2-10 systematic solution methods part 2

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Dr. Bonnie Ferri Linear Circuits School of Electrical and Computer Engineering Professor and Associate Chair School of Electrical and Computer Engineering An introduction to linear electric circuit elements and a study of circuits containing such devices.

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Page 1: 2-10 Systematic Solution Methods Part 2

Dr. Bonnie Ferri

Linear Circuits

School of Electrical and Computer Engineering

Professor and Associate ChairSchool of Electrical and Computer Engineering

An introduction to linear electric circuit elements and a study of circuits containing such devices.

Page 2: 2-10 Systematic Solution Methods Part 2

Dr. Bonnie Ferri

Systematic Solution Methods: Part 2

School of Electrical and Computer Engineering

Professor and Associate ChairSchool of Electrical and Computer Engineering

Introduce several ways of obtaining circuit equations.

Page 3: 2-10 Systematic Solution Methods Part 2

Resistance Kirchhoff’s Laws Resistors

Module 2: Resistive Circuits

Resistors Superposition Systematic Solution Methods Maximum Power Transfer Application: Sensors

3

Page 4: 2-10 Systematic Solution Methods Part 2

Demonstrate Thévenin equivalent and Norton equivalent circuits Source transformations

Lesson Objective

Source transformations

4

Page 5: 2-10 Systematic Solution Methods Part 2

Systematic solution MethodsMethod Summary When to ApplyMesh Analysis KVL to obtain simultaneous

equations for currents• Multiple currents are needed• Current sources are present

Node Analysis KCL to obtain simultaneous • Multiple voltages are needed

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Node Analysis KCL to obtain simultaneous equations for voltages

• Multiple voltages are needed• Voltage sources are present

Thévenin and NortonEquivalent Circuits

Simple equivalent circuits, source transformations

• Intermediate values notimportant; only output voltage or current

Page 6: 2-10 Systematic Solution Methods Part 2

Thévenin Equivalent

a

Circuit vTh -

+vThRTh

aisc

6

Replace circuit with equivalent resistance and voltage source

bb

Page 7: 2-10 Systematic Solution Methods Part 2

vTh : open circuit across a-b and find vab= vTh

isc : short circuit across a-b and find isc

Thévenin Equivalent CircuitscThTh iRv =

a aisc

7

RTh : circuit resistance with voltage sources shorted and current sources open circuited (when no dependent sources are present)

b

a

Circuit vTh

b

a

Circuit

sc

Page 8: 2-10 Systematic Solution Methods Part 2

Thévenin Equivalent Example0.2A

-

+1vvo

2ΩRo

+

-4Ω

10Ω

8

-

+

2v

Page 9: 2-10 Systematic Solution Methods Part 2

Norton Equivalent Circuit

-

+vThRTh

aisc

iscRTh

a

9

b b

Source Transformation: these configurations are interchangeable in a circuit

Thévenin equivalent circuit Norton equivalent circuit

Page 10: 2-10 Systematic Solution Methods Part 2

Source Transformation Example0.2A

-

+1vvo

2ΩRo

+

-4Ω

10Ω

10

-

+

2v

Page 11: 2-10 Systematic Solution Methods Part 2

Mesh and node analysis Systematic ways to find independent

simultaneous equations Thévenin and Norton methods

Summary

Thévenin and Norton methods Replace most of the circuit with a simple

equivalent circuit Source transformations Extra worked problems are given on

these methods

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Page 12: 2-10 Systematic Solution Methods Part 2

Maximum Power Transfer Uses Thévenin equivalent circuit to find the load to

Next Lesson

Uses Thévenin equivalent circuit to find the load to maximize power delivered

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