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# Chapter 19 - PowerPoint PPT Presentation

Chapter 19. Magnetism. Magnets. Poles of a magnet are the ends where objects are most strongly attracted Two poles, called north and south Like poles repel each other and unlike poles attract each other Similar to electric charges Magnetic poles cannot be isolated

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### Chapter 19

Magnetism

• Poles of a magnet are the ends where objects are most strongly attracted

• Two poles, called north and south

• Like poles repel each other and unlike poles attract each other

• Similar to electric charges

• Magnetic poles cannot be isolated

• If a permanent magnetic is cut in half repeatedly, you will still have a north and a south pole

• This differs from electric charges

• There is some theoretical basis for monopoles, but none have been detected

• An unmagnetized piece of iron can be magnetized by stroking it with a magnet

• Somewhat like stroking an object to charge an object

• Magnetism can be induced

• If a piece of iron, for example, is placed near a strong permanent magnet, it will become magnetized

• Soft magnetic materials, such as iron, are easily magnetized

• They also tend to lose their magnetism easily

• Hard magnetic materials, such as cobalt and nickel, are difficult to magnetize

• They tend to retain their magnetism

• A vector quantity

• Symbolized by B

• Direction is given by the direction a north pole of a compass needle points in that location

• Magnetic field lines can be used to show how the field lines, as traced out by a compass, would look

• A compass can be used to show the direction of the magnetic field lines (a)

• A sketch of the magnetic field lines (b)

• Iron filings are used to show the pattern of the electric field lines

• The direction of the field is the direction a north pole would point

• Iron filings are used to show the pattern of the electric field lines

• The direction of the field is the direction a north pole would point

• Compare to the electric field produced by an electric dipole

• Iron filings are used to show the pattern of the electric field lines

• The direction of the field is the direction a north pole would point

• Compare to the electric field produced by like charges

• An electric field surrounds any stationary electric charge

• A magnetic field surrounds any moving electric charge

• A magnetic field surrounds any magnetic material

• The Earth’s geographic north pole corresponds to a magnetic south pole

• The Earth’s geographic south pole corresponds to a magnetic north pole

• Strictly speaking, a north pole should be a “north-seeking” pole and a south pole a “south-seeking” pole

• The Earth’s magnetic field resembles that achieved by burying a huge bar magnet deep in the Earth’s interior

• There cannot be large masses of permanently magnetized materials since the high temperatures of the core prevent materials from retaining permanent magnetization

• The most likely source of the Earth’s magnetic field is believed to be electric currents in the liquid part of the core

• When moving through a magnetic field, a charged particle experiences a magnetic force

• This force has a maximum value when the charge moves perpendicularly to the magnetic field lines

• This force is zero when the charge moves along the field lines

• One can define a magnetic field in terms of the magnetic force exerted on a test charge

• Similar to the way electric fields are defined

• The SI unit of magnetic field is the Tesla (T)

• Wb is a Weber

• The cgs unit is a Gauss (G)

• 1 T = 104 G

• Conventional laboratory magnets

• 25000 G or 2.5 T

• Superconducting magnets

• 300000 G or 30 T

• Earth’s magnetic field

• 0.5 G or 5 x 10-5 T

• Experiments show that the direction of the magnetic force is always perpendicular to both v and B

• Fmax occurs when v is perpendicular to B

• F = 0 when v is parallel to B

• Hold your right hand open

• Place your fingers in the direction of B

• Place your thumb in the direction of v

• The direction of the force on a positive charge is directed out of your palm

• If the charge is negative, the force is opposite that determined by the right hand rule

A charged particle moves in a straight line through a certain region of space. The magnetic field in that region (a) has a magnitude of zero, (b) has a zero component perpendicular to the particle's velocity, or (c) has a zero component parallel to the particle's velocity.

QUICK QUIZ 19.1

(b). The force that a magnetic field exerts on a charged particle moving through it is given by F = qvB sin θ = qvB , where B is the component of the field perpendicular to the particle’s velocity. Since the particle moves in a straight line, the magnetic force (and hence B , since qv≠ 0) must be zero.

The north-pole end of a bar magnet is held near a stationary positively charged piece of plastic. Is the plastic (a) attracted, (b) repelled, or (c) unaffected by the magnet?

QUICK QUIZ 19.2

(c). The magnetic force exerted by a magnetic field on a charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

Magnetic Force on a Current Carrying Conductor charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• A force is exerted on a current-carrying wire placed in a magnetic field

• The current is a collection of many charged particles in motion

• The direction of the force is given by right hand rule #1

Force on a Wire charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• The blue x’s indicate the magnetic field is directed into the page

• The x represents the tail of the arrow

• Blue dots would be used to represent the field directed out of the page

• The • represents the head of the arrow

• In this case, there is no current, so there is no force

Force on a Wire, cont charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• B is into the page

• Point your fingers into the page

• The current is up the page

• Point your thumb up the page

• The force is to the left

• Your palm should be pointing to the left

Force on a Wire, final charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• B is into the page

• Point your fingers into the page

• The current is down the page

• Point your thumb down the page

• The force is to the right

• Your palm should be pointing to the right

Force on a Wire, equation charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• The magnetic force is exerted on each moving charge in the wire

• The total force is the sum of all the magnetic forces on all the individual charges producing the current

• F = B I ℓ sin θ

• θ is the angle between B and I

• The direction is found by the right hand rule, pointing your thumb in the direction of I instead of v

Force on a Charged Particle in a Magnetic Field charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• Consider a particle moving in an external magnetic field so that its velocity is perpendicular to the field

• The force is always directed toward the center of the circular path

• The magnetic force causes a centripetal acceleration, changing the direction of the velocity of the particle

Force on a Charged Particle charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• Equating the magnetic and centripetal forces:

• Solving for r:

• r is proportional to the momentum of the particle and inversely proportional to the magnetic field

Bending an Electron Beam in an External Magnetic Field charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

Particle Moving in an External Magnetic Field, 2 charge is proportional to the charge’s velocity relative to the field. If the charge is stationary, as in this situation, there is no magnetic force.

• If the particle’s velocity is not perpendicular to the field, the path followed by the particle is a spiral

• The spiral path is called a helix

As a charged particle moves freely in a circular path in the presence of a constant magnetic field applied perpendicular to the particle's velocity, its kinetic energy (a) remains constant, (b) increases, or (c) decreases.

QUICK QUIZ 19.3

(a). The magnetic force acting on the particle is always perpendicular to the velocity of the particle, and hence to the displacement the particle is undergoing. Under these conditions, the force does no work on the particle and the particle’s kinetic energy remains constant.

Two charged particles are projected into a region in which a magnetic field is perpendicular to their velocities. After they enter the magnetic field, you can conclude that (a) the charges are deflected in opposite directions, (b) the charges continue to move in a straight line, (c) the charges move in circular paths, or (d) the charges move in circular paths but in opposite directions.

QUICK QUIZ 19.4

(c). Anytime the velocity of a charged particle is perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.

Magnetic Fields – perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.Long Straight Wire

• A current-carrying wire produces a magnetic field

• The compass needle deflects in directions tangent to the circle

• The compass needle points in the direction of the magnetic field produced by the current

Direction of the Field of a Long Straight Wire perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.

• Right Hand Rule #2

• Grasp the wire in your right hand

• Point your thumb in the direction of the current

• Your fingers will curl in the direction of the field

Magnitude of the Field of a Long Straight Wire perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.

• The magnitude of the field at a distance r from a wire carrying a current of I is

• µo = 4  x 10-7 T m / A

• µo is called the permeability of free space

Magnetic Force Between Two Parallel Conductors perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.

• The force on wire 1 is due to the current in wire 1 and the magnetic field produced by wire 2

• The force per unit length is:

Force Between Two Conductors, cont perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.

• Parallel conductors carrying currents in the same direction attract each other

• Parallel conductors carrying currents in the opposite directions repel each other

If perpendicular to the magnetic field, it will follow a circular path. The two particles will move in opposite directions around their circular paths if their charges have opposite signs, but their charges are unknown so (d) is not an acceptable answer.I1 = 2 A and I2 = 6 Ain the figure below, which of the following is true:(a) F1 = 3F2, (b) F1 = F2, or (c) F1 = F2/3?

QUICK QUIZ 19.5

(b). The two forces are an action-reaction pair. They act on different wires, and have equal magnitudes but opposite directions.

Magnetic Effects of Electrons -- Orbits different wires, and have equal magnitudes but opposite directions.

• An individual atom should act like a magnet because of the motion of the electrons about the nucleus

• Each electron circles the atom once in about every 10-16 seconds

• This would produce a current of 1.6 mA and a magnetic field of about 20 T at the center of the circular path

• However, the magnetic field produced by one electron in an atom is often canceled by an oppositely revolving electron in the same atom

Magnetic Effects of Electrons – Orbits, cont different wires, and have equal magnitudes but opposite directions.

• The net result is that the magnetic effect produced by electrons orbiting the nucleus is either zero or very small for most materials

Magnetic Effects of Electrons -- Spins different wires, and have equal magnitudes but opposite directions.

• Electrons also have spin

• The classical model is to consider the electrons to spin like tops

• It is actually a relativistic and quantum effect

Magnetic Effects of Electrons – Spins, cont different wires, and have equal magnitudes but opposite directions.

• The field due to the spinning is generally stronger than the field due to the orbital motion

• Electrons usually pair up with their spins opposite each other, so their fields cancel each other

• That is why most materials are not naturally magnetic

Magnetic Effects of Electrons -- Domains different wires, and have equal magnitudes but opposite directions.

• In some materials, the spins do not naturally cancel

• Such materials are called ferromagnetic

• Large groups of atoms in which the spins are aligned are called domains

• When an external field is applied, the domains that are aligned with the field tend to grow at the expense of the others

• This causes the material to become magnetized

Domains, cont different wires, and have equal magnitudes but opposite directions.

• Random alignment, a, shows an unmagnetized material

• When an external field is applied, the domains aligned with B grow, b

Domains and Permanent Magnets different wires, and have equal magnitudes but opposite directions.

• In hard magnetic materials, the domains remain aligned after the external field is removed

• The result is a permanent magnet

• In soft magnetic materials, once the external field is removed, thermal agitation cause the materials to quickly return to an unmagnetized state

• With a core in a loop, the magnetic field is enhanced since the domains in the core material align, increasing the magnetic field