We can express the **Millman’s Theorem** in terms of voltage sources. Also, we can express in terms of current sources.

### Millman’s Theorem Applicable to Voltage Sources

This theorem combines both Thevenin’s theorem and Norton’s theorem. In order to find a common voltage across a network, we use **Millman’s Theorem**. The network contains a number of parallel voltage sources.

Suppose there are n numbers of parallel voltage sources.

Here, in the above figures, R_{1}, R_{2}, R_{3, }and R_{n }are the internal resistance of the voltage sources. On the other hand, the voltage V_{1}, V_{2}, V_{3 …} and V_{n} are the emf of the voltage sources.

The overall equivalent voltage of the above circuit across A and B is,

This voltage is nothing but the Thvenin’s voltage across terminals A and B.

### Proof of Millman’s Theorem

Millman’s theorem tells the open circuit voltage of an active circuit across two terminals of the circuit. Also, Thevenin’s theorem tells the same.

Let us consider the voltage at node A is V_{A} and voltage at node B is 0.

So, as per nodal analysis, we can write,

As the voltage at B is 0, we can write,

### Example of Millman’s Theorem

Let us take the circuit as shown below.

As per Millman’s theorem, the voltage across A and B

The Thevenin equivalent resistance of the circuit across node A and B is

Now, the rule of current through the 25Ω resistance is,

Millman’s Theorem Applicable to Current Sources. Suppose there are n numbers of current sources connected in parallel.

We can consider this circuit as a single current source. As per Millman’s theorem, the current of the source is the sum of individual source currents.

The equivalent resistance of the circuit is the internal resistance of the current source.

The equivalent resistance or Norton resistance of the network against terminals A and B, is the parallel combination of individual source resistances. That is

So, the equivalent current source of the above parallel combinations of n number of current sources is, as shown below.

#### Example of Millman’s Theorem Applicable to Connect Sources

Let us consider the circuit below.

As per Millman’s theorem, the Norton equivalent current of the circuit against terminal A and B is,

The Norton equivalent resistance of the circuit is the parallel combination of 12Ω, 4Ω and 6Ω. That is

Therefore, the Norton equivalent source of the above circuit is as below.

Hence, the current through, the resistance of 8Ω resistance, connected between A and B is,

- Millman’s Theorem to Voltage and Current Sources
- Solving Equations with Matrix Method
- Electrical Source Conversion (Voltage and Current Sources)
- Circuit Analysis or Network Analysis
- Kirchhoff’s Current Law and Kirchhoff’s Voltage Law
- Maxwell’s Loop Current Method or Mesh Analysis
- Nodal Analysis Method with Example of Nodal Analysis
- Star Delta Conversion and Delta Star Conversion
- Thevenin’s Theorem Thevenin’s Voltage and Resistance
- Norton’s Theorem – Norton’s Current and Resistance
- Maximum Power Transfer Theorem
- Superposition Theorem Statement and Theory
- Reciprocity Theorem Statement Explanation and Examples
- Compensation Theorem