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Basic Magnetic07

Jun 04, 2018

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    Design of Magnetic Component 3/7/200

    By zen

    Design of Magnetic Component;by : Ir. ZEN, MT 1

    BASIC MAGNETICSBASIC MAGNETICS

    THEORYTHEORY

    Edited by : Ir. Moh. Zaenal Efendi, MTDepartment Of Electro-industrial Engineering

    EEPIS - ITS

    Design of Magnetic Component;by : Ir. ZEN, MT 2

    BASIC MAGNETICS THEORY

    by : ZENTHE ALLIEN GENERATION

    REFERENCES :

    http://hyperphysics.phy-astr.gsu.edu

    Fundamentals of Power Electronics

    www.electronics-tutorials.com

    INTERNATIONAL RECTIFIER (IRF)

    www.electronics-tutorials.com

    www.radioelectronicschool.com

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    Design of Magnetic Component;by : Ir. ZEN, MT 3

    Basic Relationship of Magnetics

    Design of Magnetic Component;by : Ir. ZEN, MT 4

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    MMF (Magneto Motive Force)

    The quantity of magnetic field force, or "push."

    Design of Magnetic Component;by : Ir. ZEN, MT 6

    MMF can be thought of as the magneticequivalent of electromotive force. You can

    calculate it as -

    The units of MMF are often stated asampere turns (A-t).

    = H le (ampere turns)

    = I N (ampere turns)

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    Magnetic Flux ()The quantity of total field effect, or "substance" of the field.

    Analogous to electric current. (Weber (Wb) or Volt Second)

    Magnetic flux is the product of the average magnetic field times the

    perpendicular area that it penetrates. It is a quantity of convenience

    in the statement of Faraday's Law and in the discussion of objects

    like transformers and solenoids. In the case of an electric generator

    where the magnetic field penetrates a rotating coil, the area used in

    defining the flux is the projection of the coil area onto the plane

    perpendicular to the magnetic field.

    Design of Magnetic Component;by : Ir. ZEN, MT 8

    Flux Density (B)(Webers per metre2 ---- Wb/m2 or Tesla)

    Flux density is simply the total flux divided by the

    cross sectional area of the part through which it

    flows:

    B = / Ae tesla

    Flux density is related to field strength viathepermeability:

    B = H

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    Design of Magnetic Component;by : Ir. ZEN, MT 9

    Effective length ( le ) metre

    The 'effective length' of a core

    is a measure of the distance

    which flux lines travel in

    making a complete circuit of it

    In the toroid example the path length could be determined

    approximately as :

    le = (dl + dm) / 2

    le = (12.7 + 6.3) / 2 = 29.8 mm

    dl

    dm

    Design of Magnetic Component;by : Ir. ZEN, MT 10

    Cross Sectional Area

    Effective Area [ ])metresquare()AorA(

    2ec

    m

    The 'effective area' of a core

    represents the cross sectional

    area of one of its limbs.

    Usually this corresponds

    closely to the physical

    dimensions of the core

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    Cross Sectional Area of Toroid Core

    or

    Ae = hln2(R2/R1) / (1/R1-1/R2) m

    2

    Ae = h ((dl - dm) / 2)

    = 6.3

    ((12.7 - 6.3) / 2) = 20.2 mm2

    dm

    dl

    Design of Magnetic Component;by : Ir. ZEN, MT 12

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    Permeability ()(henrys per metre h/m) -----= L/d

    The specific measure of a material's acceptance of magnetic flux,analogous to the specific resistance of a conductive material () inelectric circuit.

    Just as those materials with high electrical conductivity let electriccurrent through easily, so materials with high permeabilities allowmagnetic flux through more easily than others.

    Materials with high permeabilities include iron and the otherferromagnetic materials. Most plastics, wood, non ferrous metals, airand other fluids have permeabilities very much lower: 0.

    The magnetic permeability, , of a particular material is defined as

    the ratio of flux density to magnetic field strength - = B/H

    Design of Magnetic Component;by : Ir. ZEN, MT 14

    Electric and Magnetic Constants

    The electric permittivity of free space

    The magnetic permeability of free

    space is taken to have the exact value

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    Design of Magnetic Component;by : Ir. ZEN, MT 15

    Km or r: a relative permeability.

    00m ;k ror ==

    Permeability of materials is.

    Approximate maximum permeabilities

    Design of Magnetic Component;by : Ir. ZEN, MT 16

    Magnetic Field Strength (H)(Field Intensity)

    (ampere per metre --- A/m)

    The amount of field force (mmf) distributed over the length of the

    electromagnet. Sometimes referred to as Magnetizing Force.

    The magnetic fields generated by currents and are characterized by the

    magnetic field B measured in Tesla.

    It has been common practice to define another magnetic field quantity, usually

    called the "magnetic field strength" designated by H. It can be defined by the

    relationship

    where

    If the material does not respond to the external magnetic field by producing any

    magnetization, then Km = 1.

    HBB

    H

    == ;

    0= mK

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    Reluctance ( ) or Rm

    (perhenry (H-1) or ampere-turns per weber )

    The opposition to magnetic field flux through a

    given volume of space or material. Analogous to

    electrical resistance.

    Reluctance is the ratio of mmf to flux :

    A

    le

    AeB

    leH

    =

    =

    = H

    B

    where =:

    Design of Magnetic Component;by : Ir. ZEN, MT 18

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    Design of Magnetic Component;by : Ir. ZEN, MT 20

    EMF (Electromotive Force)

    The magnetic force exerted on the charges in a moving

    conductor will generate a voltage (a motional emf). This motional

    emf is one of many settings in which the generated emf is

    described by Faraday's Law.

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    FARADAYS LAW

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    The motional emf expression is an application of Faraday's Law, as can

    be seen from:

    EMF and Faraday's Law

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    Lenz's Law

    When an emf is generated by a change in magnetic flux according to Faraday's

    Law, the polarity of the induced emf is such that it produces a current whosemagnetic field opposes the change which produces it. The induced magnetic

    field inside any loop of wire always acts to keep the magnetic flux in the loop

    constant. In the examples below, if the B field is increasing, the induced field

    acts in opposition to it. If it is decreasing, the induced field acts in the direction

    of the applied field to try to keep it constant.

    Design of Magnetic Component;by : Ir. ZEN, MT 26

    AMPERES LAW

    ----- (N I) Ampere Turns

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    Design of Magnetic Component;by : Ir. ZEN, MT 27

    ----- (N I) Ampere Turns

    Design of Magnetic Component;by : Ir. ZEN, MT 28

    Current density (J)

    (Amperes per square A/m2)

    Current density is simply the total electric

    current divided by the area over which it is

    flowing.

    Generally J is about 1.5 to 5 amps per

    square millimetre. A good starting point is3.5 A/mm2)

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    Design of Magnetic Component;by : Ir. ZEN, MT 30

    Analogy with electric quantities

    resistancereluctance

    current densitymagnetic flux density

    currentmagnetic flux

    conductivitypermeability

    electric field strengthmagnetic field strength

    electromotive force (voltage)magnetomotive force

    Electric QuantityMagnetic Quantity

    Electric analogues

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    Home work ( one week ):

    1.Whats some benefit of understanding of

    Magnetics

    2.Whats differences of MMF and EMF

    3.Explain about process of EMF generation

    4.Explain about magnetic circuit and

    compare with electric circuit

    5.Re-write this hand-out in Indonesia !!!