EMF EQUATION OF TRANSFORMER

Slides:



Advertisements
Similar presentations
TYPES & CONSTRUCTION OF TRANSFORMERS POWER IN AN IDEAL TRANSFORMER
Advertisements

12: Electromagnetic Induction 12.2 Alternating Current.
Power I, VI, V I max  V max  I, VI, V I max AC Circuits use a similar definition of power as DC circuits. The one detail that need to be included.
AC power. Resonance. Transformers.
Electromagnetic induction
Alternating Current Physics 102 Professor Lee Carkner Lecture 23.
Lecture 20-1 Alternating Current (AC) = Electric current that changes direction periodically ac generator is a device which creates an ac emf/current.
AC Circuits PH 203 Professor Lee Carkner Lecture 23.
Problem # 2-3/4 A core-type transformer rated at 37.5 kVA, 2400 – 480 V, and 60 Hz has a core whose mean length is 1.07 m and whose cross-sectional area.
Alternating Current Physics 102 Professor Lee Carkner Lecture 22.
Lecture No. 11 By. Sajid Hussain Qazi
Lecture No. 15 By. Sajid Hussain Qazi.  Physical explanation of Hysteresis loss ▪ The magnetic core of transformer is made of ′ Cold Rolled Grain Oriented.
EQUIVALENT CIRCUIT OF TRANSFORMER Lecture No. 5 By: Sajid Hussain Qazi.
Transformer Losses & Efficiency
Magnetics Design Primary Constraints:
TRANSFORMER CHAPTER-8.
Transformers.
Electrical Machine-I EE 2107 Dr. Md. Sherajul Islam
Magnetically coupled circuits
Day 4: Transformers Definition of a Transformer Transformer Windings Transformer Operation using Faraday’s Law Step-up & Step-down Transformers Turns Ratio.
12.2 Alternating current 2 hours. Alternating Current The induced emf in a coil rotated within a uniform magnetic field is sinusoidal if the rotation.
AC Circuits (Chapt 33) circuits in which the currents vary in time
Topic 12: Electromagnetic induction 12.2 Alternating current
LECTURE 27 Controlled Rectifiers Dr. Rostamkolai
Electromagnetism Topic 12.2 Alternating Current. Rotating Coils Most of our electricity comes from huge generators in power stations. Most of our electricity.
1 AC Electricity. Time variation of a DC voltage or current 2 I V Current Voltage time t.
Warm-up—1/15/14 What happens when you rotate a coil of conductive material through a uniform magnetic field (not just move it linearly)?
ELECTRICAL BASICS (Chapter 8) Electrical terms Electricity & magnetism Electricity Circuits Magnetism Electrical units Electric potential or eletromotive.
PRESENTATION ON TRANSFORMER PREPARED BY: VRUNDA RANA( ) KRIMA PATEL( ) NIKITA THAKKAR( ) ELEMENTS OF ELECTRICAL ENGINEERING.
Transformers. ► Electric Generators- the main function of an electric generator is to convert mechanical energy to electrical energy. ► Electric motors-
1 Lecture #25 EGR 272 – Circuit Theory II Transformers: Our earlier study of mutual inductance introduced the idea that the magnetic field produced by.
EEE107 Electromagnetic Induction.
Copyright R. Janow – Spring 2015 Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec The Series RLC.
Physics 212 Lecture 21, Slide 1 Physics 212 Lecture 21.
Tuesday April 19, PHYS , Dr. Andrew Brandt PHYS 1444 – Section 02 Lecture #18 Tuesday April 19, 2011 Dr. Andrew Brandt Chapter 29 Lenz Law.
Chapter 31 Lecture 33: Alternating Current Circuits: II HW 11 (problems): 30.58, 30.65, 30.76, 31.12, 31.26, 31.46, 31.56, Due Friday, Dec 11. Final.
The Transformer (Primary has N P turns) (Secondary has N S turns) The source side is called Primary The load side is called Secondary.
1 AGBell – EECT by Andrew G. Bell (260) Lecture 11.
Physics Electricity and Magnetism Lecture 14 - AC Circuits, Resonance Y&F Chapter 31, Sec The Series RLC Circuit. Amplitude and Phase.
1. A loop or wire with a radius of 0.78 m is in the plane of this page, and is rotated so that the loop forms a 23.0 o angle with the page. If there is.
Wednesday, April 11, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #18 Wednesday, April Dr. Andrew Brandt.
Lecture 04Electro Mechanical System1 Ideal Transformer  An ideal transformer  Transformer has no losses and core is infinitely permeable  All fluxes.
Load Transformers These are electromagnetic devices which can ‘step up’ or ‘step down’ ac voltages. A 240 volt supply can be converted to (for example)
Output of Transformer Let, Ø m = main flux, Wb ; B m = maximum flux density, Wb/m 2 ; δ = current density, A/m 2 ; A gi = gross core area, m 2 ; A i =
Transformer DKT Introduction to Transformer.  Transformer is a device that changes ac electrical power at one voltage level to ac electric.
Copyright R. Janow – Fall 2015 Physics Electricity and Magnetism Lecture 14E - AC Circuits & Resonance I – Series LCR Y&F Chapter 31, Sec. 3 – 8.
Practice Problems A horizontal wire is moving vertically upwards in a horizontal magnetic field of strength tesla which is perpendicular to the.
Government Engineering College, Bharuch Department of Electrical Engineering Elements of Electrical Design ( ) NAME:MASTER MUAATASIM EN NO:
AC Current An AC circuit consists of a combination of circuit elements and an AC generator or source The output of an AC generator is sinusoidal and varies.
Question 1 a.Find the magnitude of phase voltage and current b.Find the average power to each phase and the total load. c.Determine the reactive power.
NEGATIVE HALF WAVE RECTIFIERS The analysis of negative half wave rectifier is nearly identical to that of positive half wave rectifier. The only difference.
Transformer A Presentation on. Transformer2 Coil 1 i 1 (t)i 2 (t) Coil 2 M e 1 (t)e 2 (t) S1S1 S2S2 i 1 (t) i 2 (t) The Transformer (Primary has N 1 turns)
Transformer Objectives 1.Describe how a transformer works by watching a video clip. 2.Apply the transformer equations by solving problems.
{ PRESENTATION ON TRANSFORMER. 1. INTRODUCTION: - TRANSFORMER : A static device- Utilized for raising or lowering the voltages. Transfers electrical energy.
Electromagnetism Notes-3
CHAPTER 4 SINGLE-PHASE TRANSFORMER
Electromagnetism Notes-3
Classification of Transformers
There are three parts of a transformer
Electric Machine Transformers
ELE 2103 Dept . of E & E, MIT Manipal
Electromechanical Systems
Transformers A transformer changes the high voltage from the main power lines to the 120 volts your appliances use.
Energy Conversion and Transport George G. Karady & Keith Holbert
Let’s look in detail at each of these four ways of using flux change or motion to produce an emf. Method 1…
AC Transformers Source: OSHA.
C H A P T E R 20 Harmonics. C H A P T E R 20 Harmonics.
LVDT The LVDT's primary winding, P, is energized by a constant amplitude AC source. The magnetic flux thus developed is coupled by the core to the adjacent.
Unit-1 Transformer.
-: Transformer :-.
Presentation transcript:

EMF EQUATION OF TRANSFORMER Lecture No. 4 By. Sajid Hussain Qazi

EMF EQUATION OF TRANSFORMER Let, N1=Number of turns in primary N2=Number of turns in secondary Φm=Maximum flux in core in webers = Bm*A f= frequency of input a.c voltage in hertz

As shown in figure below flux increases from its zero value to its maximum value Φm in one quarter of the cycle i.e., 1/4f seconds, Average rate of change of flux is; , wb/sec or volts

Now, rate of change of flux per turn means induced emf per turn Average emf per turn= 4fΦm ,volt If flux varies sinusoidally, then r.m.s value of induced emf is obtained by multiplying the average value with form factor. Form Factor= r.m.s value/average value=1.11 r.m.s value of emf per turn = 1.11*4*f*Φm = 4.44*f*Φm ,volt

Now, r. m. s value of the induced e. m Now, r.m.s value of the induced e.m.f in whole of the primary winding will be; (induced e.m.f/turn) x no. of primary turns E1= 4.44*N1*f*Bm *A, volt ---(i) Similarly, r.m.s value of the induced e.m.f in whole of the secondary winding will be; (induced e.m.f/turn) x no. of secondary turns E2= 4.44*N2*f*Bm *A, volt ---(ii) It is seen from equation (i and ii) that E1 /N1= E2/ N2= 4.44*f*Φm. It means that e.m.f/turn is same in both the primary and secondary windings.

Assignment Question-1 What down the construction and types of transformers?