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Lecture Electromechanical energy conversion: Magnetic circuits and magnetic materials - Nguyễn Công Phương

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Lecture Electromechanical energy conversion - Magnetic circuits and magnetic materials presents the following content: Introduction to magnetic circuits; flux linkage, inductance, and energy; properties of magnetic materials; AC excitation; permanent magnets; application of permanent magnet materials.

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Nguyễn Công Phương

ELECTROMECHANICAL ENERGY

CONVERSION

Magnetic Circuits and Magnetic Materials

Trang 2

I Magnetic Circuits and Magnetic Materials

II Electromechanical Energy Conversion

Principles

III Introduction to Rotating Machines

IV Synchronous Machines

V Polyphase Induction Machines

VI DC Machines

VII.Variable – Reluctance Machines and Stepping

Motors

VIII.Single and Two – Phase Motors

IX Speed and Torque Control

Trang 3

Magnetic Circuits and Magnetic Materials

1 Introduction to Magnetic Circuits

2 Flux Linkage, Inductance, and Energy

3 Properties of Magnetic Materials

4 AC Excitation

5 Permanent Magnets

6 Application of Permanent Magnet Materials

sites.google.com/site/ncpdhbkhn 3

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Introduction to Magnetic Circuits

µ

=

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0 0.5

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Introduction to Magnetic Circuits

Trang 8

Introduction to Magnetic Circuits

(5)

µ >> µ 0 : the magnetic flux is confined

almost entirely to the core

F = Ni : magnetomotive force (mmf)

+ –

Magnetic core permeability µ

Mean core length, lc

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Introduction to Magnetic Circuits

(6)

+ –

Magnetic core permeability µ

Mean core length, lc

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Introduction to Magnetic Circuits

(7)

+ –

Magnetic core permeability µ

Mean core length, lc

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Introduction to Magnetic Circuits

c g

R R F

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The core is made of nickel – iron alloy

Find the current i?

+ –

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Introduction to Magnetic Circuits

(11)

Ex 2

Given Φ = 0.141 mWb, S c = S g = 4cm 2 ,

l c = 44cm, g = 0.2cm, N = 400 turns

The core is made of nickel – iron alloy

Find the current i?

+ –

F i

N

→ = = =

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N = 500 turns Rotor and stator are made

of iron (infinite permeability) Find the

flux of the air gap?

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Introduction to Magnetic Circuits

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Magnetic Circuits and Magnetic Materials

1 Introduction to Magnetic Circuits

2 Flux Linkage, Inductance, and Energy

3 Properties of Magnetic Materials

4 AC Excitation

5 Permanent Magnets

6 Application of Permanent Magnet Materials

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Flux Linkage, Inductance, and

R

→ =

Trang 19

Find the inductance of the winding and

the flux density of gap 2?

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Flux Linkage, Inductance, and

Find the inductance of the winding and

the flux density of gap 2?

1 1

1

Ni B

g

µ

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g

g R

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Flux Linkage, Inductance, and

Energy (5)

x 1040

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Flux Linkage, Inductance, and

Energy (7)

d e

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λ = → =

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Flux Linkage, Inductance, and

Energy (9)

Ex 3

3 A turns 3.07 10

A turns 2.49 10

dt

1000 (16 10 ) 314 cos(314 )− t

= × × × = 502 cos(314 ) t

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Magnetic Circuits and Magnetic Materials

1 Introduction to Magnetic Circuits

2 Flux Linkage, Inductance, and Energy

3 Properties of Magnetic Materials

4 AC Excitation

5 Permanent Magnets

6 Application of Permanent Magnet Materials

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Properties of Magnetic Materials

(1)

Magnetic materials can be used:

• To constrain and direct magnetic fields in well – defined paths

• In transformer:

– To maximize the coupling between the windings, and

– To lower the excitation current required for

transformer operation

• In electric machinery:

– To shape the fields to obtain desired torque –

production and electrical terminal characteristics

• The most common: ferromagnetic materials

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sites.google.com/site/ncpdhbkhn 29

Properties of Magnetic Materials

(2)

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Properties of Magnetic Materials

(2)

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Properties of Magnetic Materials

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Magnetic Circuits and Magnetic Materials

1 Introduction to Magnetic Circuits

2 Flux Linkage, Inductance, and Energy

3 Properties of Magnetic Materials

4 AC Excitation

5 Permanent Magnets

6 Application of Permanent Magnet Materials

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c c rms rms

l H I

N

ϕ =

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AC Excitation (2)

, max ,

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AC Excitation (3)

The exciting current i supplies the mmf needed to

produce:

– the core flux, and

– the power input associated with the energy in the

magnetic

• This energy:

– Part is dissipated as losses & results in heating of the

core (RI 2 )

– The rest appears as reactive power, it is not dissipated

in the core, but cyclically supplied & absorbed by the excitation source

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sites.google.com/site/ncpdhbkhn 37

AC Excitation (4)

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AC Excitation (5)

Ex.

The winding is excited with a 60-Hz voltage to

produce B = 1.6sinωt T, the steel occupies 0.94 of the

core cross-sectional area, ρc = 7.65 g/cm3 Find:

a) The applied voltage?

b) The peak current?

c) The rms exciting current?

d) The core loss?

1.6 sin(2 60 ) 1.6 sin 377 T

+ –

2(15 10 15 10) 10 70

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sites.google.com/site/ncpdhbkhn 39

AC Excitation (6)

Ex.

The winding is excited with a 60-Hz voltage to

produce B = 1.6sinωt T, the steel occupies 0.94 of the

core cross-sectional area, ρc = 7.65 g/cm3 Find:

a) The applied voltage?

b) The peak current?

c) The rms exciting current?

d) The core loss?

+ –

c

E I P

a rms

rms

P W I

E

=

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AC Excitation (7)

Ex.

The winding is excited with a 60-Hz voltage to

produce B = 1.6sinωt T, the steel occupies 0.94 of the

core cross-sectional area, ρc = 7.65 g/cm3 Find:

a) The applied voltage?

b) The peak current?

c) The rms exciting current?

d) The core loss?

+ –

c total c c

P = PW

= ×

=

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Magnetic Circuits and Magnetic Materials

1 Introduction to Magnetic Circuits

2 Flux Linkage, Inductance, and Energy

3 Properties of Magnetic Materials

4 AC Excitation

5 Permanent Magnets

6 Application of Permanent Magnet Materials

sites.google.com/site/ncpdhbkhn 41

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Permanent Magnets (1)

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Point of maximum energy product

m m

Vol B Vol

H B

µ

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Magnetic Circuits and Magnetic Materials

1 Introduction to Magnetic Circuits

2 Flux Linkage, Inductance, and Energy

3 Properties of Magnetic Materials

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Application of Permanent Magnet

Materials (1)

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N

turns

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Point of maximum energy product

Application of Permanent Magnet

a) Find the magnet length such that the system will

operate on a recoil line which intersects the

maximum B – H product point on the magnetization

curve.

b) Calculate the flux density in the air gap as the

plunger moves back and forth.

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Point of maximum energy product

a) Find the magnet length such that the system will

operate on a recoil line which intersects the

maximum B – H product point on the magnetization

curve.

b) Calculate the flux density in the air gap as the

plunger moves back and forth.

mS

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