Transformers Project report

Tanuj Gupta
DASMESH PARIVAR

INTERNATIONAL SCHOOL

  PROJECT REPORT

        ON



  TRANSFORMERS

             Submitted By:


             TANUJ GUPTA


             CLASS: XII


             ROLL NO: ________________
They are so important in our lives
that without them even the electric
bells fitted in our homes won’t
work.
Certificate
This is to certify that Tanuj Gupta, student of Class XII, Dasmesh Parivar International
School, has completed the project titled Transformers during the academic year 2012-
2013 towards partial fulfillment of credit for the Physics practical evaluation of CBSE
2013, and submitted satisfactory report, as compiled in the following pages, under my
supervision.




_________________
Department of Physics
Dasmesh Parivar International School
Acknowledgements
"There are times when silence speaks so much more loudly than words of praise to
only as good as belittle a person, whose words do not express, but only put a
veneer over true feelings, which are of gratitude at this point of time."

I would like to express my sincere gratitude to my physics mentor for his vital
support, guidance and encouragement, without which this project would not
have come forth. I would also like to express my gratitude to the staff of the
Department of Physics at Dasmesh Parivar International School for their support
during the making of this project.




                                             TANUJ GUPTA
INTRODUCTION

The transformer is a device used for converting a
low alternating voltage to a high alternating
voltage or a high alternating voltage into a low
alternating voltage. It is a static electrical device
that transfers energy by inductive coupling
between its winding circuits. Transformers range in
size from a thumbnail-sized coupling transformer
hidden inside a stage microphone to huge units
weighing hundreds of tons used in power plant
substations or to interconnect portions of the
power grid. All operate on the same basic
principles, although the range of designs is wide.
While new technologies have eliminated the need
for transformers in some electronic circuits,
transformers are still found in many electronic
devices. Transformers are essential for high-
voltage electric power transmission, which makes
long-distance transmission economically practical.
A transformer is most widely used device in both
low and high current circuit. In a transformer, the
electrical energy transfer from one circuit to
another circuit takes place without the use of
moving parts. A transformer which increases the
voltages is called a step-up transformer. A
transformer which decreases the A.C. voltages is
called a step-down transformer.

              Transformer is, therefore, an essential
piece of apparatus both for high and low current
circuits.




       Close-up of single-phase pole mount transformer.
PRINCIPLE

It is based on the principle of mutual induction that
is if a varying current is set-up in a circuit then
induced e.m.f. is produced in the neighboring
circuit. The varying current in a circuit produce
varying magnetic flux which induces e.m.f. in the
neighboring circuit.
CONSTRUCTION
A transformer consists of a rectangular shaft iron
core made of laminated sheets, well insulated from
one another. Two coils p1 & p2 and s1 & s2 are
wound on the same core, but are well insulated
with each other. Note that the both the coils are
insulated from the core, the source of alternating
e.m.f is connected to p1p2, the primary coil and a
load resistance R is connected to s1 s2, the
secondary coil through an open switch S. thus
there can be no current through the sec. coil so
long   as   the   switch   is   open.   For   an   ideal
transformer, we assume that the resistance of the
primary & secondary winding is negligible. Further,
the energy loses due to magnetic the iron core is
also negligible. For operation at low frequency, we
may have a soft iron. The soft iron core is
insulating by joining thin iron strips coated with
varnish to insulate them to reduce energy losses
by eddy currents. The input circuit is called
primary. And the output circuit is called secondary.




 An ideal voltage step-down transformer. The secondary current arises from the
       action of the secondary EMF on the (not shown) load impedance.




                   The ideal transformer as a circuit element
THEORY AND WORKING

When an altering e.m.f. is supplied to the primary
coil p1p2, an alternating current starts falling in it.
The altering current in the primary produces a
changing magnetic flux, which induces altering
voltage in the primary as well as in the secondary.
In a good-transformer, whole of the magnetic flux
linked   with   primary   is   also   linked   with   the
secondary, and then the induced e.m.f. induced in
each turn of the secondary is equal to that induced
in each turn of the primary. Thus if Ep and Es be
the instantaneous values of the e.m.f.’s induced in
the primary and the secondary and Np and Ns are
the no. of turns of the primary secondary coils of
the transformer and, Dфь / dt = rate of change of
flux in each turn of the coil at this instant, we have
Ep = -Np Dфь/dt                         (1)
Es = -Ns Dфь/dt                            (2)


Since the above relations are true at every instant,

so by dividing 2 by 1, we get


          Es / Ep = - Ns / Np                           (3)


As Ep is the instantaneous value of back e.m.f

induced     in   the       primary   coil   p1,   so    the

instantaneous current in primary coil is due to the

difference (E – Ep ) in the instantaneous values of

the applied and back e.m.f. further if Rp is the

resistance o, p1p2 coil, then the           instantaneous

current Ip in the primary coil is given by


              I =E – Ep / Rp


            E – Ep     =    Ip Rp
When the resistance of the primary is small, Rp Ip

can be neglected so therefore


               E – Ep        = 0 or Ep = E


Thus back e.m.f = input e.m.f


Hence equation 3 can be written as Es / Ep = Es / E

= output e.m.f / input e.m.f = Ns / Np = K


Where K is constant, called turn or transformation

ratio.


In a step up transformer


            Es > E so K > 1, hence Ns > Np


In a step down transformer


         Es < E so K < 1, hence Ns < Np


If Ip=value of primary current at the same instant t
And Is =value of sec. current at this instant,

then Input power at the instant t = Ep Ip and

Output power at the same instant                 =   Es Is


If there are no losses of power in the transformer,

then Input power = output power or


            Ep Ip      =       Es Is            Or


            Es / E p       =      Ip / Is   =   K


In a step up transformer

As k > 1, so Ip > Is or Is < Ip

I.e. current in sec. is weaker when secondary
voltage is higher. Hence, whatever we gain in
voltage, we lose in current in the same ratio.
Similarly it can be shown, that in a step down
transformer, whatever we lose in voltage, we gain
in current in the same ratio.Thus a step up
transformer in reality steps down the current & a
step down transformer steps up the current.




BASIC IDEA OF STEP DOWN TRANSFORMER




BASIC IDEA OF STEP UP TRANSFORMER
EFFICIENCY
Efficiency of a transformer is defined as the ratio of
output power to the input power i.e.

η = output power / input power = Es Is / Ep Ip

Thus in an ideal transformer, where there is no
power losses, η = 1. But in actual practice, there
are many power losses; therefore the efficiency of
transformer is less than one.
ENERGY LOSSES
In practice, the output energy of a transformer is always
less than the input energy, because energy losses occur
due to a number of reasons as explained below.
1. Loss of Magnetic Flux: The coupling between the
coils is seldom perfect. So, whole of the magnetic flux
produced by the primary coil is not linked up with the
secondary coil.
2. Iron Loss: In actual iron cores in spite of lamination,
Eddy currents are produced. The magnitude of eddy
current may, however be small. And a part of energy is
lost as the heat produced in the iron core.
3. Copper Loss: In practice, the coils of the transformer
possess resistance. So a part of the energy is lost due to
the heat produced in the resistance of the coil.
4. Hysteresis Loss: The alternating current in the coil
tapes the iron core through complete cycle of
magnetization. So Energy is lost due to hysteresis.
5. Magneto restriction: The alternating current in the
Transformer may be set its parts in to vibrations and
sound may be produced. It is called humming. Thus, a
part of energy may be lost due to humming.



        USES OF TRANSFORMER
A transformer is used in almost all a.c. operations

    In voltage regulator for T.V., refrigerator,
    computer, air conditioner etc.
    In the induction furnaces.
    A step down transformer is used for welding
    purposes.
    A step down transformer is used for obtaining
    large current.
    A    step   up   transformer     is   used    for   the
    production of X-Rays and NEON advertisement.
    Transformers are used in voltage regulators
    and stabilized power supplies.
Transformers are used in the transmissions of
a.c. over long distances.
Small transformers are used in Radio sets,
telephones, loud speakers and electric bells
etc.




           A Big Transformer
Bibliography
The data used in this project was taken from the
following sources:
   www.google.com
   www.wikipedia.com
   www.scribd.com
   Sears and Zemansky’s University Physics




             The End

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Transformers Project report

  • 1. DASMESH PARIVAR INTERNATIONAL SCHOOL PROJECT REPORT ON TRANSFORMERS Submitted By: TANUJ GUPTA CLASS: XII ROLL NO: ________________
  • 2. They are so important in our lives that without them even the electric bells fitted in our homes won’t work.
  • 3. Certificate This is to certify that Tanuj Gupta, student of Class XII, Dasmesh Parivar International School, has completed the project titled Transformers during the academic year 2012- 2013 towards partial fulfillment of credit for the Physics practical evaluation of CBSE 2013, and submitted satisfactory report, as compiled in the following pages, under my supervision. _________________ Department of Physics Dasmesh Parivar International School
  • 4. Acknowledgements "There are times when silence speaks so much more loudly than words of praise to only as good as belittle a person, whose words do not express, but only put a veneer over true feelings, which are of gratitude at this point of time." I would like to express my sincere gratitude to my physics mentor for his vital support, guidance and encouragement, without which this project would not have come forth. I would also like to express my gratitude to the staff of the Department of Physics at Dasmesh Parivar International School for their support during the making of this project. TANUJ GUPTA
  • 5. INTRODUCTION The transformer is a device used for converting a low alternating voltage to a high alternating voltage or a high alternating voltage into a low alternating voltage. It is a static electrical device that transfers energy by inductive coupling between its winding circuits. Transformers range in size from a thumbnail-sized coupling transformer hidden inside a stage microphone to huge units weighing hundreds of tons used in power plant substations or to interconnect portions of the power grid. All operate on the same basic principles, although the range of designs is wide. While new technologies have eliminated the need for transformers in some electronic circuits, transformers are still found in many electronic devices. Transformers are essential for high- voltage electric power transmission, which makes long-distance transmission economically practical. A transformer is most widely used device in both low and high current circuit. In a transformer, the electrical energy transfer from one circuit to another circuit takes place without the use of moving parts. A transformer which increases the voltages is called a step-up transformer. A
  • 6. transformer which decreases the A.C. voltages is called a step-down transformer. Transformer is, therefore, an essential piece of apparatus both for high and low current circuits. Close-up of single-phase pole mount transformer.
  • 7. PRINCIPLE It is based on the principle of mutual induction that is if a varying current is set-up in a circuit then induced e.m.f. is produced in the neighboring circuit. The varying current in a circuit produce varying magnetic flux which induces e.m.f. in the neighboring circuit.
  • 8. CONSTRUCTION A transformer consists of a rectangular shaft iron core made of laminated sheets, well insulated from one another. Two coils p1 & p2 and s1 & s2 are wound on the same core, but are well insulated with each other. Note that the both the coils are insulated from the core, the source of alternating e.m.f is connected to p1p2, the primary coil and a load resistance R is connected to s1 s2, the secondary coil through an open switch S. thus there can be no current through the sec. coil so long as the switch is open. For an ideal transformer, we assume that the resistance of the primary & secondary winding is negligible. Further, the energy loses due to magnetic the iron core is also negligible. For operation at low frequency, we may have a soft iron. The soft iron core is insulating by joining thin iron strips coated with varnish to insulate them to reduce energy losses
  • 9. by eddy currents. The input circuit is called primary. And the output circuit is called secondary. An ideal voltage step-down transformer. The secondary current arises from the action of the secondary EMF on the (not shown) load impedance. The ideal transformer as a circuit element
  • 10. THEORY AND WORKING When an altering e.m.f. is supplied to the primary coil p1p2, an alternating current starts falling in it. The altering current in the primary produces a changing magnetic flux, which induces altering voltage in the primary as well as in the secondary. In a good-transformer, whole of the magnetic flux linked with primary is also linked with the secondary, and then the induced e.m.f. induced in each turn of the secondary is equal to that induced in each turn of the primary. Thus if Ep and Es be the instantaneous values of the e.m.f.’s induced in the primary and the secondary and Np and Ns are the no. of turns of the primary secondary coils of the transformer and, Dфь / dt = rate of change of flux in each turn of the coil at this instant, we have Ep = -Np Dфь/dt (1)
  • 11. Es = -Ns Dфь/dt (2) Since the above relations are true at every instant, so by dividing 2 by 1, we get Es / Ep = - Ns / Np (3) As Ep is the instantaneous value of back e.m.f induced in the primary coil p1, so the instantaneous current in primary coil is due to the difference (E – Ep ) in the instantaneous values of the applied and back e.m.f. further if Rp is the resistance o, p1p2 coil, then the instantaneous current Ip in the primary coil is given by I =E – Ep / Rp E – Ep = Ip Rp
  • 12. When the resistance of the primary is small, Rp Ip can be neglected so therefore E – Ep = 0 or Ep = E Thus back e.m.f = input e.m.f Hence equation 3 can be written as Es / Ep = Es / E = output e.m.f / input e.m.f = Ns / Np = K Where K is constant, called turn or transformation ratio. In a step up transformer Es > E so K > 1, hence Ns > Np In a step down transformer Es < E so K < 1, hence Ns < Np If Ip=value of primary current at the same instant t
  • 13. And Is =value of sec. current at this instant, then Input power at the instant t = Ep Ip and Output power at the same instant = Es Is If there are no losses of power in the transformer, then Input power = output power or Ep Ip = Es Is Or Es / E p = Ip / Is = K In a step up transformer As k > 1, so Ip > Is or Is < Ip I.e. current in sec. is weaker when secondary voltage is higher. Hence, whatever we gain in voltage, we lose in current in the same ratio. Similarly it can be shown, that in a step down transformer, whatever we lose in voltage, we gain in current in the same ratio.Thus a step up
  • 14. transformer in reality steps down the current & a step down transformer steps up the current. BASIC IDEA OF STEP DOWN TRANSFORMER BASIC IDEA OF STEP UP TRANSFORMER
  • 15. EFFICIENCY Efficiency of a transformer is defined as the ratio of output power to the input power i.e. η = output power / input power = Es Is / Ep Ip Thus in an ideal transformer, where there is no power losses, η = 1. But in actual practice, there are many power losses; therefore the efficiency of transformer is less than one.
  • 16. ENERGY LOSSES In practice, the output energy of a transformer is always less than the input energy, because energy losses occur due to a number of reasons as explained below. 1. Loss of Magnetic Flux: The coupling between the coils is seldom perfect. So, whole of the magnetic flux produced by the primary coil is not linked up with the secondary coil. 2. Iron Loss: In actual iron cores in spite of lamination, Eddy currents are produced. The magnitude of eddy current may, however be small. And a part of energy is lost as the heat produced in the iron core. 3. Copper Loss: In practice, the coils of the transformer possess resistance. So a part of the energy is lost due to the heat produced in the resistance of the coil. 4. Hysteresis Loss: The alternating current in the coil tapes the iron core through complete cycle of magnetization. So Energy is lost due to hysteresis. 5. Magneto restriction: The alternating current in the
  • 17. Transformer may be set its parts in to vibrations and sound may be produced. It is called humming. Thus, a part of energy may be lost due to humming. USES OF TRANSFORMER A transformer is used in almost all a.c. operations In voltage regulator for T.V., refrigerator, computer, air conditioner etc. In the induction furnaces. A step down transformer is used for welding purposes. A step down transformer is used for obtaining large current. A step up transformer is used for the production of X-Rays and NEON advertisement. Transformers are used in voltage regulators and stabilized power supplies.
  • 18. Transformers are used in the transmissions of a.c. over long distances. Small transformers are used in Radio sets, telephones, loud speakers and electric bells etc. A Big Transformer
  • 19. Bibliography The data used in this project was taken from the following sources:  www.google.com  www.wikipedia.com  www.scribd.com  Sears and Zemansky’s University Physics The End