The Magnetic Force. x x x x x x. x x x x x x. x x x x x x q. q F = 0. q F. Phys 122 Lecture 17. Comment: What just happened...?

Size: px
Start display at page:

Download "The Magnetic Force. x x x x x x. x x x x x x. x x x x x x q. q F = 0. q F. Phys 122 Lecture 17. Comment: What just happened...?"

Transcription

1 The Magnetic orce Comment: I LOVE MAGNETISM q = qe + q q Comment: What just happened...? q = 0 Phys 122 Lecture 17 x x x x x x q G. Rybka

2 Magnetic Phenomenon ar magnet... two poles: N and S Like poles repel;; Unlike poles attract. Magnetic ield lines: (defined in same way as electric field lines, direction and density) S N Looks just like the electric dipole

3 Source of Magnetic ields? Answer: electric charge in motion Understanding source of field by bar magnet lies in understanding currents at atomic leel within bulk matter. Orbits of electrons about nuclei Intrinsic spin of electrons (more important effect) Comment: What is the difference between magnetic and electric fields? They seem similar, and although I understand that electric fields are created with charge distributions I don't understand how magnetic fields are generated with current

4 The Magnetic ield is defined by the magnetic force on a test charge Same approach for electric field: What is "magnetic force"? E = How is it distinguished from "electric" force? Start with some obserations: CRT deflection Empirical facts: a) magnitude: µ to elocity of q q q mag b) direction: to direction of q

5 Clicker An electron enters a region of space with speed and exits the region as shown with the same speed (magnitude). rom this information, what can we infer about the E y and z fields in the region? A. Only E y exists. Only z exists C. oth E y & z can exist y E? e -? x

6 Clicker An electron enters a region of space with speed and exits the region as shown with the same speed (magnitude). rom this information, what can we infer about the E y and z fields in the region? A. Only E y exists. Only z exists C. oth E y & z can exist If E y exists: orce y = q E y = ma y will accelerate charge in y direction The x elocity is unchanged. The y elocity is new Superposition: oerall speed is increasing. Therefore: NO E y possible How about z? Produces force on electron in x-y plane, perpendicular to. Therefore, z will NOT change the speed. ut it will change the direction of q. z exists in this example.

7 Lorentz orce The force on a charge q moing with elocity through a region of space with electric field E and magnetic field is gien by: = qe + q q q q = 0

8 Cross Product Reiew Cross Product different from Dot Product A is a scalar; A x is a ector A proportional to the component of parallel to A A x proportional to the component of perpendicular to A Definition of A x Magnitude: Asinθ Direction: perpendicular to plane defined by A and with sense gien by right- hand- rule

9 Remembering Directions: The Right Hand Rule = q 1. 1 st inger in direction of 2. Curl other fingers in direction of 3. Thumb points in direction of y q x z 1. Point ingers in direction of 2. Curl all fingers in direction of 3. Thumb points in direction of

10 Clicker Two protons each moe at speed toward a region of space which contains a constant field in the z direction. What is the relation between the magnitudes of the forces on the two protons in the magnetic field region? z y 1 2 X X X X X X X X X X X X x (a) 1 < 2 (b) 1 = 2 (c) 1 > 2 The magnetic force is gien by: = q = qsinθ In both cases the angle between and is 90 Therefore 1 = 2.

11 Clicker Two protons each moe at speed toward a region of space which contains a constant field in the z direction. 2 y X X X X X X X X X X X X 2What is 2x, the x-component of the force on the second proton? z x (a) 2x < 0 (b) 2x = 0 (c) 2x > 0 To determine the direction of the force, we use the right-hand rule. = q As shown in the diagram, 2x < 0.

12 Trajectory in Constant ield Suppose charge q enters field with elocity as shown below. What will be the path q follows? orce is always to elocity and. What is path? Path will be circle. will be the centripetal force needed to keep the charge in its circular orbit. Calculate R: R q

13 Radius of Circular Orbit Lorentz force: = q centripetal acc: a = R Newton's 2nd Law: 2 q R = ma Þ q = m R 2 This is momentum Þ R = m q This is an important result, with useful experimental consequences

14 ATLAS detector at CERN Radius of curature of particle tracks measures momentum

15 Project 8 Experiment at UW

16 Clicker L A proton, moing at speed, enters a region of space which contains a constant field in the z direction and is deflected as shown. Another proton, moing at 1 = 2, enters the same region of space and is deflected as shown. Compare the work done by the magnetic field W for, W 1 for 1 to deflect the protons? (a) W 1 < W (b) W 1 = W (c) W 1 > W Remember: work done W is defined as: W dx Remember: magnetic force is always perpendicular to the elocity: = q Therefore: the work done is ZERO in each case: 1 1 dx = dt = 0

17 Prelecture Reiew Question Particle A has twice the charge and 4 times the mass of particle. Suppose A and hae the same kinetic energy K and moe perpendicular to a constant magnetic field. Which particle moes in the smallest circle? Recall KE = p 2 /2m. A. Particle A moes in a smaller circle. Particle moes in a smaller circle C. Particles A and moe in circles of the same radius. 2q 4m q m KE = p A2 / 8m = p 2 / 2m à p A = 2p R = p q R A = p A / q A = 2 p / 2q = p / q R = p / q The same

18 Cross Product Practice Protons (positie charge) coming out of screen Magnetic field pointing down What is direction of force on POSITIVE charge? = q A) Left ) Right C) UP D) Down E) Zero x + x + y y y x z

19 The drawing below shows the top iew of two interconnected chambers. Each chamber has a unique magnetic field. A positiely charged particle is fired into chamber 1, and obsered to follow the dashed path shown in the figure. CheckPoint 6 q. = q

20 The drawing below shows the top iew of two interconnected chambers. Each chamber has a unique magnetic field. A positiely charged particle is fired into chamber 1, and obsered to follow the dashed path shown in the figure. CheckPoint 8 Obseration: R 2 > R 1 R = m q > 1 2

Page 1. B x x x x x x x x x x x x v x x x x x x F. q F. q F = 0. Magnetic Field Lines of a bar magnet

Page 1. B x x x x x x x x x x x x v x x x x x x F. q F. q F = 0. Magnetic Field Lines of a bar magnet Magnetism The Magnetic orce = = 0 ar Magnet ar magnet... two poles: N and S Like poles repel; Unlike poles attract. Magnetic ield lines: (defined in same way as electric field lines, direction and density)

More information

General Physics II. Magnetism

General Physics II. Magnetism General Physics II Magnetism Bar magnet... two poles: N and S Like poles repel; Unlike poles attract. Bar Magnet Magnetic Field lines [B]: (defined in a similar way as electric field lines, direction and

More information

Page 1. B x x x x x x x x x x x x v x x x x x x F. q F. q F = 0. Magnetic Field Lines of a bar magnet

Page 1. B x x x x x x x x x x x x v x x x x x x F. q F. q F = 0. Magnetic Field Lines of a bar magnet Magnetism The Magnetic orce r r r = = 0 ar Magnet ar magnet... two poles: N and S Like poles repel; Unlike poles attract. Magnetic ield lines: (defined in same way as electric field lines, direction and

More information

F = q v B. F = q E + q v B. = q v B F B. F = q vbsinφ. Lorentz. Bar Magnets. Right Hand Rule. The Magnetic Force. v +q. x x x x x x x x x x x x B

F = q v B. F = q E + q v B. = q v B F B. F = q vbsinφ. Lorentz. Bar Magnets. Right Hand Rule. The Magnetic Force. v +q. x x x x x x x x x x x x B ar Magnets ar magnet... two poles: and Like poles repel; Unlike poles attract. Magnetic ield lines: (defined in same way as electric field lines, direction and density) Attraction The unit for magnetic

More information

PHYS102 Effects of Magnetic Fields

PHYS102 Effects of Magnetic Fields PHYS102 Effects of Magnetic ields Dr. Suess March 12, 2007 Magnetic ields 2 Magnetic ields......................................................... 2 Behaior of Poles........................................................

More information

Magnetism has been observed since roughly 800 B.C. Certain rocks on the Greek peninsula of Magnesia were noticed to attract and repel one another.

Magnetism has been observed since roughly 800 B.C. Certain rocks on the Greek peninsula of Magnesia were noticed to attract and repel one another. 1.1 Magnetic ields Magnetism has been obsered since roughly 800.C. Certain rocks on the Greek peninsula of Magnesia were noticed to attract and repel one another. Hence the word: Magnetism. o just like

More information

Magnetic fields & forces

Magnetic fields & forces Phys 102 Lecture 10 Magnetic fields & forces 1 Today we will... Learn about the magnetism Magnetic field B Magnetic force F on moing charge Apply these concepts! Charged particle motion in a magnetic field

More information

F = q v B. F = q E + q v B. = q v B F B. F = q vbsinφ. Right Hand Rule. Lorentz. The Magnetic Force. More on Magnetic Force DEMO: 6B-02.

F = q v B. F = q E + q v B. = q v B F B. F = q vbsinφ. Right Hand Rule. Lorentz. The Magnetic Force. More on Magnetic Force DEMO: 6B-02. Lorentz = q E + q Right Hand Rule Direction of is perpendicular to plane containing &. If q is positie, has the same sign as x. If q is negatie, has the opposite sign of x. = q = q sinφ is neer parallel

More information

Physics 2112 Unit 12

Physics 2112 Unit 12 Physics 2112 Unit 12 Today s Concept: Magnetic Force on Moving Charges F qv B Unit 12, Slide 1 Where we are E fields B fields Stuff You asked about.. This is crazy. But also really cool. What is that "K"

More information

MAGNETIC EFFECTS OF CURRENT-3

MAGNETIC EFFECTS OF CURRENT-3 MAGNETIC EFFECTS OF CURRENT-3 [Motion of a charged particle in Magnetic field] Force On a Charged Particle in Magnetic Field If a particle carrying a positie charge q and moing with elocity enters a magnetic

More information

Physics 202, Lecture 12. Today s Topics

Physics 202, Lecture 12. Today s Topics Physics 202, Lecture 12 Today s Topics Magnetic orces (Ch. 27) Review: magnetic force, magnetic dipoles Motion of charge in uniform field: Applications: cyclotron, velocity selector, Hall effect Sources

More information

Forces & Magnetic Dipoles. Phys 122 Lecture 18 D. Hertzog

Forces & Magnetic Dipoles. Phys 122 Lecture 18 D. Hertzog orces & Magnetic Dipoles µ = τ U AI = µ = µ θ θ. Phys 122 Lecture 18 D. Hertzog µ usiness Regrade requests by 4 pm riday (no eceptions) Solutions/Key posted on home page Last Time: The Lorentz orce and

More information

Earth as a Magnet. The strength and orientation of the earth s magnetic field varies over time and location.

Earth as a Magnet. The strength and orientation of the earth s magnetic field varies over time and location. Magnetism Magnetic charges Called poles Two types, North and South Like poles repel each other Opposite poles attract each other Found only in North/South pairs (Dipoles) N S Magnetism Magnetic poles Found

More information

Force Due to Magnetic Field You will use

Force Due to Magnetic Field You will use Force Due to Magnetic Field You will use Units: 1 N = 1C(m/s) (T) A magnetic field of one tesla is very powerful magnetic field. Sometimes it may be convenient to use the gauss, which is equal to 1/10,000

More information

Magnetostatics. P.Ravindran, PHY041: Electricity & Magnetism 22 January 2013: Magntostatics

Magnetostatics. P.Ravindran, PHY041: Electricity & Magnetism 22 January 2013: Magntostatics Magnetostatics Magnetic Fields We saw last lecture that some substances, particularly iron, possess a property we call magnetism that exerts forces on other magnetic materials We also saw that t single

More information

3/7/2019 N S N S. Magnetism. Magnetism

3/7/2019 N S N S. Magnetism. Magnetism Magnetism Magnetic charges Called poles Two types, North and South Like poles repel each other Opposite poles attract each other Found only in North/South pairs (Dipoles) Magnetism Magnetic poles Found

More information

Electricity & Magnetism Lecture 12

Electricity & Magnetism Lecture 12 Electricity & Magnetism Lecture 12 Today s Concept: Magne2c Force on Moving Charges Electricity & Magne2sm Lecture 12, Slide 1 Today s rants I'm struggling a fair bit with this component of the course.

More information

Last Time: Start Rotational Motion (now thru mid Nov) Basics: Angular Speed, Angular Acceleration

Last Time: Start Rotational Motion (now thru mid Nov) Basics: Angular Speed, Angular Acceleration Last Time: Start Rotational Motion (now thru mid No) Basics: Angular Speed, Angular Acceleration Today: Reiew, Centripetal Acceleration, Newtonian Graitation i HW #6 due Tuesday, Oct 19, 11:59 p.m. Exam

More information

Version 001 HW#5 - Magnetism arts (00224) 1

Version 001 HW#5 - Magnetism arts (00224) 1 Version 001 HW#5 - Magnetism arts (004) 1 This print-out should hae 11 questions. Multiple-choice questions may continue on the net column or page find all choices before answering. Charged Particle in

More information

Agenda for Today. Elements of Physics II. Forces on currents

Agenda for Today. Elements of Physics II. Forces on currents Forces on currents Physics 132: Lecture e 20 Elements of Physics II Agenda for Today Currents are moving charges Torque on current loop Torque on rotated loop Currents create B-fields Adding magnetic fields

More information

Physics 202, Lecture 11

Physics 202, Lecture 11 Physics 202, Lecture 11 Today s Topics Magnetic Fields and Forces (Ch. 27) Magnetic materials Magnetic forces on moving point charges Magnetic forces on currents, current loops Motion of charge in uniform

More information

Magnetic Fields & Forces

Magnetic Fields & Forces Magnetic Fields & Forces Oersted discovered that an electric current will produce a magnetic field around conductor only a moving charge creates a magnetic field the magnetic field is circular around the

More information

Motion of a charged particle in an Electric Field

Motion of a charged particle in an Electric Field Motion of a charged particle in an Electric Field The electric force F that acts on a positive charge is parallel to the electric field E and causes the particle s trajectory to bend in a horizontal plane.

More information

Magnetic Force http://www-spof.gsfc.nasa.gov/education/imagnet.html The ancient Greeks, originally those near the city of Magnesia, and also the early Chinese knew about strange and rare stones (possibly

More information

Magnetic Fields & Forces

Magnetic Fields & Forces Magnetic Fields & Forces Oersted discovered that an electric current will produce a magnetic field around conductor only a moving charge creates a magnetic field the magnetic field is circular around the

More information

Chapter 27: Magnetic Field and Magnetic Forces

Chapter 27: Magnetic Field and Magnetic Forces Chapter 27: Magnetic Field and Magnetic Forces Iron ore found near Magnesia Compass needles align N-S: magnetic Poles North (South) Poles attracted to geographic North (South) Like Poles repel, Opposites

More information

a) (4 pts) What is the magnitude and direction of the acceleration of the electron?

a) (4 pts) What is the magnitude and direction of the acceleration of the electron? PHYSCS 22 Fall 2010 - MDTERM #3 SHOW ALL WORK & REASONNG FOR FULL PONTS Question 1. (5 pts): Accurately show or state the direction of the force that is felt by the following charges or currents. +q -q

More information

Chapter 27, 28 & 29: Magnetism & Electromagnetic Induction

Chapter 27, 28 & 29: Magnetism & Electromagnetic Induction Chapter 27, 28 & 29: Magnetism & Electromagnetic Induction The Magnetic Field The Magnetic Force on Moving Charges The Motion of Charged Particles in a Magnetic Field The Magnetic Force Exerted on a Current-Carrying

More information

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field.

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. MAGNETIC DEFLECTION OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. THEORY: Moving charges exert forces on one another that are not observed

More information

Magnetic Fields Permanent Magnets

Magnetic Fields Permanent Magnets 1 Magnetic Fields Permanent Magnets Magnetic fields are continuous loops leaving a North pole and entering a South pole they point in direction that an isolated North would move Highest strength near poles

More information

Solar Winds. N.G. Schultheiss translated and adapted by K. Schadenberg. This module follows upon The Sun and can be continued by Cosmic Radiation.

Solar Winds. N.G. Schultheiss translated and adapted by K. Schadenberg. This module follows upon The Sun and can be continued by Cosmic Radiation. Solar Winds N.G. Schultheiss translated and adapted by K. Schadenberg 1 Introduction This module follows upon The Sun and can be continued by Cosmic Radiation. Solar Wind The Sun emits large amounts of

More information

Even the ancients knew about magnets.

Even the ancients knew about magnets. Een the ancients knew about magnets Ho ho, foolish explorers your compasses are useless here! Magnetic Fields hae units of Tesla Magnetic Fields hae a symbol () = 01 Tesla For example: = 01 Tesla 1 = 3x10-5

More information

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field.

MAGNETIC DEFLECTION. OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. MAGNETIC DEFLECTION OBJECTIVE: To observe the effect of a magnetic field on an electron beam. To measure the Earth s magnetic field. THEORY: Moving charges exert forces on one another that are not observed

More information

Magnetic fields. The symbol we use for a magnetic field is B. The unit is the tesla (T). The Earth s magnetic field is about 5 x 10-5 T.

Magnetic fields. The symbol we use for a magnetic field is B. The unit is the tesla (T). The Earth s magnetic field is about 5 x 10-5 T. Magnetic fields The symbol we use for a magnetic field is B. The unit is the tesla (T). The Earth s magnetic field is about 5 x 10-5 T. Which pole of a magnet attracts the north pole of a compass? Which

More information

Elements of Physics II. Agenda for Today. Physics 201: Lecture 1, Pg 1

Elements of Physics II. Agenda for Today. Physics 201: Lecture 1, Pg 1 Forces on currents Physics 132: Lecture e 19 Elements of Physics II Agenda for Today Currents are moving charges Torque on current loop Torque on rotated loop Currents create B-fields Adding magnetic fields

More information

Phys102 Lecture 16/17 Magnetic fields

Phys102 Lecture 16/17 Magnetic fields Phys102 Lecture 16/17 Magnetic fields Key Points Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on an Electric Charge Moving in a Magnetic

More information

Agenda for Today. Elements of Physics II. Forces on currents

Agenda for Today. Elements of Physics II. Forces on currents Forces on currents Physics 132: Lecture e 19 Elements of Physics II Agenda for Today Currents are moving charges Torque on current loop Torque on rotated loop Currents create B-fields Adding magnetic fields

More information

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS CHAPTER B TEST REVIEW. A rocket is fired ertically. At its highest point, it explodes. Which one of the following describes what happens

More information

Magnetism. Permanent magnets Earth s magnetic field Magnetic force Motion of charged particles in magnetic fields

Magnetism. Permanent magnets Earth s magnetic field Magnetic force Motion of charged particles in magnetic fields Magnetism Permanent magnets Earth s magnetic field Magnetic force Motion of charged particles in magnetic fields Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

More information

Physics 139 Relativity. Thomas Precession February 1998 G. F. SMOOT. Department ofphysics, University of California, Berkeley, USA 94720

Physics 139 Relativity. Thomas Precession February 1998 G. F. SMOOT. Department ofphysics, University of California, Berkeley, USA 94720 Physics 139 Relatiity Thomas Precession February 1998 G. F. SMOOT Department ofphysics, Uniersity of California, erkeley, USA 94720 1 Thomas Precession Thomas Precession is a kinematic eect discoered by

More information

Physics 1202: Lecture 7 Today s Agenda. Today s Topic :

Physics 1202: Lecture 7 Today s Agenda. Today s Topic : Physics 1202: Today s Agenda Announcements: Lectures posted on: www.phys.uconn.edu/~rcote/ Office hours: Monday 2:30-3:30 Thursday 3:00-4:00 Homework #2: due this coming Friday/ Labs: Already begun last

More information

PHYSICS 3204 PUBLIC EXAM QUESTIONS (Magnetism &Electromagnetism)

PHYSICS 3204 PUBLIC EXAM QUESTIONS (Magnetism &Electromagnetism) PHYSICS 3204 PUBLIC EXAM QUESTIONS (Magnetism &Electromagnetism) NAME: August 2009---------------------------------------------------------------------------------------------------------------------------------

More information

General Physics (PHYS )

General Physics (PHYS ) General Physics (PHYS ) Chapter 22 Magnetism Magnetic Force Exerted on a current Magnetic Torque Electric Currents, magnetic Fields, and Ampere s Law Current Loops and Solenoids Magnetism in Matter Magnetism

More information

Physics Week 5(Sem. 2) Name. Magnetism. Chapter Summary. Magnetic Fields

Physics 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 information

Chapter 29. Magnetic Fields

Chapter 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 information

Your Comments. I don't understand how to find current given the velocity and magnetic field. I only understand how to find external force

Your Comments. I don't understand how to find current given the velocity and magnetic field. I only understand how to find external force Your Comments CONFUSED! Especially with the direction of eerything The rotating loop checkpoint question is incredibly difficult to isualize. All of this is pretty confusing, but 'm especially confused

More information

Magnetic field and magnetic poles

Magnetic field and magnetic poles Magnetic field and magnetic poles Magnetic Field B is analogically similar to Electric Field E Electric charges (+ and -)are in analogy to magnetic poles(north:n and South:S). Paramagnetism, Diamagnetism,

More information

Lecture #4.4 Magnetic Field

Lecture #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 information

Ch24 Page 1. Chapter 24 Magnetic Fields and Forces Thursday, March 11, :26 PM

Ch24 Page 1. Chapter 24 Magnetic Fields and Forces Thursday, March 11, :26 PM Ch24 Page 1 Chapter 24 Magnetic Fields and Forces Thursday, March 11, 2010 8:26 PM Ch24 Page 2 It seems that microscopic electric currents are the ultimate cause of magnetism. For example, each neutron

More information

Chapter 21. Magnetic Forces and Magnetic Fields

Chapter 21. Magnetic Forces and Magnetic Fields Chapter 21 Magnetic Forces and Magnetic Fields 21.1 Magnetic Fields The needle of a compass is permanent magnet that has a north magnetic pole (N) at one end and a south magnetic pole (S) at the other.

More information

Electricity and Magnetism Motion of Charges in Magnetic Fields

Electricity and Magnetism Motion of Charges in Magnetic Fields Electricity and Magnetism Motion of Charges in Magnetic Fields Lana heridan De Anza College Feb 21, 2018 Last time introduced magnetism magnetic field Earth s magnetic field force on a moing charge Oeriew

More information

Physics Electricity and Magnetism Lecture 09 - Charges & Currents in Magnetic Fields Y&F Chapter 27, Sec. 1-8

Physics Electricity and Magnetism Lecture 09 - Charges & Currents in Magnetic Fields Y&F Chapter 27, Sec. 1-8 Phsics 121 - Electricit and Magnetism Lecture 09 - Charges & Currents in Magnetic Fields Y&F Chapter 27, Sec. 1-8 What Produces Magnetic Field? Properties of Magnetic ersus Electric Fields Force on a Charge

More information

10/24/2012 PHY 102. (FAWOLE O.G.) Good day. Here we go..

10/24/2012 PHY 102. (FAWOLE O.G.) Good day. Here we go.. Good day. Here we go.. 1 PHY102- GENERAL PHYSICS II Text Book: Fundamentals of Physics Authors: Halliday, Resnick & Walker Edition: 8 th Extended Lecture Schedule TOPICS: Dates Ch. 28 Magnetic Fields 12

More information

Physics 25 Chapter 21 Dr. Alward

Physics 25 Chapter 21 Dr. Alward Physics 25 Chapter 21 Dr. Alward Magnetism and Magnetic Forces Magnetic Field of a Bar Magnet Magnetic field lines flow away from the north pole and sink on the south pole. Like Poles Repel Unlike Poles

More information

Chapter 11 Collision Theory

Chapter 11 Collision Theory Chapter Collision Theory Introduction. Center o Mass Reerence Frame Consider two particles o masses m and m interacting ia some orce. Figure. Center o Mass o a system o two interacting particles Choose

More information

Electrics. Electromagnetism

Electrics. 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 information

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS SUBAREA I. COMPETENCY 1.0 UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS MECHANICS Skill 1.1 Calculating displacement, aerage elocity, instantaneous elocity, and acceleration in a gien frame of reference

More information

AP Physics Electromagnetic Wrap Up

AP Physics Electromagnetic Wrap Up AP Physics Electromagnetic Wrap Up Here are the glorious equations for this wonderful section. This is the equation for the magnetic force acting on a moving charged particle in a magnetic field. The angle

More information

MOTION IN 2-DIMENSION (Projectile & Circular motion And Vectors)

MOTION IN 2-DIMENSION (Projectile & Circular motion And Vectors) MOTION IN -DIMENSION (Projectile & Circular motion nd Vectors) INTRODUCTION The motion of an object is called two dimensional, if two of the three co-ordinates required to specif the position of the object

More information

PHYSICS - CLUTCH CH 26: MAGNETIC FIELDS AND FORCES.

PHYSICS - CLUTCH CH 26: MAGNETIC FIELDS AND FORCES. !! www.clutchprep.com CONCEPT: HOW MAGNETS WORK Forever ago we found metals that would attract each other. First found in island of Magnesia named. - Most common are iron (Fe), cobalt (Co), nickel (Ni),

More information

Physics 1: Mechanics

Physics 1: Mechanics Physics 1: Mechanics Đào Ngọc Hạnh Tâm Office: A1.53, Email: dnhtam@hcmiu.edu.n HCMIU, Vietnam National Uniersity Acknowledgment: Most of these slides are supported by Prof. Phan Bao Ngoc credits (3 teaching

More information

PHY 1214 General Physics II

PHY 1214 General Physics II PHY 1214 General Physics II Lecture 15 Magnetic Fields and Forces June 28, 2005 Weldon J. Wilson Professor of Physics & Engineering Howell 221H wwilson@ucok.edu Lecture Schedule (Weeks 4-6) We are here.

More information

Physics H. Instructor: Dr. Alaa Mahmoud

Physics H. Instructor: Dr. Alaa Mahmoud Physics 202 1436-1437 H Instructor: Dr. Alaa Mahmoud E-mail: alaa_y_emam@hotmail.com Chapter 28 magnetic Field Magnetic fingerprinting allows fingerprints to be seen on surfaces that otherwise would not

More information

Torque on a Current Loop

Torque 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 information

PHYS ND semester Dr. Nadyah Alanazi. Lecture 16

PHYS ND semester Dr. Nadyah Alanazi. Lecture 16 1 PHYS 104 2 ND semester 1439-1440 Dr. Nadyah Alanazi Lecture 16 2 Chapter 29 Magnetic Field 29.1 Magnetic Fields and Forces 29.2 Magnetic Force Acting on a Current-Carrying Conductor 29.4 Motion of a

More information

Magnetic Fields. or I in the filed. ! F = q! E. ! F = q! v! B. q! v. Charge q as source. Current I as source. Gauss s Law. Ampere s Law.

Magnetic Fields. or I in the filed. ! F = q! E. ! F = q! v! B. q! v. Charge q as source. Current I as source. Gauss s Law. Ampere s Law. Magnetic Fields Charge q as source Gauss s Law Electric field E F = q E Faraday s Law Ampere-Maxwell Law Current I as source Magnetic field B Ampere s Law F = q v B Force on q in the field Force on q v

More information

Chapter 22 Magnetism

Chapter 22 Magnetism Chapter 22 Magnetism 1 Overview of Chapter 22 The Magnetic Field The Magnetic Force on Moving Charges The Motion of Charged Particles in a Magnetic Field The Magnetic Force Exerted on a Current-Carrying

More information

1. Draw in the magnetic field inside each box that would be capable of deflecting the particle along the path shown in each diagram.

1. Draw in the magnetic field inside each box that would be capable of deflecting the particle along the path shown in each diagram. Charged Particles in Magnetic Fields 1. Draw in the magnetic field inside each box that would be capable of deflecting the particle along the path shown in each diagram. a b c d 2. a. Three particles with

More information

So now that we ve mentioned these terms : kinetic, potential, work we should try to explain them more. Let s develop a model:

So now that we ve mentioned these terms : kinetic, potential, work we should try to explain them more. Let s develop a model: Lecture 12 Energy e are now at the point where we can talk about one of the most powerful tools in physics, energy. Energy is really an abstract concept. e hae indicators of energy (temperature, elocity

More information

AP Physics Multiple Choice Practice Gravitation

AP Physics Multiple Choice Practice Gravitation AP Physics Multiple Choice Practice Graitation. Each of fie satellites makes a circular orbit about an object that is much more massie than any of the satellites. The mass and orbital radius of each satellite

More information

Gravity Electromagnetism Weak Strong

Gravity Electromagnetism Weak Strong 19. Magnetism 19.1. Magnets 19.1.1. Considering the typical bar magnet we can investigate the notion of poles and how they apply to magnets. 19.1.1.1. Every magnet has two distinct poles. 19.1.1.1.1. N

More information

Chapter 20 Lecture Notes

Chapter 20 Lecture Notes Chapter 20 Lecture Notes Physics 2424 - Strauss Formulas: B = µ 0 I/2πr B = Nµ 0 I/(2R) B = µ 0 ni Σ B l = µ 0 I F = Bqv sinθ r = mv/bq m = (er 2 /2V) B 2 F = ILB sinθ τ = NIAB sinϕ F/L = I 2 I 1 µ 0 /2πd

More information

CHAPTER 20 Magnetism

CHAPTER 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 information

Phys 102 Lecture 12 Currents & magnetic fields

Phys 102 Lecture 12 Currents & magnetic fields Phys 102 Lecture 12 Currents & magnetic fields 1 Today we will... Learn how magnetic fields are created by currents Use specific examples Long straight wire Current loop Solenoid Apply these concepts Electromagnets

More information

The force F on a charge q moving with velocity v through a region of space with electric field E and magnetic field B is given by: F qe qv B

The force F on a charge q moving with velocity v through a region of space with electric field E and magnetic field B is given by: F qe qv B Lorentz Forces The force F on a charge q moving with velocity v through a region of space with electric field E and magnetic field B is given by: F qe qv B F qv B B F q vbsin 2/20/2018 1 Right Hand Rule

More information

Physics 11b Lecture #10

Physics 11b Lecture #10 Physics 11b Lecture #10 Magnetic Fields S&J Chapter 29 What We Did Last Time Electromotive forces (emfs) atteries are made of an emf and an internal resistance Resistor arithmetic R = R + R + R + + R series

More information

Physics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1

Physics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1 Physics 1 Lecture 1 Tday's Cncept: Magnetic Frce n mving charges F qv Physics 1 Lecture 1, Slide 1 Music Wh is the Artist? A) The Meters ) The Neville rthers C) Trmbne Shrty D) Michael Franti E) Radiatrs

More information

Physics 212. Motional EMF

Physics 212. Motional EMF Physics 212 ecture 16 Motional EMF Conductors moing in field nduced emf!! Physics 212 ecture 16, Slide 1 The ig dea When a conductor moes through a region containg a magnetic field: Magnetic forces may

More information

Chapter 21. Magnetism

Chapter 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 information

1. The figure shows two long parallel wires carrying currents I 1 = 15 A and I 2 = 32 A (notice the currents run in opposite directions).

1. The figure shows two long parallel wires carrying currents I 1 = 15 A and I 2 = 32 A (notice the currents run in opposite directions). Final Eam Physics 222 7/29/211 NAME Use o = 8.85 1-12 C 2 /N.m 2, o = 9 1 9 N.m 2 /C 2, o/= 1-7 T m/a There are additional formulas in the final page of this eam. 1. The figure shows two long parallel

More information

Lecture 23: FRI 16 OCT

Lecture 23: FRI 16 OCT Aurora Borealis Physics 2113 Jonathan Dowling Lecture 23: FRI 16 OCT Magnetic Fields I I ll be back. How Do You Use Magnetic Fields in Your Everyday Life? 28.2: What Produces Magnetic Field?: One way

More information

Magnetic Fields and Forces

Magnetic 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 information

Chapter 19. Magnetism

Chapter 19. Magnetism Chapter 19 Magnetism The figure shows the path of a negatively charged particle in a region of a uniform magnetic field. Answer the following questions about this situation (in each case, we revert back

More information

Certain iron containing materials have been known to attract or repel each other. Compasses align to the magnetic field of earth.

Certain iron containing materials have been known to attract or repel each other. Compasses align to the magnetic field of earth. Certain iron containing materials hae been known to attract or repel each other. Compasses align to the magnetic field of earth. Analogous to positie and negatie charges, eery magnet has a north and a

More information

4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion.

4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion. 4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion. We now hae deeloped a ector model that allows the ready isualization

More information

Magnetism is associated with charges in motion (currents):

Magnetism 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 information

CURRENT-CARRYING CONDUCTORS / MOVING CHARGES / CHARGED PARTICLES IN CIRCULAR ORBITS

CURRENT-CARRYING CONDUCTORS / MOVING CHARGES / CHARGED PARTICLES IN CIRCULAR ORBITS PHYSICS A2 UNIT 4 SECTION 4: MAGNETIC FIELDS CURRENT-CARRYING CONDUCTORS / MOVING CHARGES / CHARGED PARTICLES IN CIRCULAR ORBITS # Questions MAGNETIC FLUX DENSITY 1 What is a magnetic field? A region in

More information

Elements of Physics II. Agenda for Today

Elements of Physics II. Agenda for Today Physics 132: Lecture e 18 Elements of Physics II Agenda for Today Magnets and the Magnetic Field Magnetic fields caused by charged particles B-field from a current-carrying wire Magnetic fields and forces

More information

MODULE 6 ELECTROMAGNETISM MAGNETIC FIELDS MAGNETIC FLUX VISUAL PHYSICS ONLINE

MODULE 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 information

Chapter 28. Magnetic Fields. Copyright 2014 John Wiley & Sons, Inc. All rights reserved.

Chapter 28. Magnetic Fields. Copyright 2014 John Wiley & Sons, Inc. All rights reserved. Chapter 28 Magnetic Fields Copyright 28-2 What Produces a Magnetic Field? 1. Moving electrically charged particles ex: current in a wire makes an electromagnet. The current produces a magnetic field that

More information

Magnetic Force. A vertical wire carries a current and is in a vertical magnetic field. What is the direction of the force on the wire?

Magnetic Force. A vertical wire carries a current and is in a vertical magnetic field. What is the direction of the force on the wire? Magnetic Force A vertical wire carries a current and is in a vertical magnetic field. What is the direction of the force on the wire? (a) left (b) right (c) zero (d) into the page (e) out of the page B

More information

General Lorentz Boost Transformations, Acting on Some Important Physical Quantities

General Lorentz Boost Transformations, Acting on Some Important Physical Quantities General Lorentz Boost Transformations, Acting on Some Important Physical Quantities We are interested in transforming measurements made in a reference frame O into measurements of the same quantities as

More information

Today s lecture: Motion in a Uniform Magnetic Field continued Force on a Current Carrying Conductor Introduction to the Biot-Savart Law

Today s lecture: Motion in a Uniform Magnetic Field continued Force on a Current Carrying Conductor Introduction to the Biot-Savart Law PHYSICS 1B Today s lecture: Motion in a Uniform Magnetic Field continued Force on a Current Carrying Conductor Introduction to the Biot-Savart Law Electricity & Magnetism A Charged Particle in a Magnetic

More information

PHY132 Lecture 13 02/24/2010. Lecture 13 1

PHY132 Lecture 13 02/24/2010. Lecture 13 1 Classical Physics II PHY132 Lecture 13 Magnetism II: Magnetic torque Lecture 13 1 Magnetic Force MAGNETISM is yet another force that has been known since a very long time. Its name stems from the mineral

More information

3 Charged Particle Motion in a Magnetic Field

3 Charged Particle Motion in a Magnetic Field 3 Charged Particle Motion in a Magnetic Field When you have completed the Particle Annihilation section and read all the text (especially section 2.2), click the Next button in the Particle Annihilation

More information

4. An electron moving in the positive x direction experiences a magnetic force in the positive z direction. If B x

4. An electron moving in the positive x direction experiences a magnetic force in the positive z direction. If B x Magnetic Fields 3. A particle (q = 4.0 µc, m = 5.0 mg) moves in a uniform magnetic field with a velocity having a magnitude of 2.0 km/s and a direction that is 50 away from that of the magnetic field.

More information

Physics 2D Lecture Slides Jan 15. Vivek Sharma UCSD Physics

Physics 2D Lecture Slides Jan 15. Vivek Sharma UCSD Physics Physics D Lecture Slides Jan 15 Vivek Sharma UCSD Physics Relativistic Momentum and Revised Newton s Laws and the Special theory of relativity: Example : p= mu Need to generalize the laws of Mechanics

More information

Chapter 23 non calculus

Chapter 23 non calculus Chapter 23 non calculus Magnetism CHAPTER 23 MAGNETISM In our discussion of Coulomb's law, we saw that electric forces are ery strong but in most circumstances tend to cancel. The strength of the forces

More information

Magnetic Forces and Magnetic Fields

Magnetic Forces and Magnetic Fields Magnetic Forces and Magnetic Fields 21.1 Magnetic Fields The behavior of magnetic poles is similar to that of like and unlike electric charges. 21.1 Magnetic Fields The needle of a compass is permanent

More information

Intermediate Physics PHYS102

Intermediate Physics PHYS102 Intermediate Physics PHYS102 Dr Richard H. Cyburt Assistant Professor of Physics My office: 402c in the Science Building My phone: (304) 384-6006 My email: rcyburt@concord.edu My webpage: www.concord.edu/rcyburt

More information