The maximum power transfer theorem deals with the condition that when the maximum power transfer of the source to the load occurs.
Here we will be discussing the theorem along with its statement, proof of the condition, steps, and the example problems.
The theorem states that:
In a d.c. circuit, the maxim power transfer from the source to load takes place when the load resistance is equal to the internal resistance of the source as viewed from the load terminals with the load removed and all the sources replaced by their internal resistances.
In other words, the maximum power transfer shall occur when the load resistance is equal to the Thevenin’s resistance of the circuit.
Meanwhile, let’s look at an illustration.
In our illustration, a circuit supplies power to the load RL. The circuit which we are representing by using a box can be replaced by using Thevenin’s equivalent circuit consisting of a Thevenin’s voltage E (=VTH) in series with the Thevenin’s resistance RS (=RTH). As in Thevenin’s equivalent circuit, the Thevenin’s resistance turns out to be the internal resistance of the source. This also illustrates that Thevenin’s theorem is an application of a practical voltage source.
Finally, by the maximum power transfer theorem, the circuit will transfer the maximum power when the load resistance is equal to the internal resistance of the source.
In short, the condition of maximum power transfer is load resistance (RL) = Thevenin’s resistance (RS).
Condition is RL = RS.
Proof of Maximum Power Transfer Theorem
Consider the circuit below.
The power which the source delivers to the load is
In the above relation, when RL equals zero, the power P also becomes zero. Similarly, when the RL tends to infinity the power P is again zero.
Hence, we know that for the transfer of maximum power, the value of RL lies between zero and infinity.
We can calculate the value of RL when the power will be maximum, by differentiating the expression of power P concerning RL and equation it with zero.
Therefore, the condition RS = RL is the condition for maximum power transfer.
Finally, using this condition the equation (i) to obtain the power which the source delivers to the load is
Steps for Solving a Problem Using Maximum Power Transfer Theorem
We can follow the following steps to solve a problem using this theorem.
- Firstly, find the Thevenin’s resistance (RTH) by removing the load and replacing all the sources with its internal resistance. Meanwhile, for the problems containing ideal sources, replace the voltage source with short-circuit and the current source with an open-circuit.
- According to the maximum power transfer theorem, this RTH is the system load resistance, that is to say, RL =RTH that allows maximum power transfer.
- Secondly, find the Thevenin’s voltage (VTH).
- Finally, calculate the maximum power transfer using the relation.
Similarly, if you are approaching the problem using Norton’s theorem then the maximum power transfer will be
Examples of Maximum Power Transfer Theorem
Here, we will determine the value of resistance R such that maximum power transfer takes place in the circuit.
Firstly, we will calculate the Thevenin’s voltage which is the open-circuit voltage across the terminal XY.
At first, apply KVL on mesh I
Secondly, applying KVL on mesh II
Then, solving equation (i) and (ii) we have
I2 =0.25 A
Now, to find the VTH we write KVL moving from Y to X. For a clear understanding, we are writing KVL on the blue portion of the circuit in a clockwise direction.
Then, we have to find the RTH.
From the above circuit,
For the transfer of maximum power, RL should be equal to RTH.
Further, we will draw Thevenin’s equivalent circuit as
Therefore, maximum power delivered to the load is