NETWORK THEORY MESH N SUPER MESH TOPIC REVIEW
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Transcript of NETWORK THEORY MESH N SUPER MESH TOPIC REVIEW
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TOPIC :-MESH AND SUPERMESH
ANALYSIS
SUBJECT :- NETWORK THEORYSUBMITTED BY :-
Sakshi Sathdeve (73)Shubham Korde (81)
Sudhanshu Nandurkar (81)
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Methods of Analysis
1. Mesh Analysis2. Supermesh
Analysis
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Process of Mesh Analysis1. Identify every mesh in the circuit.2. Label each mesh with a mesh
current. It is recommended that all mesh
currents be labeled in the same direction (either clockwise (CW) or counter-clockwise (CCW)).
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Mesh Analysis (Cont’d)4. Within a particular mesh of interest, use
Ohm’s law to express the voltage across any element within that mesh as the difference between the two mesh currents of continuous meshes shared by the element times the element impedance. The current within the mesh of interest is always considered to be larger than the rest of the mesh currents.
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Mesh Analysis (Cont’d)5. Apply KVL to sum all voltages in that
mesh of interest. The resulting algebraic equation (called mesh equation) has all mesh currents as its unknowns.
6. Repeat steps 4 and 5 until all meshes are accounted for. The number of equations must be equal to the number of mesh currents.
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Mesh Analysis (Cont’d)8. If a current source exists only in one
mesh, the mesh current is equal to the source current, and KVL is not applied to this mesh.
9. Solve the resulting simultaneous mesh equations to obtain the values of the unknown mesh currents.
10. Use the values of mesh currents above to find voltages and/or currents throughout the rest of the circuit.
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Example
DC
DC
1R
3R5R
7R
2R
6R
8R
4R
1v 2v
3v 4v
5v 6v7v
8v
+ +
+ +
++
+
+
-
-- -
-
--
-
1sV
2sV 1i 2i
3i 4i
Number of nodes, n = 7
Number of branches, b = 10
Number of loops, l = 4
1l b n
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Example
Apply KVL to each mesh
2 1 7 5 0sV v v v
2 6 7 0v v v
15 3 0sv v v
Mesh 1:
Mesh 2:
Mesh 3:
14 8 6 0sv v V v Mesh 4:
DC
DC
1R
3R5R
7R
2R
6R
8R
4R
1v 2v
3v 4v
5v 6v7v
8v
+ +
+ +
++
+
+
-
-- -
-
--
-
1sV
2sV 1i 2i
3i 4i
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2 1 1 1 2 7 1 3 5( ) ( ) 0sV i R i i R i i R
2 2 2 4 6 2 1 7( ) ( ) 0i R i i R i i R
13 1 5 3 3( ) 0si i R V i R
Mesh 1:
Mesh 2:
Mesh 3:
14 4 4 8 4 2 6( ) 0si R i R V i i R Mesh 4:
Mesh 1:
Mesh 2:
Mesh 3:
Mesh 4:
21 5 7 1 7 2 5 3( ) sR R R i R i R i V
7 1 2 6 7 2 6 4( ) 0R i R R R i R i
15 1 3 5 3( ) sR i R R i V
16 2 4 6 8 4( ) sR i R R R i V
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Mesh 1:
Mesh 2:
Mesh 3:
Mesh 4:
21 5 7 1 7 2 5 3( ) sR R R i R i R i V
7 1 2 6 7 2 6 4( ) 0R i R R R i R i
15 1 3 5 3( ) sR i R R i V
16 2 4 6 8 4( ) sR i R R R i V
2
1
1
1 5 7 7 5 1
7 2 6 7 6 2
5 3 5 3
6 4 6 8 4
000
0 00 0
s
s
s
VR R R R R iR R R R R i
VR R R iR R R R i V
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SupermeshIf a current source exists between two
contiguous meshes, the two meshes are collapsed into a single mesh called a supermesh, and the current source and any elements connected in series with it removed. However, KVL must still be satisfied within a supermesh using the old mesh current labels. Also, the removal of the current source provides another mesh equation.
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Contd…
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Properties of a Supermesh1. The current is not completely ignored
provides the constraint equation necessary to solve for the mesh current.
2. Several current sources in adjacency form a bigger supermesh.
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620146
21
21
iiii
If a supermesh consists of two meshes, two equations are needed; one is obtained using KVL and Ohm’s law to the supermesh and the other is obtained by relation regulated due to the current source.
Example
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Similarly, a supermesh formed from three meshes needs three equations: one is from the supermesh and the other two equations are obtained from the two current sources.
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0102)(8
506)(842
443
432
21
24331
iiiiii
iiiiiii
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THANK YOU