SEMINAR PROJECT
         ON

MAGNETIZING CURRENT
         &
     EFFECT ON
 SYNCHRONOUS MOTOR


          COLLEGE OF ENGINEERING & TECHNOLOGY
          NAME: ADITYA PRASAD MISHRA
          REGD NO:0901106227
          BRANCH: ELECTRICAL ENGINEERING
Contents:

1. Definition of magnetizing current.
2. Properties
3. B-H curve
4. Magnetization principle
5. Synchronous motor relation
MAGNETIZING CURRENT:

 MAGNETIZES THE MATERIAL.
 ORIENTS THE DOMAIN OF THE
  MAGNETIC MATERIAL.
 STORES ENERGY IN THE FORM OF
  MAGNETIC FIELD.
PROPERTIES OF MAGNETISING
CURRENT:
1. Lags behind the voltage by 90 degrees phase
   shift:
  The voltage mentioned here is the
   magnitude,obeying KVL.

   V= -N*d(flux)/dt
   Or v= -N*d(L/N*i)/dt        ...as N*flux = L*i
   Or v=-L*d(i)/dt
        Taking i=i1 sin(wt)
       we have : v=-Liw sin(wt+Pi/2)
  ...neg. sign shows direction of the drop
2.Ideally in phase to the the flux,it produces.
 Ideal means the domain produces dipoles in
   proportional to the input i.e. the current.
 Magnetic saturation & Retentivity absent.
          ( Hence the magnetization curve is linear)
 Practically, the curve exerts non linearity owing to:
       1. Saturation effects.
       2. Retention property of the magnetic dipoles
         to lie on the easy axis of magnetisation.
B~H CURVE OR
MAGNETIZATION CURVE

o B~H curves are of two types:
I.  Linear curve
II. Non linear curve
o We will consider both of them in ideal and
    actual cases.
LINEAR CURVE (IDEAL)

o Ideal case of study, i.e. magnetic saturation is
  neglected.

o Flux varies linearly, with respect to magnetizing
  current.

o So, waveforms are identical as flux is
  proportional to magnetizing current.

o Also true for non-magnetic materials.
Magnetization curve
NON LINEAR CURVE(IDEAL)

o Occurs due to saturation of magnetic materials.

o The magnetic dipoles formation rate reduces as
  current increases.

o Effects is production of harmonics, especially
  the 3rd ones.

o Flux & current waveforms are always in same
  phase.
Magnetization curve
continued. . .


o Magnetic saturation doesn’t result in power loss,
 it merely distorts current waveforms.

o 3rd harmonic is neglected as these cannot be
  represented for mathematical analysis.(study of
  phasors)
ACTUAL CASE
o Magnetization curve involves hysteresis.

o Hysteresis caused by retention properties of
  magnetic dipoles.

o Retention means the presence of flux even in the
  absence of magnetizing current.

o Exists in anisotropic materials, where dipoles align
  in the easy axis of magnetization.
Magnetization curve
Continued…
o Hysteresis effect gives rise to energy loss.

o Flux lags the current, hence exciting current
  doesn’t lag the voltage by 90 degrees.

o Component which is in phase with flux
  represents magnetizing part & component in
  90 degrees phase shift with flux gives core loss

o A sinusoidal current produces a flat topped
  wave.
PRINCIPLE OF MAGNETIZATION

o It occurs due to the magnetic dipole
  moments of a compound bar magnet.
o Magnetic moment inside a bar magnet is
  influenced by:
    o    intrinsic movement of unpaired
      electrons.
    o     orbital movement of electrons around
      nucleus.
    o      intrinsic movements of protons.
The reason a piece of magnetic
material spontaneously divides
into separate domains, rather than
exist in a state with magnetization
in the same direction throughout
the material, is to minimize its
internal energy
continued.     . .
o Dipoles get aligned due to mechanical energy,
  transformed from electrical energy.

o As the current increases, dipoles alignment
  rate decreases due to crowding, thereby
  requiring more electric energy.

o When there is no current applied, dipoles
  arrange themselves n an energetically
  favorable direction of spontaneous
  magnetization.
MAGNETIZING CURRENT IN
SYNCHRONOUS MOTOR
     o Air gap flux=terminal voltage
                     1.44[3.14(fkN)]
        Where, f= frequency
                 k=winding factor
                 N=no. of turns.
        oConstant terminal voltage implies
          constant air gap flux.
        oSynchronous           motor        draws
          magnetizing current to setup the flux
          in the magnetic circuit of the device.
 Synchronous m/c: double excited.
     1. field winding: d.c. excited
     2. armature winding: a.c. excited.
Field current sufficient to generate the
flux

o Magnetizing current from ac source is zero.

o Normal excitation leads to unity power factor.

Field current lesser than normal one
o allows ac source to give magnetizing current.

o Under excitation it leads to lagging power
  factor.
field current greater than normal current

o Motor is over excited.
o Excess flux is neutralized by armature
  winding.
o Demagnetizing current (leads voltage by 90
  degrees) is drawn from ac source.
o Operates under leading power factor.
Powerfactor: physical analogy

Mac here is dragging a heavy load . Mac’s Working Power (or
Actual Power) in the forward direction, where he most wants his load to
travel, is KW.
Unfortunately, he would
get a tremendous backache, so his shoulder height adds a little Reactive
Power, or KVAR.
  The Apparent Power Mac is dragging, KVA, is this “vectorial
summation”
of KVAR and KW.
POWER FACTOR VARIATION IN A SYNCHRONOUS
MOTOR

o Inverted V graph shows the variation of
  power factor w.r.t field current at const load.



o The compounding curve justifies the
  magnetizing current needed to balance the
  operation of a motor.
CONTROL OF POWER FACTOR BY SYNCHRONOUS
 MOTOR
o Power factor control decides the losses & real
  power needed to fetch a load.

o Poor power factor means more real power
  supply to meet a load demand.

o Synchronous power factor can operate at
  leading power factor, hence improves power
  factor of the system.
Continued. . .

o This reduces the KVA demand of load &
   hence :
i. Less KVA supplied from the supply.
ii. Less current implies less losses.
o Special type of synchronous motor is
    used, synchronous condenser.
NOTE
The magnetizing property of magnetic materials sets up an open field
   for storage of energy in magnetic form. This is vital because
   electromagnetic device works on the conversion of electrical energy
   into mechanical energy & vice-versa.
ELECTRICAL ENERGY MAGNETIC ENERGY MECHANICAL ENERGY
Studying the magnetic energy we need to learn, what actually creates
   this energy & how it is stored??? This is what we need to explore.
The main reason for the control of power factor of a synchronous motor
   is this magnetization.
Therefore, to have power factor control we need to have basic idea for
   the magnetizing current & then atomic view (electrons protons)
   responsible for the game. . .
Thank you

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Magnetization curve

  • 1. SEMINAR PROJECT ON MAGNETIZING CURRENT & EFFECT ON SYNCHRONOUS MOTOR COLLEGE OF ENGINEERING & TECHNOLOGY NAME: ADITYA PRASAD MISHRA REGD NO:0901106227 BRANCH: ELECTRICAL ENGINEERING
  • 2. Contents: 1. Definition of magnetizing current. 2. Properties 3. B-H curve 4. Magnetization principle 5. Synchronous motor relation
  • 3. MAGNETIZING CURRENT:  MAGNETIZES THE MATERIAL.  ORIENTS THE DOMAIN OF THE MAGNETIC MATERIAL.  STORES ENERGY IN THE FORM OF MAGNETIC FIELD.
  • 4. PROPERTIES OF MAGNETISING CURRENT: 1. Lags behind the voltage by 90 degrees phase shift: The voltage mentioned here is the magnitude,obeying KVL. V= -N*d(flux)/dt Or v= -N*d(L/N*i)/dt ...as N*flux = L*i Or v=-L*d(i)/dt Taking i=i1 sin(wt) we have : v=-Liw sin(wt+Pi/2) ...neg. sign shows direction of the drop
  • 5. 2.Ideally in phase to the the flux,it produces.  Ideal means the domain produces dipoles in proportional to the input i.e. the current.  Magnetic saturation & Retentivity absent. ( Hence the magnetization curve is linear)  Practically, the curve exerts non linearity owing to: 1. Saturation effects. 2. Retention property of the magnetic dipoles to lie on the easy axis of magnetisation.
  • 6. B~H CURVE OR MAGNETIZATION CURVE o B~H curves are of two types: I. Linear curve II. Non linear curve o We will consider both of them in ideal and actual cases.
  • 7. LINEAR CURVE (IDEAL) o Ideal case of study, i.e. magnetic saturation is neglected. o Flux varies linearly, with respect to magnetizing current. o So, waveforms are identical as flux is proportional to magnetizing current. o Also true for non-magnetic materials.
  • 9. NON LINEAR CURVE(IDEAL) o Occurs due to saturation of magnetic materials. o The magnetic dipoles formation rate reduces as current increases. o Effects is production of harmonics, especially the 3rd ones. o Flux & current waveforms are always in same phase.
  • 11. continued. . . o Magnetic saturation doesn’t result in power loss, it merely distorts current waveforms. o 3rd harmonic is neglected as these cannot be represented for mathematical analysis.(study of phasors)
  • 12. ACTUAL CASE o Magnetization curve involves hysteresis. o Hysteresis caused by retention properties of magnetic dipoles. o Retention means the presence of flux even in the absence of magnetizing current. o Exists in anisotropic materials, where dipoles align in the easy axis of magnetization.
  • 14. Continued… o Hysteresis effect gives rise to energy loss. o Flux lags the current, hence exciting current doesn’t lag the voltage by 90 degrees. o Component which is in phase with flux represents magnetizing part & component in 90 degrees phase shift with flux gives core loss o A sinusoidal current produces a flat topped wave.
  • 15. PRINCIPLE OF MAGNETIZATION o It occurs due to the magnetic dipole moments of a compound bar magnet. o Magnetic moment inside a bar magnet is influenced by: o intrinsic movement of unpaired electrons. o orbital movement of electrons around nucleus. o intrinsic movements of protons.
  • 16. The reason a piece of magnetic material spontaneously divides into separate domains, rather than exist in a state with magnetization in the same direction throughout the material, is to minimize its internal energy
  • 17. continued. . . o Dipoles get aligned due to mechanical energy, transformed from electrical energy. o As the current increases, dipoles alignment rate decreases due to crowding, thereby requiring more electric energy. o When there is no current applied, dipoles arrange themselves n an energetically favorable direction of spontaneous magnetization.
  • 18. MAGNETIZING CURRENT IN SYNCHRONOUS MOTOR o Air gap flux=terminal voltage 1.44[3.14(fkN)] Where, f= frequency k=winding factor N=no. of turns. oConstant terminal voltage implies constant air gap flux. oSynchronous motor draws magnetizing current to setup the flux in the magnetic circuit of the device.
  • 19.  Synchronous m/c: double excited. 1. field winding: d.c. excited 2. armature winding: a.c. excited.
  • 20. Field current sufficient to generate the flux o Magnetizing current from ac source is zero. o Normal excitation leads to unity power factor. Field current lesser than normal one o allows ac source to give magnetizing current. o Under excitation it leads to lagging power factor.
  • 21. field current greater than normal current o Motor is over excited. o Excess flux is neutralized by armature winding. o Demagnetizing current (leads voltage by 90 degrees) is drawn from ac source. o Operates under leading power factor.
  • 22. Powerfactor: physical analogy Mac here is dragging a heavy load . Mac’s Working Power (or Actual Power) in the forward direction, where he most wants his load to travel, is KW. Unfortunately, he would get a tremendous backache, so his shoulder height adds a little Reactive Power, or KVAR. The Apparent Power Mac is dragging, KVA, is this “vectorial summation” of KVAR and KW.
  • 23. POWER FACTOR VARIATION IN A SYNCHRONOUS MOTOR o Inverted V graph shows the variation of power factor w.r.t field current at const load. o The compounding curve justifies the magnetizing current needed to balance the operation of a motor.
  • 24. CONTROL OF POWER FACTOR BY SYNCHRONOUS MOTOR o Power factor control decides the losses & real power needed to fetch a load. o Poor power factor means more real power supply to meet a load demand. o Synchronous power factor can operate at leading power factor, hence improves power factor of the system.
  • 25. Continued. . . o This reduces the KVA demand of load & hence : i. Less KVA supplied from the supply. ii. Less current implies less losses. o Special type of synchronous motor is used, synchronous condenser.
  • 26. NOTE The magnetizing property of magnetic materials sets up an open field for storage of energy in magnetic form. This is vital because electromagnetic device works on the conversion of electrical energy into mechanical energy & vice-versa. ELECTRICAL ENERGY MAGNETIC ENERGY MECHANICAL ENERGY Studying the magnetic energy we need to learn, what actually creates this energy & how it is stored??? This is what we need to explore. The main reason for the control of power factor of a synchronous motor is this magnetization. Therefore, to have power factor control we need to have basic idea for the magnetizing current & then atomic view (electrons protons) responsible for the game. . .