Magnetism and Vectors

Size: px
Start display at page:

Download "Magnetism and Vectors"

Transcription

1 Physics 1051 Workshop 5 Magnetism and Vectors

2 Workshop 5 - Contents I. Where do Vector Cross Products Appear? II. Review of What We've Seen Already I. Magnetic Force on a Charge Particle II.Magnetic Force on Current Carrying Wire III. Cross Product I. Unit Vector Notation Method II.Magnitude Angle Method III.A Few Tips IV. Example 2

3 I Where do Vector Cross Products Appear? 3

4 Magnetic Cross Product Magnetic Force Magnetic Field Torque F B =q v d = 0 4 = r F I ds r r 2 F B =I l = =I A 4

5 II Review of What We've Seen Already 5

6 Magnetic Force On a Charge F B =q v Quantity Type SI Unit Vector N F B q is magnetic force due to magnetic field is charge on charge object (include sign!) v is velocity vector of object is magnetic field [B]=Tesla=Ns/Cm 6

7 Magnetic Force on a Current Carrying Wire F B =I l Quantity Type SI Unit Vector N F B I l is magnetic force on a wire due magnetic field is current in the wire is length vector of object (points in direction of current) is magnetic field [B]=Tesla=Ns/Cm 7

8 III - Cross Product 8

9 Review of Cross Product There are two methods Unit Vector Notation Magnitude Angle Method You will need to be familiar with these methods. With experience some. In the mean time, there are some tips or suggestions that might help... 9

10 Cross Product - Unit Vector Notation Method The steps for this method are Write both vectors in unit vector notation May require finding components Multiply Using Distributive Law Use known information about cross product of the unit vectors A A= A x i A y j A z k =B x i y j z k C= A i i=0 i j= k i k = j j i= k j j=0 j k= i k i = j k j= i k k=0 10

11 Cross Product - Magnitude Angle Method The steps for this method are A Find magnitude of both vectors and angle between them Might need to find angle Might need to find magnitudes Find magnitude using magnitude formula C= A B sin Find direction using right and rule A B C z Still need to specify as angle from coordinate axes. x A y 11

12 Magnitude Angle Method - Right Hand Rule This applies to finding the direction for the result of the cross product between any two vectors. With open palm and thumb off at right angle, point your fingers along first vector Rotate your wrist until hand is oriented such that when you curl fingers they can point along second vector Thumb points in direction of resultant C= A x z C A 12 y

13 Tips for Choosing Method for Finding Cross Product Use Magnitude Angle Method If both vectors are in the same Cartesian plane. Direction can easily be found/specified as unit vector perpendicular from that plane. Possibly if you are given magnitude of both vectors and angle between Use Unit Vector Notation Example x C z z I y Basically any other time Example x A 13 y

14 IV - Example 14

15 Simple Example A Vertical Line of Charge A wire in the figure has a current of 4.0 A. One segment is vertical and of length 0.05 m. The other makes an angle of 10º with the horizontal and has a length of 2.5 m. If it is in a uniform magnetic field of magnitude 0.08 T, what is the total magnetic force on the wire? I 15

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

Biot-Savart. The equation is this:

Biot-Savart. The equation is this: Biot-Savart When a wire carries a current, this current produces a magnetic field in the vicinity of the wire. One way of determining the strength and direction of this field is with the Law of Biot-Savart.

More information

CH 19-1 Magnetic Field

CH 19-1 Magnetic Field CH 19-1 Magnetic Field Important Ideas A moving charged particle creates a magnetic field everywhere in space around it. If the particle has a velocity v, then the magnetic field at this instant is tangent

More information

May 08, Magnetism.notebook. Unit 9 Magnetism. This end points to the North; call it "NORTH." This end points to the South; call it "SOUTH.

May 08, Magnetism.notebook. Unit 9 Magnetism. This end points to the North; call it NORTH. This end points to the South; call it SOUTH. Unit 9 Magnetism This end points to the North; call it "NORTH." This end points to the South; call it "SOUTH." 1 The behavior of magnetic poles is similar to that of like and unlike electric charges. Law

More information

Chapter 19. Magnetism

Chapter 19. Magnetism Chapter 19 Magnetism Magnetic Fields When moving through a magnetic field, a charged particle experiences a magnetic force This force has a maximum value when the charge moves perpendicularly to the magnetic

More information

Chapter 24: Magnetic Fields & Forces

Chapter 24: Magnetic Fields & Forces Chapter 24: Magnetic Fields & Forces We live in a magnetic field. The earth behaves almost as if a bar magnet were located near its center. The earth s axis of rotation and Magnetic axis are not the same

More information

Chapter 24. Magnetic Fields

Chapter 24. Magnetic Fields Chapter 24 Magnetic Fields 1 Magnetic Poles Every magnet, regardless of its shape, has two poles Called north and south poles Poles exert forces on one another Similar to the way electric charges exert

More information

MOMENT OF A FORCE ABOUT A POINT

MOMENT OF A FORCE ABOUT A POINT MOMENT OF A FORCE ABOUT A POINT The tendency of a body to rotate about an axis passing through a specific point O when acted upon by a force (sometimes called a torque). 1 APPLICATIONS A torque or moment

More information

Engineering Mechanics Statics

Engineering Mechanics Statics Mechanical Systems Engineering -2016 Engineering Mechanics Statics 3. Force Vectors; Position Vector & Dot product Position Vector A position vector is a fixed vector that locates a point in space relative

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

VECTORS. Given two vectors! and! we can express the law of vector addition geometrically. + = Fig. 1 Geometrical definition of vector addition

VECTORS. Given two vectors! and! we can express the law of vector addition geometrically. + = Fig. 1 Geometrical definition of vector addition VECTORS Vectors in 2- D and 3- D in Euclidean space or flatland are easy compared to vectors in non- Euclidean space. In Cartesian coordinates we write a component of a vector as where the index i stands

More information

Tute UV2 : VECTORS 1

Tute UV2 : VECTORS 1 Tute UV2 : VECTORS 1 a b = ab cos θ a b = ab sin θ 1. A vector s is 4.2 m long and is directed at an angle of 132 anticlockwise relative to the x-axis as drawn below. Express s in i, j, k components. [

More information

Magnetic Forces and Fields

Magnetic Forces and Fields Magnetic Forces and Fields Physics 102 Lecture 3 21 February 2002 IF NOT REGISTERED FOR PHYSICS 102, SEE REGISTRAR ASAP, AND REGISTER 21 Feb 2002 Physics 102 Lecture 3 1 RC Puzzler 21 Feb 2002 Physics

More information

PHYS152 Lecture 8. Eunil Won Korea University. Ch 30 Magnetic Fields Due to Currents. Fundamentals of Physics by Eunil Won, Korea University

PHYS152 Lecture 8. Eunil Won Korea University. Ch 30 Magnetic Fields Due to Currents. Fundamentals of Physics by Eunil Won, Korea University PHYS152 Lecture 8 Ch 3 Magnetic Fields Due to Currents Eunil Won Korea University Calculating the Magnetic Field Due to a Current Recall that we had the formula for the electrostatic force: d E = 1 ɛ dq

More information

Three-Dimensional Coordinate Systems. Three-Dimensional Coordinate Systems. Three-Dimensional Coordinate Systems. Three-Dimensional Coordinate Systems

Three-Dimensional Coordinate Systems. Three-Dimensional Coordinate Systems. Three-Dimensional Coordinate Systems. Three-Dimensional Coordinate Systems To locate a point in a plane, two numbers are necessary. We know that any point in the plane can be represented as an ordered pair (a, b) of real numbers, where a is the x-coordinate and b is the y-coordinate.

More information

Physics 4. Magnetic Forces and Fields. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 4. Magnetic Forces and Fields. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Physics 4 Magnetic Forces and Fields What creates a magnetic field? Answer: MOVING CHARGES What is affected by a magnetic field? Answer: MOVING CHARGES We have a formula for magnetic force on a moving

More information

Physics 1051 Laboratory #10 Simple DC Motor The Simple DC Motor

Physics 1051 Laboratory #10 Simple DC Motor The Simple DC Motor 1 The 2 Prelab Write experiment title, your name and student number at top of the page. Prelab 1: Write the objective of this experiment. Prelab 2: Write the relevant theory of this experiment. Prelab

More information

Chapter -4- Force System Resultant

Chapter -4- Force System Resultant Ishik University / Sulaimani Civil Engineering Department Chapter -4- Force System Resultant 1 2 1 CHAPTER OBJECTIVES To discuss the concept of the moment of a force and show how to calculate it in two

More information

Mechanics 1: Coordinates

Mechanics 1: Coordinates Mechanics 1: Coordinates We have emphasized that our development of the definition and properties of vectors did not utilize at all the notion of a coordinate system, i.e., an agreed upon set of locations

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

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

Physics 152. Magnets Earth/Dipole Field Charges & Magnetic Fields. Announcements. Friday, April 13, 2007

Physics 152. Magnets Earth/Dipole Field Charges & Magnetic Fields. Announcements. Friday, April 13, 2007 ics ri Apr.13. Announcements Magnets arth/dipole ield Charges & Magnetic ields riday, April 13, 2007 Help sessions 9-10 pm in C 119 Masteringics U #20 due Mon., April 16 U #21 due ri., April 20 Rework

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

Magnets. Magnetic vs. Electric

Magnets. Magnetic vs. Electric Magnets A force is applied to the iron filings causing them to align themselves to the direction of the magnetic field. A compass needle will tell you the direction of the field. Show Fields of little

More information

Physics 2212 G Quiz #4 Solutions Spring 2018 = E

Physics 2212 G Quiz #4 Solutions Spring 2018 = E Physics 2212 G Quiz #4 Solutions Spring 2018 I. (16 points) The circuit shown has an emf E, three resistors with resistance, and one resistor with resistance 3. What is the current through the resistor

More information

Problem Solving 4 Solutions: Magnetic Force, Torque, and Magnetic Moments

Problem Solving 4 Solutions: Magnetic Force, Torque, and Magnetic Moments MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.0 Spring 004 Problem Solving 4 Solutions: Magnetic Force, Torque, an Magnetic Moments OJECTIVES 1. To start with the magnetic force on a moving

More information

VCE PHYSICS AOS 1 UNIT 4. Presented by Nick Howes

VCE PHYSICS AOS 1 UNIT 4. Presented by Nick Howes VCE PHYSICS AOS 1 UNIT 4 Presented by Nick Howes Forces on wires and DC Motors Key knowledge calculate magnitudes, including determining the directions of, and magnetic forces on, current carrying wires,

More information

$ B 2 & ) = T

$ B 2 & ) = T Solutions PHYS 251 Final Exam Practice Test 1D If we find the resultant velocity, v, its vector is 13 m/s. This can be plugged into the equation for magnetic force: F = qvb = 1.04 x 10-17 N, where q is

More information

Section 13.4 The Cross Product

Section 13.4 The Cross Product Section 13.4 The Cross Product Multiplying Vectors 2 In this section we consider the more technical multiplication which can be defined on vectors in 3-space (but not vectors in 2-space). 1. Basic Definitions

More information

Magnetic Force Acting on a Current- Carrying Conductor IL B

Magnetic Force Acting on a Current- Carrying Conductor IL B Magnetic Force Acting on a Current- Carrying Conductor A segment of a current-carrying wire in a magnetic field. The magnetic force exerted on each charge making up the current is qvd and the net force

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

Kirchhoff s rules, example

Kirchhoff s rules, example Kirchhoff s rules, example Magnets and Magnetism 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

More information

Experiment No: EM 4 Experiment Name: Biot-Savart Law Objectives:

Experiment No: EM 4 Experiment Name: Biot-Savart Law Objectives: Experiment No: EM 4 Experiment Name: Biot-Savart Law Objectives: Measuring the magnetic field of a current passing through long straight and conductor wire as a function of the current. Measuring the magnetic

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

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

μ 0 I enclosed = B ds

μ 0 I enclosed = B ds Ampere s law To determine the magnetic field created by a current, an equation much easier to use than Biot-Savart is known as Ampere s law. As before, μ 0 is the permeability of free space, 4π x 10-7

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

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

Chapter 21. Magnetic Forces and Magnetic Fields

Chapter 21. Magnetic Forces and Magnetic Fields Chapter 21 Magnetic Forces and Magnetic Fields 1 21.1 Magnetic Fields The phenomenon of magnetism (1) The magnetic compass In Class Demo The needle of a compass is a permanent magnet that has a north magnetic

More information

(arrows denote positive direction)

(arrows denote positive direction) 12 Chapter 12 12.1 3-dimensional Coordinate System The 3-dimensional coordinate system we use are coordinates on R 3. The coordinate is presented as a triple of numbers: (a,b,c). In the Cartesian coordinate

More information

The Cross Product. In this section, we will learn about: Cross products of vectors and their applications.

The Cross Product. In this section, we will learn about: Cross products of vectors and their applications. The Cross Product In this section, we will learn about: Cross products of vectors and their applications. THE CROSS PRODUCT The cross product a x b of two vectors a and b, unlike the dot product, is a

More information

So far. Chapter 19. Today ( ) Magnets. Types of Magnetic Materials. More About Magnetism 10/2/2011

So far. Chapter 19. Today ( ) Magnets. Types of Magnetic Materials. More About Magnetism 10/2/2011 So far Chapter 19 Magnetism Electrostatics, properties of stationary charges Coulomb s law Electric field, electric potential Capacitors Ohm s law and resistance Today (19.1-19.4) Magnets Magnetism Earth

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 1A Lecture 10B

Physics 1A Lecture 10B Physics 1A Lecture 10B "Sometimes the world puts a spin on life. When our equilibrium returns to us, we understand more because we've seen the whole picture. --Davis Barton Cross Products Another way to

More information

7.1 THE MAGNETIC FIELD

7.1 THE MAGNETIC FIELD 7.1 THE MAGNETIC IEL - If one pours small iron particles around a permanent magnet ( natural lodestones or manmade ) an ordered pattern appears(fig.1). One can easily discern the presence of lines that

More information

Vectors a vector is a quantity that has both a magnitude (size) and a direction

Vectors a vector is a quantity that has both a magnitude (size) and a direction Vectors In physics, a vector is a quantity that has both a magnitude (size) and a direction. Familiar examples of vectors include velocity, force, and electric field. For any applications beyond one dimension,

More information

Note that a current-carrying solenoid produces a dipole field similar to that of a bar magnet. The field is uniform within the coil.

Note that a current-carrying solenoid produces a dipole field similar to that of a bar magnet. The field is uniform within the coil. An electrical current produces a magnetic field that is directed around it. Conventional current is the flow of positive charge. Hence, it is directed from the positive terminal of the power supply, through

More information

VECTORS IN COMPONENT FORM

VECTORS IN COMPONENT FORM VECTORS IN COMPONENT FORM In Cartesian coordinates any D vector a can be written as a = a x i + a y j + a z k a x a y a x a y a z a z where i, j and k are unit vectors in x, y and z directions. i = j =

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

Chapter 2: Force Vectors

Chapter 2: Force Vectors Chapter 2: Force Vectors Chapter Objectives To show how to add forces and resolve them into components using the Parallelogram Law. To express force and position in Cartesian vector form and explain how

More information

Magnetic Fields due to Currents

Magnetic Fields due to Currents Observation: a current of moving charged particles produces a magnetic field around the current. Chapter 29 Magnetic Fields due to Currents Magnetic field due to a current in a long straight wire a current

More information

Exam 2: Tuesday, March 21, 5:00-6:00 PM

Exam 2: Tuesday, March 21, 5:00-6:00 PM Exam 2: Tuesday, March 21, 5:00-6:00 PM Test rooms: Instructor Sections Room Dr. Hale F, H 104 Physics Dr. Kurter, N 125 CH Dr. Madison K, M 199 Toomey Dr. Parris J, L -10 ertelsmeyer* Mr. Upshaw A, C,

More information

The rectangular loop shown in the figure is pivoted about the y axis and carries a current of 15.0 in the direction indicated. T +

The rectangular loop shown in the figure is pivoted about the y axis and carries a current of 15.0 in the direction indicated. T + Heimadæmi 6 Due: 11:00pm on Thursday, February 25, 2016 You will receive no credit for items you complete after the assignment is due. Grading Policy Problem 27.68 The rectangular loop shown in the figure

More information

College Physics B - PHY2054C. Magnetic Fields and Forces 09/24/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building.

College Physics B - PHY2054C. Magnetic Fields and Forces 09/24/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building. Motion of a d College - PHY2054C and 09/24/2014 My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building Outline Motion of a d 1 2 Motion of a d 3 4 5 6 Right-Hand Rule Motion of a d Point the thumb

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

Vectors. J.R. Wilson. September 28, 2017

Vectors. J.R. Wilson. September 28, 2017 Vectors J.R. Wilson September 28, 2017 This chapter introduces vectors that are used in many areas of physics (needed for classical physics this year). One complication is that a number of different forms

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

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

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

Handout 8: Sources of magnetic field. Magnetic field of moving charge

Handout 8: Sources of magnetic field. Magnetic field of moving charge 1 Handout 8: Sources of magnetic field Magnetic field of moving charge Moving charge creates magnetic field around it. In Fig. 1, charge q is moving at constant velocity v. The magnetic field at point

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

SUPPLEMENT I. Example. Graph the vector 4, 3. Definition. Given two points A(x 1, y 1 ) and B(x 2, y 2 ), the vector represented by # AB is # AB =,

SUPPLEMENT I. Example. Graph the vector 4, 3. Definition. Given two points A(x 1, y 1 ) and B(x 2, y 2 ), the vector represented by # AB is # AB =, SUPPLEMENT I 1. Vectors Definition. A vector is a quantity that has both a magnitude and a direction. A twodimensional vector is an ordered pair a = a 1, a 2 of real numbers. The numbers a 1 and a 2 are

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

Chapter 30. Sources of the Magnetic Field Amperes and Biot-Savart Laws

Chapter 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 information

Vectors Mike Bailey Oregon State University Oregon State University Computer Graphics

Vectors Mike Bailey Oregon State University Oregon State University Computer Graphics 1 Vectors Mike Bailey mjb@cs.oregonstate.edu vectors.pptx Vectors have Direction and Magnitude 2 Magnitude: V V V V 2 2 2 x y z A Vector Can Also Be Defined as the Positional Difference Between Two Points

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 GOT

More information

Ishik University / Sulaimani Architecture Department Structure ARCH 214 Chapter -4- Force System Resultant

Ishik University / Sulaimani Architecture Department Structure ARCH 214 Chapter -4- Force System Resultant Ishik University / Sulaimani Architecture Department 1 Structure ARCH 214 Chapter -4- Force System Resultant 2 1 CHAPTER OBJECTIVES To discuss the concept of the moment of a force and show how to calculate

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

Chapter 6: Vector Analysis

Chapter 6: Vector Analysis Chapter 6: Vector Analysis We use derivatives and various products of vectors in all areas of physics. For example, Newton s 2nd law is F = m d2 r. In electricity dt 2 and magnetism, we need surface and

More information

Chapter 5. Magnetostatics

Chapter 5. Magnetostatics Chapter 5. Magnetostatics 5.1 The Lorentz Force Law 5.1.1 Magnetic Fields Consider the forces between charges in motion Attraction of parallel currents and Repulsion of antiparallel ones: How do you explain

More information

Physics / Higher Physics 1A. Electricity and Magnetism Revision

Physics / 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 information

Problem Solving 6: Magnetic Force & Torque

Problem Solving 6: Magnetic Force & Torque OBJECTIVES MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Problem Solving 6: Magnetic Force & Torque 1. To look at the behavior of a charged particle in a uniform magnetic field by studying

More information

POSITION VECTORS & FORCE VECTORS

POSITION VECTORS & FORCE VECTORS POSITION VECTORS & FORCE VECTORS Today s Objectives: Students will be able to : a) Represent a position vector in Cartesian coordinate form, from given geometry. b) Represent a force vector directed along

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 12. Magnetism

Chapter 12. Magnetism Chapter 12 Magnetism Chapter 12 is mostly finished, but is not in camera-ready format. This file doesn't have any of the many diagrams, but it does have selected excerpts from the text, with omissions

More information

Recap I. Angular position: Angular displacement: s. Angular velocity: Angular Acceleration:

Recap I. Angular position: Angular displacement: s. Angular velocity: Angular Acceleration: Recap I Angular position: Angular displacement: s Angular velocity: Angular Acceleration: Every point on a rotating rigid object has the same angular, but not the same linear motion! Recap II Circular

More information

Ampere s law. Lecture 15. Chapter 32. Physics II. Course website:

Ampere s law. Lecture 15. Chapter 32. Physics II. Course website: Lecture 15 Chapter 32 Physics II Ampere s law Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii Ampere s Law Electric Field From Coulomb s law 1 4 Magnetic Field Bio-Savart law 4

More information

VISUAL PHYSICS ONLINE THE LANGUAGE OF PHYSICS SCALAR AND VECTORS

VISUAL PHYSICS ONLINE THE LANGUAGE OF PHYSICS SCALAR AND VECTORS VISUAL PHYSICS ONLINE THE LANGUAGE OF PHYSICS SCALAR AND VECTORS SCALAR QUANTITES Physical quantities that require only a number and a unit for their complete specification are known as scalar quantities.

More information

SCS 139 Applied Physics II

SCS 139 Applied Physics II SCS 139 Applied Physics II Dr. Prapun Suksompong prapun@siit.tu.ac.th www.prapun.com Office Hours: BKD 3601-7 Monday 9:20-10:20 Wednesday 9:20-10:20 1 i Course Web Site Please check the course website

More information

(1) I have completed at least 50% of the reading and study-guide assignments associated with the lecture, as indicated on the course schedule.

(1) I have completed at least 50% of the reading and study-guide assignments associated with the lecture, as indicated on the course schedule. iclicker Quiz (1) I have completed at least 50% of the reading and study-guide assignments associated with the lecture, as indicated on the course schedule. a) True b) False Hint: pay attention to how

More information

Lecture Outlines Chapter 22. Physics, 3 rd Edition James S. Walker

Lecture Outlines Chapter 22. Physics, 3 rd Edition James S. Walker Lecture Outlines Chapter 22 Physics, 3 rd Edition James S. Walker 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in

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 due to Currentss

Chapter 29. Magnetic Fields due to Currentss Chapter 29 Magnetic Fields due to Currentss Refresher: The Magnetic Field Permanent bar magnets have opposite poles on each end, called north and south. Like poles repel; opposites attract. If a magnet

More information

Brief Review of Vector Algebra

Brief Review of Vector Algebra APPENDIX Brief Review of Vector Algebra A.0 Introduction Vector algebra is used extensively in computational mechanics. The student must thus understand the concepts associated with this subject. The current

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

Vector Operations. Vector Operations. Graphical Operations. Component Operations. ( ) ˆk

Vector Operations. Vector Operations. Graphical Operations. Component Operations. ( ) ˆk Vector Operations Vector Operations ME 202 Multiplication by a scalar Addition/subtraction Scalar multiplication (dot product) Vector multiplication (cross product) 1 2 Graphical Operations Component Operations

More information

III.Sources of Magnetic Fields - Ampere s Law - solenoids

III.Sources of Magnetic Fields - Ampere s Law - solenoids Magnetism I. Magnetic Field - units, poles - effect on charge II. Magnetic Force on Current - parallel currents, motors III.Sources of Magnetic Fields - Ampere s Law - solenoids IV.Magnetic Induction -

More information

Force between parallel currents Example calculations of B from the Biot- Savart field law Ampère s Law Example calculations

Force between parallel currents Example calculations of B from the Biot- Savart field law Ampère s Law Example calculations Today in Physics 1: finding B Force between parallel currents Example calculations of B from the Biot- Savart field law Ampère s Law Example calculations of B from Ampère s law Uniform currents in conductors?

More information

Application Of Faraday s Law

Application Of Faraday s Law Application Of Faraday s Law Dr Miguel Cavero September 2, 2014 Application Of Faraday s Law September 2, 2014 1 / 23 The PHYS120 Exam will be divided into three sections as follows: Section A: Short Questions

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

Ch 30 - Sources of Magnetic Field

Ch 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 information

ENGR-1100 Introduction to Engineering Analysis. Lecture 3

ENGR-1100 Introduction to Engineering Analysis. Lecture 3 ENGR-1100 Introduction to Engineering Analysis Lecture 3 POSITION VECTORS & FORCE VECTORS Today s Objectives: Students will be able to : a) Represent a position vector in Cartesian coordinate form, from

More information

Section 9: Magnetic Forces on Moving Charges

Section 9: Magnetic Forces on Moving Charges Section 9: Magnetic Forces on Moving Charges In this lesson you will derive an expression for the magnetic force caused by a current carrying conductor on another current carrying conductor apply F = BIL

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

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

Chapter 29. Magnetic Fields

Chapter 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 information

Objective 1. Lesson 87: The Cross Product of Vectors IBHL - SANTOWSKI FINDING THE CROSS PRODUCT OF TWO VECTORS

Objective 1. Lesson 87: The Cross Product of Vectors IBHL - SANTOWSKI FINDING THE CROSS PRODUCT OF TWO VECTORS Lesson 87: The Cross Product of Vectors IBHL - SANTOWSKI In this lesson you will learn how to find the cross product of two vectors how to find an orthogonal vector to a plane defined by two vectors how

More information

Lecture 27: More on Rotational Kinematics

Lecture 27: More on Rotational Kinematics Lecture 27: More on Rotational Kinematics Let s work out the kinematics of rotational motion if α is constant: dω α = 1 2 α dω αt = ω ω ω = αt + ω ( t ) dφ α + ω = dφ t 2 α + ωo = φ φo = 1 2 = t o 2 φ

More information

COLLEGE PHYSICS Chapter 23 ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES

COLLEGE PHYSICS Chapter 23 ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES COLLEGE PHYSICS Chapter 23 ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES Induced emf: Faraday s Law and Lenz s Law We observe that, when a magnet is moved near a conducting loop,

More information

Vectors. J.R. Wilson. September 27, 2018

Vectors. J.R. Wilson. September 27, 2018 Vectors J.R. Wilson September 27, 2018 This chapter introduces vectors that are used in many areas of physics (needed for classical physics this year). One complication is that a number of different forms

More information