Maximum Power Transfer and Thevenin-Norton Equivalents, Slides of Electrical Circuit Analysis

An outline and explanations for the concepts of maximum power transfer, thevenin's and norton's equivalents in electrical engineering. It covers topics like linear circuits, thevenin and norton equivalent circuits, maximum power transfer condition, and examples. Students can use this document for understanding these concepts, solving problems related to them, and preparing for exams.

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2012/2013

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Engineering 43
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Download Maximum Power Transfer and Thevenin-Norton Equivalents and more Slides Electrical Circuit Analysis in PDF only on Docsity!

Engineering 43

MaxPower

SuperPosition

OutLine: MaxPwr & SuperPose

  • Work On WhtBd Student Suggest

HomeWork Problem

  • Thevénin & Norton Review
    • Example Problem (WhtBd)
  • Maximum Power Transfer

Theorem Derivation

  • MaxPwr Application Examples
  • Thevénin & Norton Summary

      ^        L s

s L L

s S L sS LL

LL L sS LL s SL sS LL

L L L S s L L sS LL

LL L L S s LL

R R

R R R

RVR RV RR

RP R RVRR RVR RVRR

P VR R V RRR RVRR

RP P VR V V RRR

 

  

       

       

     

2

2

(^0) dd dd 2

1

(^0) dd

(^2223)

(^222223)

(^22) 2 2

2

Thevénin’s Equivalence Theorem

LINEAR CIRCUIT May contain independent and dependent sources with their controlling variables PART A

LINEAR CIRCUIT May contain independent and dependent sources with their controlling variables PART B

a

_ b

v O

i

LINEAR CIRCUIT PART B

a

_ b

v O

i

R TH

v TH

PART A

 Thevenin Equivalent Circuit for PART A

 vTH = Thévenin Equivalent VOLTAGE Source  RTH = Thévenin Equivalent SERIES RESISTANCE

Norton’s Equivalence Theorem

 Norton Equivalent Circuit for PART A

 iN = Norton Equivalent CURRENT Source  RN = Norton Equivalent PARALLEL RESISTANCE

LINEAR CIRCUIT May contain independent and dependent sources with their controlling variables PART A

LINEAR CIRCUIT May contain independent and dependent sources with their controlling variables PART B

a

_ b

v O

i

LINEAR CIRCUIT PART B

a

_ b

v O

i

iN R N

PART A

Maximum Power Transfer

  • Consider The Amp-Speaker Matching Issue

From PreAmp (voltage ) (^) To speakers

+-

RTH

VTH

Maximum Power Xfer Cont

  • The Simplest Model for a Speaker is to Consider it as a RESISTOR only

 Since the “Load” Does the “Work” We Would like to Transfer the Maximum Amount of Power from the “Driving Ckt” to the Load

  • Anything Less Results in Lost Energy in the Driving Ckt in the form of Heat

+-

RTH

VTH SPEAKER MODEL BASIC MODEL FOR THE ANALYSIS OF POWER TRANSFER

Max Power Xfer cont

  • Find Max Power Condition Using Differential Calculus

 Set The Derivative To Zero To Find MAX or MIN Points

  • For this Case Set To Zero The NUMERATOR

    

 

 

 

 

   (^2 )

2

TH L

TH L L TH L

L R R

R R R V dR

dP

 Solving for “Best” (Pmax) Load RL  RTH

 This is The Maximum Power Transfer Theorem

  • The load that maximizes the power transfer for a circuit is equal to the Thevenin equivalent resistance of the circuit

   

  (^20)

0

2 3

2

   

  

 

 

 

  

TH L L

TH L

TH L L TH L R

L

R R R

R R

R R R V dR

dP

L

Max Power Quantified

  • By Calculus we Know

RL for PL,max

RL  RTH

 Recall the Power

Transfer Eqn

 

2 2 TH TH L

L L V R R

R P 

 Sub RTH for RL

 

2 , max 2 TH TH TH

TH L V R R

R P 

 

2 2

2 ,max (^24) 2

TH TH

TH TH TH

TH L V R

R V R

R P  

 So Finally

TH

TH L R

V P

2

, max 4

1 

Max Pwr Xfer Example cont

  • To Find VTH Use Meshes
  • The Eqns for Loops 1 & 2

 Solving for I 2

8 [ ] 2 [ ] 10 [ ]

3

1 4 * 2 6 *

4 * 1 6 * 2

V V V

k mA k mA

VOC k I k I

  

   

 

I 1  2 mA

3 k ^ I 2  I 1 ^  6 kI 2  3 V  0

[ ]

9 [ ]

3 [ ]

2 k I 1 mA

V

I  

 Now Apply KVL for VOC

 Recall

2 2 TH TH L

L L (^) R R V

R
P

 At Max: PL = PMX, RL = RTH

TH

MX TH R

P V 4

2 

[ ] 6

25 4 * 6

100 [ 2 ] mW k

P V MX   

Max Pwr Xfer

  • Determine RL and Max Power Transferred
  • Find Thevenin Equiv. At This Terminal-Set

 Recall for Max Pwr Xfer

a

b

RL  RTH TH

MX TH R

V P 4

2 

 This is a MIXED Source Circuit

  • Analysis Proceeds More Quickly if We start at c-d and Adjust for the 4kΩ at the end

c

d  Use Loop Analysis

 Eqns for Loops 1 & 2 I 1  4 mA 4 k (I 2  I 1 ) 2 kI (^) X'   2 kI 2  0

6 I 2  2 I (^) X'   4 I 1  16 mA

I 1 I 2

Thevenin & Norton Summary

  • Independent

Sources Only

  • RTH = RN by Source Deactivation
  • VTH
    • = VOC or
    • = RN·ISC
  • IN
    • = ISC or
    • = VOC/RTH
      • Mixed INdep and Dep Srcs - Must Keep Indep & dep Srcs Together in Driving Ckt - VTH = VOC - IN = ISC - RTH = RN = VOC/ ISC

 DEPENDENT Sources Only

  • Must Apply V or I PROBE - Pick One, say IP = 1. mA, then Calculate the other, say VP
  • VTH = IN = 0
  • RTH = RN = VP/ IP

WhiteBoard Work

 Let’s Work this nice

Max Power Problem

 Find Pmax for Load RL

Linearity

  • Models Used So Far Are All LINEAR - Mathematically This Implies That They satisfy the principle of SUPERPOSITION
  • The Model T(u) is Linear IF AND ONLY IF

T 1 u 1  2 u 2   1 Tu 1    2 Tu 2 

  • For All Possible
    • Input Pairs: u 1 & u 2
    • Scalars α 1 & α 2  AN Alternative, And Equivalent, Linearity & Superposition Definition
  • The Model T(u) is Linear IF AND ONLY IF It Exhibits
  • ADDITIVITY
  • HOMOGENEITY

Linearity cont.

  • Linearity

Characteristics

  • Additivity

 NOTE

  • Technically, Linearity Can Never Be Verified Empirically on a System
  • But It Could Be Disproved by a SINGLE Counter Example.
  • It Can Be Verified Mathematically For The Models Used

T u 1 u 2  Tu 1  Tu 2 

T(u )  T u

  • Homogeneity
    • a.k.a. Scaling