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Magnetism

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Title: Magnetism


1
Magnetism
2
Magnetic Poles
  • Magnets exert force on one another
  • Regions of magnetic poles produce magnetic forces
  • The end that points northward is called the
    north-seeking pole and vice-versa
  • Each magnet has both poles-even if you take a
    magnet and break it in two, each part will have
    both poles
  • Likes poles repel opposite poles attract
  • Electric charges can be isolated, magnetic poles
    cannot

3
Magnetic Fields
  • The space around a magnet in which a magnetic
    force is exerted, is filled with a magnetic field
  • The shape of the field is revealed by magnetic
    field lines
  • Magnetic Domains The magnetic field of
    individual iron atoms is so strong that
    interactions among adjacent iron atoms cause
    large clusters of them to line up with each
    other. These clusters of aligned atoms are called
    magnetic domains
  • The difference between a piece of ordinary iron
    and an iron magnet is alignment of domains
  • Permanent magnets are made by simple placing
    pieces of iron or certain iron alloys in strong
    magnetic fields

4
The Nature of a Magnetic Field
  • A magnetic field is produced by the motion of
    electric charge
  • The magnet as a whole is stationary while the
    electrons are in constant motion
  • Every spinning electron is a tiny magnet

5
The Earths Magnetic Field
  • The discrepancy between the orientation of a
    compass and true north is called the magnetic
    declination
  • The magnetic field of the earth is not stable

6
Oersteds Discovery
  • In a public experiment, Oersted showed that
    electric current could affect the motion of a
    compass needle
  • The effect decreases by distance, but is not
    affected by blockage by other materials(glass,pape
    r,water, even metal)
  • The effect on a compass is a torque, proportional
    to field strength B and magnetic dipole moment m
    so that tmBsinq
  • Units for field strength tesla symbolized T
  • Direction of the field around the wire is in
    concentric circles rotationg according to a
    right-hand rule If the thumb of the right hand
    is in the direction of the current, the curling
    fingers show the direction of the field

7
Electric Currents and Magnetic Fields
  • A moving charge produces a magnetic field, many
    of these with an electric current
  • Magnetic field lines about a current-carrying
    wire crowd up when the wire is bent into a loop
  • A piece of iron placed in a current-carrying coil
    of wire is an electromagnet

8
Magnetic Forces on Current-Carrying Wires
  • Current-carrying wires respond to deflected
    force, moving the wire
  • If the direction of the current is reversed, the
    deflected force acts in the opposite direction
  • The force is maximum when the current is
    perpendicular to the magnetic field lines
  • The value of this force depends on current,
    length of the wire in the field, field strength,
    and angle between direction of current and field
    F I l B sin q

9
Example 19.1
  • A straight wire thru a field of 1.00 T which is
    0.250 m wide is perpendicular to the field. What
    current must be in the wire to produce a force of
    9.81 N?
  • Rearrange the force equation to find current
  • I F 9.81
    39.2 A
  • l B sin q (.250)(1.00)(1.00)

10
Magnetic Forces on Moving Charged Particles
  • A charged particle at rest will not interact with
    a static magnetic field
  • A charged particle that moves in a magnetic
    field, the magnetic character of its motion
    becomes evident, experiencing a deflected force
  • The force is greatest when the particle moves in
    a direction perpendicular to the magnetic field
    lines
  • At other angles the force is less
  • It becomes zero when the particle moves parallel
    to the field lines
  • Value of this force depends on charge, velocity,
    field strength, and angle between field and
    motion
  • F q v B sin q
  • If a charged particle were injected into a
    magnetic field, it would follow a circular path,
    with radius controlled by mass, velocity, charge,
    and field r m v This equation is
    used in nuclear research.
  • q B

11
Magnetic Field of a Current Carrying Wire
  • The value of field strength at any point around a
    current carrying wire was found by Biot and
    Savart not long after Oersteds experiment
  • The equation for B where k has value
  • of 10-7 N/A2
  • Example 19.5
  • What is the magnitude of the magnetic field 3.0 m
    from a wire carrying 15 A?
  • Use the equation B k 2I (10-7) (2)(15)
    1.0 10-6 T
  • d 3.0

12
Force Between Two Wires
  • Two current carrying wires exert forces on each
    other, depending on relative current direction
  • If both currents are in same direction, the force
    is attractive if opposite, the forces are
    repulsive
  • The force per unit length is easiest to measure
    and its equation, if the currents are equal, is

13
Magnetic Field in a Wire Loop
  • A special case is that of a magnetic field at the
    center of a circular wire loop
  • Re-defining k in terms of mo allows elimination
    of p in equations k mo / 4p
  • This makes the equation for B moI
  • 2r

14
Example 19.6
  • What radius loop will a copper wire of resistance
    per unit length 0.068 W/m, connected to a 6.3 V
    battery, have the same field as the earth, 5.0
    10-5 T ?
  • Resistance would be (R/l) x circumference(2pr)
    and IV/R so IV/ (2pr)(R/l)
  • Field strength becomes B moI /2r mo V/
    (4pr2)(R/l)
  • Rearranging for r
  • r 0.43 m

15
Magnetic Force on a Current Loop
  • If a rectangular loop in a constant field is
    considered, two sides will be parallel and two
    perpendicular to the field. Those parallel to
    the field have forces equal and opposite and thus
    no torque is created, but those perpendicular
    will have torques adding to make tIAB sin q
    where A is the area of the loop.
  • The current loop becomes a magnetic dipole with
    moment mIA and direction related to another
    right-hand rule
  • The direction of the magnetic moment is the
    direction of the right thumb as the fingers curl
    in the direction of the current
  • Since loops can be multiplied, the moment can be
    calculated for N loops as mNIA

16
Example 19.7
  • A flat coil of 25 loops has a radius of 5.5 cm.
  • a. What is the magnetic moment if the current is
    1.5 A?
  • b. What is the maximum torque exerted on it by
    the earths magnetic field? (B 5.0 x 10-5 T)
  • a. mNIA (25)(1.5)(p(5.5x10-2)2) 0.36 A m2
  • b. tmBsinq (0.36)(5.0 x 10-5)(1.0) 1.8 x 10-5
    Nm

17
Meters for Current and Voltage
  • A current-indicating instrument which utilizes
    the torque from a magnetic field is the
    galvanometer
  • A galvanometer may be calibrated to measure
    current in amperes to make an ammeter. Ammeters
    are usually constructed with a resistance in
    parallel to control current range.
  • Ammeters calibrated to measure electric potential
    (volts) is a voltmeter. Voltmeters are
    constructed with a resistance in series to limit
    the current passing thru the meter.

18
Example 19.8
  • What resistance must be used in series with a
    galvanometer of resistance 10 kW with full
    deflection at 100 mA to make a meter which will
    measure 100 V?
  • The required resistance for the total meter would
    be Rv V/I 100 / (100x 10-6) 106 W
  • The added series resistor would be
  • R Rv -Rm 106 - 10 x 103 990,000 W

19
Homework Chapter 19
  • Pp.552-554
  • 6, 7, 14, 20, 34, 36, 43, 48

20
Electromagnetic Induction
  • Faraday discovered that a current carrying wire
    can induce a current in a nearby wire if the
    current in the first wire is continually changing
  • The amount of voltage induced depends on how
    quickly the magnetic field lines are traversed by
    the wire (the quicker the more voltage) V? rate
    of change of magnetic flux
  • Formula for magnetic flux fm thru area A and
    magnetic field B is fm BA cos q
  • The greater number of loops of wire that move in
    a magnetic field, the greater the induced voltage
    and the greater the current in the wire
  • The voltage, or emf, in a series of N loops
    becomes
  • E

21
Electromagnetic Induction
  • Lenzs Law states the direction of the induced
    current in a coil is such that its own magnetic
    field opposes the original change in magnetic
    flux that induced the current.
  • This means it is more difficult to push the
    magnet into a coil with more loops because the
    magnetic field of each current loop resists the
    motion of the magnet.
  • The phenomena of inducing voltage by changing the
    magnetic field around a conductor is called
    electromagnetic induction.

22
Examples 20.1 20.2
  • What emf is produced in a square coil of wire
    with 20 turns and 10 cm on a side which is
    removed from a field of 0.25 T in 0.10 s?
  • Use fm BA cos q where since q 0º, then cos q
    1 and fm BA
  • so fm (0.25)(.10)2 0.0025
  • E -Nfm/t -20(0.0025) / 0.10 0.50 V
  • Find the current thru a 37 W resistor connected
    to a 5 turn circular loop of diameter 10 cm with
    a field change rate of 0.050 T/s.
  • I E /R (-NDfm/DtR) (-NDBA/DtR)(-NDBp(D/2)2/Dt
    R)
  • I -NpD2(DB/Dt) - 5 p(0.10)2(0.050)
    -53 x 10-6 A
  • 4 R 4(37)

23
Motional EMF
  • If a wire moves in a constant field, the effect
    is the same as a stationary wire in a changing
    field
  • E

Example 20.3 How fast must a 0.27 m aluminum rod
be moved in a 0.89 T field to generate an emf of
1.5 V? E Blv so v E/Bl 1.5 / (0.89)(0.27)
6.2 m/s
24
Generators and Alternating Current
  • Generators convert mechanical energy into
    electrical by rotating a coil of wire in a
    magnetic field. This induced voltage alternates
    in direction and the frequency of the induced
    alternating voltage is equal to the frequency of
    the changing magnetic field within the loop.
  • As the coil is rotated, the magnetic flux thru
    the coil continually changes. The induced emf is
    drawn off the coil by rotating contacts.
  • The emf created varies in value from positive to
    negative in a sinusoidal fashion. Since q can be
    expressed as w t ,angular speed times seconds,
    then emf can be expressed likewise E w BA
    sin w t
  • In a closed circuit, it produces an alternating
    current

25
Example 20.4
  • A 25 loop coil of area 0.010 m2 rotated in
    earths magnetic field at a frequency of 60 Hz
    produces an emf. What is its value?
  • E Nw BA at peak, where sin w t 1
  • since w 2p f, this becomes E N 2p f BA
  • E (25)(2p)(60)(5.0 x 10-5)(0.010) 4.7 x 10-3 V

26
Electric Motors
  • If the design of the generator is reversed, you
    have an electric motor, where electric current
    causes repulsion against a magnet to produce
    motion
  • Large motors are usually made with an
    electromagnet that is energized by a power source
    with many loops of wire that are wound about an
    iron cylinder, called an armature which then
    rotates when energized with electric current
  • Motor and Generator Comparison Moving charges
    experience a force that is perpendicular to both
    their motion and the magnetic field that they
    traverse.
  • The deflected wire is the motor effect, and the
    law of induction is the generator effect

27
Transformers
  • Transformers are made from two multiturn coils of
    wire on an iron core. It allows an increase or
    decrease of AC voltage without appreciable power
    loss. The iron core allows better transfer of
    magnetic flux and better magnetic coupling than
    thru air. The relationship between the two
    circuits is shown in the formula
  • primary voltage
    secondary voltage
  • number of primary turns number of
    secondary turns
  • V1 V2 V1 N1
  • N1 N2 V2 N2
  • Power into primary power out of secondary
  • (voltage current)primary (voltage
    current)secondary

28
Example 20.6
  • A 20 W desk lamp has resistance of 7.2 W. If the
    current to the lamp comes from a transformer with
    primary voltage of 120 V AC,
  • a. What is the ratio of primary to secondary
    turns?
  • b. What is the minimum current thru the primary?
  • P2 V22 /R2 so V2 ? P2R2 ? (20)(7.2) 12 V
  • V1/ V2 N1/ N2 120 / 12 10
  • V1I1 V2I2 I2 V2 / R2 12 / 7.2 1.67 A
  • (120)I1 (12)(1.67) I1 0.167 A

29
Power Transmission
  • Almost all power today is AC and the voltage is
    transferred in different levels
  • Power created at 6000 V then raised to 120000 V
  • Power is reduced when it comes to user

30
Induction of Electric and Magnetic Fields
  • An electric field is induced in any region of
    space in which a magnetic field is changing with
    time.
  • The magnitude of the induced electrical field is
    proportional to the rate at which the magnetic
    field changes.
  • The direction of the induced electric field is at
    right angles to the changing magnetic field
  • A magnetic field is induced in any region of
    space in which an electric field is changing with
    time.
  • The magnitude of the induced magnetic field is
    proportional to the rate at which the electric
    field changes.
  • The direction of the induced magnetic field is at
    right angles to the changing electric field

31
Electromagnetic Waves
  • Shake a charged object to and fro and you produce
    electromagnetic waves.
  • An electromagnetic wave is composed of vibrating
    electric and magnetic fields that regenerate each
    other

32
Homework
  • pp. 576-578
  • 2, 6, 10, 15, 16, 20, 22

33
Hooo-RAH!!
  • Nada--NOTHING from chapter 21 on the B test!!!!
  • Scared you for nothing I guess!!

34
EQUATIONS!!
tmBsinq F I l B sin q F q v B sin q r
m v / q B B k2I/d moI/2pd mNIA tIAB sin
q mBsinq fm BA cos q E -NDfm/ D t E
Blv E w BA sin w t V1 V2
V1 N1 N1 N2 V2
N2 V1I1 V2I2
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