Active Magnetic Bearing

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“DESIGN OF ACTIVE MAGNETIC BEARING” Presented By JADHAV MANORANJAN A. Guided By Prof . S. B. BELKAR

Transcript of Active Magnetic Bearing

Page 1: Active Magnetic Bearing

“DESIGN OF ACTIVE MAGNETIC BEARING”

Presented ByJADHAV

MANORANJAN A.Guided By

Prof . S. B. BELKAR

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Introduction

MagnetismMagnetic field

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Magnetism Magnetic Flux Density

B = magnetic flux densitym = magnetic permeability

H = magnetic field

HB

r 0m0 = permeability of free

spacemr = relative permeability

1

1

diamagnetic

paramagnetic

ferromagnetic

r

niH

2

multiple loops of wire, n

1

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Magnetism Magnetic Field

Magnetic field, H, is found around a magnet or a current carrying body.

r

iH

2

idsH

(for one current loop)

H

i

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Magnetism Lorentz Force

f = forceQ = electric chargeE = electric fieldV = velocity of charge

QB = magnetic flux

density

BvEQf

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Magnetism Lorentz Force

Simplification:

BvQf

Source: MIT Physics Dept.

website

BvEQf

BvE

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Magnetism Lorentz Force

Further simplification:

Bif

BvQf

vQi

force perpendicular to flux!

f

i

B

Analogous Wire

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MAGNETIC BEARINGBearing which supports a load using magnetic levitation

Advantages of magnetic bearings: contact-free no lubricant (no) maintenance tolerable against heat, cold, vacuum, chemicals low losses very high rotational speeds

Disadvantages: complexity high initial cost

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MAGNETIC BEARING TYPESPASSIVE MAGNETIC BEARING Not electrically controlled, Permanent magnets

ACTIVE MAGNETIC BEARING Electrically controlled, Electromagnets

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Principle of operation: Magnetic Levitation

Model of Active Magnetic Bearing

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Active Magnetic Bearings Elements of System

Electromagnet Rotor Stator Position Sensor Controller Amplifier

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Radial Bearing Configuration: for radial force balancingAxial Bearing Configuration: for axial force balancingPosition Transducers:

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Auxiliary Bearing System

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Sensors

Controller

Power Amplifiers

Control system:

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Principle of radial and axial force

Where ,

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magnetic flux in the air gap

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The axial force

permeances of bias & axial control fluxes Pb & Px

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Analysis of AMB system using Finite Element Method

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Performance relative to hydrodynamic bearing

REQUIREMENTS

MAGNETIC BEARING

HYDRODYNAMIC BEARING

High loads low high

Speed high low

Sealing Not required required

Unbalance no yes

Losses Very low high

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ADVANTAGES OF AMB

•NON CONTACT MOTION

•HIGH ROTATING SPEED

•NO LUBRICATION

•INCREASE IN OPERATING TEMPERATURE

RANGE

•ACTIVE NATURE

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DISADVANTAGES OF AMB

•NO LINEARITY

•ROTOR HEATING

•LARGER SIZE

•HIGH COST

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APPLICATIONS OF AMB

•Image display unit

•High precision lathe

•Turbo expander

•Turbo compressor

•High speed milling

•Machine tool spindle

•Maglev Trains

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Applications Maglev Trains

Maglev = Magnetic Levitation150 mm levitation over guideway track

undisturbed from small obstacles (snow, debris, etc.)

typical ave. speed of 350 km/h (max 500 km/h)what if? Paris-Moscow in 7 hr 10 min (2495 km)!

stator: track, rotor: magnets on train

Source: DiscoveryChannel.com

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Applications Maglev Trains

Maglev in Shanghai- complete in 2004- airport to financial district (30 km)- world‘s fastest maglev in commercial operation

(501 km/h)- service speed of 430 km/h

Source: www.monorails.org

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THANK YOU