In this method, we set up and solve a system of equations in which the unknowns are the voltages at the principal nodes of the circuit. From these nodal voltages the currents in the various branches of the circuit are easily determined. The steps in the nodal analysis method are:
For example, for the node to the right KCL yields the equation:
Ia + Ib + Ic = 0
Express the current in each branch in terms of the nodal voltages at each end of the branch using Ohm’s Law (I = V / R). Here are some examples:
The current downward out of node 1 depends on the voltage
difference V1 - V3 and the resistance in the
branch.
In this case the voltage difference across the resistance is
V1 - V2 less the voltage across the voltage
source. Thus the downward current is as
shown.
In this case the voltage difference across the resistance
must be 100 volts greater than the difference V1 - V2. Thus
the downward current is as shown.The result, after simplification, is a system of m linear equations in the m unknown nodal voltages (where m is one less than the number of nodes; m = n - 1). The equations are of this form:
where G11, G12, . . . , Gmm and I1, I2, . . . , Im are constants.
Alternatively, the system of equations can be gotten (already in simplified form) by using the inspection method.
Use nodal analysis to find the voltage at each node of this circuit.
We will number the nodes as shown to the right.
node 1 and the second equation results from KCL applied at node 3. Collecting terms this becomes:
This form for the system of equations could have been gotten immediately by using the inspection method.
Use nodal analysis to find the voltage at each node of this circuit.
Use nodal analysis to find the voltage at each node of this circuit.
Written by Eric Hiob, Tuesday, December 31, 1996