Magnetic Force Physics 102 Professor Lee Carkner Lecture 18.

Slides:



Advertisements
Similar presentations
Chapter 26: The Magnetic Field
Advertisements

Chapter 20 Magnetism.
Ch 20 1 Chapter 20 Magnetism © 2006, B.J. Lieb Some figures electronically reproduced by permission of Pearson Education, Inc., Upper Saddle River, New.
Magnetism Magnets are used in meter, motors, speakers, CDs, MRIs, cyclotrons and to store computer data. They are used to move heavy objects, propel trains.
Magnetic Force PH 203 Professor Lee Carkner Lecture 16.
Magnetism! Chapter 19.
Chapter 29 Magnetic Fields Physics Differences Between Electric Fields and Magnetic Fields 1)What creates the field a) Electric - charge created.
Magnetic Fields Magnetic Field Forces on a Charged Particle Magnetic Field Lines Crossed Fields and Hall Effect Circulating Charged Particles Cyclotrons.
Magnetic Forces. Forces in Magnetism The existence of magnetic fields is known because of their affects on moving charges. What is magnetic force (F B.
Wednesday, Oct. 26, 2005PHYS , Fall 2005 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #16 Wednesday, Oct. 26, 2005 Dr. Jaehoon Yu Charged Particle.
Copyright © 2009 Pearson Education, Inc. Force on an Electric Charge Moving in a Magnetic Field.
Chapter 22 Magnetism.
1.Moving electric charges produce magnetic fields, B B measured in Tesla (1T = 10 4 Gauss) Earth’s B field ~ 0.5 Gauss Largest permanent magnet.
Magnetic Force. Moving Charge  A charge in an electric field is subject to a force. Charge at rest or in motion In the direction of field  A charge.
Ampere’s Law PH 203 Professor Lee Carkner Lecture 17.
Electricity&… Magnetism Review of Coulomb`s Force,Magnetic Fields and Magnetic Force Lecture 22 Monday: 5 April 2004.
Magnetic Field Physics 102 Professor Lee Carkner Lecture 16.
Magnetism (sec. 27.1) Magnetic field (sec. 27.2) Magnetic field lines and magnetic flux (sec. 27.3) Motion of charges in a B field (sec. 27.4) Applications.
PH 203 Professor Lee Carkner Lecture 18
Ampere’s Law Physics 102 Professor Lee Carkner Lecture 19.
Physical Modeling, Fall THE MAGNETIC FIELD B is the symbol for the magnetic field. Magnetic field lines run from north poles to south poles. Like.
Ampere’s Law Physics 102 Professor Lee Carkner Lecture 19.
Magnetic Field Physics 102 Professor Lee Carkner Lecture 17.
Magnetic Force Physics 102 Professor Lee Carkner Lecture 17.
Induction Physics 102 Professor Lee Carkner Lecture 19.
Copyright © 2009 Pearson Education, Inc. Lecture 8 - Magnetism.
Announcements WebAssign HW Set 5 due October 10
Magnetic Fields Magnetic fields emerge from the North pole of a magnet and go into the South pole. The direction of the field lines show the direction.
Lecture Outline Chapter 19 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
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.
Announcements WebAssign HW Set 6 due this Friday Problems cover material from Chapters 19 Prof. Kumar tea and cookies today from 5 – 6 pm in room 2165.
Chapter 29 Magnetism Ferromagnetism
Chapter 26 Magnetism Poles – Location where the magnetic effect is the strongest –North pole – pole of a freely suspended magnet which points towards geographic.
Fields Model used when force act a distance. Quantity / unit measure.
Magnetism Force of Mystery demo. Magnetism Standards Students know magnetic materials and electric currents (moving electric charges) are sources of magnetic.
Today4/9 Lab “Current Balance” Right Hand Rule for:
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 22 Physics, 4 th Edition James S. Walker.
Chapter 19 Magnetism. General Physics Review – Magnetic Fields ELECTRIC FIELDS From (+) to (–) charges Field lines (electric flux) Start / End at charges.
Magnetism AP Physics Chapter 20. Magnetism 20.1 Mangets and Magnetic Fields.
Lecture 14 Magnetism. Magnets... two poles: N and S Like poles repel Unlike poles attract.
Chapter 19 Magnetism. Magnets Poles of a magnet are the ends where objects are most strongly attracted Poles of a magnet are the ends where objects are.
Announcements WebAssign HW Set 5 due October 10 Problems cover material from Chapters 18 HW set 6 due on October 17 (Chapter 19) Prof. Kumar tea and cookies.
Magnetic Forces. Forces in Magnetism The existence of magnetic fields is known because of their affects on moving charges. What is magnetic force (F B.
Chapter 19: Magnetism Magnets  Magnets Homework assignment : 18,25,38,45,50 Read Chapter 19 carefully especially examples.
Chapter 19 Magnetism. Fig. 19.1, p.587 Magnets Poles of a magnet are the ends where objects are most strongly attracted – Two poles, called north and.
Tuesday March 29, PHYS Dr. Andrew Brandt PHYS 1444 – Section 02 Lecture #15 Tuesday Mar Dr. Andrew Brandt HW7 Ch 27 is due Fri.
PHYS 1442 – Section 004 Lecture #12 Wednesday February 26, 2014 Dr. Andrew Brandt Chapter 20 -Charged Particle Moving in Magnetic Field -Sources of Magnetic.
Lecture 27 Magnetic Fields: II
Magnetism Chapter 27 opener. Magnets produce magnetic fields, but so do electric currents. An electric current flowing in this straight wire produces a.
2/8/2010 Do Now: 12/16/2013 (on last week’s paper) What makes a magnet a magnet? What makes a magnet a magnet? Why are some magnets stronger than others?
Magnetic Field Lines Graphical Illustration of Magnetic Fields Lines start on north pole and end on south pole Opposite poles attract, like poles reply.
Magnetic Fields A vector quantity Symbolized by
Magnetism. Magnets and Magnetic Fields Magnets have two ends – poles – called north and south. Like poles repel; unlike poles attract.
PHY 102: Lecture Magnetic Field 6.2 Magnetic Force on Moving Charges 6.3 Magnetic Force on Currents 6.4 Magnetic Field Produced by Current.
Chapter 20 Magnetism Conceptual Quiz 20 Conceptual Quiz Questions.
Nighttime exam? If we have the exam in the evening of July 3 rd, we would cancel class on July 5 th and you get a long weekend. Would you prefer to have.
Phys102 Lecture 13, 14, 15 Magnetic fields
PHYS 1444 – Section 501 Lecture #15
Chapter 20: Magnetism Purpose: To describe magnetic field around a permanent magnet. Objectives: Describe a magnetic poles Describe magnetic field. Magnetic.
Magnetic Fields and Forces
Force on an Electric Charge Moving in a Magnetic Field
Force on an Electric Charge Moving in a Magnetic Field
Force on an Electric Charge Moving in a Magnetic Field
Starter: Determine the direction of the missing vector.
Chapter 27 Magnetism Chapter 27 opener. Magnets produce magnetic fields, but so do electric currents. An electric current flowing in this straight wire.
Magnetism Force of Mystery demo.
PHYS 1444 – Section 002 Lecture #18
PHYS 1444 – Section 002 Lecture #18
Magnetic Forces.
Magnetic Fields Exert Forces on Moving Charges
Presentation transcript:

Magnetic Force Physics 102 Professor Lee Carkner Lecture 18

PAL #17 Magnetic Field  Direction electron is fired into magnetic field that points north if it is deflected up  Force equation: F = qvB sin     = sin -1 [(1.7X )/((1.6X )(3X10 5 )(0.5))]   =  v vector points 45 west of north, which is pointed northwest, so electron was fired from southeast

Electron in B Field v B  North West South East From right hand rule: B is north and force is up so v is from west (reversed to east for electron)

A beam of electrons is pointing right at you. What direction would a magnetic field have to have to produce the maximum deflection in the right direction? A)Right B)Left C)Up D)Down E)Right at you

A beam of electrons is pointing right at you. What direction would a magnetic field have to have to produce the maximum deflection in the up direction? A)Right B)Left C)Up D)Down E)Right at you

A beam of electrons is pointing right at you. What direction would a magnetic field have to have to produce no deflection? A)Right B)Left C)Up D)Down E)Right at you

Electric and Magnetic Force  How do the electric and magnetic forces differ?  Dependences   Magnetic force depends on v and , as well as B and q  Vector   Force vector does change for a magnetic field, since as the particle is deflected the v vector changes 

Particle Motion  A particle moving freely in a magnetic field will have one of three paths, depending on   Straight line   Circle   Helix   This assumes a uniform field that the particle does not escape from

Circular Motion

 If the particle moves at right angles to the field the force vector will cause the path to bend   The particle will move in a circle  How big is the circle?  Magnetic force is F =  Centripetal force is F =  We can combine to get r = mv/qB  Radius of orbit of charged particle in a uniform magnetic field

Circle Properties  Circle radius is inversely proportional to q and B   r is directly proportional to v and m   Can use this idea to make mass spectrometer   Send mixed atoms through the B field they will come out separated by mass

Today’s PAL  How long would it take an electron to complete one circular orbit around a 1 G magnetic field?

Helical Motion  If the initial velocity is not completely perpendicular to the field, instead of a circle you get a spiral or helix  Charged particles will spiral around magnetic field lines   For example, if the lines begin and end at a pole   Examples:   Gyrosynchrotron radio emission from planets and stars

Helical Motion

Solar Wind Particles in Earth’s Magnetic Field

Magnetic Field and Current  Since a current is moving charge, a magnet will produce a force on a wire with a current flowing through it   So qv = IL, thus: F = BIL sin    We can use the right hand rule to get the direction of the force  Use the direction of the current instead of v

Force on a Wire

Force on a Loop of Wire   Consider a loop of wire placed so that it is lined up with a magnetic field   Two sides will have forces at right angles to the loop, but in opposite directions  The loop will experience a torque

Loop of Current

Torque on Loop  For a loop of width w and height h, force is F = BIL sin  for each long side  Since  = 90 and L = h,  The torque is the force times the moment arm (distance to the center), which is w/2  Total torque =  but hw is the area of the loop, A   If the field is at angle  to the loop then 

Torque on Loop

General Loops  If there are multiple loops (N), the torque is the sum of each  = IBAN sin    A loop placed along a magnetic field will try to align such that the field goes straight through it   Can harness the spin to do work  Called a motor

Next Time  Read  Homework: Ch 20, P 4, 17, 38, 49  Exam #2 Friday