1 CHAPTER 2 EET 101 [Electric Circuit I]: V2009 School of Computer and Communication Engineering, UniMAP Prepared By: Prepared By: Wan Nur Suryani Firuz.

Slides:



Advertisements
Similar presentations
Quiz 1 a) Find the currents i1 and i2 in the circuit in the figure. b) Find the voltage vo. c) Verify that the total power developed equals the total power.
Advertisements

Copyright ©2011, ©2008, ©2005 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electric Circuits, Ninth Edition James.
Basic Electronics Ninth Edition Basic Electronics Ninth Edition ©2002 The McGraw-Hill Companies Grob Schultz.
THEVENIN’S THEOREM Thevenin’s theorem permits the reduction of a two-terminal dc network with any number of resistors and sources (Complex Circuit) to.
CHAPTER 6 Direct-Current Bridge.
Chapter 7.
Basic Electrical Engineering Lecture # 05 & 06 Course Instructor: Engr. Sana Ziafat.
CHAPTER 7 Alternating Current Bridge.
EET 110 – Survey of Electronics Chapter 3. FIGURE 3-17 Parallel electrical circuit. Dale R. Patrick Electricity and Electronics: A Survey, 5e Copyright.
electronics fundamentals
ECE 201 Circuit Theory I1 Back to the Bridge Which resistors are in series? Which resistors are in parallel?
1 Faraday’s Law of Induction If C is a stationary closed curve and S is a surface spanning C then The changing magnetic flux through S induces a non-electrostatic.
Week 04, Day 2 W10D2 DC Circuits Today’s Reading Assignment W10D2 DC Circuits & Kirchhoff’s Loop Rules Course Notes: Sections Class 09 1.
Lecture 2: Resistive Circuits Nilsson 2.5, , 3.7 ENG17 : Circuits I Spring April 2, 2015.
EE 1270 Introduction to Electric Circuits Suketu Naik 0 EE 1270: Introduction to Electric Circuits Lecture 4: Equivalent Networks Chapter 3 Simple Resistive.
Series-Parallel Circuits
Series-Parallel Circuits
electronics fundamentals
Water Analogy A simple electrical circuit - consisting of a battery and a resistor - can be modeled by a pump to simulate a battery and a paddle to simulate.
Basic Electrical Circuit 1
DC Circuits Muhajir Ab. Rahim School of Mechatronic Engineering Universiti Malaysia Perlis.
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.
EKT 451 CHAPTER 5 DC & AC Bridge..
Introduction To Engineering Electrical Circuits - 2 Agenda Kirchhoff’s Law Resistors & Resistance Wheatstone Bridge.
Delta-Wye Conversions
1 Chapter 3 Resistive Circuits. 2 Figure The circuit being designed provides an adjustable voltage, v, to the load circuit. Figure (a) A proposed.
EGR 101 Introduction to Engineering I1 Resistors in Parallel Resistors connected at a single node pair Voltage across each resistor is the same.
Series/Parallel Combination Circuits
Simple Resistive Circuites
09/16/2010© 2010 NTUST Chapter 6 Yu-Chi Lai 賴祐吉. 09/16/2010© 2010 NTUST Most practical circuits have combinations of series and parallel components. Components.
Chapter 6 Series and Parallel Circuits 1 of 81 MECH of 81 Chapter 6 Series and Parallel Circuits MECH1100 Topics Identifying Series- Parallel Relationships.
Series and Parallel.  a single resistance that can replace all the resistances in an electrical circuit while maintaining the same current when connected.
Lesson 6: Current Sources Source Conversion
RESISTIVE CIRCUIT Topic 2.
EGR 1011 Chapter 6 Series-Parallel Circuits. EGR 1012 Examples of Series-Parallel Circuits.
Chapter 18 Electric Circuits Chapter Opening 18.1 Electric circuits and electric current 18.2 Electrical energy and voltage 18.3 Resistance and Ohm’s law.
Series-Parallel Circuits. Most practical circuits have both series and parallel components. Components that are connected in series will share a common.
DC CIRCUITS: CHAPTER 2 DET 101/3 Basic Electrical Circuit 1.
Chapter 2 Resistive Circuits 1. Overview of Chapter Series Resistors and Parallel Resistors 2.2Voltage Divider Circuit 2.3 Current Divider Circuit.
Pusan National University power PNU 세계로 미래로 Electric Circuits Fall, 2014 Chapter 6 Series-Parallel Circuits.
Topics Identifying Series- Parallel Relationships
EKT101 Electric Circuit Theory
Fundamentals of Electric Circuits Chapter 2
Fundamentals of Electric Circuits Chapter 2
Electric Circuits (EELE 2312)
Simple Resistive Circuites
Resistors in Series Req=equivalent resistance.
Lesson 7: Current Sources / Source Conversion
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
Chapter 7.
RESISTIVE CIRCUIT Topic 2.
RESISTANCE CIRCUITS.
Capacitors and Inductors
3.1 Resistors in Series When two elements connected at a single node, they are said to be in series Series-connected circuit elements carry the same.
Network Reduction: Star–Delta Transformation
Chapter 8 DC Circuits.
Circuit in DC Instruments
Delta-Wye Conversions
Electric Circuits Fundamentals
CHAPTER 7 Alternating Current Bridge.
Back to the Bridge Which resistors are in series?
Fundamentals of Electric Circuits Chapter 2
Midterm Solutions Source Transformations
Resistance in Series and Parallel
Chapter 7.
Resistors in Parallel Resistors connected at a single node pair
Back to the Bridge Which resistors are in series?
Circuit Principles Kirchhoff’s Current Law (KCL)
Electric Circuits I (EELE 2310)
Presentation transcript:

1 CHAPTER 2 EET 101 [Electric Circuit I]: V2009 School of Computer and Communication Engineering, UniMAP Prepared By: Prepared By: Wan Nur Suryani Firuz bt Wan Ariffin Amir Razif A. b. Jamil Abdullah Resistive Circuit

2 RESISTIVE CIRCUIT  Series/parallel resistor  Voltage divider circuit  Current divider circuit  Voltage and current measurement  Wheatstone bridge  Delta-wye (Pi-Tee) equivalent circuit

3 SERIES/PARALLEL RESISTOR  Resistors in series: Resistance equivalent R eq = R 1 + R 2 + ……….+ R N

4 Current in Series Circuit  Current in series circuit is same at all circuit elements VOLTAGE IN SERIES CIRCUIT  Voltage (V T ) in series circuit is the total of voltage for each elements.

5 Resistors in Parallel

6 Equivalent Resistors in Parallel:

7  Two resistors in parallel:

8 Current in Parallel Circuit  Currents in parallel circuit is the total of current for each elements. VOLTAGE IN PARALLEL CIRCUIT  Voltage (V T ) in parallel circuit is same at all circuit elements.

9 Example #1  Find the equivalent resistor (R eq ) in the circuit.

10 RESISTIVE CIRCUIT  Series/parallel resistor  Voltage divider circuit  Current divider circuit  Voltage and current measurement  Wheatstone bridge  Delta-wye (Pi-Tee) equivalent circuit

11 Voltage Divider 2 2 2

12  Using Ohm law, we will get:  Voltage at resistor R 2 :

13 RESISTIVE CIRCUIT Series/parallel resistorSeries/parallel resistor Voltage divider circuitVoltage divider circuit Current divider circuitCurrent divider circuit Voltage and current measurementVoltage and current measurement Wheatstone bridgeWheatstone bridge Delta-wye (Pi-Tee) equivalent circuitDelta-wye (Pi-Tee) equivalent circuit

14 Current Divider

15  From the Ohm’s law, (1)

16  Series/parallel resistor  Voltage divider circuit  Current divider circuit  Voltage and current measurement  Wheatstone bridge  Delta-wye (Pi-Tee) equivalent circuit RESISTIVE CIRCUIT

17 Voltage and Current Measurement  An ammeter is an instrument designed to measure current.  It is placed in series with the circuit element whose current is being measured.  An ideal ammeter has an equivalent resistance of 0Ω and functions as a short circuit in series with the element whose current is being measured.

18  A voltmeter is an instrument designed to measure voltage.  It is placed in parallel with the element whose voltage is being measured.  An ideal voltmeter has an infinite equivalent resistance and thus functions as an open circuit in parallel with the element whose voltage is being measured.

19  The configurations for an ammeter and voltmeter to measure current and voltage

20 RESISTIVE CIRCUIT  Series/parallel resistor  Voltage divider circuit  Current divider circuit  Voltage and current measurement  Wheatstone bridge  Delta-wye (Pi-Tee) equivalent circuit

21 Wheatstone Bridge  The Wheatstone bridge circuit is used to precisely measure resistance of medium values, that is in the range of 1Ω to 1MΩ.  The bridge circuit consists of four resistors, a dc voltage source and a detector.

22  The Wheatstone bridge circuit: Wheatstone Bridge

23  When the bridge is balanced:  Combining these equation, gives Wheatstone Bridge

24  Solving these equation, yields Wheatstone Bridge

25  Series/parallel resistor  Voltage divider circuit  Current divider circuit  Voltage and current measurement  Wheatstone bridge  Delta-wye (Pi-Tee) equivalent circuit RESISTIVE CIRCUIT

26 Delta-Wye (PI-TEE) Circuit  If the galvanometer in Wheatstone bridge is replace with its equivalent resistance R m,

27  The resistor R 1, R 2 and R m (or R 3, R m and R x ) are referred as a delta (∆) interconnection.  It is also referred as a pi (π) interconnection because the ∆ can be shaped into a π without disturbing the electrical equivalent of the two configurations.

28  Delta configuration

29  The resistors R 1, R m dan R 3 (or R 2, R m and R x ) are referred as a wye (Y) interconnection because it can be shaped to look like the letter Y.  The Y configuration also referred as a tee (T) interconnection.

30  Wye configuration

31 The ∆ - Y Transformation

32  Using series and parallel simplifications in Δ-connected, yield

33  Using straightforward algebraic manipulation gives,

34  The expression for the three Δ- connected resistors as functions of three Y-connected resistors are

35 Example #2  Find the current and power supplied by the 40 V sources in the circuit shown below.

36 Solution:  We can find this equivalent resistance easily after replacing either the upper Δ (100Ω, 125Ω, 25Ω) or the lower Δ (40Ω, 25Ω, 37.5Ω) with its equivalent Y.  We choose to replace the upper Δ. Thus, Example #2

37 Example #2

38  Substituting the Y-resistor into the circuit,

39  The equivalent circuit,

40  Calculate the equivalent resistance,  Simplify the circuit,

41  Then, the current and power values are,

42 Example #3 Find no load value of v o. Find vo when RL = 150 kΩ How much power is dissipated in the 25 kΩ resistor if the load terminals are short- circuited ?

43 a) b) Example #3

44 c) Example #3

45 Example #4  Find the power dissipated in the 6 Ω resistor.

46 Solution:  Equivalent resistance  current i o, Example #4

47  Note that i o is the current in the 1.6Ω resistor.  Use current divider to get current in the 6Ω resistor,  Then the power dissipated by the resistor is Example #4

48 Example #5  Find the voltage of v o and v g.

49 Solution:  Equivalent resistance  Current in resistor 30Ω Example #5

50  Voltage v 0  Total voltage at the resistor

51  Voltage v g

52 Example #6  Find the current of i g and io in the circuit. Solution:  Equivalent resistance:

53  The current values,  Thus, Example #6

54 Example #7  Determine the value of i o

55 Example #8  Find i and V o

56 Example #9  Calculate the value of current; I.