Norton’s Theorem and Maximum Power Transfer Theorem Lecture No.7 By – Engr Sajid Hussain Qazi Lecturer Mehran University C.E.T Khairpur.

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Norton’s Theorem and Maximum Power Transfer Theorem Lecture No.7 By – Engr Sajid Hussain Qazi Lecturer Mehran University C.E.T Khairpur

Norton’s Theorem The theorem states the following: “Any two-terminal linear bilateral dc network can be replaced by an equivalent circuit consisting of a current source and a parallel resistor, as shown in Figure.” The discussion of Thevenin’s theorem with respect to the equivalent circuit can also be applied to the Norton equivalent circuit. The steps leading to the application of Norton’s Theorem are listed below Engr. S.H.Qazi

1. Remove that portion of the network across which the Norton equivalent circuit is found. 2. Mark the terminals of the remaining two-terminal network. 3. Calculate RN by first setting all sources to zero (voltage sources are replaced with short circuits, and current sources with open circuits) and then finding the resultant resistance between the two marked terminals. 4.Calculate IN by first returning all sources to their original position and then finding the short-circuit current between the marked terminals. 5. Draw the Norton equivalent circuit with the portion of the circuit previously removed replaced between the terminals of the equivalent circuit.

Engr. S.H.Qazi Maximum Power Transfer Theorem The maximum power transfer theorem states the following: “A load will receive maximum power from a linear bilateral dc network when its total resistive value is exactly equal to the Thevenin resistance of the network as seen by the load.” For the network of Fig-1, maximum power will be delivered to the load when, Figure-1 For the network of Fig-2, maximum power will be delivered to the load when, Figure-2

Engr. S.H.Qazi For the network of Figure-1. For the maximum power;

Engr. S.H.Qazi For the network of Figure-2. Eth=InRn For the maximum power;