Magnetic Fields & Electromagnetic Inductio

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51 Terms

1
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Explain the concept of a magnetic field

  • A magnetic field is the region around a magnet, current-carrying wire, or moving charged particle where another magnetic material or moving charge experiences a force.

  • The field is made up of invisible lines called magnetic field lines or lines of force.

  • The direction of a magnetic field at a point is the direction in which the north pole of a small magnet would move if placed at that point.

  • The strength of the magnetic field is shown by how close the lines are:

    • Closer lines = stronger field

    • Lines farther apart = weaker field.

<p></p><ul><li><p><span>A magnetic field is the region around a magnet, current-carrying wire, or moving charged particle where another magnetic material or moving charge experiences a force.</span></p></li><li><p><span>The field is made up of invisible lines called magnetic field lines or lines of force.</span></p></li><li><p><span>The direction of a magnetic field at a point is the direction in which the north pole of a small magnet would move if placed at that point.</span></p></li><li><p><span>The strength of the magnetic field is shown by how close the lines are:<br></span></p><ul><li><p><span>Closer lines = stronger field</span></p></li><li><p><span>Lines farther apart = weaker field.</span></p></li></ul></li><li><p></p></li></ul><p></p>
2
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Define electromagnetic induction

Electromagnetic induction is the production of an electromotive force (e.m.f.) across a conductor when there is a change in magnetic flux linking the conductor.

3
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What’s the relationship between electric force and magnetic force

They are equal and opposite in direction

<p>They are equal and opposite in direction</p>
4
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Draw a diagram showing how a charged particle would act when an electric field and magnetic field are at right angle to each other

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5
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What happens to a charge when it enters a magnetic field and why

It moves towards the plate (positive plate if the charge is an electron) and (negative plate if the charge is a proton) in a parabolic path

Because velocity is horizontal and

Acceleration is vertical

<p>It moves towards the plate (positive plate if the charge is an electron) and (negative plate if the charge is a proton) in a <strong>parabolic path</strong></p><p><strong><u>Because velocity is horizontal and</u></strong></p><p><strong><u>Acceleration is vertical</u></strong></p>
6
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When a charge enters a magnetic field,

If the magnetic field is wide enough, so that the charged particle stays in the field for a longer time, what will happen?

the charge will continue to move in a curve and will complete a complete circle.

<p><span>the charge will continue to move in a curve and will complete a complete circle.</span></p>
7
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When a charge enters a magnetic field,

If the magnetic field is not uniform then what will happen?

the path becomes a decreasing spiral

<p><span>the path becomes a decreasing spiral</span></p>
8
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The direction of a field produced by current flowing through a wire can be determined by…

Right hand grip rule

<p>Right hand grip rule</p>
9
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Define the direction of a magnetic field

  • The direction of the magnetic field line at a point is the direction of the force that would act on a north pole placed at that point

10
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Sketch the flux pattern for a long straight wire

  • A long straight current-carrying wire (concentric circles around wire).

<p></p><ul><li><p>A long straight current-carrying wire (concentric circles around wire).</p><ul><li><p></p></li></ul></li></ul><p></p>
11
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Sketch the flux pattern for a flat coil

  • A flat circular coil (looped lines through and around the coil).

<p></p><ul><li><p>A flat circular coil (looped lines through and around the coil).</p><ul><li><p></p></li></ul></li></ul><p></p>
12
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Equation for the magnetic flux density for a at a distance, r, from a straight current carting conductor

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13
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Equation for the magnetic flux density for a from the center of flat circular coil

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14
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Equation for the magnetic flux density from the center of A long solenoid with, n, number of turns and carrying current, I

<p></p>
15
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Draw diagrams of how force can act in current carrying conductor between magnetic field

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16
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The direction of force that can act in current carting conductor between magnetic field

Can be determined by

Flemming’s left hand rule

<p>Flemming’s left hand rule </p>
17
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Sketch the flux pattern for a solenoid

  • A long solenoid (similar to a bar magnet, with clear north and south poles)

<p></p><ul><li><p><span>A long solenoid (similar to a bar magnet, with clear north and south poles)</span></p><ul><li><p></p></li></ul></li></ul><p></p>
18
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True or false - a force might act on a current carrying conductor when placed in a magnetic field

True

19
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Define magnetic flux density

  • Magnetic flux is the total number of magnetic field lines (or the total magnetic field) passing through a given area.

  • It is a measure of how much magnetic field passes through a surface.

20
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Define Tesla

  • 1 tesla is defined as the magnetic flux density that produces a force of 1 newton on a conductor 1 metre long carrying a current of 1 ampere at right angles to the magnetic field.

  • In other words:
    1 T = 1 N A⁻¹ m⁻¹

21
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Equation for force acting on a conductor

  • F = BILsin θ
    where:

    • F = force (N)

    • B = magnetic flux density (T)

    • I = current (A)

    • l = length of conductor (m)

    • θ = angle between current and magnetic field

<p></p><ul><li><p><strong>F = BILsin </strong>θ<br>where:<br></p><ul><li><p>F = force (N)</p></li><li><p>B = magnetic flux density (T)</p></li><li><p>I = current (A)</p></li><li><p>l = length of conductor (m)</p></li><li><p>θ = angle between current and magnetic field</p></li></ul></li><li><p></p></li></ul><p></p>
22
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What is the effect of force when the angle is changed

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23
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Equation for magnetic flux density

Just transpose - F = BILsin θ

  • B = F / (ILsinθ)

where:

  • B = magnetic flux density (tesla, T)

  • F = force on the conductor (newtons, N)

  • I = current (amperes, A)

  • l = length of conductor in the field (metres, m)

  • θ = angle between the conductor and the magnetic field

24
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T or F -

  • magnetic field is the region where a magnetic force is experienced.

True

25
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Equation for force on a moving charge

  • F = BQv sin θ
    where:

    • F = force on charge (N)

    • B = magnetic flux density (T)

    • Q = charge (C)

    • v = speed (m/s)

    • θ = angle between v and B

26
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What is the condition for no deflection on a moving charge

  • Condition for no deflection: E = Bv.

27
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A particle can move in a circular path or a helical path.

What causes this?

  • depends on their angle to B

28
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T or F For a moving charge

No change in speed; only direction changes

True

29
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  • Explain the Hall effect:.

  • A potential difference is set up transversely across a current-carrying conductor when a perpendicular magnetic field is applied

<p></p><ul><li><p><span>A potential difference is set up transversely across a current-carrying conductor when a perpendicular magnetic field is applied</span></p></li></ul><p></p>
30
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explain how a Hall probe is used to measure magnetic flux density

A Hall probe is used to measure magnetic flux density. It consists of a thin slice of semiconductor carrying a steady current. When the probe is placed in a magnetic field at right angles to the direction of the current, a potential difference, called the Hall voltage, is generated across it. The Hall voltage is proportional to the magnetic flux density.

<p><span>A Hall probe is used to measure magnetic flux density. It consists of a thin slice of semiconductor carrying a steady current. When the probe is placed in a magnetic field at right angles to the direction of the current, a potential difference, called the Hall voltage, is generated across it. The Hall voltage is proportional to the magnetic flux density.</span></p>
31
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32
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describe and explain the force between two current-carrying conductors

Two parallel current-carrying conductors exert a force on each other. If the currents are in the same direction, the force is attractive. If the currents are in opposite directions, the force is repulsive.

<p><span>Two parallel current-carrying conductors exert a force on each other. If the currents are in the same direction, the force is attractive. If the currents are in opposite directions, the force is repulsive.</span></p>
33
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state the formula for the force per unit length between two parallel current-carrying conductors

<p></p>
34
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<p>T or F </p>

T or F

True

35
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describe the construction and operation of an electromagnet

An electromagnet consists of a coil of insulated wire wound around a soft iron core. When a current flows through the coil, the core becomes magnetised.

36
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state the properties of a soft iron core in an electromagnet

The soft iron enhances the magnetic field because it has high magnetic permeability and low retentivity, which means it loses its magnetism easily when the current is switched off and it’s able to concentrate magnetic field lines

<p>The soft iron enhances the magnetic field because it has high magnetic permeability and low retentivity, which means it loses its magnetism easily when the current is switched off and it’s able to concentrate magnetic field lines </p>
37
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State applications of electromagnets

Electromagnets are used in devices such as electric bells, relays, circuit breakers, and magnetic cranes used for lifting heavy iron objects

<p>Electromagnets are used in devices such as electric bells, relays, circuit breakers, and magnetic cranes used for lifting heavy iron objects</p>
38
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discuss applications of electromagnets For

  • magnetic door locks

  • Relays

  • Electric bells

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39
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state Faraday’s law of electromagnetic induction

Faraday’s law states that the magnitude of the induced e.m.f. is proportional to the rate of change of magnetic flux linkage

40
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Faraday’s law Equation

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41
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state Lenz’s law and determine the direction of an induced e.m.f.

Lenz’s law states that the direction of the induced current is such that it opposes the change that causes it.

<p>Lenz’s law states that the direction of the induced current is such that it opposes the change that causes it.</p>
42
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discuss Lenz’s law as an example of conservation of energy

Lenz’s law is a consequence of the law of conservation of energy because the induced current must oppose the change that produces it, otherwise energy would be created or destroyed.

<p>Lenz’s law is a consequence of the law of conservation of energy because the induced current must oppose the change that produces it, otherwise energy would be created or destroyed.</p>
43
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explain the principle of a simple d.c. motor

A current-carrying coil placed in a magnetic field experiences a force. The forces on the sides of the coil produce a turning moment, causing the coil to rotate.

<p>A current-carrying coil placed in a magnetic field experiences a force. The forces on the sides of the coil produce a turning moment, causing the coil to rotate.</p>
44
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describe the construction and operation of a simple d.c. motor

A simple d.c. motor consists of a rectangular coil of wire positioned between the poles of a permanent magnet. A split-ring commutator reverses the direction of the current in the coil every half-turn, ensuring continuous rotation in one direction

<p>A simple d.c. motor consists of a rectangular coil of wire positioned between the poles of a permanent magnet. A split-ring commutator reverses the direction of the current in the coil every half-turn, ensuring continuous rotation in one direction</p>
45
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describe the construction and operation of a simple a.c. motor

A simple a.c. motor is similar in construction to a simple d.c. motor except that it uses slip rings instead of a split-ring commutator. The slip rings maintain contact with the external circuit while allowing the coil to rotate freely. In an a.c. motor, the direction of current changes every half-cycle of the alternating supply, and the motor continues to rotate.

<p>A simple a.c. motor is similar in construction to a simple d.c. motor except that it uses slip rings instead of a split-ring commutator. The slip rings maintain contact with the external circuit while allowing the coil to rotate freely. In an a.c. motor, the direction of current changes every half-cycle of the alternating supply, and the motor continues to rotate.</p>
46
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describe the construction and operation of a simple d.c. generator

A simple d.c. generator consists of a coil rotating between the poles of a magnet. A split-ring commutator is used so that the current in the external circuit flows in one direction only. The induced e.m.f. varies with time, but always in the same direction.

<p><span>A simple d.c. generator consists of a coil rotating between the poles of a magnet. A split-ring commutator is used so that the current in the external circuit flows in one direction only. The induced e.m.f. varies with time, but always in the same direction.</span></p>
47
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describe the construction and operation of a simple a.c generator

A simple a.c. generator consists of a coil rotating between the poles of a magnet. Slip rings are used to maintain continuous contact with the external circuit, allowing the current to reverse direction every half-turn, producing an alternating current.

<p><span>A simple a.c. generator consists of a coil rotating between the poles of a magnet. Slip rings are used to maintain continuous contact with the external circuit, allowing the current to reverse direction every half-turn, producing an alternating current.</span></p>
48
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The total amount to magnetic flux through an area at right angles to the magnetic field is given by what equation

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49
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State 3 examples of electromagnetic induction

  1. Faraday’s disc

  2. Magnet moving in a coil

  3. A current carrying solenoid placed near to a search coil

  4. A washer resting on a solenoid

50
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Explain the use of electromagnetic induction on the following:

  1. Faraday’s disc

  2. Magnet moving in a coil

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51
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Explain the use of electromagnetic induction on the following:

  1. A current carrying solenoid placed near to a search coil

  2. A washer resting on a solenoid

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