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Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

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Page 1: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Lesson 20

Magnetism

Eleanor Roosevelt High SchoolChin-Sung Lin

Page 2: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

History of Magnetism

Page 3: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

History

The lodestone, which contains iron ore, was found more than 2000 years ago in the region of Magnesia in Greece

Page 4: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

History

The earliest Chinese literature reference to magnetism lies in the 4th century BC writings Guiguzi (鬼谷子 ): "The lodestone attracts iron”

Page 5: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

History

Zheng He used the Chinese compass as a navigational aid in his voyage between 1405 and 1433

Page 6: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

History

In the 18th century, the French physicist Charles Coulomb studied the force between lodestones

Page 7: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

History

In 1820 Danish physicist and chemist who discovered that electric currents create magnetic fields

Page 8: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Poles

Page 9: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Poles

Magnets attract and repel without touching

The interaction depends on the distance

Magnetic poles produce magnetic forces

Page 10: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Poles

Magnet can act as a compass

The end that points northward is called north pole, and the end that points south is call the south pole

Page 11: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Poles

All magnets have north and south poles

They can never be separated from each other

If you break the magnet in half, what will happen?

Page 12: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Poles

Each half will become a complete magnet

Unlike electric charge, you cannot have north or south pole alone

Page 13: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Poles

Like poles repels; opposite poles attract

Page 14: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

Page 15: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

The space around the magnet is filled with a magnetic field

Page 16: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

The magnetic field lines spread from the north pole to the south pole

Where the lines are closer (at the poles), the field strength is stronger

Page 17: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

The magnetic field unit:

Units: tesla (T) or gauss (G)

1 tesla = 10,000 gauss

Page 18: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

What will happen If we place a compass in the field?

Page 19: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

A magnet or small compass in the field will line up with the field

Page 20: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

Electric charge is surrounded by an electric filed

The same charge is surrounded by a magnetic field if it is moving

Which types of electron motion exist in magnetic materials?

Page 21: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

Electrons are in constant motion about atomic nuclei

This moving charge constitutes a tiny current and produces a magnetic field

Page 22: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

Electrons spinning about their own axes constitute a charge in motion and thus creates another magnetic field

Every spinning electron is a tiny magnet

Page 23: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

Electrons spinning in the same direction makes up a stronger magnet

Spinning in opposite directions cancels out

The field due to spinning is larger than the one due to orbital motion

Page 24: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Fields

For ferromagnetic elements: iron, nickel, and cobalt, the fields do not cancel one another entirely

Each iron atom is a tiny magnet

Page 25: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Domain

Page 26: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Domain

Interactions among iron atoms cause large clusters of them to line up with one another

These cluster of aligned atoms are called magnetic domains

Page 27: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Domain

There are many magnetic domains in a crystal iron

The difference between a piece of ordinary iron and an iron magnet is the alignment of domains

Page 28: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Domain

Iron in a magnetic field:

A growth in the size of the domains that is oriented in the direction of the magnetic field

A rotation of domains as they are brought into alignment

Page 29: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Domain

Permanent magnets:

Place pieces of iron or certain iron alloys in strong magnetic fields

Stroke a piece of iron with a magnet

Page 30: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents &Magnetic Fields

Page 31: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Current-Carrying Wire:

A moving electron produces a magnetic field

Electric current also produces magnetic field

A current-carrying conductor is surrounded by a magnetic field

Page 32: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Right-hand rule:

Grasp a current-carrying wire with your right hand

Your thumb pointing to the direction of the current

Your fingers would curl around the wire in the direction of the magnetic field (from N to S)

Page 33: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

What will happen to the compasses if the current is upward?

?

Page 34: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

The current-carrying wire deflects a magnetic compass

Page 35: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Current-Carrying Loop:

A wire loop with current produces a magnetic field

Page 36: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Current-Carrying Loop:

A wire loop with current produces a magnetic field

Page 37: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Coiled wire— Solenoid:A solenoid can be made of many wire loops

Page 38: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Coiled wire— Solenoid:A current-carrying coil of wire with many loopsThe magnetic field lines bunch inside the loop

Page 39: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Coiled wire— Solenoid:A coil wound into a tightly packed helix which produces a magnetic field when an electric current is passed through it

Solenoids can create controlled magnetic fields and can be used as electromagnets

Page 40: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Intensity of Magnetic Field of Electromagnet (B):Increased as the number of loops increased (B ~ N)Increased as the Current increased (B ~ I)Intensity is enhanced by the iron core (B ~ μ)

BN

I

Page 41: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Permeability:The measure of the ability of a material to support the formation of a magnetic field within itself. Magnetic permeability is typically represented by the Greek letter μ

B μ

Page 42: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Permeability:

Medium Permeability μ [H/m]

Relative Permeability μ/μ0

Mu-metal (nickel-iron alloy) 2.5×10−2 20,000

Ferrite (nickel zinc) 2.0×10−5 – 8.0×10−4 16 – 640

Steel 8.75×10−4 100

Vacuum 1.2566371×10−6 (μ0) 1

Water 1.2566270×10−6 0.999992

Superconductors 0 0

Page 43: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Electric Currents & Magnetic Fields

Direction of magnetic field of electromagnet follows the Right-hand Rule:

Your fingers indicate the direction of the current (I)your thumb points the direction of the field (B)

B

I

Page 44: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

Page 45: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

When a charged particle moves in a magnetic field, it will experience a deflecting force (FB)

I

+

Page 46: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

When a charged particle moves in a magnetic field, it will experience a deflecting force (FB)

FB = qvB

FB magnetic force [N]

q electric charge [C]v velocity perpendicular to the field

[m/s]B magnetic field strength [T, Teslas]

I

Page 47: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

The magnetic field unit:

Units: tesla (T) or gauss (G)

1 tesla = 10,000 gauss

tesla = (newton × second)/(coulomb × meter)

T = Ns / (Cm)

Page 48: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

Direction of the magnetic force (FB) follows the

Fleming’s Left Hand Motor Rule

I

Page 49: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

What will happen to the positively charged particle?

+

Page 50: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

The positively charged particle will experience a force always perpendicular to the motion

The particle will have a circular motion

Page 51: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

The magnetic field has been used to detect particles in the cloud chamber

What will happen to the different radiation?

Page 52: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

The magnetic field has been used to detect particles in the cloud chamber

α He2+ helium nucleus (+)

β e– electron (–)

γ uncharged EM ray

Page 53: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

The magnetic field has been used to detect particles in the cloud chamber

α He2+ helium nucleus (+)

β e– electron (–)

γ uncharged EM ray

Page 54: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

The magnetic field has been used to deflect the electron beam. Where will the electron beam hit the screen?

electron beam S

N screen

magnet

A

BC

D

Page 55: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

Mass spectrometry:To determine masses of particles, for determining the elemental composition of a molecule

Page 56: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

Mass spectrometry:

magnetic force = centripetal force

FB = FC

qvB = mv2/r

r = (mv)/(qB)

Page 57: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

Mass spectrometry:

r = (mv)/(qB)• the faster it is travelling the bigger the circles

• the bigger its mass is the bigger the circles

• the bigger its momentum the larger the circles

• the stronger the magnetic field the smaller the circles

• the larger the charge the smaller the circles

Page 58: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

A positively charged particle moving along a spiral path inside a uniform magnetic field

Page 59: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

Page 60: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

What will happen to the current carrying wires?

I I

Page 61: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

The current-carrying wire also follows Fleming’s left hand motor rule

Page 62: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

The current-carrying wire deflects a magnetic compass and a magnet deflects a current-carrying wire are different effect of the same phenomena

Page 63: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

Magnetic Force Between Wires:

What will happen to the parallel wires if both current are in the same direction?

I1I2

Page 64: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

Magnetic Force Between Wires:

Parallel wires carrying currents will exert forces on each other

When the current goes the same way in the two wires, the force is attractive

When the currents go opposite ways, the force is repulsive

Page 65: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Force on Current-Carrying Wires

Magnetic Force Between Wires:

What will happen to the parallel wires if the current are in the opposite direction?

I1I2

Page 66: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Galvanometers & Motors

Page 67: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Galvanometer

A sensitive current-indicating instrument The coil turns against a spring, so the greater the current, the greater its deflection

Page 68: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Galvanometer

A galvanometer may be calibrated to measure current— an ammeter

A galvanometer may be calibrated to measure voltage— a voltmeter

Page 69: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Motor

Converts electrical energy into mechanical energy

Motors operate through interacting magnetic fields and current-carrying conductors to generate force

Page 70: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

DC Motor

The current-carrying wire of the motor coil follows Fleming’s left hand motor rule

Page 71: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

DC Motor

Page 72: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

AC Motor

Page 73: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

AC Motor

Page 74: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Page 75: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Earth itself is a huge magnet

The magnetic poles of Earth do not coincide with the geographic North pole – magnetic declination

Page 76: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Magnetic Pole Shift:

The magnetic poles of Earth keep changing

The pole kept going north at an average speed of 10 km per year, lately accelerating to 40 km per year

Page 77: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Magnetic Pole Weakening:The strength of the magnetic field of Earth keep decreasingThe magnetic field has weakened 10% since the 19th century Earth's Magnetic Field Trends

52,000.00

53,000.00

54,000.00

55,000.00

56,000.00

57,000.00

58,000.00

59,000.00

60,000.00

Year

Tota

l Int

ensi

ty (

nT)

Page 78: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

A geomagnetic reversal is a change in the Earth's magnetic field such that the positions of magnetic north and magnetic south are interchanged

Page 79: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Magnetic Forces on Moving Charged Particles

A positively charged particle moving along a spiral path inside a uniform magnetic field

Page 80: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Earth’s magnetic field will deflect the charged particles from outer space to reduce the cosmic rays striking Earth’s surface

Page 81: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Van Allen radiation belt: is a torus of energetic charged particles around Earth, which is held in place by Earth's magnetic field

Page 82: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Van Allen radiation belt: energetic electrons forming the outer belt and a combination of protons and electrons creating the inner belt

Page 83: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

Earth’s Magnetic Field

Aurora: a natural light display in the sky, particularly in the polar regions, caused by the collision of charged particles directed by the Earth's magnetic field

Page 84: Lesson 20 Magnetism Eleanor Roosevelt High School Chin-Sung Lin

The End