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2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: [email protected] Department

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Page 1: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

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Page 2: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

Circuit Analysis-1 Fall-2014EE -1111

Instructor: Hafiz Zaheer HussainEmail: [email protected]

www.hafizzaheer.pbworks.com

Department of Electrical EngineeringThe University of Lahore

Lecture # 25 & 26

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3

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Content

Introduction

Capacitor

Energy storage in capacitor

Series and parallel Capacitors

Inductor

Energy storage in Inductor

Series and parallel Inductors

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An inductor is a passive element that stores energy in its magnetic field. Generally. An inductor consists of a coil of conducting wire wound around a core.

Inductor

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An inductor is a passive element that stores energy in its magnetic field. Generally. An inductor consists of a coil of conducting wire wound around a core. For the inductor

Inductance

( )( )

di tv t L

dt

where L is the inductance in henrys (H), and 1 H = 1 volt second/ampere.

Inductance is the property whereby an inductor exhibits opposition to the change of current flowing through it

+

-

Lv

Page 7: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

Symbols of Inductors

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where i(t0) = the total current evaluated at t0 and i() 0 (which is reasonable since at some time there was no current in the inductor).

( )( )

di tv t L

dt

Relationship Between Current and Voltage

Integrating gives

Or

Page 9: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

Relationship Between Current and Voltage

Page 10: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

Content

Introduction

Capacitor

Energy storage in capacitor

Series and parallel Capacitors

Inductor

Energy storage in Inductor

Series and parallel Inductors

Page 11: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

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Energy Storage in an Inductor

The instantaneous power delivered to an inductor is

( ) ( )t t

L

diw t p t dt L i dt L idi

dt

( )di

p t vi Lidt

The energy stored in the magnetic field is thus

21( ) ( ) joules

2Lw t Li t

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An Inductor Properties

An inductor has the following important properties:

1. An inductor acts like a short circuit to dc, since from

v = 0 when i = a constant.

2. The current through an inductor cannot change instantaneously, since an instantaneous change in current would require an infinite voltage, which is not physically possible.

( )( )

di tv t L

dt

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An Inductor PropertiesAn inductor has the following important properties:

3. Like the ideal capacitor, the ideal inductor does not dissipate energy.

4. A real inductor has a significant resistance due to the resistance of the coil, as well as a “winding capacitance”. Thus, the model for a real inductor is shown below.

In this course, however, we will use ideal inductors and assume that an ideal inductor is a good model.

C

RW

W

L

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Page 20: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

Content

Introduction

Capacitor

Energy storage in capacitor

Series and parallel Capacitors

Inductor

Energy storage in Inductor

Series and parallel Inductors

Page 21: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

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Series Inductor

1 1

div L

dt 2 2

div L

dt N N

div L

dt

1 2 1 2N N eq

di div v v v L L L L

dt dt

The equivalent inductance of series connected inductors is the sum of the individual inductances. Note: inductances in series combine in the same way as resistors in series.

DC

1L 2L NL

1v 2v Nv+ + + -- -

v

i

i

eqLv+

-

DC

Page 22: 2 22/12/2014. Circuit Analysis-1 Fall-2014 EE -1111 Instructor: Hafiz Zaheer Hussain Email: zaheer.hussain@ee.uol.edu.pk  Department

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Parallel Inductor

11

1i vdt

L

1 21 2

1 1 1 1N

N eq

i i i i vdt vdtL L L L

The equivalent inductance of parallel connected inductors is the reciprocal of the sum of the reciprocals of the individual inductances.

22

1i vdt

L

1N

N

i vdtL

1i 2i Ni

1L 2L NLv+

-

i

i

v+

-

eqLi

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