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EENG223 Mesh Analysı s 1 Mesh Analysis Dr. M. K. Uyguroglu

Mesh Analysis - Eastern Mediterranean University · 2007. 3. 28. · 2 EENG223 Mesh Analysıs Mesh Analysis zNodal analysis was developed by applying KCL at each non-reference node

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  • EENG223 Mesh Analysıs1

    Mesh Analysis

    Dr. M. K. Uyguroglu

  • EENG223 Mesh Analysıs2

    Mesh Analysis

    Nodal analysis was developed by applying KCL at each non-reference node.Mesh analysis is developed by applying KVL around meshes/loops in the circuit.Mesh analysis results in a system of linear equations which must be solved for unknown currents.

  • EENG223 Mesh Analysıs3

    Mesh Analysis

    quantity of interest is currenta mesh is a loop that does not contain another loop within itwork for planar circuit onlyplanar circuit -> no branch passes over or under other branchM-meshes -> assign clockwise current for each meshapply KVL around each mesh

  • EENG223 Mesh Analysıs4

    Planar Circuit

    Nonplanar Circuit

  • EENG223 Mesh Analysıs5

    Steps of Mesh Analysis

    1. Identify meshes.2. Assign a current to each mesh.3. Apply KVL around each loop to get an

    equation in terms of the loop currents.4. Solve the resulting system of linear

    equations.

  • EENG223 Mesh Analysıs6

    Identifying the Meshes

    Mesh 2

    1kΩ

    1kΩ

    1kΩ

    V1 V2Mesh 1+–

    +–

  • EENG223 Mesh Analysıs7

    Steps of Mesh Analysis

    1. Identify mesh (loops).2. Assign a current to each mesh.3. Apply KVL around each loop to get an

    equation in terms of the loop currents.4. Solve the resulting system of linear

    equations.

  • EENG223 Mesh Analysıs8

    Assigning Mesh Currents

    1kΩ

    1kΩ

    1kΩ

    V1 V2I1 I2+–

    +–

  • EENG223 Mesh Analysıs9

    Steps of Mesh Analysis

    1. Identify mesh (loops).2. Assign a current to each mesh.3. Apply KVL around each loop to get an

    equation in terms of the loop currents.4. Solve the resulting system of linear

    equations.

  • EENG223 Mesh Analysıs10

    Voltages from Mesh Currents

    R

    I1

    + –VR

    VR = I1 R

    R

    I1

    + –VRI2

    VR = (I1 - I2 ) R

  • EENG223 Mesh Analysıs11

    KVL Around Mesh 1

    1kΩ

    1kΩ

    1kΩ

    V1 V2I1 I2+–

    +–

    + - +

    -

    -V1 + I1 1kΩ + (I1 - I2) 1kΩ = 0I1 1kΩ + (I1 - I2) 1kΩ = V1

  • EENG223 Mesh Analysıs12

    KVL Around Mesh 2

    1kΩ

    1kΩ

    1kΩ

    V1 V2I1 I2+–

    +–

    --

    +

    +

    (I2 - I1) 1kΩ + I2 1kΩ + V2 = 0(I2 - I1) 1kΩ + I2 1kΩ = -V2

  • EENG223 Mesh Analysıs13

    Steps of Mesh Analysis

    1. Identify mesh (loops).2. Assign a current to each mesh.3. Apply KVL around each loop to get an

    equation in terms of the loop currents.4. Solve the resulting system of linear

    equations.

  • EENG223 Mesh Analysıs14

    Matrix Notation

    The two equations can be combined into a single matrix/vector equation.

    =

    Ω+ΩΩ−

    Ω−Ω+Ω

    2

    1

    2

    1

    k1k1k1k1k1k1

    VV

    II

  • EENG223 Mesh Analysıs15

    Solving the Equations

    Let: V1 = 7V and V2 = 4VResults:

    I1 = 3.33 mAI2 = -0.33 mA

    FinallyVout = (I1 - I2) 1kΩ = 3.66V

  • EENG223 Mesh Analysıs16

    Another Example

    1kΩ

    2kΩ

    2kΩ

    12V 4mA

    2mA

    I0

    +–

  • EENG223 Mesh Analysıs17

    1. Identify Meshes

    Mesh 2

    Mesh 3

    Mesh 1

    1kΩ

    2kΩ

    2kΩ

    12V 4mA

    2mA

    I0

    +–

  • EENG223 Mesh Analysıs18

    2. Assign Mesh Currents

    I1 I2

    I31kΩ

    2kΩ

    2kΩ

    12V 4mA

    2mA

    I0

    +–

  • EENG223 Mesh Analysıs19

    Current Sources

    The current sources in this circuit will have whatever voltage is necessary to make the current correct.We can’t use KVL around the loop because we don’t know the voltage.What to do?

  • EEE 223 Mesh Analysıs20

    Current Sources

    The 4mA current source sets I2:I2 = -4 mA

    The 2mA current source sets a constraint on I1 and I3:

    I1 - I3 = 2 mAWe have two equations and three unknowns. Where is the third equation?

  • EENG223 Mesh Analysıs21

    1kΩ

    2kΩ

    2kΩ

    12V 4mA

    2mA

    I0

    I1 I2

    I3The Supermesh surrounds this source!

    The Supermesh

    does not include this

    source!

    +–

  • EENG223 Mesh Analysıs22

    KVL Around the Supermesh

    -12V + I3 2kΩ + (I3 - I2)1kΩ + (I1 - I2)2kΩ = 0

    I3 2kΩ + (I3 - I2)1kΩ + (I1 - I2)2kΩ = 12V

  • EENG223 Mesh Analysı s23

    Matrix Notation

    The three equations can be combined into a single matrix/vector equation.

    −=

    Ω+ΩΩ−Ω−Ω−

    V12mA2mA4

    1k2k2k1k2k101

    010

    3

    2

    1

    III

  • EENG223 Mesh Analysıs24

    Solve Using MATLAB

    >> A = [0 1 0; 1 0 -1;2e3 -1e3-2e3 2e3+1e3];

    >> v = [-4e-3; 2e-3; 12];>> i = inv(A)*vi = 0.0012

    -0.0040-0.0008

  • EENG223 Mesh Analysıs25

    Solution

    I1 = 1.2 mAI2 = -4 mAI3 = -0.8 mA

    I0 = I1 - I2 = 5.2 mA

  • EENG223 Mesh Analysıs26

    Class Example

    Mesh AnalysisMesh AnalysisMesh AnalysisPlanar CircuitSteps of Mesh AnalysisIdentifying the MeshesSteps of Mesh AnalysisAssigning Mesh CurrentsSteps of Mesh AnalysisVoltages from Mesh CurrentsKVL Around Mesh 1KVL Around Mesh 2Steps of Mesh AnalysisMatrix NotationSolving the EquationsAnother Example1. Identify Meshes2. Assign Mesh CurrentsCurrent SourcesCurrent SourcesKVL Around the SupermeshMatrix NotationSolve Using MATLABSolution