Introduction-Applied Physics-Lecture Slides, Slides of Applied Chemistry

This course includes Motion, Oscillations, waves and propagation, Electric Charge and Coulomb Law, Electric Field, Electric Potential, Capacitors and Dielectric, Current and Resistance, AC and DC, Magnetic fields, Ampere Law and Faraday law, Maxwell equations and Traveling waves. This file includes: Inductance, Property, Electromagnetic, Field, Energy, Characteristic, Electrical, Henry, Ampere, Magnetic, Conductor

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2011/2012

Uploaded on 07/31/2012

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Introduction
Inductance
“Inductance is the property of a circuit by which energy is
stored in the form of an electromagnetic field".
Inductance is the characteristic of an electrical conductor
that OPPOSES CHANGE in CURRENT
The symbol for inductance is L and the basic unit of
inductance is the HENRY (H). One henry is equal to the
inductance required to induce one volt in an inductor by a
change of current of one ampere per second.
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1

Introduction

Inductance

“Inductance is the property of a circuit by which energy is stored in the form of an electromagnetic field".

Inductance is the characteristic of an electrical conductor that OPPOSES CHANGE in CURRENT

The symbol for inductance is L and the basic unit of inductance is the HENRY (H). One henry is equal to the inductance required to induce one volt in an inductor by a change of current of one ampere per second.

2

The process of generating electrical current in a

conductor by placing the conductor in a

changing magnetic field is called

electromagnetic induction or just induction. It

is called induction because the current is said

to be induced in the conductor by the magnetic

field.

Inductance

4

Inductance

5

Inductance

7

Calculating the inductance

 If ΦB is the magnetic flux through each turn of the coil

 N is the number of turns of coil

 The emf according to Faraday’s law can be given as

εL = dt

d(NΦB)

From equations 2 and 4

dt

d(NΦB)

dt

di

L

8

Calculating the inductance

 Integrating with respect to time

 Li = NΦB

i

L =

NΦB

 In above equation inductance “ L ” is independent of

current “I” like capacitance is independent of charge “q” but depends upon the geometry of the device and the magnetic flux linkages i.e. NΦB

10

The inductance of a solenoid

 Where μo is the permeability of free space

 n, is the number of turns per unit length

 i, is the current passing through the coils

 The number of flux linkages in the length l is

NΦB = nl (BA) (8)

 Substitute equations 7 in equation 8

NΦB = μon^2 l i A (9)

 Substitute equation 9 in 6

 L = μon^2 l A (10)

11

The inductance of a Toroid

http://www.ndt-ed.org/EducationResources/CommunityCollege/EddyCurrents/Physics/circuitsphase.htm

The magnetic field in a toroid is

2 πr

B =

Niμo (11)

docsity.com

13

b

ΦB = ∫ h dr

a^2 πr

μoiN

Φ^ dr

B =

b

2 π a

μoiN h

r

Φ^ h dr

B =

b

2 π a

μoiN

r

Φ^ b

B =^2 π ln

μoiN h

a

The inductance of a Toroid

14

The inductance of a Toroid

i

L =

NΦB

 The inductance of the toroid can be written from equations 6 and 12

i

NΦB

L ln b

μoN^2 h

a

L = ln b

μoN^2 h

a

Inductance only depends on the geometry of toroid

16

Inductance with magnetic materials

 The inductor with no magnetic material has magnetic field Bo, while the inductor with magnetic material has magnetic field B

 The inductance of an inductor with magnetic material can be given as

L = KmLo

 Inductance of solenoid with magnetic substance of permeability constant Km is

L = Km μon^2 l A

17

Inductance with magnetic materials

 Three types of magnetic materials

 Paramagnetic

 Diamagnetic

 Ferromagnetic

 The permeability constant of paramagnetic and diamagnetic doesn't differ from 1 , thus by inserting these two types of materials the magnetic field almost remains same as with out materials

 The permeability constant for ferromagnetic materials about is 103 to 104 , thus the inductance of an inductor filled with ferromagnetic materials increases

19

LR Circuits

 A similar rise and fall of current occurs by inserting an emf source in a circuit containing inductor L and resistor R

 If the inductor were not present the current would rise

rapidly to ε/R

 But due the presence of the inductor an induced emf εL

appears in the circuit, which according to Lenz’s law opposes the increase in the current

20

 As long as the inductor is there in the circuit, the current, in the resistor depends upon the two emfs, one from battery

ε and the other from inductor εL with opposite sign

 that’s why the current in the circuit rises exponentially

LR Circuits

 Vy – Vx = -iR

 (x is at higher potential than y) docsity.com