l16 ch29 magnetism · 2019. 7. 30. · microsoft powerpoint - l16 ch29 magnetism author: andriy...

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PHYS.1440 Lecture 16 A.Danylov Department of Physics and Applied Physics Lecture 16 Chapter 29 Magnetism Physics II Bye, bye, Electricity. You won’t be missed. Course website: https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

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Page 1: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Lecture 16

Chapter 29

Magnetism

Physics II

Bye, bye, Electricity.You won’t be missed.

Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

Page 2: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

A)CapacitorA.B)CapacitorB.C)Theydischargeatthe

samerate.D)Can’tsaywithout

knowingtheinitialamountofcharge.

Whichcapacitordischargesmorequicklyaftertheswitchisclosed?

ConcepTest RC circuit 1

time constant = RC

= 12 µs = 15 µs

So the capacitor A discharges faster than B

Page 3: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

A)5sB)4sC)2sD)1s

Whatisthetimeconstantforthedischargeofthecapacitorshowninthefigure?

ConcepTest RC circuit 3

time constant by definition = ReqC

+ =

= ReqC =4Ωx1F=4 seconds

How about this?

= ReqCeq

Page 4: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Today we are going to discuss:

Chapter 29:

Section 29.1-3 Section 29.5 (skip) Section 29.7

Page 5: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Sources of Magnetic FieldWehavelearnedthatelectricchargeqproducesanelectricfieldE

qE

Itturnsoutthatthereisanotherfield,magneticfield B,whichisproducedbyamovingelectricchargeq.

q v

(I)MovingqB B

Current

B (II)Current(manyq) B (III)Magnet B(orbitingelectrons)

B

So,therearethree systemsproducingBfield.Let’slookatthemseparately.

Page 6: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

(III) Permanent Magnet

Page 7: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Magnets interact (repel/attract, observation)

The north pole of one magnet exerts anattractive force on the south pole ofanother magnet.

Like poles repel Unlike poles attract.

If the north pole of one magnet is broughtnear the north pole of another magnet,they repel each other.

Page 8: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

There are no magnetic monopolesIf you cut a magnet in half, you don’t get a north pole and a south pole – you get two

smaller magnets.

Sheldon: “if I’m able to detect slow‐moving magneticmonopoles there, I will be the scientist to confirm string theory.People will write books about me. Third‐graders will createmacaroni‐art dioramas depicting scenes frommy life.”

Hisfriendstamperedwithhisexperimentonmagneticmonopolesbyusinganelectriccanopener.

There is no magnetic monopole

Oneofthe“BigBangTheory”episodeswasarrangedaroundthisfact.

Thereisnoexperimentalevidencethatmagneticmonopolesexist.

Anumberofattemptshavebeenmadetodetectmagneticmonopoles.SheldonCooperhasalsomadeone:

Page 9: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Probe object. Magnet Pole Convention

If we position a compass needle in the Earth field, one side will point to the geographical North pole.

(I) The end of a needle that points to the North geograph. pole is called the north pole (by CONVENTION).The end of a magnet that points south is called the south pole.As the result, if we follow the convention, the Earth’s “Geogr. North Pole” is a south magnetic pole, as the north end of the compass needle is attracted to it.The magnetic poles are slightly offset from the geographical poles.

*The Earth is a huge magnet due to currents in the molten iron core.

North Magnetic Pole

South Magnetic Pole

Again?

Now, we know that the magnetic field (B) exists. How can we detect B? Which object can be used as a probe system?

(0) A compass needle will be used as a probe system.

Which side of the needle should be called the North pole?Lets use the Earth’s Magnetic field*

(II) The North pole of a compass shows the direction of the magnetic field at the point.

Page 10: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Magnetic Fields Lines

Magneticfieldscanbevisualizedusingmagneticfieldlines,whicharealwaysclosedloops(consequenceofthefactthattherearenomagneticmonopoles).

Howtofindthesemagneticlines? With a compass needlelike a “probe charge”

B

Density of magn. lines is smaller so the magn. field is weaker

The North Pole of a compass needle shows the direction of the magnetic field

https://www.youtube.com/watch?v=8llkHQtaOlg

(II) Density of magn. lines is higher so the magnetic field is stronger

Demo:Iron filings are suspended in liquid in a clear rectangle box.

Now,sincewehaveaprobesystem,acompassneedle,wecanuseittomapamagneticfieldof,forexample,apermanentmagnet.

Page 11: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Vector notation and the cross (vector) product

Before we proceed with magnetic field we need to look at

Page 12: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Notation for Vectors and Currents Perpendicular to the Page

Magnetismrequiresathree‐dimensionalperspective,buttwo‐dimensionalfiguresareeasiertodraw.

Wewillusethefollowingnotation:

Bad karma

Page 13: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

The Vector (Cross) Product

=(ab sinθ,directiongivenbytheright‐handrule)

Fromnowon,almostallequationswillhaveacrossproduct

Thecrossproductofvectorsa andb isavectorperpendiculartobotha andb.

[I]Pointfingersinthedirectionofthe1st (a)vector,thenbendtheminthedirectionofthe2nd one(b).Theoutstretchedthumbwillgiveadirectionofthecrossproduct

[II]Usethreefingersasshowninthefigure

Orderisimportantinthecrossproduct:

Page 14: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

ConcepTest Cross Product

Find a direction of a cross product

Page 15: L16 Ch29 Magnetism · 2019. 7. 30. · Microsoft PowerPoint - L16 Ch29 Magnetism Author: Andriy Danylov Created Date: 7/30/2019 10:46:57 AM

PHYS.1440Lecture16 A.DanylovDepartmentofPhysicsandAppliedPhysics

Thank you