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BASIC MAGNETICSBASIC MAGNETICS
THEORYTHEORY
Edited by : Ir. Moh. Zaenal Efendi, MTDepartment Of Electro-industrial Engineering
EEPIS - ITS
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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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Basic Relationship of Magnetics
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MMF (Magneto Motive Force)
The quantity of magnetic field force, or "push."
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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.
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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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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
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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
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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
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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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Km or r: a relative permeability.
00m ;k ror ==
Permeability of materials is.
Approximate maximum permeabilities
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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 =:
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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.
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AMPERES LAW
----- (N I) Ampere Turns
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----- (N I) Ampere Turns
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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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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 !!!