Transcript
  • Analysis Methods Overview

    Solving Linear Equations

    Nodal Analysis

    Supernodes (Nodal Analysis with Voltage Sources)

    Mesh Analysis

    Supermeshes (Mesh Analysis with Current Sources)

    This is a very important chapter.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 1

  • Review of Basic Concepts: Current

    i4 i5i3i2i1

    What goes in, has to come out

    Kirchhoffs current law

    Similar to conservation of mass

    Conservation of electrons

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 2

  • Review of Basic Concepts: Voltage

    10 V-

    +

    -

    ++ - + -

    2 k2 k

    5 k 7 kv1 v2

    v3 v4

    The voltage drop from one node to another is the same, nomatter what path is chosen

    Kirchhoffs voltage law

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 3

  • Resistors in Parallel with Voltage Sources

    CircuitRVs vo-

    +

    CircuitVs vo-

    +

    What is vo in each case?

    What effect does the resistor have on the current pumped into thecircuit?

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 4

  • Resistors in Series with Current Sources

    CircuitIs CircuitIs

    Rio

    io

    What is io in each case?

    What effect does the resistor have on the voltage seen by thecircuit?

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 5

  • Solving Linear Equations

    Much of our circuit analysis will focus on finding a set of linearequations and solving these equations

    Need as many equations as there are unknowns

    Three possible approaches

    Algebra (elimination, substitution, etc.)

    Cramers rule

    Linear algebra

    Last is easiest and least susceptible to errors

    Requires use your scientific calculators

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 6

  • Example 1: Solving Linear Equations

    i1 = i2 + i3

    i4 = i3 + 2m

    10 = (1k)i1 + (5k)i2

    (5k)i2 = (2k)i3 + (10k)i4

    Rewrite so variables are in consistent order on left side and constantsare on the right side

    i1 i2 i3 = 0 i3 + i4 = 2m

    (1k)i1 + (5k)i2 = 10+ (5k)i2 (2k)i3 (10k)i4 = 0

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 7

  • Example 1: Continued (1)

    i1 i2 i3 = 0 i3 + i4 = 2m

    (1k)i1 + (5k)i2 = 10+ (5k)i2 (2k)i3 (10k)i4 = 0

    In Matrix form this becomes

    1 1 1 00 0 1 11k 5k 0 00 5k 2k 10k

    i1

    i2

    i3

    i4

    =

    02m100

    or

    Ai = b

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 8

  • Example 1: Continued (2)

    Ai = b where

    A =

    1 1 1 00 0 1 11k 5k 0 00 +5k 2k 10k

    i =

    i1

    i2

    i3

    i4

    b =

    02m100

    Your calculator should be able to solve this directly

    You should only need to enter A and b

    Your calculator will return a vector i

    Simultaneously solves for all the unknown variables

    Much faster than Cramers rule or brute-force algrebra

    Read the manuals for your calculators

    This will save you time (homework & exams) and reduce errors

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 9

  • Example 1: Continued (3)

    Linear Equations:1 1 1 00 0 1 11k 5k 0 00 5k 2k 10k

    i1

    i2

    i3

    i4

    =

    02m100

    Calculator should return:

    i1

    i2

    i3

    i4

    =

    +0.909+1.8180.909+1.091

    mA

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 10

  • Network Terminology

    Planar Circuit A circuit that can be drawn on a plane with nocrossing branches

    Node Point or portion of a circuit where 2 or more elements arejoined

    Essential Node Point or portion of a circuit where 3 or moreelements are joined

    Branch Path that connects 2 nodes

    Essential Branch Path that connects 2 essential nodes w/o passingthrough an essential node

    Loop Path with last node same as starting node that does not crossitself

    Mesh Loop that does not enclose any other loops

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 11

  • Example 2: Terminology

    20 V 2 A

    R1 R2

    R3 R4 R4

    R6 R7 R8

    35ip

    ip

    Identify the following informationNodes: Essential Nodes:Branches: Essential Branches:EBs with Unknown Current: Meshes:

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 12

  • Example 3: Circuit Analysis The Hard Way

    10 V

    i1 i3

    i2 i42 mA

    1 k 2 k

    5 k 10 k

    Can solve with KCL & KVL. Four unknowns.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 13

  • Nodal Analysis: Introduction

    There is an another way to solve for currents and voltages

    Easier

    More methodical

    Still based on Ohms law, KVL, & KCL

    Nodal analysis is one of two key methods

    Mesh analysis is the other

    We will discuss nodal analysis first

    Based on KCL

    Must understand terminology introduced earlier

    Use to solve for voltages

    All voltages have a common reference point

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 14

  • Nodal Analysis Steps

    1. Identifiy essential nodes

    2. Pick a reference node

    3. Label all other essential nodes

    4. Apply KCL to all labelled nodes

    5. Solve linear equations for all node voltages

    6. Solve for variables of interest

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 15

  • Nodal Analysis: Step 1 Identify Essential Nodes

    10 V 2 mA

    1 k 2 k

    5 k 10 k

    Some essential nodes may include portions of the circuit (pieces ofwire)

    Circle the entire node to prevent errors

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 16

  • Nodal Analysis: Step 2 Pick a Reference

    10 V 2 mA

    1 k 2 k

    5 k 10 k

    Second step is to pick a reference node

    Is often easiest to choose the node that interconnects the mostbranches

    Must be an essential node

    Usually is at bottom of circuit

    Label with the same symbol used for ground

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 17

  • Nodal Analysis: Step 3 Label Other Essential Nodes

    10 V 2 mA

    1 k 2 k

    5 k 10 k

    Also a bit easier if voltages are labeled

    All voltages are measured relative to the reference node

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 18

  • Nodal Analysis: Step 4 Apply KCL All Labeled Nodes

    10 V 2 mA

    1 2

    -

    +

    v2-

    +

    v1

    1 k 2 k

    5 k 10 k

    50 k

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 19

  • Nodal Analysis: Step 5 Solve Linear Equations

    Linear Equations:

    Solution (from calculator):

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 20

  • Nodal Analysis: Step 6 Solve for Variables of Interest

    10 V 2 mA

    1 2

    -

    +

    v2-

    +

    v1

    i1 i3

    i2 i4

    1 k 2 k

    5 k 10 k

    50 k

    i1 =

    i2 =

    i3 =

    i4 =

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 21

  • Nodal Analysis: Review of Steps

    1. Identify essential nodes

    2. Pick a reference

    Must be an essential node

    Always label with the ground symbol

    Best to pick essential node with most branches

    Often at the bottom of the circuit diagram

    3. Label other essential nodes

    4. Apply KCL to all labelled nodes except reference node

    5. Solve linear equations

    Generates voltage at each node (relative to reference node)

    6. Solve for variables of interest

    Usually easy after Step 5

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 22

  • Nodal Analysis: Use of Laws

    All three laws are used

    KCL is applied at each labelled node except the reference node

    Ohms law is used to determine the current in branches thatcontain resistors

    KVL is used to determine the voltage drop across the resistors

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 23

  • Example 4: Nodal Analysis

    144 V-

    +

    v2-

    +

    v1 3 A

    4

    5 10

    80

    Solve for v1 and v2.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 24

  • Example 4: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 25

  • Example 5: Nodal Analysis

    20 mA-

    +

    v2-

    +

    v1-

    +

    v3 5 V2 k

    2.7 k2.7 k

    3.3 k

    4.7 k

    10 k

    Solve for v1, v2, and v3.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 26

  • Example 5: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 27

  • Example 6: Dependent Voltage Source

    50 V-

    +

    10

    10

    30 39 78

    80 k

    v/5

    v

    Solve for v.

    What effect does the 10 resistor have on the circuit?

    What is the current flowing through the dependent source?

    How can we apply KCL at the essential nodes without thisinformation?

    Ans: One extra variable

    Implies we need an extra equation

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 28

  • Example 6: Continued

    50 V-

    +

    10

    10

    30 39 78

    100 k

    v/5

    v

    Solve for v.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 29

  • Example 6: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 30

  • Nodal Analysis and Supernodes

    Supernodes eliminate the need to introduce an extra variable(unknown current)

    Necessary when a voltage source is between two labeled nodes(excluding reference node)

    Still need to use voltage source to generate one of the equations

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 31

  • Example 7: Dependent Source Continued

    50 V-

    +

    10

    10

    30 39 78

    160 k

    v/5

    v

    Solve for v. Use a supernode.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 32

  • Example 7: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 33

  • Example 8: Dependent Voltage Source

    20 V

    + -

    1 2 4

    20 40 80 3.125v

    v

    35i

    i

    Find the power developed by the 20 V source.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 34

  • Example 8: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 35

  • Example 9: Nodal Analysis

    11 mA

    i1

    20 Vi2

    10 Vi3

    250

    500

    1 k

    25 k

    Solve for i1, i2, and i3.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 36

  • Example 9: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 37

  • Example 10: Nodal Analysis

    1 A

    3i

    i

    -

    +

    v

    1

    1

    2

    2 4

    Solve for v.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 38

  • Example 10: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 39

  • Mesh Analysis: Introduction

    Recall: There is an easier way to solve for currents and voltagesthan applying KVL and KCL directly

    Nodal analysis is one of two key methods

    Mesh analysis is the other

    Applies KVL to solve for currents

    More abstract

    Work with imaginary currents

    Only applies to planar circuits

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 40

  • Mesh Analysis: Step 1 Label Meshes

    40 V 64 V

    ia

    ic

    ib

    1.5 2

    3 4

    45

    Find the branch currents ia, ib, and ic.

    Recall: A mesh is a loop that does not enclose any other loops

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 41

  • Mesh Analysis: Step 2 Apply KVL to Each Mesh

    40 V 64 V

    ia

    ic

    ib

    1.5 2

    3 4

    45

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 42

  • Mesh Analysis: Step 3 Solve Linear Equations[50 4545 50.5

    ] [i1

    i2

    ]=

    [4064

    ]

    i1 = 9.8 A

    i2 = 10 A

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 43

  • Mesh Analysis: Step 4 Solve for Variables of Interest

    40 V 64 V

    ia

    ic

    ib

    1.5 2

    3 4

    45

    ia =

    ib =

    ic =

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 44

  • Mesh Analysis: Review of Steps

    Step 1 Label Meshes

    Step 2 Apply KVL to Each Mesh

    Step 3 Solve Linear Equations

    Step 4 Solve for Variables of Interest

    Usually easy after Step 3

    Limitation: Only works with planar circuits

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 45

  • Example 11: Mesh Analysis

    12 V

    110 V 70V

    2

    3

    4

    6

    10 12

    Find the total power developed in the circuit.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 46

  • Example 11: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 47

  • Example 12: Mesh Analysis

    18 V 15 V3 A

    2

    3

    6

    9

    Find the total power dissipated.

    Problem: What is the voltage across the 3 A source?

    Solutions

    1 Add it as a variable

    2 Use a supermesh

    Second option requires less work

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 48

  • Example 12: Mesh Analysis

    18 V 15 V3 A

    2

    3

    6

    9

    Find the total power dissipated. Add a variable.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 49

  • Example 12: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 50

  • Example 13: Mesh Analysis

    18 V 15 V3 A

    2

    3

    6

    9

    Find the total power dissipated. Use a supermesh.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 51

  • Example 13: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 52

  • Example 14: Mesh Analysis

    200 V

    4.3 id

    ie

    ib

    id

    ia

    ic

    10

    10

    25

    50

    100

    Find the branch currents ia ie.

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 53

  • Example 14: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 54

  • Example 15: Mesh Analysis

    1.5 mA

    8 V

    2 k

    3 k

    4 k

    4 k 4 k

    5 k

    7 k

    3i

    i

    Solve for i

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 55

  • Example 15: Workspace

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 56

  • Nodal versus Mesh Analysis

    You should know how to do both

    Which is more efficient depends on the problem

    Will learn which to use with experience

    Nodal analysis used more often

    On exams, I will specify which method to use

    Concise Summary:

    Nodal Analysis Mesh AnalysisMethod KCL KVLSolve For Node Voltages Mesh CurrentsSuper Conditions Voltage Sources Current Sources

    J. McNames Portland State University ECE 221 Analysis Methods Ver. 1.68 57


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