Electromagnetic Induction Flashcards

(36 cards)

1
Q

What is electromagnetic induction

A

Electromagnetic induction is the process through which an induced e.m.f is produced in a conductor due to a changing magnetic field.

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2
Q

Magnitude of induced e.m.f could be increased by increasing:

A

No of turns in the solenoid
Strength of magnet
Speed at which magnet moves with respect to solenoid.

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3
Q

What is Faraday Law of electromagnetic induction

A

Faraday’s Law of electromagnetic induction states that the magnitude of the induced e.m.f is directly proportional to the rate of change of magnetic flux in the circuit.

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4
Q

What is Len’s Law

A

Len’s Law states that the direction of the induced e.m.f and hence the induced current in a closed circuit, is always such that the magnetic effect opposes the motion or change producing it.

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5
Q

Explain the shape of the graph sketched in a)
Refer to pg 429
Part 1

A
  • As the North Pole of magnet enters solenoid, magnetic influx in solenoid changes.
  • By Faraday’s Law, the change in magnetic influx in the solenoid results in an induced e.m.f in the circuit. This e.m.f drives an induced current through the closed circuit.
  • By Len’z law, the induced current creates an N pole at the right end of the solenoid to repel incoming N pole. Thus, the needle is deflected momentarily to 1 side.
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6
Q

Part 2

A
  • At the instant when the magnet travels past the mid-length point of the solenoid, there is no change in magnetic flux in the solenoid.
  • There is no induced e.m.f and hence no induced current to cause the needle to be deflected
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7
Q

Part 3

A
  • As the S pole of the magnet exits the solenoid, there is again a change in magnetic flux in the solenoid
  • By Faradays Law, this produces an induced e.m.f and hence an induced current
  • By Len’s Law, the induced current creates a N pole at the left side of the solenoid to attract the S pole of magnet.
  • This causes needle to be deflected momentarily to 1 side
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8
Q

Simple a.c. Generator part 1

A
  • A rectangular coil of wire ABCD is mounted on an axle.
  • By rotating the handle, the coil rotates between the poles of the 2 permanent magnets.
  • As the coil rotates in the magnetic field, the change in magnetic flux creates an induced e.m.f and hence an induced current.
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9
Q

A.c generator part 2

A
  • Slip rings are always in contact with the carbon brushes as the axle rotates. The slip rings Ensure that the induced current in the coil is transferred to the external circuit.
  • The induced current powers the electrical load connected to the external circuit, lighting up the lamp.
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10
Q

Output voltage against time graph for simple a.c. generator .
Part 1

A

1) When the plane of the coil is parallel to the magnetic field, the arms AD and BC cut across the magnetic field lines at the greatest rate. Since the rate of change in magnetic flux is maximum, the magnitude of induced e.m.f is maximum

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11
Q

Output voltage against time graph for a simple a.c. Generator part 2

A

2) when the plane of the coil is perpendicular to the magnetic field, the arms AD and BC do not cut across the magnetic field lines. Since the rate of change of magnetic flux is 0, the magnitude of induced e.m.f is 0.

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12
Q

Output voltage against time graph for simple a.c. generator

Part 3

A

3) As the coil rotates half a cycle, it is parallel to the magnetic field again. The magnitude of induced e.m.f. is maximum. Note that since arms AD and CB are moving in directions opposite to those in step 1, the direction of induced e.m.f is opposite to that in step 1

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13
Q

Output voltage against time graph for simple a.c. Generator

Part 4 and 5

A

4) The arms AD and BC do not cut across the magnetic field lines. The magnitude of induced e.m.f is 0.
5) The coil has rotated 1 complete cycle. It is parallel to the magnetic field again. Hence, maximum induced e.m.f is produced

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14
Q

Fleming left hand rule and right hand rule

A

Left hand rule used for d.c. motors

Right hand rule used for a.c. Generators

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15
Q

We can increase the magnitude of the induced e.m.f of an a.c. Generator by:

A
  • Increasing the number of turns in the coil
  • Using stronger permanent magnets
  • Increasing frequency of rotation of coil
  • Winding the coil around a soft iron core to strengthen the magnetic flux linking the coil.
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16
Q

Practical design of a.c. Generator

Part 1

A

1) A magnet is attached to an axle and a wheel. As the wheel rotates, the magnet rotates too.

17
Q

Practical design of a.c. Generator

Part 2

A

2) The magnetic field rotates with respect to a fixed coil. This changes the magnetic flux in the coil. An induced e.m.f is generated and hence an induced current.

18
Q

Practical design of a.c generators

Part 3

A

3 ) The induced current is channelled directly to the external circuit through the output terminals. Slip rings and carbon brushes are not needed.

19
Q

A fixed coil a.c. Generator is favoured for the following reasons:

A
  • It does not require carbon brushes, which wear out easily and need to be replaced frequently.
  • It is Less likely to break down from overheating. This is as it does not use slip rings and carbon brushes. An eroded connection between slip rings and carbon brushes has increased resistance, which can generate large quantities of heat.
  • It is more compact
20
Q

What is a transformer?

A

A transformer is a device that can change high alternating voltage (at Low current) to a Low alternating voltage(at high current), or vice versa

21
Q

Transformers are used in:

A
  • Electrical power transmission from power stations to households and industries
  • Regulating voltages for the proper operation of electrical appliances
22
Q

Structure if transformer (Don’t really need to memorise except for important points)

A
  • The primary coil and the secondary coil are wound around a laminated soft iron core.
  • Each coil has a certain number of turns.
  • The laminated soft iron core comprises thin sheets of soft iron. These sheets are insulated from one another by lacquer.
  • Soft iron is used as it is easily magnetised and demagnetised. This ensures better magnetic flux between the 2 coils.
  • The lamination reduces heat loss.
23
Q

How does a transformer work

A

1) The primary coil is connected to an alternating voltage- the input voltage Vp
2) A varying magnetic field is set up in the laminated soft iron core.
3) An e.m.f. is induced in the secondary coil. This voltage is called the output voltage. Since the circuit is closed, a current is also induced in the coil.

24
Q

Formula for transformer

A
Vs/Vp= Ns/Np
Where;
Vs= secondary(output voltage)
Vp= primary(input voltage)
Ns=no. of turns in secondary coil
Np= No. of turns in primary coil.
25
What is a transformer?
A transformer is a device that can change high alternating voltage (at Low current) to a Low alternating voltage(at high current), or vice versa
26
Transformers are used in:
- Electrical power transmission from power stations to households and industries - Regulating voltages for the proper operation of electrical appliances
27
Structure if transformer (Don’t really need to memorise except for important points)
- The primary coil and the secondary coil are wound around a laminated soft iron core. - Each coil has a certain number of turns. - The laminated soft iron core comprises thin sheets of soft iron. These sheets are insulated from one another by lacquer. - Soft iron is used as it is easily magnetised and demagnetised. This ensures better magnetic flux between the 2 coils. - The lamination reduces heat loss.
28
How does a transformer work
1) The primary coil is connected to an alternating voltage- the input voltage Vp 2) A varying magnetic field is set up in the laminated soft iron core. 3) An e.m.f. is induced in the secondary coil. This voltage is called the output voltage. Since the circuit is closed, a current is also induced in the coil.
29
Formula for transformer
``` Vs/Vp= Ns/Np Where; Vs= secondary(output voltage) Vp= primary(input voltage) Ns=no. of turns in secondary coil Np= No. of turns in primary coil. ```
30
Step-up and step-down transformer
In a step up transformer, the number of coils in the secondary coil is greater than that in the primary coil. This results in an output voltage that is higher than input voltage. In a step down transformer, the number of coils in the secondary coil is less than that in the primary coil. This results in an output voltage that is lower than the input voltage.
31
Power transmission in a transformer.
Power in primary coil= power in secondary coil ``` VpIp=VsIs where; Vs= secondary(output) voltage Vp=primary(input) voltage Is=current in secondary coil Ip=current in primary coil ```
32
Comparing step-up and step-down transformers
Step up transformer Ns>Np Vs>VP IsIp
33
Efficiency formula
Efficiency= output power in secondary coil/input power in primary coil x100%
34
Transformers and the transmission of electricity | Possible solutions to minimise loss of power due to joule heating:
- Use very thick cables so that resistance is Low. In this way, power lost as heat is reduced. However, thicker cables increase cable and construction costs. - Reduce magnitude of current flowing in the cables. This can be done with a step- up transformer. When the transmission voltage is stepped up, current in cables is stepped down.
35
Power output and power loss
P out= VI | P loss=I square R
36
The function of step down and step up transformers
As electricity is transmitted more efficiently at high voltages, electricity produced in power stations has its voltage stepped up by the step up transformers. The high voltage electricity is then transmitted to households and industries through transmission cables. Step down transformers then reduce the voltage to suitable values, so that households and industries can use electricity safely.