Part I

Measuring Insulation Resistance of Capacitors

Light Bulbs in Parallel Circuits

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

Parallel and Series Resistors, Kirchoff s Law

Series and Parallel Circuits

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

GROUND DETECTION CIRCUITS FOR STATIONARY APPLICATIONS (IN PLAIN DOWN TO EARTH LANGUAGE)

Measurement and Instrumentation. Analog Electrical Devices and Measurements

Measuring Electric Phenomena: the Ammeter and Voltmeter

Equipment: Power Supply, DAI, Variable resistance (8311), Variable inductance (8321)

Chapter 1. Fundamental Electrical Concepts

Essential Electrical Concepts

ECE 431. Experiment #1. Three-Phase ac Measurements. PERFORMED: 26 January 2005 WRITTEN: 28 January Jason Wells

SERIES-PARALLEL DC CIRCUITS

Fundamentals of Signature Analysis

Application Note 82 Using the Dallas Trickle Charge Timekeeper

Transcription:

SIMPLE ESISTIVE CICUIT ANALYSIS C.T. Pan 1 3.1 Series esistive Circuits 3. Parallel esistive Circuits 3.3 Voltage-divider and Current-divider Circuits 3.4 Measuring Current and Voltage 3.5 Measuring esistance-the Wheatstone Bridge 3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits C.T. Pan

3.1 Series esistive Circuits Linear resistors (Ohm s s law) = ρ l A ρ: : resistivity of material C.T. Pan 3 3.1 Series esistive Circuits example of fixed resistors wirewound type carbon film type A resistor with zero resistance is called short circuit. A resistor with infinite resistance is called open circuit. C.T. Pan 4

3.1 Series esistive Circuits Color code 黑 棕 紅 橙 黃 綠 藍 紫 灰 白 0 1 3 4 5 6 7 8 9 金銀, error 金 ± 5%, 銀 ± 10% 10-1 10 - no color ± 0% C.T. Pan 5 3.1 Series esistive Circuits A : yellow B : violet C : red D : gold 47 X 10 Ω ± 5% C.T. Pan 6

3.1 Series esistive Circuits red Yellow Green blue Violet ed Yellow 4 Green 5 blue 6 Violet 7 C.T. Pan 7 3.1 Series esistive Circuits a + v 1 - i 1 b v s i s + 1 v 3 - + v - i d i 3 3 c C.T. Pan 8

3.1 Series esistive Circuits High school solution = + + eq 1 3 vs eq C.T. Pan 9 3.1 Series esistive Circuits i = i = i = 1 3 v 1 = 1 i 1 v = i v 3 = 3 i 3 v s eq i s = -i 1 C.T. Pan 10

3.1 Series esistive Circuits v s a d i s i 3 + v - 1 1 + v - 3 3 i 1 + v - b c i N=4 nodes b=4 branches b method Problem: Find b unknowns i 1, i, i 3, i s C.T. Pan v 1, v, v 3, v s ( Passive sign convention ) 11 3.1 Series esistive Circuits Solution: Step1. KCL for N-1=3 N nodes node a i s = -i 1 node b i 1 = i node c i = i 3 node d i 3 = -i s (1) () (3) (4) Only N-1 KCL equations are independent! e.g. Eq (4) can be obtained from the previous three equations C.T. Pan 1

3.1 Series esistive Circuits Step. KVL equation v 1 + v + v 3 + (-vs)= 0 (5) Step3. Component models v 1 = 1 i 1 (6) v = i (7) v 3 = 3 i 3 (8) vs = given (9) There are b (=8) equations for b unknowns. Normally, there exists a unique solution. Unless the modeling is not accurate enough. C.T. Pan 13 3. Parallel esistive Circuits i s v s v 1 1 v 3 3 i1 i i 3 v High school solution 1 1 1 1 = + + eq 1 3 C.T. Pan 14

3. Parallel esistive Circuits vs i s eq vs is = = ( i1 + i + i3) i k = v s k eq, k=1,,3 Problem : Find b unknowns v 1, v, v 3, v s i 1, i, i 3, i s C.T. Pan 15 3. Parallel esistive Circuits Solution : Step1. KCL for N-1=1 1 node node a i s +i 1 +i +i 3 = 0 (1) Step. KVL equations loop A : v s +(-v 1 ) = 0 () loop B : v s +(-v ) = 0 (3) loop C : v s +(-v 3 ) = 0 (4) C.T. Pan 16

3. Parallel esistive Circuits Step3. Component models v 1 = 1 i 1 (5) v = i (6) v 3 = 3 i 3 (7) v s = given (8) There are b = 8 unknowns and there are 8 equations. One can find the unique solution. C.T. Pan 17 3.3 Voltage-divider and Current-divider Circuits The voltage-divider v v 1 = = 1 + 1 + 1 v v s s C.T. Pan 18

3.3 Voltage-divider and Current-divider Circuits The loading effect ( L ) L eq = + L eq vo = v + = 1 1 Ł eq s 1+ + L ł v s C.T. Pan 19 3.3 Voltage-divider and Current-divider Circuits Generalized case v j eq = n 1 j = i = k C.T. Pan 0 j eq v s

3.3 Voltage-divider and Current-divider Circuits The current divider i1 is 1 1 1 1 = + eq 1 i vk = i s eq k C.T. Pan 1 i i 1, = 1, v1 = = + 1 1 v 1 = = + 1 i i s s 3.3 Voltage-divider and Current-divider Circuits Generalized case i 1 s i i1 j i j n i n 1 v \ eq j = s n = i 1 k eq j 1 v j eq i j = = i C.T. Pan j s

3.4 Measuring Current and Voltage An ammeter is an instrument designed to measure current and must be placed in series with current being measured. Example : An analog ammeter based on the d Arsonval meter movement. C.T. Pan Picture from ELECTIC CICUITS 8th EDITION by Nilsson iedel 8th EDITION, 3 A dc ammeter equivalent circuit A The movable coil is characterized by a voltage rating and a current rating. e.g. a commercial meter movement is rated at 50mV and 1mA1 This means when the coil current is 1mA1 at full-scale position, the voltage drop across the coil is 50mV mv. C.T. Pan 4

A dc ammeter equivalent circuit An analog ammeter consists of a d Arsonval d movement in parallel with a resister A Example1 : A 50mV, 1mA1 d Arsonval movement is to be used in an ammeter of 1A1 rating. Determine A C.T. Pan 5 A dc ammeter equivalent circuit Solution : At full scale rating 1.0A 1mA = 50mV Loading effect due to ammeter or ( ) A 50 = 999 A Ω 50mV m = = 0.05 Ω 1A 50 50 999 m = = 0.05 Ω 50+50 999 C.T. Pan 6

Analog DC Ammeter To allow multiple ranges, shunt resistors are connected in parallel with the movement meter. + n I = I, current divider m fs A dc ammeter equivalent circuit n m I I -I m = n m fs m C.T. Pan 7 A dc ammeter equivalent circuit Example :Design an ammeter for the following multiple ranges (A) 0 ~ 1 A (B) 0 ~ 100 ma (C) 0 ~ 10 ma Assume that m =50Ω and I m = 1mA for the adopted d Arsonval movement meter. C.T. Pan 8

A dc ammeter equivalent circuit Ans : current divider I I = I = m fs n + I -I n m m n m fs m -3 10 50 (A) shunt resistance = ; 0.05 Ω 1 1A-1mA 1 50 50 (B) = = =0.505 Ω (100-1)mA 99 1 50 50 (C) = = =5.556Ω 3 10-1 9 C.T. Pan 9 A dc ammeter equivalent circuit An ideal ammeter has an equivalent resistance of 0 Ω and functions as a short circuit. C.T. Pan 30

A dc voltmeter equivalent circuit An analog voltmeter consists of a d Arsonvald movement in series with a series resister V. V The added V determines the full-scale reading of the voltmeter. C.T. Pan 31 A dc voltmeter equivalent circuit Example 3: A 50mV, 1mA1 d Arsonval movement is used in a voltmeter of 150V rating. Determine V. C.T. Pan 3

A dc voltmeter equivalent circuit Solution: From voltage divider formula 50 50mV= 150 V +50 v =149950 Ω v Loading effect of the meter m =149950+50=150 kω which is in parallel with the element to be measured. C.T. Pan 33 A dc voltmeter equivalent circuit V = I ( + ) fs fs n m Vfs = - n I fs m The design is based on the worst case which occurs when the full-scale current I fs =I m flows through the meters. C.T. Pan 34

A dc voltmeter equivalent circuit Example 4 : Design a voltmeter for the following multiple ranges (A) 0 ~ 1 V (B) 0 ~ 5 V (C) 0 ~ 100 V Assume the d Arsonval movement meter has m =kω with full scale I fs =100μA. C.T. Pan 35 A dc voltmeter equivalent circuit Ans : (A) V =I ( +) fs fs m 1 Vfs 1 = - = -000=8000Ω 1 m I 100μ fs 5 (B) = -000=48KΩ 100μ 100 (C) = -000=998KΩ 3 100μ C.T. Pan 36

3.5 Measuring esistance The Wheatstone Bridge The Wheatstone bridge circuit is used to measure resistance of mediumvalues :1Ω ~ 1MΩ, with an accuracy of about ± 0.1 % The Wheatstone bridge circuit C.T. Pan 37 3.5 Measuring esistance The Wheatstone Bridge current detector : a galvanometer X : the unknown resister C.T. Pan 38

3.5 Measuring esistance The Wheatstone Bridge Measuring X Adjust 3 until zero current in the galvanometer. C.T. Pan i = i, i = i 1 3 x V = V, V = V ab ac bd cd i=i, i =i 1 1 1 3 X = 1 3 X = X 3 1 39 3.5 Measuring esistance The Wheatstone Bridge 1 and : 1, 10, 100, 1000 Ω such that = 0.001~1000 1 in decimal steps 3 : adjustable in integral values of resistance from 1 to 11,000 Ω. Lower than 1Ω1 and higher than 1MΩ resistances are difficult to measure due to thermal heating effect and current leakage effect, respectively. C.T. Pan 40

3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Delta (Δ)( ) or Pi (π)( ) circuit b a c Wye (Y) or Tee (T) circuit C.T. Pan 41 3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Δ Y transformation c 1 b a 3 C.T. Pan 4

3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits = // ( + ) = + ab c a b 1 = // ( + ) = + bc a b c 3 = // ( + ) = + ca b c a 3 1 = + + b c 1 a b c c a = a + b + c a b = 3 a + b + c C.T. Pan 43 3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Y to Δ transformation Similarly, given 1,, 3 ; one can find a, b, c = a = b = c + + 1 3 3 1 + + C.T. Pan 44 1 1 3 3 1 + + 1 3 3 1 3

3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Special case, if 1 = = 3 =, then a = b = c =3 C.T. Pan 45 3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Example : Use Y Δ transformation to find V in the following circuit. C.T. Pan 46

3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Solution : C.T. Pan 47 3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits Solution : 0 10+ 10 5+ 5 0 35 = = Ω a 0 350 = = 35 Ω b 10 350 = = 70 Ω c 5 C.T. Pan 48

3.6 Delta-to to-wye (Pi-to to-tee) Equivalent Circuits 70 // 8 = 0 Ω + V - 35 Ω 35 // 105 = 15 Ω 35Ω V = A = 35V C.T. Pan 49 Summary Objective 1 : eview series and parallel resistive circuit solution approach. Objective : ecognize the b method by standard mathematical formulation. ( KCL + KVL + Ohm s s Law ) Objective 3 : Know how to use simple voltage-divider and current- divider concepts to solve simple circuit. C.T. Pan 50

Summary Objective 4 : Be able to determine the reading of ammeters and voltmeters. Objective 5 : Understand how to a Wheatstone bridge is used to measure resistance. Objective 6 : Know when and how to use delta-to to-wye equivalent circuits to solve a simple circuit. C.T. Pan 51 Assignment : Chapter Problems Problem : 3.14 3.4 3.30 3.33 3.50 3.64 Due within one week. C.T. Pan 5

C.T. Pan 53