Magnetic Field of a Wire

Similar documents
Course Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday

Magnetic Fields Due to Currents

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

Physics 122, Fall October 2012

Review for 2 nd Midterm

Magnetic fields (origins) CHAPTER 27 SOURCES OF MAGNETIC FIELD. Permanent magnets. Electric currents. Magnetic field due to a moving charge.

Sources of the Magnetic Field. Moving charges currents Ampere s Law Gauss Law in magnetism Magnetic materials

A moving charged particle creates a magnetic field vector at every point in space except at its position.

MAGNETIC FIELD INTRODUCTION

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

Unit 7: Sources of magnetic field

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields

Magnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M.

Collaborative ASSIGNMENT Assignment 3: Sources of magnetic fields Solution

( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

Gauss s Law: Circuits

Physics Spring 2012 Announcements: Mar 07, 2012

Faraday s Law (continued)

Magnetic Field. Conference 6. Physics 102 General Physics II

Sources of Magnetic Fields (chap 28)

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law

The Law of Biot-Savart & RHR P θ

Physics 2112 Unit 14

PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101

Flux. Area Vector. Flux of Electric Field. Gauss s Law

How Electric Currents Interact with Magnetic Fields

16.1 Permanent magnets

21 MAGNETIC FORCES AND MAGNETIC FIELDS

TUTORIAL 9. Static magnetic field

Conventional Current B = In some materials current moving charges are positive: Ionic solution Holes in some materials (same charge as electron but +)

Force between two parallel current wires and Newton s. third law

F Q E v B MAGNETOSTATICS. Creation of magnetic field B. Effect of B on a moving charge. On moving charges only. Stationary and moving charges

3-Axis Vector Magnet: Construction and Characterisation of Split Coils at RT. Semester Project Petar Jurcevic

PHYS 1441 Section 001 Lecture #14

Electrostatics (Electric Charges and Field) #2 2010

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m

Objectives: After finishing this unit you should be able to:

? this lecture. ? next lecture. What we have learned so far. a Q E F = q E a. F = q v B a. a Q in motion B. db/dt E. de/dt B.

( )( )( ) ( ) + ( ) ( ) ( )

Your Comments. Do we still get the 80% back on homework? It doesn't seem to be showing that. Also, this is really starting to make sense to me!

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Chapter 23: GAUSS LAW 343

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak

Chapter 26: Magnetism: Force and Field

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Exam 3, vers Physics Spring, 2003

MTE2 Wed 26, at 5:30-7:00 pm Ch2103 and SH 180. Contents of MTE2. Study chapters (no 32.6, 32.10, no 32.8 forces between wires)

Current, Resistance and

( ) ( )( ) ˆ. Homework #8. Chapter 28

Last time RC circuits. Exam 2 is Tuesday Oct. 27 5:30-7 pm, Birge 145. Magnetic force on charged particle. Magnetic force on electric charges

Physics 2212 GH Quiz #2 Solutions Spring 2016

DYNAMICS OF UNIFORM CIRCULAR MOTION

PY208 Matter & Interactions Final Exam S2005

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

Module 19: Sections 9.1 through 9.2 Module 20: Sections 9.3 through Table of Contents

MAGNETIC EFFECT OF CURRENT AND MAGNETISM

Fields and Waves I Spring 2005 Homework 8. Due: 3 May 2005

PHY2061 Enriched Physics 2 Lecture Notes. Gauss Law

PHYS 1444 Lecture #5

PS113 Chapter 5 Dynamics of Uniform Circular Motion

Name. Date. Period. Engage Examine the pictures on the left. 1. What is going on in these pictures?

Chapter 28 Sources of Magnetic Field

FI 2201 Electromagnetism

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines

Physics: Work & Energy Beyond Earth Guided Inquiry

Chapter 31 Faraday s Law

3. Magnetostatic fields

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0

Unit 7. Sources of magnetic field


Today s Plan. Electric Dipoles. More on Gauss Law. Comment on PDF copies of Lectures. Final iclicker roll-call

Phys-272 Lecture 13. Magnetism Magnetic forces

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

Your Comments. Conductors and Insulators with Gauss's law please...so basically everything!

Review. Electrostatic. Dr. Ray Kwok SJSU

UNIT 3:Electrostatics

ELECTROMAGNETISM (CP2)

Circular motion. Objectives. Physics terms. Assessment. Equations 5/22/14. Describe the accelerated motion of objects moving in circles.

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased

Gauss s Law Simulation Activities

Centripetal Force. Lecture 11. Chapter 8. Course website:

( ) ( ) ( ) ( ) ( ) # B x ( ˆ i ) ( ) # B y ( ˆ j ) ( ) # B y ("ˆ ( ) ( ) ( (( ) # ("ˆ ( ) ( ) ( ) # B ˆ z ( k )

Chapter 22 The Electric Field II: Continuous Charge Distributions

Module 05: Gauss s s Law a

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

CHAPTER: 4 MOVING CHARGES AND MAGNETISM

Course Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.

Physics NYB problem set 5 solution

Physics 11 Chapter 20: Electric Fields and Forces

7.2.1 Basic relations for Torsion of Circular Members

CHAPTER 25 ELECTRIC POTENTIAL

Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields

Current Balance Warm Up

Math Section 4.2 Radians, Arc Length, and Area of a Sector

r cos, and y r sin with the origin of coordinate system located at

constant t [rad.s -1 ] v / r r [m.s -2 ] (direction: towards centre of circle / perpendicular to circle)

1 2 U CV. K dq I dt J nqv d J V IR P VI

Motion in a Plane Uniform Circular Motion

FARADAY'S LAW dt

Transcription:

Magnetic Field of a Wie Fundamental Laws fo Calculating B-field Biot-Savat Law (long method, but woks always) Ampee s Law (high symmety) B-Field of a Staight Wie Fo a thin staight conducto caying cuent the magnetic field is: We epect B fom wie to be popotional to /R. Chapte 28 1

2

B-Field of a Staight Wie Whee B 2 Magnetic Field of a Wie 7. 4 1 Tm A is the Pemeability of fee space Use the ight hand ule to detemine the diection. (Place thumb in diection of cuent and B Field is in diection of finges gabbing the wie.) dl 3

Ampee s Law dl 4

Today Eample B-field Calculations (Application of Ampee s Law) nside a Long Staight Wie nfinite Cuent Sheet Solenoid Tooid Biot-Savat Law Cicula Loop 5

Ampee s Law A) Evaluate the integal dl aound each loop R dl 1) 3) 2R 2) R 2 4) not enough infomation a b 1) 3) ab 2) 2(a + b) 4) Not enough info dl 6

Ampee s Law - Eamples Two identical loops ae placed in poimity to two identical cuent caying wies. 3) Fo which loop is B dl the geatest? 1) A 2) B 3) Same A B 7

Two identical loops ae placed in poimity to two identical cuent caying wies. C B D) Now compae loops B and C. Fo which loop is B dl the geatest? 1) B 2) C 3) Same 8

Suppose a total cuent flows though the wie of adius a into the sceen as shown. B Field nside a Long Wie To calculate B field as a function of, fom cente of the wie: Take an ampeian loop of adius outside the wie, using Ampee s Law: Bdl The enclosed cuent is all of cuent though wie: The B-field diminishes as 1/ outside the wie Chapte 28 enc B d B 2 enc R B 2 9

Now B-field inside the wie: We choose an ampeean loop of adius inside the wie: B dl B Field nside a Long Wie B d 2 B enc But the enclosed cuent is a faction of total; since cuent is unifom: enc R 2 2 nside the wie the B-field is linea with. enc theefoe B 2 R 2 R Chapte 28 1

nside the wie: ( < R) μ B 2 π R Outside the wie:( >R ) 2 B Field nside a Long Wie y = B b1();b2() 1 B = 2 R 4 = 11

B Field of Cuent Sheet Conside an sheet of cuent descibed by n wies/length each caying cuent into the sceen as shown. Calculate the B field. What is the diection of the field? Fom the Symmety +/ y diection Calculate using Ampee's law fo a squae of side w B dl Bw Bw 2Bw nwi theefoe, B dl μ B μ ni 2 w constant y constant 12

B-Field of A Solenoid A unifom magnetic field can be poduced by a solenoid A solenoid is defined by a cuent flowing though a wie that is wapped n tuns pe unit length on a cylinde of adius a and length L. Bdl Bl N N B n l dl l 13

B-Field of A Tooid Tooid defined by a solenoid of N total tuns with cuent connected at both ends. t becomes a donut shape with a coil wapped aound it. outside Tooid B = integating B on cicle outside tooid, enclosed cuent = +(- ) = nside the Tooid Bdl B2 N B 2 N Get a concentated field inside the tooid. dl 14

Eamples Two cylindical conductos, one solid and the othe hallow in middle, each cay cuent into the sceen as shown. The conducto has adius R=4a. The conducto on the ight has a hole in the middle and caies cuent only between R=a and R=4a. a 4a 4a At R = 5a which conducto poduces stonge B-field? 1) Left conducto 3) Both ae the same 2) Right Conducto 4) both ae zeo 15

Eamples Two cylindical conductos, one solid and the othe hallow in middle, each cay cuent into the sceen as shown. The conducto has adius R=4a. The conducto on the ight has a hole in the middle and caies cuent only between R=a and R=4a. a 4a 4a At R = 2a which conducto poduces stonge B-field? 1) Left conducto 3) Both ae the same 2) Right Conducto 4) both ae zeo 16

Eamples Use Ampee s Law in both cases by dawing a loop in the plane of the sceen at R = 5a and R = 2a. Both fields have cylindical symmety, so the fields ae tangent to the loop at all points, thus the field at R=5a only depends on cuent enclosed enc = in both cases Field only depends on enclosed cuent 4a a 4a 17

Eamples A cuent caying wie is wapped aound an ion coe, foming an electo-magnet. Which diection does the magnetic field point inside the ion coe? 1) left 4) ight 2) up 5) down 3) out of the sceen 6) into the sceen Which side of the solenoid should be labeled as the magnetic noth pole? 1) left 3) ight 2) up 4) down 18

nside the wie: ( < R) μ B 2 π R 2 B Field nside a Long Wie y = 1 R b1();b2() Outside the wie:( >R ) B = 2 4 = 19

B Field of Cuent Sheet Conside an sheet of cuent descibed by n wies/length each caying cuent into the sceen as shown. Calculate the B field. What is the diection of the field? Fom the Symmety +/ y diection Calculate using Ampee's law fo a squae of side w B dl Bw Bw 2Bw nwi theefoe, B dl μ B μ ni 2 w constant y constant Chapte 28 2