Super mesh Analysis in Network theory

A supermesh forms when two meshes have a common current source (dependent or independent). Consider a circuit as shown below in Figure 1 in which the current source branch is common between meshes 1 and 2 so remove the current source branch and supermesh forms as shown in Figure 2.

super mesh

 

super mesh

Procedure (steps) for applying mesh analysis:

  1. Identify the total number of meshes.
  2. Assign the mesh currents and check for supermesh in the circuit.
  3. If supermesh found, develop the KVL equation for it.
  4. Solve the equations to find the mesh currents.

Example

Example 1. For the given network, find current I using Mesh analysis.

Circuit theory Super mesh Analysis
Solution:

As shown above, Figure is given in example 1, 2 A current source is connected between meshes 1 and 2 so this problem is based on supermesh.

Step 1: – The total number of meshes is 2.

Step 2: – Let us assign mesh currents I1 and I2 for meshes 1 and 2 respectively as shown in Figure 1. As shown in Figure 1, 2 A current source should be removed from the circuit because 2 A current source is connected between meshes 1 and 2.

Super mesh Analysis

Figure 1.

Step 3: – The reduced circuit having supermesh shown in Figure 2.

Super mesh

Figure 2.

Apply KVL to supermesh

\[{\text{ – 4 + }}{I_1} + {I_2} + 2 = 0\]

${I_1} + {I_2} = 2$             ….(1)

Apply KCL to node 0,

\[{I_2} – {I_1} = 2{\text{ }}\]

${I_2} = {I_1} + 2$             ….(2)

Put equation (2) in equation (1), we get

\[{I_1} + {I_1} + 2 = 2\]

\[2{I_1} + 2 = 2\]

${I_1} = 0{\text{ A }}$         ….(3)

From Equation (1) ,

\[{I_1} + {I_2} = 2\]

Put equation (3) in equation (1), we get

\[0 + {I_2} = 2\]

\[{I_2} = 2\]

also \[I = {I_2}\]

Therefore,

\[I = 2{\text{ A}}{\text{.}}\]

 

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