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Lecture 25: MON 16 MAR Lecture 25: MON 16 MAR Magnetic fields Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis
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Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Jan 18, 2016

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Page 1: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Lecture 25: MON 16 Lecture 25: MON 16 MARMARMagnetic fields Magnetic fields

Ch.28.1–4

Physics 2113

Jonathan Dowling

“I’ll be back….

Aurora Borealis

Page 2: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

How Do You Use Magnetic Fields in Your

Everyday Life!?

Page 3: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.
Page 4: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

28.2: What Produces Magnetic Field?:

One way that magnetic fields are produced is to use moving electrically charged particles, such as a current in a wire, to make an electromagnet. The current produces a magnetic field that is utilizable.

The other way to produce a magnetic field is by means of elementary particles such as electrons, because these particles have an intrinsic magnetic field around them.

The magnetic fields of the electrons in certain materials add together to give a net magnetic field around the material. Such addition is thereason why a permanent magnet, has a permanent magnetic field.

In other materials, the magnetic fields of the electrons cancel out, giving no net magnetic field surrounding the material.

Page 5: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Electric vs. Magnetic FieldsElectric vs. Magnetic Fields

Electric fields are created:• microscopically, by electric charges (fields) of elementary particles (electrons, protons)• macroscopically,by adding the field of many elementary charges of the same sign

Magnetic fields are created :• microscopically, by magnetic “moments” of elementary particles (electrons, protons, neutrons)• macroscopically, by

• adding many microscopic magnetic moments (magnetic materials); or by• electric charges that move (electric currents)

Page 6: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Magnetic Field Direction

FROM North Poles

TO South Poles

B

+

Compare to ElectricField Directions

E

Page 7: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Law of Attraction and Repulsion for Magnets

Opposite Poles Attract

Like Poles Repel

Page 8: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

We know that an electric fields exists because it accelerates electric charges, with a force independent of the velocity of the charge, proportional to the electric charge: FE = qE

We know that a magnetic field exists because it accelerates electric charges in a direction perpendicular to the velocity of the charge, with a magnitude proportional to the velocity of the charge and to the magnitude of the charge: FB= q v x B

Magnetic forces are perpendicular to both the velocity of chargesand to the magnetic field (electric forces are parallel to the field).

Since magnetic forces are perpendicular to the velocity,they do no work! (W = F · r = F r cos(90°) = 0

Speed of particles moving in a magnetic field remains constantin magnitude, ONLY the direction changes. Kinetic energy is constant! (no work).

Magnetic vs. Electric Magnetic vs. Electric ForcesForces

Page 9: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.
Page 10: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Magnetic vs. Electric ForcesMagnetic vs. Electric Forces

Electric Force on Charge Parallel to E:

Electric Force on Charge Parallel to E:

Magnetic Force on Charge Perpendicular to B and v.

Magnetic Force on Charge Perpendicular to B and v.

+q

+q

Page 11: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

28.3: Finding the Magnetic Force on a Particle:

Always assume particle is POSITIVELY charged to workOut direction then flip your thumb over if it is NEGATIVE.

Page 12: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.
Page 13: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Definition of Magnetic FieldDefinition of Magnetic Field

Definition of Electric Field:Definition of Electric Field:

Definition of Magnetic Field:Definition of Magnetic Field:

Page 14: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

28.3: The Definition of B:

The SI unit for B that follows is newton per coulomb-meter per second. For convenience, this is called the tesla (T):

An earlier (non-SI) unit for B is the gauss (G), and

Page 15: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Thompson Experiment& The Discovery of the Electron

Forces Balance: v=E/B

Page 16: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

L

y

II: E≠0, B=0

I: E=0, B=0

III: vB=E

Page 17: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.
Page 18: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

28.4: Crossed Fields, Discovery of an Electron:

When the two fields in Fig. 28-7 are adjusted so that the two deflecting forces acting on the charged particle cancel, we have

Thus, the crossed fields allow us to measure the speed of the charged particles passingthrough them. The deflection of a charged particle, moving through an electric field, E, between two plates, at the far end of the plates (in the previous problem) is

Here, v is the particle’s speed, m its mass, q its charge, and L is the length of the plates.

Experiment measured electrons mass to charge ratio m/q.

Page 19: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.
Page 20: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.

Example, Magnetic Force on a Moving Charged Particle :

Page 21: Lecture 25: MON 16 MAR Magnetic fields Ch.28.1–4 Physics 2113 Jonathan Dowling “I’ll be back…. Aurora Borealis.