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



Similar documents
Thevenin Equivalent Circuits

Mesh-Current Method (Loop Analysis)

Circuit Analysis using the Node and Mesh Methods

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

Nodal and Loop Analysis

How To Find The Current Of A Circuit

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

Series-Parallel Circuits. Objectives

Series and Parallel Resistive Circuits

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

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

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

Kirchhoff's Current Law (KCL)

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

Circuits 1 M H Miller

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

Analysis of a single-loop circuit using the KVL method

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

Resistors in Series and Parallel Circuits

Series and Parallel Circuits

Equivalent Circuits and Transfer Functions

DC mesh current analysis

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

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

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

ES250: Electrical Science. HW7: Energy Storage Elements

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 8 Series-Parallel Circuits

13.10: How Series and Parallel Circuits Differ pg. 571

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

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

DC Circuits (Combination of resistances)

Tutorial 12 Solutions

Series and Parallel Circuits

(6)(2) (-6)(-4) (-4)(6) + (-2)(-3) + (4)(3) + (2)(-3) = = 0

Lecture 7 Circuit analysis via Laplace transform

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

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

Experiment NO.3 Series and parallel connection

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

Current and Voltage Measurements. Current measurement

Lecture 3: DC Analysis of Diode Circuits.

x = + x 2 + x

Experiment 4 ~ Resistors in Series & Parallel

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

Student Exploration: 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

2.1 Introduction. 2.2 Terms and definitions

Fig. 1 Analogue Multimeter Fig.2 Digital Multimeter

Parallel DC circuits

Electrical Fundamentals Module 3: Parallel Circuits

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

Lecture 12: DC Analysis of BJT Circuits.

Lab 7: Operational Amplifiers Part I

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

Kirchhoff s Laws Physics Lab IX

Physics 133: tutorial week 4 Ohm s law, electrical power, emf and internal resistance.

Series and Parallel Resistive Circuits Physics Lab VIII

Current Electricity Lab Series/Parallel Circuits. Safety and Equipment Precautions!

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

Chapter 1. Fundamental Electrical Concepts

Chapter 10. RC Circuits ISU EE. C.Y. Lee

V out = V in x R 2 (R 1 + R 2 ) V o = V i R 1 FXA 2008 POTENTIAL DIVIDER CIRCUIT 1. Candidates should be able to : SUPPLYING A FIXED PD

EXAMPLE 8: An Electrical System (Mechanical-Electrical Analogy)

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

Application of Linear Algebra in. Electrical Circuits

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

ÇANKAYA UNIVERSITY Faculty of Engineering and Architecture

Last time : energy storage elements capacitor.

TECH TIP # 37 SOLVING SERIES/PARALLEL CIRCUITS THREE LAWS --- SERIES CIRCUITS LAW # THE SAME CURRENT FLOWS THROUGH ALL PARTS OF THE CIRCUIT

Series and Parallel Circuits

Light Bulbs in Parallel Circuits

Superposition Examples

Touch Screen Technology. Taking apart a tablet

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

6 Series Parallel Circuits

Resistors in Series and Parallel

The Infinite Resistor Chain

Lab 3 - DC Circuits and Ohm s Law

45. The peak value of an alternating current in a 1500-W device is 5.4 A. What is the rms voltage across?

Small Signal Analysis of a PMOS transistor Consider the following PMOS transistor to be in saturation. Then, 1 2

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

Fundamentals of Electrical Engineering 2 Grundlagen der Elektrotechnik 2

Environmental Monitoring with Sensors: Hands-on Exercise

SERIES-PARALLEL DC CIRCUITS

CURRENT ELECTRICITY - I

AP1 Electricity. 1. A student wearing shoes stands on a tile floor. The students shoes do not fall into the tile floor due to

SIMULATIONS OF PARALLEL RESONANT CIRCUIT POWER ELECTRONICS COLORADO STATE UNIVERSITY

DOKUZ EYLUL UNIVERSITY FACULTY OF ENGINEERING OFFICE OF THE DEAN COURSE / MODULE / BLOCK DETAILS ACADEMIC YEAR / SEMESTER. Course Code: EEE 2073

Exercises on Static Circuits

Experiment: Series and Parallel Circuits

Problem Solving 8: RC and LR Circuits

CHAPTER 28 ELECTRIC CIRCUITS

Figure 1. Diode circuit model

Σ I in = Σ I out E = IR 1 + IR 2 FXA 2008 KIRCHHOFF S LAWS 1. Candidates should be able to : LAW 1 (K1)

Lesson Plan. Parallel Resistive Circuits Part 1 Electronics

Curcuits and Differential Equaitons

Transcription:

Example: Determine the power supplied by each of the sources, independent and dependent, in this circuit: Solution: We ll begin by choosing the bottom node to be the reference node. Next we ll label the other nodes and some element oltages: Notice that the 8 Ω resistor, the 0 Ω resistor and the two independent current sources are all connected in parallel. Consequently, the element oltages of theses elements can be labeled so that they are equal. Similarly, the 4 Ω resistor and the dependent current source are connected in parallel so their oltages can be labeled so as to be equal. Using Ohm s Law we see that the current directed downward in the 8 Ω resistor is directed downward in the 0 Ω resistor is Ω resistor is, current 8, and the current directed from left to right in the 0. Applying Kirchhoff s Current Law (KCL) at node a gies 5 = +.5 + + 0.5+ 0.5 =.5 () 8 0 Using Ohm s Law we see that the current directed downward in the 4 Ω resistor is Kirchhoff s Current Law (KCL) at node a gies. Applying 4

+.5 =.5+ 0.5 0.5 = 0 () 4 Applying Kirchhoff s Voltage Law (KVL) to the mesh consisting of the 0 Ω resistor, the Ω resistor and the dependent source to get + = 0 () Equations, and comprise a set of three simultaneous equations in the three unknown oltages, and. We can write these equations in matrix form as 0.5 0.5 0.5.5 0.5 0.5 = 0 0 We can sole this matrix equation using MATLAB: Hence = 4.096 V, = 6.849 V and = 0.9589 V

The power supplied by the 5 A current source is ( ) supplied by the.5 A current source is ( ) 5 = 5 4.096 = 0.548 W. The power.5 =.5 4.096 = 0.47 W. The power.5 =.5 4.096 0.9589 = 67.555 W. supplied by the dependent current source is ( ) ( )( ) Obseration: Changing the order of the 8 Ω resistor, the 0 Ω resistor and the two independent current sources only changes the order of the terms in the KCL equation at node a. We know that addition is commutatie, so change the order of the terms will not affect the alues of the oltages, and. For example, if the positions of the.5 A current source and 8 Ω resistor are swithched: The KCL equation at node a is Similarly, when the circuit is drawn as 5 =.5 + + + 0.5+ 0.5 =.5 8 0 The KCL equation at node a is 5 = + +.5 + 0.5+ 0.5 =.5 0 8 The changes do not affect the alues of the oltages, and.

Example: Determine the power supplied by each of the sources, independent and dependent, in this circuit: Solution: We ll begin by choosing the bottom node to be the reference node. Next we ll label the other nodes and some element currents: Notice that two 4 Ω resistors, an 8 Ω resistor and the two independent oltage sources are all connected in series. Consequently, the element currents of theses elements can be labeled so that they are equal. Similarly, a 4 Ω resistor and the dependent oltage source are connected in series so their currents can be labeled so as to be equal. The current in each resistor has been labeled so we can use Ohm s Law to calculate resistor oltages from the resistor currents and the resistances. Apply Kirchhoff s Voltage Law (KVL) to the left mesh to get 6 + 8i + 8i + 4i 5 + 4i = 0 6i + 8i = 9 () Apply Kirchhoff s Voltage Law (KVL) to the right mesh to get 4i + 5i 8i = 0 () Applying Kirchhoff s Current Law (KCL) at node a to get i = i + i i+ i + i = 0 () 4

Equations, and comprise a set of three simultaneous equations in the three unknown oltages, and. We can write these equations in matrix form as 6 8 0 i 9 5 8 4 i = 0 0 i We can sole this matrix equation using MATLAB: Hence i = 0.409 A, i = 0.068 A and i = 0.0 A The power supplied by the 5 V oltage source is ( ) supplied by the 6 V oltage source is i ( ) the dependent oltage source is ( i ) i ( )( ) 5i = 5 0.409 = 6.65 W. The power 6 = 6 0.409 =.4546 W. The power supplied by 5 = 5 0.068 0.0 = 0.569 W. 5

Obseration: Changing the order of the two 4 Ω resistors, an 8 Ω resistor and the two independent oltage sources in the left mesh changes the order of the terms in the KVL equation for that mesh. We know that addition is commutatie, so change the order of the terms will not affect the alues of the currents, and i. For example, when the circuit is drawn as i i The KVL equation for the left mesh is 6 5+ 8i + 4i + 8i + 4i = 0 6i + 8i = 9 When the circuit is drawn as The KVL equation for the left mesh is 4i + 4i + 8i + 6 5 + 8i = 0 6i + 8i = 9 These changes do not affect the alues of the currents, and i. i i 6