Nodal Analysis of Electric Circuit

Nodal Analysis Nodal analysis is the general technique for analysing an electric circuit and it is based on Krichhoff’s Current law (KCL) which states that the sum of all current entering into a node is equal to the total current leaving from a node. In nodal analysis we are interested in finding node voltages. Choosing node voltage rather than voltage across elements as a circuit variable is convenient and it reduces the number of equations to be solved. In nodal analysis we have to write KCL equations for each non reference node. The number of equations derived for a circuit having n number of nodes is (n – 1).

Nodal Analysis with Current Source The process of a nodal analysis of an electric circuit having current source involves the following steps to be taken Step 1 Identify the total number of nodes in the given electric circuit. A node is point in electric circuit where two or more than two branches are connected.

For example refer the given figure.

Step 2 Out of all the nodes, designate a node as a reference node. A reference node a common node for all the other node against which node voltages of all the nodes measured. Generally, the ground is taken as reference node.

Step 3 Assign unknown voltage variables to all non-reference nodes.

Step 4 Develop KCL equations for each non reference node ( i.e. the sum of current coming towards the node is equal to the sum of current going outwards from the node).

Step 5 Express the driven equation in terms of nodal voltages by the help of Ohm's Law i.e. (I = V/R) and also express any other unknown voltage and current other than the node voltage in terms of nodal voltage.

Step 6 Arrange the driven equation and solve them for finding the node voltage.

Let us understand these steps with the help of an example Consider the circuit shown in the given figure.

According to the first step, identify the number of nodes in the given circuit i.e. three (node 1, node 2 and node 3).

According to second step, designate a reference node. In the given circuit we have clearly seen that node 3 is common for all other node (node 1 and node2) and its potential is at ground potential that's why it is taken as reference node.

Once the reference node is selected then as per step 3 assign the voltage designation to all other non-reference nodes. In the given example we have assign V1 variable of node 1 and V2 for node 2.

After assigning variables for each node now moving forward to the next step that is develop the KCL equations for each non reference node.

At node 1 applying KCL I 1 = i1 + i 3

………………… (1)

At node 2 applying KCL

i1 = i2 + I2

……………………(2)

According to step 5 there is no any unknown voltage or current present in the given circuit rather than node voltage. Actually, this happens in the circuit having dependent sources.

Write the derived equation in the form of voltage by the help of Ohm's Law (I = V/R).

Put these Values in equation (1) and (2)

After writing these equations in the form of node voltages we have got two equations to be solved for the given circuit having three nodes. As in the introduction part we discuss that in Nodal analysis (n – 1) equations to be solved for the circuit analysis.

Nodal Analysis with Voltage Source Nodal analysis of an electric circuit having voltage source connected between two non-reference nodes introduces the concept of supernode . In an electric circuit a voltage source is connected in two ways either it is connected between a non-reference node and a reference node or it is connected between two non-reference nodes.

If voltage source is connected between a non-reference node and a reference node than the node voltage of non-reference node is equal to the voltage of the voltage source.

If voltage is connected between two non-reference nodes than it is difficult to find the current in that branch. Hence, KCL equation cannot be developed for such nodes. That’s why the branch having voltage source connected between two non-reference node is considered as supernode. Let us understand the concept of supernode the help of an example.

Consider the circuit as shown in given figure

In the given figure we saw that there are two voltage sources present in the circuit. In which one voltage source is connected between a reference (node 4) and a non-reference (node 1) and other voltage source is connected between two non-reference node (node 2 and node 3).

So, if we calculate the voltage at node 1 it is simply equals to the voltage of the voltage source V1.

But if we drive the KCL equations for node 2 and node 3 for calculating the node voltages we will run into some difficulty because we do not know the current in the branch having voltage source or there is no way by which we can express the current in the form of voltage. So, for the convenience node 2, node 3 and voltage of source together treated as supernode, the supernode is indicated by the region enclosed by the broken line shown in figure. By considering it as supernode we can apply KCL to the both node at same time.

Let us develop the nodal equations for this circuit.

In the given circuit there are four nodes (node 1,2,3 and 4) in which node 4 is the reference node and node 1, 2, 3 are the non-reference nodes. As per step second assigning voltage variables for each non reference node v a vb and vc are the voltage variables for node 1, 2, 3 respectively. Now develop the KCL equations for each no-reference node keeping the supernode concept in mind that we have discussed previously.

At node 1 va = V1 I

discussed earlier

= i 1 + i2

……………….(1)

Put these values in equation 1

At node 2 and 3 Remember that node 2 and node 3 combined treated as supernode. i1 - i3 - i4 + I1 = 0 I 1 = i3 + i 4 - i1