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Presentation on -Transformers
By-SUNEEL KUMAR
Transformer
An A.C. device used to change high voltage low
current A.C. into low voltage high current A.C. and
vice-versa without changing the frequency
In brief,
1. Transfers electric power from one circuit to another
2. It does so without a change of frequency
3. It accomplishes this by electromagnetic induction
4. Where the two electric circuits are in mutual
inductive influence of each other.
Principle of operation
It is based on
principle of MUTUAL
INDUCTION.
According to which
an e.m.f. is induced
in a coil when
current in the
neighbouring coil
changes.
Constructional detail : Shell type
• Windings are wrapped around the center leg of a
laminated core.
Core type
• Windings are wrapped around two sides of a laminated square
core.
Sectional view of transformers
Note:
High voltage conductors are smaller cross section conductors
than the low voltage coils
Construction of transformer from
stampings
Core type
Fig1: Coil and laminations of
core type transformer
Fig2: Various types of cores
Shell type
• The HV and LV
windings are split
into no. of sections
• Where HV winding
lies between two LV
windings
• In sandwich coils
leakage can be
controlledFig: Sandwich windings
Cut view of transformer
Transformer with conservator and
breather
Working of a transformer
1. When current in the primary coil
changes being alternating in
nature, a changing magnetic field
is produced
2. This changing magnetic field gets
associated with the secondary
through the soft iron core
3. Hence magnetic flux linked with
the secondary coil changes.
4. Which induces e.m.f. in the
secondary.
Ideal Transformers
• Zero leakage flux:
-Fluxes produced by the primary and secondary currents
are confined within the core
• The windings have no resistance:
- Induced voltages equal applied voltages
• The core has infinite permeability
- Reluctance of the core is zero
- Negligible current is required to establish magnetic
flux
• Loss-less magnetic core
- No hysteresis or eddy currents
Ideal transformer
V1 – supply voltage ; I1- noload input current ;
V2- output voltgae; I2- output current
Im- magnetising current;
E1-self induced emf ; E2- mutually induced emf
Phasor diagram: Transformer on No-
load
Approximate equivalent circuit
• Since the noload current is 1% of the full load
current, the nolad circuit can be neglected
Transformer Efficiency
Electrical Machines
Transformer efficiency is defined as (applies to motors, generators and
transformers):
%100×=
in
out
P
P
η
%100×
+
=
lossout
out
PP
P
η
Types of losses incurred in a transformer:
Copper I2
R losses
Hysteresis losses
Eddy current losses
Therefore, for a transformer, efficiency may be calculated using the following:
%100
cos
cos
x
IVPP
IV
SScoreCu
SS
θ
θ
η
++
=
All day efficiency
hours)24(
kWhinInput
kWhinoutput
in wattsinput
in wattsputout
efficiencycommercialordinary
day forall =
=
η
•All day efficiency is always less than the commercial efficiency
THANK YOU

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Transformer

  • 2. Transformer An A.C. device used to change high voltage low current A.C. into low voltage high current A.C. and vice-versa without changing the frequency In brief, 1. Transfers electric power from one circuit to another 2. It does so without a change of frequency 3. It accomplishes this by electromagnetic induction 4. Where the two electric circuits are in mutual inductive influence of each other.
  • 3. Principle of operation It is based on principle of MUTUAL INDUCTION. According to which an e.m.f. is induced in a coil when current in the neighbouring coil changes.
  • 4. Constructional detail : Shell type • Windings are wrapped around the center leg of a laminated core.
  • 5. Core type • Windings are wrapped around two sides of a laminated square core.
  • 6. Sectional view of transformers Note: High voltage conductors are smaller cross section conductors than the low voltage coils
  • 8. Core type Fig1: Coil and laminations of core type transformer Fig2: Various types of cores
  • 9. Shell type • The HV and LV windings are split into no. of sections • Where HV winding lies between two LV windings • In sandwich coils leakage can be controlledFig: Sandwich windings
  • 10. Cut view of transformer
  • 12. Working of a transformer 1. When current in the primary coil changes being alternating in nature, a changing magnetic field is produced 2. This changing magnetic field gets associated with the secondary through the soft iron core 3. Hence magnetic flux linked with the secondary coil changes. 4. Which induces e.m.f. in the secondary.
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  • 14. Ideal Transformers • Zero leakage flux: -Fluxes produced by the primary and secondary currents are confined within the core • The windings have no resistance: - Induced voltages equal applied voltages • The core has infinite permeability - Reluctance of the core is zero - Negligible current is required to establish magnetic flux • Loss-less magnetic core - No hysteresis or eddy currents
  • 15. Ideal transformer V1 – supply voltage ; I1- noload input current ; V2- output voltgae; I2- output current Im- magnetising current; E1-self induced emf ; E2- mutually induced emf
  • 17. Approximate equivalent circuit • Since the noload current is 1% of the full load current, the nolad circuit can be neglected
  • 18. Transformer Efficiency Electrical Machines Transformer efficiency is defined as (applies to motors, generators and transformers): %100×= in out P P η %100× + = lossout out PP P η Types of losses incurred in a transformer: Copper I2 R losses Hysteresis losses Eddy current losses Therefore, for a transformer, efficiency may be calculated using the following: %100 cos cos x IVPP IV SScoreCu SS θ θ η ++ =
  • 19. All day efficiency hours)24( kWhinInput kWhinoutput in wattsinput in wattsputout efficiencycommercialordinary day forall = = η •All day efficiency is always less than the commercial efficiency