Electromagnetic Induction

Slides:



Advertisements
Similar presentations
Electromagnetic Induction
Advertisements

Alternating Current Circuits
Transformers Noadswood Science, 2011.
Electromagnetic Oscillations and Alternating Current
12: Electromagnetic Induction 12.2 Alternating Current.
Alternating Current Circuits
Alternating Current Circuits
Noadswood Science,  To understand how step-up and step-down transformers work Monday, August 10, 2015.
Day 4: Transformers Definition of a Transformer Transformer Windings Transformer Operation using Faraday’s Law Step-up & Step-down Transformers Turns Ratio.
Induction and Alternating Current
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.
Principles of Physics Electromagnetic Induction. Changing magnetic fields can create a voltage (and thus cause current to flow) in a conductor A wire.
Chapter 22 Alternating-Current Circuits and Machines.
Electromagnetic Induction
Remember?  An electron is moving downward with a velocity, v, in a magnetic field directed within the page, determine direction of force.
AC Circuits (Chapt 33) circuits in which the currents vary in time
Alternating Current Circuits
Topic 12: Electromagnetic induction 12.2 Alternating current
Alternating Current Circuits
Electricity and Magnetism 29 Alternating Currents and Power Transmission Chapter 29 Alternating Currents and Power Transmission.
Producing Electric Current
Chapter 31 Faraday’s Law.
ELECTRICAL BASICS (Chapter 8) Electrical terms Electricity & magnetism Electricity Circuits Magnetism Electrical units Electric potential or eletromotive.
Transformers. ► Electric Generators- the main function of an electric generator is to convert mechanical energy to electrical energy. ► Electric motors-
110/16/2015 Applied Physics Lecture 19  Electricity and Magnetism Induced voltages and induction Energy AC circuits and EM waves Resistors in an AC circuits.
Induced Voltage and Inductance
ELECTROMAGNETIC INDUCTION
Lecture 17 AC circuits RLC circuits Transformer Maxwell.
MagnetismSection 3 Section 3: Electric Currents from Magnetism Preview Key Ideas Bellringer Electromagnetic Induction The Electromagnetic Force Transformers.
Production and Control of High Voltage
Electromagnetic Induction. Current can be created in a wire by a magnetic field British scientist Michael Faraday and American scientist Joseph Henry.
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 8 Alternating Current Circuits. AC Circuit An AC circuit consists of a combination of circuit elements and an AC generator or source An AC circuit.
Electromagnetic Induction. Motion of a magnet in a coil or loop creates (induces) voltage If coil is connected to complete circuit, current flows Relative.
© Houghton Mifflin Harcourt Publishing Company Preview Objectives Electromagnetic Induction Characteristics of Induced Current Sample Problem Chapter 20.
Mutual Inductance As in a transformer, changing the current in the primary coil causes an induced voltage in the secondary coil i.e. mutual induction has.
Generators, Motors, Transformers
 Electromagnetic Induction – The production of an emf (the energy per unit charge supplied by a source of electric current) in a conducting circuit by.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Electromagnetic Induction
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.
Announcements Midterm Exam next Wednesday Exam starts at 6 PM, ~1 hr. Closed book, one page of notes Bring a calculator (not phone, computer, iPad, etc.)
Chapter-13 Outline 1Electric Circuits and Electric Current, I 2 Ohm’s Law, V = I R; and Resistance, R. 3 Series and Parallel Circuits 4 Electric Energy.
Chapter 33 Alternating Current Circuits. Electrical appliances in the house use alternating current (AC) circuits. If an AC source applies an alternating.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
Lecture 60 – Lecture 61 Producing Electric Current Ozgur Unal
Electromagnetism Notes-3
Chapter 20 Preview Objectives Electromagnetic Induction
Electromagnetism Notes-3
SYLLABUS AC Fundamentals AC Analysis AC power Three phase circuit
When we generate power we ramp up the voltage for transmission (up to V) and then when it arrives at homes we ramp it back down for convenient use.
Chapter 22: AC Circuits Figure (a) Direct current. (b) Alternating current.

Electromagnetic induction
An {image} series circuit has {image} , {image} , and {image}
Electric Currents from Magnetism
Electromagnetic Induction
Section 14.3.
General Physics (PHY 2140) Lecture 19 Electricity and Magnetism
Alternating Current Circuits and Electromagnetic Waves
MAGNETISM AND ITS USES Producing Electric Current
OCR 21st Century Science Unit P5 a and b Revision
Electromagnetic Induction & Transformers
Generators.
Electromagnetic Induction
Alternating Current Circuits
Transformers.
Alternating Current Circuits
Unit-1 Transformer.
Presentation transcript:

Electromagnetic Induction AC Circuits and transformers

Effective Current Emf in ac circuits is equivalent to potential difference in dc circuits Resistance, current, and emf can all be measured using a multimeter Induced emf as a function of time = maximum emf * sine of the angular frequency of rotation * time Δv = Δvmax * sinω * t Instantaneous current = maximum current * sine of the angular frequency of rotation * time i = Imax * sinω * t

Effective Current

Effective Current Since alternating current is constantly reversing, maximum current and emf values are not as useful as they are in direct current Of more importance are instantaneous and root-mean-square (rms) values Rms current – the amount of direct current that dissipates as much energy in a resistor as an instantaneous alternating current does during a complete cycle - the value of alternating current that gives the same heating effect that the corresponding value of direct current does An equivalent value allowing for accurate comparisons between alternating and direct current Power can be calculated by using the appropriate rms values in the equations given previously

Effective Current Potential Difference Current Instantaneous values v Maximum values Vmax Imax rms values Vrms=Vmax/√2 = 0.707*Vmax Irms = Imax/√2 = 0.707*Imax

Effective Current Power = rms current squared * resistance Power = one-half * maximum current squared * resistance P = (Irms)2R = ½(Imax)2R Ohm’s law still applies in ac circuits Rms potential difference = rms current * resistance Vrms = Irms*R

Effective Current Sample problem: A generator with a maximum output emf of 205V is connected to a 115 resistor. Calculate the rms potential difference. Find the rms current through the resistor. Find the maximum ac current in the circuit. Vmax = 205V R = 115 Vrms = ? Irms = ? Imax = ? Vrms = .707*Vmax Irms = Vrms / R Irms = .707*Imax

Effective Current

Effective Current Resistance influences current in an ac circuit The ac potential difference (ac voltage) measured in an electrical outlet is a rms emf with a value of 120V Maximum emf value for an outlet is about 170V Ammeters and voltmeters (and therefore multimeters) that measure alternating current are calibrated to measure rms values for current and emf (voltage)

Transformers Transformer – a device that increases or decreases the emf of alternating current In its simplest form, a transformer consists of two coils of wire wrapped around an iron core The first coil, or primary or input coil, is connected to a voltage source The second coil, or secondary or output coil, is connected to a resistor or other load The relative number of times the coils are wrapped around the iron core determines what happens to the voltage If the primary coil has more loops, the voltage decreases Step-down transformer If the secondary coil has more loops, the voltage increases Step-up transformer

Transformers Transformer Equation Induced emf in secondary coil = (number of turns in secondary coil) / (number of turns in primary coil) * applied emf in primary coil ΔV2 =N2 / N1 * ΔV1 Can’t have something for nothing Due to energy loss due to heating and radiation, so the output power will be less than the input power Any increase in voltage must be offset by a proportional decrease in current Real transformers have efficiency values of 90-99% To minimize power lost by resistive heating (I2R loss) in transmission lines, electric lines have high emf values and low currents Main lines have emf = 230000V Regional lines have emf = 20000V Customer lines have emf = 120V

Transformers The ignition coil in a gasoline engine is a transformer Changes 12 dc V into an emf of 100000V to ignite and burn fuel when sparkplug fires Crank angle sensor detects the crankshafts position to determine when the engine cylinder’s contents are at maximum compression