Thevenin Norton MaxPower

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Principles of Electric Circuits - Floyd Chapter Chapter 8 8 1 May 7, 2 022 Chapter 8

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Thevenin_Norton_MaxPower

Transcript of Thevenin Norton MaxPower

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Principles of Electric Circuits - Floyd

Chapter 8Chapter 8 1

Apr 27, 2023

Chapter 8

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Principles of Electric Circuits - Floyd

Chapter 8Chapter 8 2SummarySummary

Thevenin’s theorem states that any two-terminal, resistive circuit can be replaced with a simple equivalent circuit when viewed from two output terminals. The equivalent circuit is:

Thevenin’s theorem

V T H

R T H

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Chapter 8Chapter 8 3SummarySummary

VTH is defined as

Thevenin’s theorem

RTH is defined as

the open circuit voltage between the two output terminals of a circuit. the total resistance appearing between the two output terminals when all sources have been replaced by their internal resistances.

V T H

R T H

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Chapter 8Chapter 8 4SummarySummary

Thevenin’s theorem

R

R

1

R 2R 2 L

V SV S

1 2 V1 0 k

6 8 k 2 7 k

Output terminals

What is the Thevenin voltage for the circuit? 8.76 V

What is the Thevenin resistance for the circuit? 7.30 k

Remember, the load resistor has no affect on the Thevenin parameters.

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Chapter 8Chapter 8 7

Thevenizing from two different sets of terminals

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Chapter 8Chapter 8 8

Thevenizing a portion of a circuit

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Chapter 8Chapter 8 9SummarySummary

Thevenin’s theorem

Thevenin’s theorem is useful for solving the Wheatstone bridge. One way to Thevenize the bridge is to create two Thevenin circuits from A to ground and from B to ground. The thevinin’s resistance between point A and ground is R1||R3 and the resistance from B to ground is R2||R4. The voltage on each side of the bridge is found using the voltage divider rule.

R3 R4

R2

RL

R1VS

-

+A B

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Chapter 8Chapter 8 10

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Chapter 8Chapter 8 11

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Chapter 8Chapter 8 12SummarySummary

Norton’s theorem states that any two-terminal, resistive circuit can be replaced with a simple equivalent circuit when viewed from two output terminals. The equivalent circuit is:

Norton’s theorem

RNIN

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Chapter 8Chapter 8 13SummarySummary

Norton’s theorem

the output current when the output terminals are shorted. the total resistance appearing between the two output terminals when all sources have been replaced by their internal resistances.

IN is defined as

RN is defined as

RNIN

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Chapter 8Chapter 8 14SummarySummary

Norton’s theorem

Output terminals

What is the Norton current for the circuit? 17.9 mAWhat is the Norton resistance for the circuit? 359

R2

R1

RL

VS +10 V

560

820 1.0 k

The Norton circuit is shown on the following slide.

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Chapter 8Chapter 8 15SummarySummary

Norton’s theorem

RNIN17.9 mA 359

The Norton circuit (without the load) is:

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Chapter 8Chapter 8 18SummarySummary

Maximum power transfer

The maximum power is transferred from a source to a load when the load resistance is equal to the internal source resistance.

The maximum power transfer theorem assumes the source voltage and resistance are fixed.

RS

RL

VS +

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Chapter 8Chapter 8 19SummarySummary

Maximum power transfer

What is the power delivered to the matching load?

The voltage to the load is 5.0 V. The power delivered is

RS

RL

VS + 50

50 10 V

22

LL

5.0 V= 0.5 W

50 VPR

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Chapter 8Chapter 8 23SummarySummary

-to-Y and Y-to- conversion

The -to-Y and Y-to- conversion formulas allow a three terminal resistive network to be replaced with an equivalent network.

For the -to-Y conversion, each resistor in the Y is equal to the product of the resistors in the two adjacent branches divided by the sum of all three resistors.

RC

RA RB

R1 R2

R3

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RC

RA RB

R1 R2

R3

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Chapter 8Chapter 8 25SummarySummary

-to-Y and Y-to- conversion

The -to-Y and Y-to- conversion formulas allow a three terminal resistive network to be replaced with an equivalent network.

For the Y-to- conversion, each resistor in the is equal to the sum of all products of Y resistors, taken two at a time divided by the opposite Y resistor.

RC

RA RBR1 R2

R3

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RC

RA RB

R1 R2

R3

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