Electronics/Mesh Analysis
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[edit] Meshes
A 'mesh' (also called a loop) is simply a path through a circuit that starts and ends at the same place. For the purpose of mesh analysis, a mesh is a loop that does not enclose other loops.
[edit] Mesh Analysis
Similar to nodal analysis, mesh analysis is a formalized procedure based on KVL equations. A caveat: mesh analysis can only be used on 'planar' circuits (i.e. there are no crossed, but unconnected, wires in the circuit diagram.)
Steps:
1. Draw circuit in planar form (if possible.)
2. Identify meshes and name mesh currents. Mesh currents should be in the clockwise direction. The current in a branch shared by two meshes is the difference of the two mesh currents.
3. Write a KVL equation in terms of mesh currents for each mesh.
4. Solve the resulting system of equations.
[edit] Complication in Mesh Analysis
1. Dependent Voltage Sources
Solution: Same procedure, but write the dependency variable in terms of mesh currents.
2. Independent Current Sources
Solution: If current source is not on a shared branch, then we have been given one of the mesh currents! If it is on a shared branch, then use a 'super-mesh' that encircles the problem branch. To make up for the mesh equation you lose by doing this, use the mesh current relationship implied by the current source (i.e. I2 − I1 = 4mA).
3. Dependent Current Sources
Solution: Same procedure as for an independent current source, but with an extra step to eliminate the dependency variable. Write the dependency variable in terms of mesh currents.
[edit] Example
Given the Circuit below, find the currents I1, I2.

The circuit has 2 loops indicated on the diagram. Using KVL we get:
Loop1: 0 = 9 - 1000I1 - 3000(I1 - I2)
Loop2: 0 = 3000(I1 - I2) - 2000I2 - 2000I2
Simplifying we get the simultaneous equations:
0 = 9 - 4000I1 + 3000I2
0 = 0 + 3000I1 - 7000I2
solving to get:
I1 = 3.32mA
I2 = 1.42mA