Objective of Lecture State Thévenin’s and Norton Theorems.

Chapter 4.5 and 4.6 Fundamentals of Electric Circuits

Demonstrate how Thévenin’s and Norton theorems can be used to simplify a circuit to one that contains three components: a power source, equivalent resistor, and load.

Thévenin’s Theorem A linear two-terminal circuit can be replaced with an

equivalent circuit of an ideal voltage source, VTh, in series with a resistor, RTh.

VTh is equal to the open-circuit voltage at the terminals.

RTh is the equivalent or input resistance when the independent sources in the linear circuit are turned off.

Circuit Schematic:Thévenin’s Theorem

Definitions for Thévenin’s Theorem

Linear circuit is a circuit where the

voltage is directly proportional to the

current (i.e., Ohm’s Law is followed).

Two terminals are the 2 nodes/2

wires that can make a connection

between the circuit to the load.

Definitions for Thévenin’s Theorem

Open-circuit voltage Voc is the voltage, V, when the load is an open

circuit (i.e., RL = ∞W).

+

Voc

_

ThOC VV

Definitions for Thévenin’s Theorem Input resistance is the resistance seen by the load

when VTh = 0V.

It is also the resistance of the linear circuit when the load is a short circuit (RL = 0W).

SCThThin iVRR

Steps to Determine VTh and RTh1. Identify the load, which may be a resistor or a part of

the circuit.

2. Replace the load with an open circuit .

3. Calculate VOC. This is VTh.

4. Turn off all independent voltage and currents sources in the linear 2-terminal circuit.

5. Calculate the equivalent resistance of the circuit. This is RTh. The current through and voltage across the load in

series with VTh and RTh is the load’s actual current and voltage in the original circuit.

Norton’s Theorem A linear two-terminal circuit can be replaced with an

equivalent circuit of an ideal current source, IN, in parallel with a resistor, RN.

IN is equal to the short-circuit current at the terminals.

RN is the equivalent or input resistance when the independent sources in the linear circuit are turned off.

Circuit Schematic:Norton’s Theorem

Definitions for Norton’s Theorem

Short-circuit current Isc is the current, i, when the load is a short circuit

(i.e., RL = 0W).

NSC II

Definitions for Norton’s Theorem Input resistance is the resistance seen by the load

when IN = 0A.

It is also the resistance of the linear circuit when the load is an open circuit (RL = ∞W).

NOCNin IVRR

Steps to Determine IN and RN1. Identify the load, which may be a resistor or a part of

the circuit.

2. Replace the load with a short circuit .

3. Calculate ISC. This is IN.

4. Turn off all independent voltage and currents sources in the linear 2-terminal circuit.

5. Calculate the equivalent resistance of the circuit. This is RN. The current through and voltage across the load in

parallel with IN and RN is the load’s actual current and voltage in the original circuit.

Source Conversion A Thévenin equivalent circuit can easily be

transformed to a Norton equivalent circuit (or visa versa).

If RTh = RN, then VTh = RNIN and IN = VTh/RTh

Voltage Polarity and Current Flow

Value of Theorems Simplification of complex circuits.

Used to predict the current through and voltage across any load attached to the two terminals.

Provides information to users of the circuit.

Example #1

Example #1 (con’t)Find IN and RN

Example #1 (con’t) Calculation for IN

Look at current divider equation:

If RTh = RN= 1kW, then IN = 6mA

N

N

N

N

loadNload

NloadN

load

eq

load

IRk

RmA

IRRR

RRI

R

RI

W

22

1

Why chose RTh = RN? Suppose VTh = 0V and IN = 0mA

Replace the voltage source with a short circuit.

Replace the current source with an open circuit.

Looking towards the source, both circuits have the identical resistance (1kW).

Source TransformationEquations for Thévenin/Norton Transformations

VTh = IN RTh

IN = VTh/RTh

RTh= RN

Example #1: Norton’s TheoremIN is the current that flows when a short circuit is used as the load with a voltage source

IN = VTh/RTh = 6mA

Example #1: Norton’s TheoremRN is the resistance of the linear circuit when the power sources in the original circuit are turned off (VTh is replaced with a short circuit).

Example #1: Norton’s Theorem The Norton equivalent circuit is:

Check: Thévenin TheoremVTh is the voltage across the load when an open short circuit is used as the load with a current source

VTh = IN RTh = 6V

Check: Iload and Vload

VV

kmAV

mAI

mAkk

kI

load

load

load

load

4

)2(2

2

621

1

W

WW

W

Example #2Simplification through Transformation

Example #2 (con’t)

Example #2 (con’t)Find Req to obtain a Norton equivalent circuit

Example #2 (con’t)

RTh = 3W

VTh = 0.1A (3W) = 0.3V

0.3V

Current Source to Voltage Source

Example #2 (con’t)

0.3V

Example #2 (con’t)

RTh = 2W

IN = 3V/2W = 1.5A

Voltage Source to Current Source

0.3V

Example #2 - Solution 1 Simplify to Minimum Number of Current Sources

Example #2 (con’t)

RTh = 6W

IN = 0.3V/6W = 50.0mA

0.3V

Voltage Source to Current Source

Example #2 (con’t)

Example #2 (con’t)Current Sources in Parallel Add

Example #2 - Solution 2 Simplify to Minimum Number of Voltage Sources

0.3V

Example #2 (con’t)Transform solution for Norton circuit to Thévenin circuit to obtain single voltage source/single equivalent resistor in series with load.

PSpice

Example #2 - Solution 1

Example #2 – Solution 2

Summary Thévenin and Norton transfomrations are performed

to simplify a circuit for analysis and design.

Two techniques were described.

Examples using the source transformation technique were given.