lecture 6: thevenin and norton equivalents, maximum power transfer, & superposition nilsson...

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Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1 April 17, 2014

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Page 1: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Lecture 6:Thevenin and Norton Equivalents,Maximum Power Transfer, &SuperpositionNilsson & Riedel 4.10-4.13

ENG17 (Sec. 2): Circuits I

Spring 2014

April 17, 2014

Page 2: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Overview

• Thevenin Equivalent• Norton Equivalent• Special Cases• Maximum Power

Transfer• Superposition

Page 3: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Thevenin Equivalent Circuit

• Independent voltage source in series with resistor• Provides simplified equivalence to more complex circuit

Page 4: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Finding Thevenin Equivalent

Page 5: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Overview

• Thevenin Equivalent• Norton Equivalent• Special Cases• Maximum Power

Transfer• Superposition

Page 6: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Norton Equivalent Circuit

• Independent current source in parallel with resistor• Provides simplified equivalence to more complex circuit• Relates to Thevenin Equivalent (source transformation)

Page 7: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Finding Norton Equivalent

Page 8: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Overview

• Thevenin Equivalent• Norton Equivalent• Special Cases• Maximum Power

Transfer• Superposition

Page 9: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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With Dependent Source

Page 10: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Alternate Method

Page 11: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Overview

• Thevenin Equivalent• Norton Equivalent• Special Cases• Maximum Power

Transfer• Superposition

Page 12: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Power Transfer

• Two issues:– Efficiency of Power Transfer– Amount of Power Transfer

Page 13: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Maximum Power Transfer

Page 14: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Example

• Find value of RL that results in maximum power transfer.

• Use Thevenin Equivalent circuit.

Page 15: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Overview

• Thevenin Equivalent• Norton Equivalent• Special Cases• Maximum Power

Transfer• Superposition

Page 16: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Superposition

• Applies to linear system• Defined: when linear system is excited by >1

independent energy sources, the total response is the sum of individual responses.

• Clarified– Deactivate 1st source, find response from 2nd

source– Deactivate 2nd source, find response from 1st

source– Add these responses

Page 17: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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In practice

• May not help so much right now…

Page 18: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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w/Dependent Sources

Page 19: Lecture 6: Thevenin and Norton Equivalents, Maximum Power Transfer, & Superposition Nilsson & Riedel 4.10-4.13 ENG17 (Sec. 2): Circuits I Spring 2014 1

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Overview

• Thevenin Equivalent• Norton Equivalent• Special Cases• Maximum Power

Transfer• Superposition