The document discusses the technique of mesh analysis for solving circuits. It begins by defining mesh analysis as applying Kirchhoff's voltage law around loops in a circuit to obtain equations relating loop currents. It then outlines the steps of mesh analysis as: 1) identifying meshes, 2) assigning currents to meshes, 3) applying KVL to obtain equations, 4) solving the resulting system of equations. Examples are provided to demonstrate identifying meshes, assigning currents, writing KVL equations, and setting up the matrix equations to solve.
The difference between mesh and nodal analysis is that nodal analysis is an application of Kirchhoff's current law, which is used for calculating the voltages at each node in an equation. While mesh analysis is an application of Kirchhoff's voltage law which is used for calculating the current.
THIS PPT IS MAINLY BASED ON ELECTRICAL CIRCUIT ANALYSIS PROBLEM AND THIS PPT ALSO SOLVED THEORETICALLY AND SOLVED BY USING THE MATLAB SOFTWARE AND THIS ALSO CONTAINS THE CODE AND RESULTS ARE ALSO THERE.SO THIS IS USEFUL
The difference between mesh and nodal analysis is that nodal analysis is an application of Kirchhoff's current law, which is used for calculating the voltages at each node in an equation. While mesh analysis is an application of Kirchhoff's voltage law which is used for calculating the current.
THIS PPT IS MAINLY BASED ON ELECTRICAL CIRCUIT ANALYSIS PROBLEM AND THIS PPT ALSO SOLVED THEORETICALLY AND SOLVED BY USING THE MATLAB SOFTWARE AND THIS ALSO CONTAINS THE CODE AND RESULTS ARE ALSO THERE.SO THIS IS USEFUL
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2. EENG223 Mesh Analysıs
2
Mesh Analysis
z Nodal analysis was developed by applying
KCL at each non-reference node.
z Mesh analysis is developed by applying KVL
around meshes/loops in the circuit.
z Mesh analysis results in a system of linear
equations which must be solved for unknown
currents.
3. EENG223 Mesh Analysıs
3
Mesh Analysis
z quantity of interest is current
z a mesh is a loop that does not contain
another loop within it
z work for planar circuit only
planar circuit -> no branch passes over or
under other branch
z M-meshes -> assign clockwise current for
each mesh
z apply KVL around each mesh
5. EENG223 Mesh Analysıs
5
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.
7. EENG223 Mesh Analysıs
7
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.
9. EENG223 Mesh Analysıs
9
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.
13. EENG223 Mesh Analysıs
13
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.
14. EENG223 Mesh Analysıs
14
Matrix Notation
z The two equations can be combined into a
single matrix/vector equation.
−
=
Ω
+
Ω
Ω
−
Ω
−
Ω
+
Ω
2
1
2
1
k
1
k
1
k
1
k
1
k
1
k
1
V
V
I
I
15. EENG223 Mesh Analysıs
15
Solving the Equations
Let: V1 = 7V and V2 = 4V
Results:
I1 = 3.33 mA
I2 = -0.33 mA
Finally
Vout = (I1 - I2) 1kΩ = 3.66V
19. EENG223 Mesh Analysıs
19
Current Sources
z The current sources in this circuit will have
whatever voltage is necessary to make the
current correct.
z We can’t use KVL around the loop because
we don’t know the voltage.
z What to do?
20. EEE 223 Mesh Analysıs
20
Current Sources
z The 4mA current source sets I2:
I2 = -4 mA
z The 2mA current source sets a constraint on
I1 and I3:
I1 - I3 = 2 mA
z We have two equations and three unknowns.
Where is the third equation?