Introduction to Electromagnetism
|
|
- Myles Short
- 5 years ago
- Views:
Transcription
1 Introduction to Electromagnetism
2 Electric Field Lines If a charge feels an electrostatic force (Coulombic Force), it is said to be in an electric field. We like to represent electric fields with lines. The lines basically show where a positive test charge would feel a force. The lines also go off into infinity! The farther apart the lines, the weaker the field; the closer the lines, the stronger the field. The electric field lines of a positive charge point outwards and negative charge point inwards Like charges repel (Force is +), unlike attract (Force is -) + q - q
3 Magnetic field The magnetic force exerted in the region around the magnet is the magnetic field. Direction of magnetic field at any point is defined as the direction of motion of a charged particle on which the magnetic field would not exert a force Magnetic field lines show the direction of the field and it always go from the N pole to the S pole. Magnetic fields are vector quantities i.e., they have a magnitude and a direction written as B S N Strongest field at poles
4 Magnetic Flux, Φ The group of force lines going from the N pole to the S pole of a magnet is called the magnetic flux, symbolized by Φ. No. of magnetic field lines determines the value of the flux. The more lines of force, the greater the flux and the stronger the magnetic field. Unit of magnetic flux is the weber (Wb); One weber = 10 8 lines. Magnetic Flux Density, (B) is the amount of flux per unit area (i.e. B = Φ/A) perpendicular to the magnetic field. Unit 1 tesla (T) = one weber/square meter.
5 The Earth is a magnet William Gilbert, an English physician, i first proposed in 1600 that the earth itself is a magnet, and he predicted that the earth would be found to have magnetic poles. The Earth has an immense magnetic field around it called the magnetosphere. The circulation of the molten iron and nickel in the Earth s outer core produces a magnetic field. It exerts magnetic forces and is strongest near the North and South magnetic poles. A compass s needle points to the north geographic pole due to the south magnetic pole being nearby.
6 Origin of AURORA BOREALIS and AURORA AUSTRALIS Aurora Borealis Aurora Australis They are formed when charged particles from the sun (known as solar wind) hit oxygen and nitrogen atoms in the air. The atoms become excited and then give off many colors of light. The reason for the appearance at the poles is that the Earth s magnetic poles pull the sun s high- speed, charged particles towards them. North Pole - Northern lights: aurora borealis South Pole - Southern lights: aurora australis
7 Electromagnetism Explain the connection between electricity and magnetism A changing magnetic field produces an electric field, and a changing electric field produces a magnetic field. Electric and Magnetic fields can produce forces on charges An accelerating charge produces electromagnetic waves (radiation) Both electric and magnetic fields can transport energy Electric field energy used in electrical circuits, e.g., released in lightning Magnetic field carries energy through transformer.
8 Electric Current and Magnetism connection For a long time, magnetism and electricity were thought to be separate phenomena in nature. April 1820: Hans Christian Ørsted discovers deflection of compass needle when close to a wire carrying a current just as if the wire were e a magnet. When the battery was off the needle return to the true north.
9 Oersted s Law The flow of electricity through a wire conductor produces a magnetic field around the wire. Implication: the current carrying wire itself behaves like a magnet (since it can exert a force on another magnet like a permanent magnet would). An application of Oersted s Effect is the electromagnet and all the devices using it such as telephone receiver, speaker, electrical motors etc.
10 Biot-Savart Law In 1820, Jean-Baptiste Biot and Felix Savart published their observations that current in a wire induced a magnetic field around the wire. They noticed that the field was perpendicular to both the direction of current and the radius of the wire, leading to a precise mathematical form of the Biot-Savart Law. (B is the magnitude of the magnetic field produced by current I). B long wire μ 0 is the permeability of free space. 0 I 2r Right-hand rule
11 Ampère s Law Ampère s law relates the magnetic field around a closed loop to the total current flowing through the loop. September 1820: André-Marie Ampère publishes mathematical explanation of Ørsted s oberservation, now known as Ampère s Law. Ampère s Law states that along any closed path through a magnetic field, the sum of the products of the scalar component of B is directly proportional to the net electric current passing through hth the area enclosed db by the path.
12 Electromagnets An electromagnet is a type of magnet. The magnetic field is produced by the flow of electric current. The magnetic field is porportional to The number of turns in the winding The current in the wire Enhanced by a iron core
13 Faraday s Laws of EM Induction Michael Faraday was an experimental scientist discovered the principle of electromagnetic induction in Faraday's two observations in EM induction: 1) The amount of voltage induced in a coil is directly proportional to the rate of change of the magnetic field w.r.t. the coil. 2) The amount of voltage induced in a coil is directly proportional to the no. of turns of wire in the coil. If a circuit contains N tightly wound loops and the flux changes by ΔΦ B during a time interval Δt, the average emf induced is given by Faraday s Law: N t B
14 Application of Faraday s Law AC generator simulation
15 Maxwells s Electromagnetic Equations
16 Maxwell s Theory for electromagnetism In 1865, James Clerk Maxwell developed a theory of electricity and magnetism. Found a way to account for the phenomena of electricity, magnetism, and light itself, in a single system of wave equations. Electric and magnetic fields travel through space in the form of waves at the speed of light. A changing magnetic field will induce a changing g electric field, and vice versa.
17 Maxwell s Theory His starting points were: 1. Electric field lines originate on + charges and terminate on - charges 2. Magnetic field lines form closed loops 3. A varying magnetic field induces an electric field 4. A magnetic field is created by a current
18 Gauss s Law Electricity The total flux within a closed surface is proportional to the enclosed charge. E da = Q enclosed 0 Gauss s Law is always true, but is only useful for certain very simple problems with great symmetry.
19 E Maxwell s 1 st Equation 0 Equivalent to Gauss Flux Theorem: E E dv E ds 1 0 V S 0 V dv Q The flux of electric field out of a closed region is proportional to the total electric charge Q enclosed within the surface. A point charge q generates an electric field sphere q E r r q ds q EdS 2 4 r 0 sphere Area integral gives a measure of the net charge enclosed. 0 0
20 Gauss s Law for Magnetism Since there are no magnetic monopoles there is no place for magnetic field lines to begin or end. Gauss, states that an enclosed magnet will have a net magnetic flux (B) of zero. Thus, Gauss ss Lawfor magnetic charges must be: B da 0 Every magnet has a north pole and a south pole, so that if you were to enclose even a part of a magnet within a soap bubble, the total number of magnetic field lines entering the bubble would equal the total number of magnetic field lines exiting the bubble, with a net of zero.
21 B 0 Maxwell s 2 nd Equation Gauss law for magnetism: B 0 B ds 0 There are no magnetic monopoles The net magnetic flux out of any closed surface is zero. Surround a magnetic dipole with a closed surface. The magnetic flux directed inward towards the south pole will equal the flux outward from the north pole. If there were a magnetic monopole source, this would give a non-zero integral.
22 Faraday s Law of Induction A changing g magnetic field creates an electric field. is the electromotive force (EMF) in volts is the magnetic flux through the circuit (in webers) A change in flux of one weber per second will induce EMF of 1 volt.
23 E B t Maxwell s 3 rd Equation Equivalent to Faraday s LawofInduction: B E ds ds t S S d d E dl B ds dt dt C (for a fixed circuit C) The electromotive force round a E dl circuit is proportional to the rate of change of flux of magnetic field, B ds S through the circuit. Faraday s Law is the basis for electric generators. It also forms the basis for inductors and transformers. N S
24 Ampère-Maxwell Law Oersted and Ampere and Gauss showed that a current (I) would create a magnetic field (B). Hence, Bdl 0 I Steady current implies constant charge density so Ampere s law consistent with the Continuity equation for steady currents. However, Maxwell took it further and showed that a magnetic field (B) is created by a current (I) and a changing electric field (d E /dt). Therefore, Maxwell s revision of Ampere s Law becomes... Bdl 0I00 ddt E
25 B dl 0I 00 ddt E Maxwell s 4 th Equation Oii Originates from Ampère s (Circuital) it Law : B dl B ds C S S 0 j ds I 0 Satisfied by the field for a steady line current (Biot- Savart Law, 1820): 0I dl r B 3 4 r For a straight line current B 0I 2 r
26 Changing E field creates B field! Faraday: Varying B-field generate E-field Maxwell: varying E-field should then produce a B-field, but not covered by Ampère s Law. Surface 1 Surface 2 Apply Ampère to surface 1 (flat disk): line integral of B = 0 I Current I Closed loop Applied to surface 2, line integral is zero since no current penetrates the deformed surface. E Q ε A In capacitor,, so Displacement current density is 0 dq de A dt E dt j d 0 t I 0 26
27 Maxwell solved this problem by realizing that... Inside the capacitor there must be an induced magnetic field... B E How?. Inside the capacitor there is a changing E A changing electric field induces a magnetic field Therefore, Maxwell s revision of Ampere s Law becomes... d Bdl E 00 I 0 dt where I d is called the displacement current B dl I d ddt E 0 0 0
28 Maxwell s Equations of Electromagnetism q Gauss Law for Electrostatics E da 0 Gauss Law for Magnetism Faraday s Law of Induction B da 0 E dl ddt d B Revised da Ampere s Law B dl I d dt E
29 Electromagnetic Waves let there be light. B B dl d d E E dl B 0 0 dt dt v de dt E db dt These two equations can be solved simultaneously give plane waves resulting in EM waves E(x, t) = E max sin (kx-t)ĵ B(x, t) = B max sin (kx-t)ẑ
30 B z Plane Electromagnetic Waves E y Alternating electric field induces alternating magnetic field & vice versa. Self-propagating electromagnetic disturbance = light. c E(x, t) = E max sin (kx-t) jˆ B(x, t) = B max sin (kx-t) ẑz x
31 Properties of EM Waves The radiated EM waves have certain properties: EM waves all travel at the speed of light c. The E and B fields are perpendicular to each other. The E and B fields are in phase (both reach a maximum and minimum at the same time). The E and B fields are perpendicular to the direction of travel (transverse waves).
32 The Electromagnetic Spectrum There are many more forms of electromagnetic radiation than just visible light. The visible band we know is a pretty small section bt between ultraviolet ilt(uv) and dif infrared d(ir) (IR).
33 Production of Electromagnetic Waves Oscillating charges will produce electromagnetic waves. When Maxwell calculated the speed of propagation of electromagnetic waves, he found: This is the speed of light in a vacuum. Over the years, measurements have become more and more precise; now the speed of light is defined to be: In 1888, Heinrich Hertz demonstrated the existence of electromagnetic waves and proved Maxwell s theory.
Magnetizing a substance
Magnetism What is a magnet? Any material that has the property of attracting Iron (or steel), Nickel or Cobalt Magnets exert a force on other magnets or particles with an electrical charge Magnets may
More informationChapter 19. Magnetism. 1. Magnets. 2. Earth s Magnetic Field. 3. Magnetic Force. 4. Magnetic Torque. 5. Motion of Charged Particles. 6.
Chapter 19 Magnetism 1. Magnets 2. Earth s Magnetic Field 3. Magnetic Force 4. Magnetic Torque 5. Motion of Charged Particles 6. Amperes Law 7. Parallel Conductors 8. Loops and Solenoids 9. Magnetic Domains
More informationIntroduction to Electromagnetic Theory
Introduction to Electromagnetic Theory Lecture topics Laws of magnetism and electricity Meaning of Maxwell s equations Solution of Maxwell s equations Electromagnetic radiation: wave model James Clerk
More informationChapter 18 Study Questions Name: Class:
Chapter 18 Study Questions Name: Class: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. The region around a magnet in which magnetic forces
More informationMagnetism. and its applications
Magnetism and its applications Laws of Magnetism 1) Like magnetic poles repel, and 2) unlike poles attract. Magnetic Direction and Strength Law 3 - Magnetic force, either attractive or repelling varies
More informationChapter 30. Sources of the Magnetic Field Amperes and Biot-Savart Laws
Chapter 30 Sources of the Magnetic Field Amperes and Biot-Savart Laws F B on a Charge Moving in a Magnetic Field Magnitude proportional to charge and speed of the particle Direction depends on the velocity
More informationMaxwell s equations and EM waves. From previous Lecture Time dependent fields and Faraday s Law
Maxwell s equations and EM waves This Lecture More on Motional EMF and Faraday s law Displacement currents Maxwell s equations EM Waves From previous Lecture Time dependent fields and Faraday s Law 1 Radar
More informationPhysics / Higher Physics 1A. Electricity and Magnetism Revision
Physics / Higher Physics 1A Electricity and Magnetism Revision Electric Charges Two kinds of electric charges Called positive and negative Like charges repel Unlike charges attract Coulomb s Law In vector
More informationCHAPTER 20 Magnetism
CHAPTER 20 Magnetism Units Magnets and Magnetic Fields Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on Electric Charge Moving in a Magnetic
More informationELECTROMAGNETIC FIELD
UNIT-III INTRODUCTION: In our study of static fields so far, we have observed that static electric fields are produced by electric charges, static magnetic fields are produced by charges in motion or by
More informationChapter 29. Magnetic Fields
Chapter 29 Magnetic Fields A Brief History of Magnetism 13 th century BC Chinese used a compass Uses a magnetic needle Probably an invention of Arabic or Indian origin 800 BC Greeks Discovered magnetite
More informationUNIT-III Maxwell's equations (Time varying fields)
UNIT-III Maxwell's equations (Time varying fields) Faraday s law, transformer emf &inconsistency of ampere s law Displacement current density Maxwell s equations in final form Maxwell s equations in word
More informationPhysics 12. Unit 8 Magnetic Field and Electromagnetism Part I
Physics 12 Unit 8 Magnetic Field and Electromagnetism Part I 1. Basics about magnets Magnets have been known by ancient people since long time ago, referring to the iron-rich rocks, called magnetite or
More informationPHYS 1444 Section 004 Lecture #22
PHYS 1444 Section 004 Lecture #22 Monday, April 23, 2012 Dr. Extension of Ampere s Law Gauss Law of Magnetism Maxwell s Equations Production of Electromagnetic Waves Today s homework is #13, due 10pm,
More informationCHETTINAD COLLEGE OF ENGINEERING & TECHNOLOGY NH-67, TRICHY MAIN ROAD, PULIYUR, C.F , KARUR DT.
CHETTINAD COLLEGE OF ENGINEERING & TECHNOLOGY NH-67, TRICHY MAIN ROAD, PULIYUR, C.F. 639 114, KARUR DT. DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING COURSE MATERIAL Subject Name: Electromagnetic
More informationn Higher Physics 1B (Special) (PHYS1241) (6UOC) n Advanced Science n Double Degree (Science/Engineering) n Credit or higher in Physics 1A
Physics in Session 2: I n Physics / Higher Physics 1B (PHYS1221/1231) n Science, dvanced Science n Engineering: Electrical, Photovoltaic,Telecom n Double Degree: Science/Engineering n 6 UOC n Waves n Physical
More informationAP Physics C - E & M
AP Physics C - E & M Electromagnetic Induction 2017-07-14 www.njctl.org Table of Contents: Electromagnetic Induction Click on the topic to go to that section. Induced EMF Magnetic Flux and Gauss's Law
More informationElectromagnetic Field Theory (EMT) Lecture # 25
Electromagnetic Field Theory (EMT) Lecture # 25 1) Transformer and Motional EMFs 2) Displacement Current 3) Electromagnetic Wave Propagation Waves & Applications Time Varying Fields Until now, we have
More informationChapter 21. Magnetism
Chapter 21 Magnetism Magnets Poles of a magnet are the ends where objects are most strongly attracted Two poles, called north and south Like poles repel each other and unlike poles attract each other Similar
More informationVersion The diagram below represents lines of magnetic flux within a region of space.
1. The diagram below represents lines of magnetic flux within a region of space. 5. The diagram below shows an electromagnet made from a nail, a coil of insulated wire, and a battery. The magnetic field
More informationCalculus Relationships in AP Physics C: Electricity and Magnetism
C: Electricity This chapter focuses on some of the quantitative skills that are important in your C: Mechanics course. These are not all of the skills that you will learn, practice, and apply during the
More informationε induced Review: Self-inductance 20.7 RL Circuits Review: Self-inductance B induced Announcements
Announcements WebAssign HW Set 7 due this Friday Problems cover material from Chapters 20 and 21 We re skipping Sections 21.1-21.7 (alternating current circuits) Review: Self-inductance induced ε induced
More informationUnit-1 Electrostatics-1
1. Describe about Co-ordinate Systems. Co-ordinate Systems Unit-1 Electrostatics-1 In order to describe the spatial variations of the quantities, we require using appropriate coordinate system. A point
More informationMagnetic inductance & Solenoids. P.Ravindran, PHY041: Electricity & Magnetism 22 February 2013: Magnetic inductance, and Solenoid
Magnetic inductance & Solenoids Changing Magnetic Flux A changing magnetic flux in a wire loop induces an electric current. The induced current is always in a direction that opposes the change in flux.
More information2 The science of electricity and magnetism
1 Introduction Electromagnetism is one of the fundamental interactions in nature. Its physical origin lies in a property possessed by elementary particles of matter electrons and protons called electric
More informationMODULE 6 ELECTROMAGNETISM MAGNETIC FIELDS MAGNETIC FLUX VISUAL PHYSICS ONLINE
VISUAL PHYSICS ONLINE MODULE 6 ELECTROMAGNETISM MAGNETIC FIELDS MAGNETIC FLUX Magnetic field (-field ): a region of influence where magnetic materials and electric currents are subjected to a magnetic
More informationMichael Faraday. Chapter 31. EMF Produced by a Changing Magnetic Field, 1. Induction. Faraday s Law
Michael Faraday Chapter 31 Faraday s Law Great experimental physicist and chemist 1791 1867 Contributions to early electricity include: Invention of motor, generator, and transformer Electromagnetic induction
More information> What happens when the poles of two magnets are brought close together? > Two like poles repel each other. Two unlike poles attract each other.
CHAPTER OUTLINE Section 1 Magnets and Magnetic Fields Key Idea questions > What happens when the poles of two magnets are brought close together? > What causes a magnet to attract or repel another magnet?
More informationElectromagnetic field theory
1 Electromagnetic field theory 1.1 Introduction What is a field? Is it a scalar field or a vector field? What is the nature of a field? Is it a continuous or a rotational field? How is the magnetic field
More informationMagnets. Domain = small magnetized region of a magnetic material. all the atoms are grouped together and aligned
Magnetic Fields Magnets Domain = small magnetized region of a magnetic material all the atoms are grouped together and aligned Magnets Ferromagnetic materials domains can be forced to line up by applying
More informationCHAPTER 7 ELECTRODYNAMICS
CHAPTER 7 ELECTRODYNAMICS Outlines 1. Electromotive Force 2. Electromagnetic Induction 3. Maxwell s Equations Michael Faraday James C. Maxwell 2 Summary of Electrostatics and Magnetostatics ρ/ε This semester,
More informationLecture 27: MON 26 OCT Magnetic Fields Due to Currents II
Physics 212 Jonathan Dowling Lecture 27: MON 26 OCT Magnetic Fields Due to Currents II Jean-Baptiste Biot (1774-1862) Felix Savart (1791 1841) Electric Current: A Source of Magnetic Field Observation:
More informationqq k d Chapter 16 Electric and Magnetic Forces Electric charge Electric charges Negative (electron) Positive (proton)
Chapter 16 Electric and Magnetic Forces Electric charge Electric charges Negative (electron) Positive (proton) Electrons and protons in atoms/molecules Ions: atoms/molecules with excess of charge Ions
More informationINTRODUCTION ELECTRODYNAMICS BEFORE MAXWELL MAXWELL S DISPLACEMENT CURRENT. Introduction Z B S. E l = Electrodynamics before Maxwell
Chapter 14 MAXWELL S EQUATONS ntroduction Electrodynamics before Maxwell Maxwell s displacement current Maxwell s equations: General Maxwell s equations in vacuum The mathematics of waves Summary NTRODUCTON
More information1 Basic electromagnetism
1 Basic electromagnetism 1.1 Introduction Two thousand years ago, the Chinese invented the compass, a special metallic needle with one end always pointing to the North Pole. That was the first recorded
More informationElectrics. Electromagnetism
Electrics Electromagnetism Electromagnetism Magnetism is associated with charges in motion (currents): microscopic currents in the atoms of magnetic materials. macroscopic currents in the windings of an
More informationVector field and Inductance. P.Ravindran, PHY041: Electricity & Magnetism 19 February 2013: Vector Field, Inductance.
Vector field and Inductance Earth s Magnetic Field Earth s field looks similar to what we d expect if 11.5 there were a giant bar magnet imbedded inside it, but the dipole axis of this magnet is offset
More informationMagnetism is associated with charges in motion (currents):
Electrics Electromagnetism Electromagnetism Magnetism is associated with charges in motion (currents): microscopic currents in the atoms of magnetic materials. macroscopic currents in the windings of an
More informationWhere k = 1. The electric field produced by a point charge is given by
Ch 21 review: 1. Electric charge: Electric charge is a property of a matter. There are two kinds of charges, positive and negative. Charges of the same sign repel each other. Charges of opposite sign attract.
More informationElectromagnetism. Christopher R Prior. ASTeC Intense Beams Group Rutherford Appleton Laboratory
lectromagnetism Christopher R Prior Fellow and Tutor in Mathematics Trinity College, Oxford ASTeC Intense Beams Group Rutherford Appleton Laboratory Contents Review of Maxwell s equations and Lorentz Force
More informationPhysics Week 5(Sem. 2) Name. Magnetism. Chapter Summary. Magnetic Fields
Physics Week 5(Sem. 2) Name Chapter Summary Magnetism Magnetic Fields Permanent magnets have long been used in navigational compasses. The needle in a compass is supported to allow it to freely rotate
More informationPHYSICS. Chapter 29 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT
PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 29 Lecture RANDALL D. KNIGHT Chapter 29 The Magnetic Field IN THIS CHAPTER, you will learn about magnetism and the magnetic field.
More informationDisplacement Current. Ampere s law in the original form is valid only if any electric fields present are constant in time
Displacement Current Ampere s law in the original form is valid only if any electric fields present are constant in time Maxwell modified the law to include timesaving electric fields Maxwell added an
More informationPHYS:1200 LECTURE 27 ELECTRICITY AND MAGNETISM (5)
1 PHYS:1200 LECTURE 27 ELECTRICITY AND MAGNETISM (5) Everyone has played with magnets and knows that they stick to some materials and not to others. This lecture explores the physical principles behind
More informationr r 1 r r 1 2 = q 1 p = qd and it points from the negative charge to the positive charge.
MP204, Important Equations page 1 Below is a list of important equations that we meet in our study of Electromagnetism in the MP204 module. For your exam, you are expected to understand all of these, and
More information1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields.
1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields. 2. An isolated moving point charge produces around it.
More informationChapter 2 Basics of Electricity and Magnetism
Chapter 2 Basics of Electricity and Magnetism My direct path to the special theory of relativity was mainly determined by the conviction that the electromotive force induced in a conductor moving in a
More informationTorque on a Current Loop
Today Chapter 19 Magnetism Torque on a current loop, electrical motor Magnetic field around a current carrying wire. Ampere s law Solenoid Material magnetism Clicker 1 Which of the following is wrong?
More informationCourse no. 4. The Theory of Electromagnetic Field
Cose no. 4 The Theory of Electromagnetic Field Technical University of Cluj-Napoca http://www.et.utcluj.ro/cs_electromagnetics2006_ac.htm http://www.et.utcluj.ro/~lcret March 19-2009 Chapter 3 Magnetostatics
More informationElectromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance
Lesson 7 Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance Oscillations in an LC Circuit The RLC Circuit Alternating Current Electromagnetic
More informationChapter 22. Induction
Chapter 22 Induction Induced emf A current can be produced by a changing magnetic field First shown in an experiment by Michael Faraday A primary coil is connected to a battery A secondary coil is connected
More informationMagnetic Forces and Fields (Chapters 29-30)
Magnetic Forces and Fields (Chapters 29-30) Magnetism Magnetic Materials and Sources Magnetic Field, Magnetic Force Force on Moving Electric Charges Lorentz Force Force on Current Carrying Wires Applications
More informationPES 1120 Spring 2014, Spendier Lecture 38/Page 1
PES 1120 Spring 2014, Spendier Lecture 38/Page 1 Today: Start last chapter 32 - Maxwell s Equations James Clerk Maxwell (1831-1879) Scottish mathematical physicist. He united all observations, experiments
More informationModule 3: Electromagnetism
Module 3: Electromagnetism Lecture - Magnetic Field Objectives In this lecture you will learn the following Electric current is the source of magnetic field. When a charged particle is placed in an electromagnetic
More informationKey Contents. Magnetic fields and the Lorentz force. Magnetic force on current. Ampere s law. The Hall effect
Magnetic Fields Key Contents Magnetic fields and the Lorentz force The Hall effect Magnetic force on current The magnetic dipole moment Biot-Savart law Ampere s law The magnetic dipole field What is a
More informationREVIEW SESSION. Midterm 2
REVIEW SESSION Midterm 2 Summary of Chapter 20 Magnets have north and south poles Like poles repel, unlike attract Unit of magnetic field: tesla Electric currents produce magnetic fields A magnetic field
More informationMagnetic Fields
Magnetic circuits introduction Becomes aware of the similarities between the analysis of magnetic circuits and electric circuits. Develop a clear understanding of the important parameters of a magnetic
More informationMagnetism & Electromagnetism
Magnetism & Electromagnetism By: Dr Rosemizi Abd Rahim Click here to watch the magnetism and electromagnetism animation video http://rmz4567.blogspot.my/2013/02/electrical-engineering.html 1 Learning Outcomes
More informationChapter 21 Magnetic Induction Lecture 12
Chapter 21 Magnetic Induction Lecture 12 21.1 Why is it called Electromagnetism? 21.2 Magnetic Flux and Faraday s Law 21.3 Lenz s Law and Work-Energy Principles 21.4 Inductance 21.5 RL Circuits 21.6 Energy
More informationElectromagnetic Induction (Chapters 31-32)
Electromagnetic Induction (Chapters 31-3) The laws of emf induction: Faraday s and Lenz s laws Inductance Mutual inductance M Self inductance L. Inductors Magnetic field energy Simple inductive circuits
More informationB for a Long, Straight Conductor, Special Case. If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes
B for a Long, Straight Conductor, Special Case If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes μ I B = o 2πa B for a Curved Wire Segment Find the field at point
More informationDiscipline Course-I Semester-II
Maxwell's equation: "Introduction of Displacement Current" Discipline Course-I Semester-II Paper No: Electricity and Magnetism Lesson: Maxwell's equation: "Introduction of Displacement Current" Lesson
More informationPhysics 17 Part M Dr. Alward
Physics 17 Part M Dr. Alward Elementary Facts Concerning Magnets Magnets have north and south poles. Like Poles Repel Unlike Poles Attract Magnetic Dipoles Magnets have two poles, one north, the other
More informationChapter 27, 28 & 29: Magnetism & Electromagnetic Induction. Magnetic flux Faraday s and Lenz s law Electromagnetic Induction Ampere s law
Chapter 27, 28 & 29: Magnetism & Electromagnetic Induction Magnetic flux Faraday s and Lenz s law Electromagnetic Induction Ampere s law 1 Magnetic Flux and Faraday s Law of Electromagnetic Induction We
More informationAP Physics C. Magnetism - Term 4
AP Physics C Magnetism - Term 4 Interest Packet Term Introduction: AP Physics has been specifically designed to build on physics knowledge previously acquired for a more in depth understanding of the world
More informationMagnetic Fields and Forces
Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 20 Magnetic Fields and Forces Marilyn Akins, PhD Broome Community College Magnetism Magnetic fields are produced by moving electric charges
More informationChapter 27 Magnetic Fields and Magnetic Forces
Chapter 27 Magnetic Fields and Magnetic Forces In this chapter we investigate forces exerted by magnetic fields. In the next chapter we will study the sources of magnetic fields. The force produced by
More informationHIGH SCHOOL SCIENCE. Physical Science 7: Electricity & Magnetism
HIGH SCHOOL SCIENCE Physical Science 7: Electricity & Magnetism WILLMAR PUBLIC SCHOOL 2013-2014 EDITION CHAPTER 7 Electricity & Magnatism In this chapter you will: 1. Analyze factors that affect the strength
More informationPhysics 208, Spring 2016 Exam #3
Physics 208, Spring 206 Exam #3 A Name (Last, First): ID #: Section #: You have 75 minutes to complete the exam. Formulae are provided on an attached sheet. You may NOT use any other formula sheet. You
More informationSliding Conducting Bar
Motional emf, final For equilibrium, qe = qvb or E = vb A potential difference is maintained between the ends of the conductor as long as the conductor continues to move through the uniform magnetic field
More informationElectromagnetics in Medical Physics
Electromagnetics in Medical Physics Part 4. Biomagnetism Tong In Oh Department of Biomedical Engineering Impedance Imaging Research Center (IIRC) Kyung Hee University Korea tioh@khu.ac.kr Dot Product (Scalar
More informationElectromagnetic Field Theory Chapter 9: Time-varying EM Fields
Electromagnetic Field Theory Chapter 9: Time-varying EM Fields Faraday s law of induction We have learned that a constant current induces magnetic field and a constant charge (or a voltage) makes an electric
More informationChapter 8. Electricity and Magnetism. Law of Charges. Negative/Positive
Chapter 8 Electricity and Magnetism Electricity and Magnetism (1) Electric Charge Electric charge is a fundamental conserved property of some subatomic particles, which determines their electromagnetic
More informationLecture #4.4 Magnetic Field
Lecture #4.4 Magnetic Field During last several lectures we have been discussing electromagnetic phenomena. However, we only considered examples of electric forces and fields. We first talked about electrostatics
More informationChapter 23. Electric Fields
Chapter 23 Electric Fields Electricity and Magnetism The laws of electricity and magnetism play a central role in the operation of many modern devices. The interatomic and intermolecular forces responsible
More informationElectromagnetic Theory PHYS 401/402
Electromagnetic Theory PHYS 401/402 Fall 2017 Lalith Perera, lpperera@olemiss.edu Office: Kennon 1 Office hours: M,Tu Th 3:00-4:00 PM Web page: http://www.phy.olemiss.edu/~perera/em 1 Electromagnetic Theory
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 8 Electricity and Magnetism 1. Magnetism Application of magnetic forces Ampere s law 2. Induced voltages and induction Magnetic flux http://www.physics.wayne.edu/~alan/2140website/main.htm
More informationXII PHYSICS ELECTROMAGNETISM] CHAPTER NO. 14 [MAGNETISM AND LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.
XII PHYSICS LECTURER PHYSICS, AKHSS, K affan_414@live.com https://promotephysics.wordpress.com [MAGNETISM AND ELECTROMAGNETISM] CHAPTER NO. 14 OERSTED s EXPERIMENT During a lecture demonstration, on April
More informationMagnetostatics III. P.Ravindran, PHY041: Electricity & Magnetism 1 January 2013: Magntostatics
Magnetostatics III Magnetization All magnetic phenomena are due to motion of the electric charges present in that material. A piece of magnetic material on an atomic scale have tiny currents due to electrons
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 15 Electricity and Magnetism Magnetism Applications of magnetic forces Induced voltages and induction Magnetic flux and induced emf Faraday s law http://www.physics.wayne.edu/~apetrov/phy2140/
More informationElectric vs Magnetic Comparison
5. MAGNETOSTATICS Electric vs Magnetic Comparison J=σE Most dielectrics µ = µo excluding ferromagnetic materials Gauss s Law E field is conservative Gauss s law (integral) Conservative E field Electric
More informationAP Physics C Mechanics Objectives
AP Physics C Mechanics Objectives I. KINEMATICS A. Motion in One Dimension 1. The relationships among position, velocity and acceleration a. Given a graph of position vs. time, identify or sketch a graph
More informationMaxwell Equations Dr. Anurag Srivastava
Maxwell Equations Dr. Anurag Srivastava Web address: http://tiiciiitm.com/profanurag Email: profanurag@gmail.com Visit me: Room-110, Block-E, IIITM Campus Syllabus Electrodynamics: Maxwell s equations:
More informationChapter 22, Magnetism. Magnets
Chapter 22, Magnetism Magnets Poles of a magnet (north and south ) are the ends where objects are most strongly attracted. Like poles repel each other and unlike poles attract each other Magnetic poles
More informationwe can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron.
Physics II we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron. Particle Symbol Charge (e) Mass (kg) Proton P +1 1.67
More informationOutside the solenoid, the field lines are spread apart, and at any given distance from the axis, the field is weak.
Applications of Ampere s Law continued. 2. Field of a solenoid. A solenoid can have many (thousands) of turns, and perhaps many layers of windings. The figure shows a simple solenoid with just a few windings
More informationChapter 29. Magnetic Fields
Chapter 29 Magnetic Fields Outline 29.1 Magnetic Fields and Forces 29.2 Magnetic Force Acting on a Current-Carrying Conductor 29.4 Motion of a Charged Particle in a Uniform Magnetic Field 29.5 Applications
More information1 RF components. Cambridge University Press Radio Frequency Integrated Circuits and Systems Hooman Darabi Excerpt More information
9780521190794 Radio Frequency ntegrated Circuits and ystems 1 RF components n this chapter basic components used in RF design are discussed. A detailed modeling and analysis of MO transistors at high frequency
More informationTransmission Lines and E. M. Waves Prof. R. K. Shevgaonkar Department of Electrical Engineering Indian Institute of Technology, Bombay
Transmission Lines and E. M. Waves Prof. R. K. Shevgaonkar Department of Electrical Engineering Indian Institute of Technology, Bombay Lecture 18 Basic Laws of Electromagnetics We saw in the earlier lecture
More informationELECTROMAGNETIC INDUCTION AND FARADAY S LAW
ELECTROMAGNETIC INDUCTION AND FARADAY S LAW Magnetic Flux The emf is actually induced by a change in the quantity called the magnetic flux rather than simply py by a change in the magnetic field Magnetic
More informationFerromagnetism. we saw that with the propane torch on Thursday
Announcements l Help room hours (1248 BPS) Ian La Valley(TA) Mon 4-6 PM Tues 12-3 PM Wed 6-9 PM Fri 10 AM-noon l LON-CAPA #7 due Oct. 25 l Final Exam Tuesday Dec 11 7:45-9:45 AM Ferromagnetism l What makes
More informationPart 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is
1 Part 4: Electromagnetism 4.1: Induction A. Faraday's Law The magnetic flux through a loop of wire is Φ = BA cos θ B A B = magnetic field penetrating loop [T] A = area of loop [m 2 ] = angle between field
More informationCh 30 - Sources of Magnetic Field
Ch 30 - Sources of Magnetic Field Currents produce Magnetism? 1820, Hans Christian Oersted: moving charges produce a magnetic field. The direction of the field is determined using a RHR. Oersted (1820)
More informationYell if you have any questions
Class 36: Outline Hour 1: Concept Review / Overview PRS Questions Possible Exam Questions Hour : Sample Exam Yell if you have any questions P36-1 Before Starting All of your grades should now be posted
More informationLecture 10 Induction and Inductance Ch. 30
Lecture 10 Induction and Inductance Ch. 30 Cartoon - Faraday Induction Opening Demo - Thrust bar magnet through coil and measure the current Topics Faraday s Law Lenz s Law Motional Emf Eddy Currents LR
More informationChapter 12. Magnetism and Electromagnetism
Chapter 12 Magnetism and Electromagnetism 167 168 AP Physics Multiple Choice Practice Magnetism and Electromagnetism SECTION A Magnetostatics 1. Four infinitely long wires are arranged as shown in the
More informationTopic 6.3 Magnetic Force and Field. 2 hours
Topic 6.3 Magnetic Force and Field 2 hours 1 Magnetic Fields A magnetic field is said to exist at a point if a compass needle placed there experiences a force. The appearance of a magnetic field can be
More informationCollege Physics B - PHY2054C
Force on a Torque on a College - PHY2054C & 09/29/2014 My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building Outline Force on a Torque on a 1 Force on a Torque on a 2 3 4 Force on a Torque on a Force
More informationElectricity (& Magnetism)
EA Notes (Scen 101), Tillery Chapter 6 Electricity (& Magnetism) Introduction First five chapters are "Newtonian Physics", mechanical explanations based on Newton's Laws applied to explain the motion of
More informationMansfield Independent School District AP Physics C: Electricity and Magnetism Year at a Glance
Mansfield Independent School District AP Physics C: Electricity and Magnetism Year at a Glance First Six-Weeks Second Six-Weeks Third Six-Weeks Lab safety Lab practices and ethical practices Math and Calculus
More information