Electricity and Magnetism Force on Parallel Wires

Similar documents
Electricity and Magnetism Magnetic Field from Moving Charges

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

Electricity and Magnetism. Motional EMF Faraday s Law

Magnetic Fields due to Currents

Electricity and Magnetism Coulomb s Law

Chapter 29. Magnetic Fields due to Currentss

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

Electricity and Magnetism B-Fields from Moving Charges

Electricity and Magnetism Electric Field

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

LECTURE 22 MAGNETIC TORQUE & MAGNETIC FIELDS. Instructor: Kazumi Tolich

Electricity and Magnetism Coulomb s Law

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

Ch 30 - Sources of Magnetic Field

Chapter 24. Magnetic Fields

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

Magnetic Field Lines for a Loop

Lecture 27: MON 26 OCT Magnetic Fields Due to Currents II

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

Ampere s Law. Outline. Objectives. BEE-Lecture Notes Anurag Srivastava 1

Electricity and Magnetism Eddy Currents Faraday s Law and Electric Field

1) in the direction marked 1 2) in the direction marked 2 3) in the direction marked 3 4) out of the page 5) into the page

Electricity and Magnetism Electric Potential Energy Electric Potential

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

Electricity and Magnetism Current

Key Contents. Magnetic fields and the Lorentz force. Magnetic force on current. Ampere s law. The Hall effect

Chapter 19. Magnetism

General Physics II. Magnetism

Last time. Gauss' Law: Examples (Ampere's Law)

Electricity and Magnetism Current Loops and Magnetic Dipoles Magnetism in Matter

Phys 102 Lecture 12 Currents & magnetic fields

Electricity and Magnetism DC Circuits Using Kirchhoff s Laws

PHYSICS ASSIGNMENT ES/CE/MAG. Class XII

Midterms and finals from previous 4 years are now posted on the website (under Exams link). Check the main course website for practice problems

General Physics (PHYS )

Physics 202, Lecture 13. Today s Topics. Magnetic Forces: Hall Effect (Ch. 27.8)

Ch. 28: Sources of Magnetic Fields

Magnetic Force Cyclotron motion

Electricity and Magnetism Implications of Gauss s Law Electric Potential Energy

Electricity and Magnetism Energy of the Magnetic Field Mutual Inductance

Gravity Electromagnetism Weak Strong

Chapter 24: Magnetic Fields & Forces

Every magnet has a north pole and south pole.

Chapter 22 Magnetism

Magnetism. February 27, 2014 Physics for Scientists & Engineers 2, Chapter 27 1

Electricity and Magnetism Charge and Conduction Coulomb s Law

Introduction to Mechanics Dynamics Forces Newton s Laws

Physics / Higher Physics 1A. Electricity and Magnetism Revision

FARADAY S AND LENZ LAW B O O K P G

Electricity and Magnetism DC Circuits Resistance-Capacitance Circuits

Magnetic inductance & Solenoids. P.Ravindran, PHY041: Electricity & Magnetism 22 February 2013: Magnetic inductance, and Solenoid

Physics 4B Chapter 29: Magnetic Fields Due to Currents

SCS 139 Applied Physic II Semester 2/2011

AP Physics C Electricity and Magnetism

Mechanics Units, Dimensional Analysis, and Unit Conversion

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.

Thermodynamics Heat Transfer

Lecture 22 Chapter 31 Maxwell s equations

PHYSICS. Chapter 29 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

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

Magnetic Fields Permanent Magnets

Magnetic Flux. Conference 8. Physics 102 General Physics II

Chapter 30. Sources of the Magnetic Field

AMPERE'S LAW. B dl = 0

Chapter 28 Source of Magnetic Field

Electricity and Magnetism Relativity and the Magnetic Field

Version The diagram below represents lines of magnetic flux within a region of space.

Torque on a Current Loop

Magnetic Fields Part 2: Sources of Magnetic Fields

Sources of Magnetic Field I

Inductors Maxwell s equations

Magnetic Fields due to Currents

Welcome back to PHY101: Major Concepts in Physics I. Photo: J. M. Schwarz

Lorentz Force. Velocity Selector

Physics 2212 GH Quiz #4 Solutions Spring 2016

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

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

University Physics 227N/232N Ch 27: Inductors, towards Ch 28: AC Circuits Quiz and Homework This Week

B for a Long, Straight Conductor, Special Case. If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes

MODULE 4.2 MAGNETISM ELECTRIC CURRENTS AND MAGNETISIM VISUAL PHYSICS ONLINE

CHAPTER 30: Sources of Magnetic Fields

Kinematics Kinematic Equations and Falling Objects

Chapter 21. Magnetism

Electromagnetics in Medical Physics

Exercise Exercise Correct. Correct. Part A

A little history. Electricity and Magnetism are related!

Magnetic field creation (example of a problem)

Magnetic Forces and Fields (Chapters 29-30)

Magnetostatics: Part 1

21 MAGNETIC FORCES AND MAGNETIC FIELDS

Introduction to Mechanics Dynamics Forces Newton s Laws

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 110A. Homework #6. Benjamin Stahl. February 17, 2015

PHYS 1444 Section 501 Lecture #17

Electricity and Magnetism DC Circuits Resistance-Capacitance Circuits

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2013 Exam 3 Equation Sheet. closed fixed path. ! = I ind.

CHAPTER 4: MAGNETIC FIELD

Physics 1402: Lecture 18 Today s Agenda

Dr. Todd Satogata (ODU/Jefferson Lab) Wednesday, March

Magnetic Force Acting on a Current- Carrying Conductor IL B

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

Transcription:

Electricity and Magnetism Force on Parallel Wires Lana Sheridan De Anza College Mar 2, 2018

Last time Gauss s Law for magnetic fields Ampère s Law magnetic field around a straight wire solenoids

Overview magnetic field inside a solenoid forces between current-carrying wires

Solenoids Additional examples, video solenoid A helical coil of tightly wound wire that can carry a current. turn i Fig. 29-16 A solenoid carrying current i. i 29-5 Solenoi Magnetic Field o We now turn our useful. It concerns wound helical coil that the length of t Figure 29-17 sh The solenoid s ma A single complete loop of wire in a solenoid. This solenoid has 10 turns, means it has 10 complete loops.

apply Ampere s law, Magnetic Field of an ideal solenoid In an ideal solenoid B : ds : (with 0 i enc, infinite length) the field(29-21) outside is small (and perpendicular to the Amp. loop) and inside is uniform. enoid (Similar of Fig. 29-19, to a where capacitor!) B : is uniform within the solenoid and using the rectangular Amperian loop abcda. We write B : ds : as Can use an Amperian loop to find the B-field inside: d h c i B ds = µ 0 I enc B a b plication of Ampere s law to a section of a long ideal solenoid carrying mperian loop is the rectangle abcda.

apply Ampere s law, Magnetic Field of an ideal solenoid In an ideal solenoid B : ds : (with 0 i enc, infinite length) the field(29-21) outside is small (and perpendicular to the Amp. loop) and inside is uniform. enoid (Similar of Fig. 29-19, to a where capacitor!) B : is uniform within the solenoid and using the rectangular Amperian loop abcda. We write B : ds : as Can use an Amperian loop to find the B-field inside: d h c i B ds = µ 0 I enc B a b plication Here, of Ampere s supposelaw there to a section are n of turns a long per ideal unit solenoid lengthcarrying the solenoid, mperian then loop Iis enc the = rectangle Inh abcda. Bh = µ 0 Inh Inside an ideal solenoid: B = µ 0 In

Two Wires carrying Current With two long, straight current carrying wires, each creates its own magnetic field: B = µ 0I 2πa The result is that the wires interact, much like two bar magnets producing magnetic fields would.

Forces on parallel wires Currents in opposite directions repel, currents in the same direction attract. 1 Figure from salisbury.edu.

Forces on parallel wires 1 Figure from Stonebrook Physics ic.sunysb.edu.

Forces on parallel wires To find the magnitude of the force, we need to recall how force relates to the magnetic field for a wire. The force on a long, straight current carrying wire is: F = IL B

Forces on parallel wires 770 CHAPTER 29 MAGNETIC FIELDS DUE TO C Suppose that wire a produces a field at b: B a = µ 0I a 2πd i a The force on wire b is: The field due to a at the position of b creates a force on b. i b Fig. 29-9 Two parallel wires carrying currents in the same direction attract each other. B : a is the magnetic field at wire b produced by the current in wire a. F : ba is the resulting force acting on wire b because it carries current in. B : a F ba a L L d b B a (due to i a ) F b = I b L B a = I b L µ 0I a 2πd sin(90 ) [toward a] F B = µ 0I a I b 2πd L 29-3 Force Two long parall shows two such Let us analyze th We seek firs current produce causes the force direction of the wire b is, from E The curled stra down, as Fig. 29- Now that w Equation 28-26

Forces on parallel wires It is a bit more intuitive to think about the force per unit length on the wires (since longer wires will experience larger forces). The force per unit length on a wire due to another parallel wire at a distance d: F B L = µ 0I 1 I 2 2πd

10 6 g,and then launches it with a speed of 10km/s,all within 1ms.S rail Question guns may be used to launch materials into space from mining opera e Moon or an asteroid. The figure here shows three long, straight, parallel, equally spaced HECKPOINT 1 wires with identical currents either into or out of the page. Rank e figure thehere wires shows according three to long, thestraight, magnitude parallel, of theequally force on spaced each wires due towith iden rrents the either currents into or in out the of other the two page.rank wires, greatest the wires first. according to the magnitud e force on each due to the currents in the other two wires, greatest first. a b c A a, b, c 4 Ampere s Law B b, c, a an find C c, the b, net a electric field due to any distribution of charges by first w ifferential electric field de : due to a charge element and then summin ributions of de : from all the elements. However, if the distribution is co d, we may have to use a computer. Recall, however, that if the distrib 1 Halliday, Resnick, Walker, pg 771.

10 6 g,and then launches it with a speed of 10km/s,all within 1ms.S rail Question guns may be used to launch materials into space from mining opera e Moon or an asteroid. The figure here shows three long, straight, parallel, equally spaced HECKPOINT 1 wires with identical currents either into or out of the page. Rank e figure thehere wires shows according three to long, thestraight, magnitude parallel, of theequally force on spaced each wires due towith iden rrents the either currents into or in out the of other the two page.rank wires, greatest the wires first. according to the magnitud e force on each due to the currents in the other two wires, greatest first. a b c A a, b, c 4 Ampere s Law B b, c, a an find C c, the b, net a electric field due to any distribution of charges by first w ifferential electric field de : due to a charge element and then summin ributions of de : from all the elements. However, if the distribution is co d, we may have to use a computer. Recall, however, that if the distrib 1 Halliday, Resnick, Walker, pg 771.

Definition of the Ampère (Amp) This relation: F B L = µ 0I 1 I 2 2πd gives us the formal definition of the Ampère. Ampère Unit Two long parallel wires separated by 1 m are said to each carry 1 A of current when the force per unit length on each wire is 2 10 7 N/m.

Summary Solenoids and Ampère s Law Forces on parallel wires 3rd Test Friday, Mar 9. Homework Collected homework 3, posted online, due on Monday. Serway & Jewett: PREVIOUS: Ch 30, Problems: 21, 25, 31, 33, 34, 47 NEW: Ch 30, Problems: 41, 45