Lesson 7 Basic Laws of Electric Circuits Mesh Analysis.

Slides:



Advertisements
Similar presentations
Basic Laws of Electric Circuits Kirchhoff’s Voltage Law
Advertisements

Voltage and Current Division
ECE 201 Circuit Theory I1 Assessment Problem # 4.12 Mesh-Current Method Special Case Current Source in a branch.
© The McGraw-Hill Companies, Inc McGraw-Hill 1 PRINCIPLES AND APPLICATIONS OF ELECTRICAL ENGINEERING THIRD EDITION G I O R G I O R I Z Z O N I C.
1 ECE 221 Electric Circuit Analysis I Chapter 5 Branch Currents Herbert G. Mayer, PSU Status 1/5/2015.
Kirchhoff's Rules Continued
EE2010 Fundamentals of Electric Circuits Lecture - 6 Voltage Sources, Current Sources, Mesh Analysis.
DC CIRCUIT ANALYSIS: NODE AND MESH METHOD
1 Lecture 2 Dr Kelvin Tan Electrical Systems 100.
Lecture 21 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Basic Laws of Electric Circuits
Chapter 3 Methods of Analysis
Basic Electric Circuits Thevenin’s and Norton’s
Lesson 5 Basic Laws of Electric Circuits Equivalent Resistance.
Methods of Analysis PSUT 1 Basic Nodal and Mesh Analysis Al-Qaralleh.
3.6 The Mesh-Current Method Figure 3.21 Illustrations of the concept of a mesh. A mesh is a circuit loop that does not enclose any elements The mesh currents.
Dr. Jie ZouPHY Chapter 28 Direct Current Circuits (Cont.)
Section 06. Multiple Sources What if more than one source in the circuit? How to solve for all currents? Slide 2.
Chapter 8 Methods of Analysis. 2 Constant Current Sources Maintains same current in branch of circuit –Doesn’t matter how components are connected external.
Methods of Analysis Eastern Mediterranean University 1 Methods of Analysis Mustafa Kemal Uyguroğlu.
Chapter 26 DC Circuits. I Junction rule: The sum of currents entering a junction equals the sum of the currents leaving it Kirchhoff’s Rules.
1 Chapter 3 Methods of Analysis Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 Mesh Analysis Discussion D2.4 Chapter 2 Section 2-8.
Chapter 3 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 Chapter 3 Methods of Analysis Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
The second systematic technique to determine all currents and voltages in a circuit IT IS DUAL TO NODE ANALYSIS - IT FIRST DETERMINES ALL CURRENTS IN A.
Chapter 8 Methods of Analysis. Constant Current Sources Maintains the same current in the branch of the circuit regardless of how components are connected.
RESISTIVE CIRCUITS MULTI NODE/LOOP CIRCUIT ANALYSIS.
BYST Circuit -F2003: Nodal and Mesh Analysis 92 CPE220 Electric Circuit Analysis Chapter 3: Nodal and Mesh Analyses.
METHODS OF CIRCUIT ANALYSIS
Lecture - 5 Nodal analysis. Outline Terms of describing circuits. The Node-Voltage method. The concept of supernode.
305221, Computer Electrical Circuit Analysis การวิเคราะห์วงจรไฟฟ้าทาง คอมพิวเตอร์ 3(2-3-6) ณรงค์ชัย มุ่งแฝงกลาง คมกริช มาเที่ยง สัปดาห์ที่ 3 Nodal.
1 © Unitec New Zealand DE4401&APTE 5601 Topic 4 N ETWORK A NALYSIS.
CIRCUITS and SYSTEMS – part I Prof. dr hab. Stanisław Osowski Electrical Engineering (B.Sc.) Projekt współfinansowany przez Unię Europejską w ramach Europejskiego.
LOOP ANALYSIS The second systematic technique to determine all currents and voltages in a circuit IT IS DUAL TO NODE ANALYSIS - IT FIRST DETERMINES ALL.
Chapter 8 – Methods of Analysis Lecture 10 by Moeen Ghiyas 05/12/
Circuit Theory Chapter 2 Basic Laws
University Physics: Waves and Electricity Ch27. Circuit Theory Lecture 11 Dr.-Ing. Erwin Sitompul
1 Loop (Mesh) Analysis. 2 Loop Analysis Nodal analysis was developed by applying KCL at each non-reference node. Loop analysis is developed by applying.
University Physics: Waves and Electricity Ch27. Circuit Theory Lecture 11 Dr.-Ing. Erwin Sitompul
Mesh Analysis Introducing Supermeshes!!!. Mesh Analysis A mesh is a loop with no other loops within it; an independent loop. Mesh analysis provides another.
Lecture-5. Md.Kausher ahmed Electrical department.
Ch 3: Methods of Analysis
The second systematic technique to determine all currents and voltages in a circuit IT IS DUAL TO NODE ANALYSIS - IT FIRST DETERMINES ALL CURRENTS IN A.
CHAPTER 3 Resistive Network Analysis. Figure Branch current formulation in nodal analysis.
Techniques of Circuit Analysis 1 Electrical Circuits CEN270.
E E 1205 Lecture 08 -Mesh Current Analysis. Introduction to Mesh Current Method More direct than branch equations Fewer equations to solve Express all.
Method 2a: KVL & KCL Kirchhoff’s Voltage Law (KVL)
RESISTORS IN SERIES - In a series circuit, the current is the same
EKT101 Electric Circuit Theory
KITRC CIRCUIT & NETWORKS MADE BY AGNA PATEL:
Additional Circuit Analysis Techniques
Chapter 3 Methods of Analysis
By: Patel Pratik ( ) Patel Sandip( )
EGR 2201 Unit 4 Mesh Analysis Read Alexander & Sadiku, Sections 3.4 to Homework #4 and Lab #4 due next week. Quiz next week. Handouts: Quiz 3, Unit.
Resistance Year 9 Science.
Part B - Mesh Analysis Ch. 3 – Methods of Analysis Based on KVL
Alexander-Sadiku Fundamentals of Electric Circuits
Ch. 3 – Methods of Analysis
University Physics: Waves and Electricity
Basic Laws of Electric Circuits
C H A P T E R 3 Resistive Network Analysis.
Chapter 9.
Lecture 02 -Mesh Current Analysis
The Mesh Current Method
Basic Laws of Electric Circuits Equivalent Resistance
Basic Laws of Electric Circuits
Basic Laws of Electric Circuits
طرق تحليل الدوائر الكهربائية
Chapter 3 – Methods of Analysis
Presentation transcript:

Lesson 7 Basic Laws of Electric Circuits Mesh Analysis

Basic Circuits Mesh Analysis: Basic Concepts:  In formulating mesh analysis we assign a mesh current to each mesh.  Mesh currents are sort of fictitious in that a particular mesh current does not define the current in each branch of the mesh to which it is assigned.

Basic Circuits Mesh Analysis: Basic Concepts: Figure 7.2: A circuit for illustrating mesh analysis. Eq 7.1 Around mesh 1:

Basic Circuits Mesh Analysis: Basic Concepts: Eq 7.2 Eq 7.3 Eq 7.4

Basic Circuits Mesh Analysis: Basic Concepts: We are left with 2 equations: From (7.1) and (7.4) we have, Eq 7.5 Eq 7.6 We can easily solve these equations for I 1 and I 2.

Basic Circuits Mesh Analysis: Basic Concepts: The previous equations can be written in matrix form as: Eq (7.7) Eq (7.8)

Basic Circuits Mesh Analysis: Example 7.1. Write the mesh equations and solve for the currents I 1, and I 2. Figure 7.2: Circuit for Example 7.1. Mesh 1 4I 1 + 6(I 1 – I 2 ) = Mesh 2 6(I 2 – I 1 ) + 2I 2 + 7I 2 = Eq (7.9) Eq (7.10)

Basic Circuits Mesh Analysis: Example 7.1, continued. Simplifying Eq (7.9) and (7.10) gives, 10I 1 – 6I 2 = 8 -6I I 2 = 22 Eq (7.11) Eq (7.12) » % A MATLAB Solution » » R = [10 -6;-6 15]; » » V = [8;22]; » » I = inv(R)*V I = I 1 = I 2 =

Basic Circuits Mesh Analysis: Example 7.2 Solve for the mesh currents in the circuit below. Figure 7.3: Circuit for Example 7.2. The plan: Write KVL, clockwise, for each mesh. Look for a pattern in the final equations.

Basic Circuits Mesh Analysis: Example 7.2 Mesh 1: 6I (I 1 – I 3 ) + 4(I 1 – I 2 ) = Mesh 2: 4(I 2 – I 1 ) + 11(I 2 – I 3 ) + 3I 2 = Mesh 3: 9I (I 3 – I 2 ) + 10(I 3 – I 1 ) = Eq (7.13) Eq (7.14) Eq (7.15)

Basic Circuits Mesh Analysis: Example 7.2 Clearing Equations (7.13), (7.14) and (7.15) gives, 20I 1 – 4I 2 – 10I 3 = 30 -4I I 2 – 11I 3 = I 1 – 11I I 3 = 20 In matrix form: WE NOW MAKE AN IMPORTANT OBSERVATION!! Standard Equation form

Basic Circuits Mesh Analysis: Standard form for mesh equations Consider the following: R 11 = of resistance around mesh 1, common to mesh 1 current I 1. R 22 = of resistance around mesh 2, common to mesh 2 current I 2. R 33 = of resistance around mesh 3, common to mesh 3 current I 3.

Basic Circuits Mesh Analysis: Standard form for mesh equations R 12 = R 21 = - resistance common between mesh 1 and 2 when I 1 and I 2 are opposite through R 1,R 2. R 13 = R 31 = - resistance common between mesh 1 and 3 when I 1 and I 3 are opposite through R 1,R 3. R 23 = R 32 = - resistance common between mesh 2 and 3 when I 2 and I 3 are opposite through R 2,R 3. = sum of emf around mesh 1 in the direction of I 1. = sum of emf around mesh 2 in the direction of I 2. = sum of emf around mesh 3 in the direction of I 3.

Basic Circuits Mesh Analysis: Example Direct method. Use the direct method to write the mesh equations for the following. Figure 7.4: Circuit diagram for Example 7.3. Eq (7.13)

Basic Circuits Mesh Analysis: With current sources in the circuit Example 7.4: Consider the following: Figure 7.5: Circuit diagram for Example 7.4. Use the direct method to write the mesh equations.

Basic Circuits Mesh Analysis: With current sources in the circuit This case is explained by using an example. Example 7.4: Find the three mesh currents in the circuit below. Figure 7.5: Circuit for Example 7.4. When a current source is present, it will be directly related to one or more of the mesh current. In this case I 2 = -4A.

Basic Circuits Mesh Analysis: With current sources in the circuit Example 7.4: Continued. An easy way to handle this case is to remove the current source as shown below. Next, write the mesh equations for the remaining meshes. Note that I 2 is retained for writing the equations through the 5  and 20  resistors.

Basic Circuits Mesh Analysis: With current sources in the circuit Example 7.4: Continued. Equation for mesh 1: 10I 1 + (I 1 -I 2 )5 = 10 or 15I 1 – 5I 2 = 10 Equations for mesh 2: 2I 3 + (I 3 -I 2 )20 = 20 or - 20I I 3 = 20 Constraint Equation I 2 = - 4A

Basic Circuits Mesh Analysis: With current sources in the circuit Example 7.4: Continued. Express the previous equations in Matrix form: I 1 = A I 2 = - 4 A I 3 = A

End of Lesson 7 circuits Mesh Analysis