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Lecture Electric circuit theory: Magnetically coupled circuits - Nguyễn Công Phương

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XIII.Frequency Response XIV.The Laplace Transform XV.. Analysis of Magnetically Coupled Circuits 4.[r]

(1)

Electric Circuit Theory

(2)

Contents

I. Basic Elements Of Electrical Circuits II. Basic Laws

III Electrical Circuit Analysis IV Circuit Theorems

V Active Circuits

VI Capacitor And Inductor VII First Order Circuits VIII.Second Order Circuits

IX Sinusoidal Steady State Analysis X AC Power Analysis

XI Three-phase Circuits

XII Magnetically Coupled Circuits

XIII.Frequency Response XIV.The Laplace Transform XV Two-port Networks

(3)

Magnetically Coupled Circuits

1 Mutual Inductance 2 Dot Convention

3 Analysis of Magnetically Coupled Circuits 4 Energy in a Coupled Circuit

(4)

Mutual Inductance (1)

Magnetically Coupled Circuits - sites.google.com/site/ncpdhbkhn

d

v N

dt

Faraday’s law:

+

+

( )

i t

v

turns

N

d di N

di dt

L di

dt

d

L N

di

(5)

Mutual Inductance (2)

1 11 12

   1 1 1 d v N dt   12 2 2 d v N dt  

1 1

1

d di di

N L

di dt dt

  12 1 1

2 21

d di di

N M

di dt dt

   1 21 di M dt+ +

1( )

i t v 12  turns N 11 

L L2

+

v2

2 turns

(6)

Mutual Inductance (3)

Magnetically Coupled Circuits - sites.google.com/site/ncpdhbkhn

+

+

2( )

i t v 21  turns N 22 

L L2

+

v2

2 turns N + +

1( )

i t v 12  turns N 11 

L L2

(7)

Mutual Inductance (4)

+

+

1( )

i t

1

v

12

1 turns

N 11

1

L L2

+

v

2 turns

N

1 21

di

v M

dt

1( )

i t

1

v v2

12

11

 

(8)

Mutual Inductance (5)

Magnetically Coupled Circuits - sites.google.com/site/ncpdhbkhn

1( )

i t v 12  11     

1( )

i t v 12  11      di v M dtdi v M dt  

1( )

i t v 12  11      di v M dt  

1( )

(9)

Magnetically Coupled Circuits

1 Mutual Inductance

2 Dot Convention

3 Analysis of Magnetically Coupled Circuits 4 Energy in a Coupled Circuit

(10)

Dot Convention (1)

Magnetically Coupled Circuits - sites.google.com/site/ncpdhbkhn 10

+

1( )

i t

1

L

2

L

+

2

v M

1 2

di

v M

dt

 • If a current enters a dotted

terminal of one coil, it induces a positive voltage at the dotted terminal of the second coil

• If a current leaves a dotted

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