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Magnetism Magnetism; MF lines and Magnetic flux; motion of charged particles; MF on current-carrying loops; Applications; DC motors Magnetic Fields and Magnetic Forces

Magnetism

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Electricity and Magnetism: Magnetic force, field, and electromagnetic induction

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Page 1: Magnetism

Magnetism; MF lines and Magnetic flux; motion of charged particles; MF on current-carrying loops; Applications; DC motors

Magnetic Fields and Magnetic Forces

Page 2: Magnetism

Magnetism

• The fundamental nature of magnetism is the interaction of moving electric charges.

Page 3: Magnetism

Magnetism

• Electric forces may act on charges whether they are at rest or moving.• Magnetic forces act

only on moving charges.

Page 4: Magnetism

Magnetism• It’s N geographic

pole is close to a magnetic S-pole.

• Magnetic declination or magnetic variation is observed.

Page 5: Magnetism

Magnetism

• No single isolated magnetic pole exists.• Poles always

appear in pairs.

Page 6: Magnetism

• First to discover the relationship of magnetism to moving charges

• A compass needle was deflected by a current-carrying wire

Hans Christian Oersted

Page 7: Magnetism

• Discovered that moving a magnet near a conducting loop can cause a current in the loop.

Michael Faraday and Joseph Henry

Page 8: Magnetism

Magnetic Field and Force

• A moving charge or a current creates a magnetic field in the surrounding space.

• The magnetic field exerts a force on any other moving charge or current that is present in the field.

Page 9: Magnetism

Magnetic Field and ForceAt any position, the direction of B is defined as that which the N-pole of a compass needle tends to point.

Magnetic field (B) is a vector field.

Page 10: Magnetism

F is always perpendicular to B and v.

The magnitude of a magnetic force also depends on the particle’s velocity.

The magnitude of a magnetic force is proportional to the magnitude of the field.

The magnitude of a magnetic force is proportional to the magnitude of the charge.

Magnetic Field and Force

Page 11: Magnetism

Coulomb’s Law for Magnetism

Where m is magnetic pole strength; k= 10-7N.m2/(Amp.m)2

d = distance

F = k(m1m2/d2)

Page 12: Magnetism

Draw vectors v and B with their

tails together.

Imagine turning v until it points in

the direction of B.

Your thumb then points in the direction of F.

F = qv x BF = qvBsinɸ

Magnetic Field and Force

Page 13: Magnetism

• Find the forces exerted by the N poles of the magnets to each other.

Example

4.10x10-14N

Page 14: Magnetism

A beam of protons (q=1.6x10-19C) moves at 3.0x105m/s through a uniform magnetic field with magnitude 2.0T that is directed along the positive z-axis. The velocity of each proton lies in the xz-plane at an angle of 30° to the +z-axis. Find the force on a proton.

Example

4.8x10-14N

Page 15: Magnetism

Magnetism

What is the direction of the magnetic force on the

charge?

Page 16: Magnetism

Field lines• The idea is the same

for the electric field lines.

• When adjacent field lines are close together, the field magnitude is large.

Magnetic flux ΦB

• Same idea as the electric flux: The net magnetic flux through the surface of an enclosed area is directly proportional to the magnitude of the net charge enclosed

Magnetic Field Lines and Flux

Page 17: Magnetism

Magnetic Flux

B

B

Page 18: Magnetism

Magnetic Flux

ΦB = BAcosɸ

Where B is magnetic field; A is area vector

Page 19: Magnetism

Magnetic Flux

• SI unit is weber (Wb)• B may also be called

magnetic flux density.• The total magnetic

flux through a closed surface is always zero.

B

Page 20: Magnetism

A flat surface has an area of 3.0 cm2 in a uniform magnetic field. If the magnetic flux through this area is 0.90 mWb, calculate the magnitude of the magnetic field and find the direction of the area vector.

Example

B = 6.0 TArea vector = perpendicular

Page 21: Magnetism

Motion of Charged particles in a Magnetic field

• Motion of a charged particle under the action of a magnetic field alone is always motion with constant speed.

Page 22: Magnetism

Motion of Charged particles in a Magnetic field

ac = v2 / R

Where v is velocity; R is radius

Page 23: Magnetism

Motion of Charged particles in a Magnetic field

F = qvB = mv2 / R

Where q is charge R is radius m is mass

Page 24: Magnetism

Motion of Charged particles in a Magnetic field

ω= v/R = qB/m = 2πf

Where q is charge, R is radius, m is mass, f is frequency

Page 25: Magnetism

• A magnetron in a microwave oven emits electromagnetic waves with frequency 2450 MHz. What magnetic field strength is required for electrons to move in a circular path with this frequency?

• m= 9.11x10-31kg; q= 1.60x10-19C

Example

B = 0.0877 T

Page 26: Magnetism

Applications of Motions of Charged Particles

Velocity selector

Page 27: Magnetism

Magnetic Forceon a Current Carrying Conductor

The force is always perpendicular to both the conductor and field

Page 28: Magnetism

Magnetic Forceon a Current Carrying Conductor

F = qvd x B = qvdB sinɸ

Where F = force; vd = drift velocity;

B = magnetic field

Page 29: Magnetism

Magnetic Forceon a Current Carrying Conductor

F = I l x B = IlB sinɸ

Where F = force; I = current; l = length; B = magnetic field

Page 30: Magnetism

Magnetism

Page 31: Magnetism

Example

A straight horizontal copper rod carries a current of 50.0 A from west to east in a region between the poles of a large electromagnet. In these region, there is a horizontal magnetic field toward the northeast (45° N of E) with magnitude 1.20 T.

A. Find the magnitude of the force on a 1.00 m section of rod.B. While keeping the rod horizontal, how should it be oriented to maximize the magnitude of force?

Page 32: Magnetism

MagnetismExample

A. 42.4 NB. Perpendicular (F=60.0 N)

Page 33: Magnetism

Force and Torqueon a Current Carrying Loop

•The net force on a current loop in a uniform magnetic field is zero.

•However, the net torque is not, in general, equal to zero.

Page 34: Magnetism

Force and Torqueon a Current Carrying Loop

τ = IBA sin ɸ

μ = IA

τ = μB sin ɸ = μ x B

Page 35: Magnetism

Magnetism

a

B

I

Page 36: Magnetism

Example

A circular coil 0.0500 m in radius lies in a horizontal plane. It carries a current of 5.00 A in a counter-clockwise sense when viewed from above. The coil is in uniform magnetic field directed toward the right with magnitude 1.20 T. Find the magnitudes of the magnetic moment and the torque on the coil.

Page 37: Magnetism

Example

A circular coil 0.0500 m in radius with 30 turns of wire lies in a horizontal plane. It carries a current of 5.00 A in a counter-clockwise sense when viewed from above. The coil is in uniform magnetic field directed toward the right with magnitude 1.20 T. Find the magnitudes of the magnetic moment and the torque on the coil.

Page 38: Magnetism

Example

μ = 3.93 x 10-2 Am2 ; μtotal = 1.18 Am2 ;

τ = 0.0471 Nm τtotal = 1.41 Nm

Page 39: Magnetism

The Direct-Current Motor

In a motor:• The magnetic

torque acts on a current-carrying conductor

• Electric energy is converted to mechanical energy

The Direct-Current Motor

Page 40: Magnetism

The Direct-Current Motor

Rotor• Is the moving part of

the motor• It is a loop of wire

formed into an open ended loop and free to rotate about an axis

The Direct-Current Motor

Page 41: Magnetism

The Direct-Current Motor

Commutator• Formed by the

attachment of the rotor wires to circular conducting segments

The Direct-Current Motor

Page 42: Magnetism

The Direct-Current Motor

Brushes• makes contact with

the each commutator segment

• are parts of an external circuit that includes a source of emf

The Direct-Current Motor

Page 43: Magnetism

The Direct-Current MotorThe Direct-Current Motor

Page 44: Magnetism

MagnetismThe Direct-Current Motor

Vab= Ԑ + Ir

Where Vab = voltage; Ԑ = electromotive force;

I = current;r = internal resistance

Page 45: Magnetism

MagnetismThe Direct-Current Motor

P = VabI= I2R

Where Vab = voltage; I = current;R= resistance

Page 46: Magnetism

Magnetism• A dc motor with its rotor and field coils

connected in series has an internal resistance of 2.00Ω. When running at full load on a 120-V line, it draws a current of 4.00A.

a) What is the emf in the rotor?

b) What is the power delivered to the motor?

c) What is the rate of dissipation of energy in the resistance of the motor?

Example

Page 47: Magnetism

Magnetism

a) ԑ=112Vb)P input= 480W

c) P dissipated= 32W

Source: Young, Hugh D., and Freedman, Roger A. 2002, Reprinted. University Physics with Modern Physics. 10th ed. Singapore: Pearson Education Asia Pte Ltd. Copyright ©

2000 by Addison-Wesley Publishing Longman, Inc.

PowerPoint edited by Mr. Jon Sithli Mendoza