Kirchhoff's voltage law (KVL) is the foundation of mesh analysis. The validity of KVL for ac circuit may be demonstrated in the
Mesh Analysis for dc circuit page.
Keep in mind that mesh analysis is intended to be used on a planar circuit.
Planar circuits are circuits that can be drawn on a plane surface with no wires crossing each other.
Before examining the application of the method to ac networks, the student should first review the appropriate sections on mesh analysis in Chapter 6 since the content of this section will be limited to the general conclusions of
Chapter 6.
The general approach to mesh analysis for independent sources includes the same sequence of steps appearing in Chapter 6. In fact,
throughout this section the only change from the dc coverage will be to
substitute impedance for resistance and admittance for conductance in
the general procedure.
- Assign a distinct current in the clockwise direction to each
independent closed loop of the network. It is not absolutely
necessary to choose the clockwise direction for each loop current.
However, it eliminates the need to have to choose a direction for
each application. Any direction can be chosen for each loop
current with no loss in accuracy as long as the remaining steps are
followed properly.
- Indicate the polarities within each loop for each impedance as
determined by the assumed direction of loop current for that loop.
- Apply Kirchhoff's voltage law around each closed loop in the
clockwise direction. Again, the clockwise direction was chosen to
establish uniformity and to prepare us for the format approach to
follow.
- If an impedance has two or more assumed currents through it,
the total current through the impedance is the assumed current
of the loop in which Kirchhoff's voltage law is being applied,
plus the assumed currents of the other loops passing through in
the same direction, minus the assumed currents passing
through in the opposite direction.
- The polarity of a voltage source is unaffected by the direction of
the assigned loop currents.
- Solve the resulting simultaneous linear equations for the assumed
loop currents.
The technique is applied as above for all networks with independent
sources or for networks with dependent sources where the controlling
variable is not a part of the network under investigation. If the controlling variable is part of the network being examined, a method to be
described shortly must be applied.
Example 1: find the
current $I_1$ in
[Fig. 1] using mesh analysis.
Fig. 1: Example 1.
View Solution
Example 2: Write the mesh currents for the network of
[Fig. 3] having a dependent voltage source.
Fig. 3: Applying mesh analysis to a network with a voltage-controlled voltage source.
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