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Electromagnetic Induction

Electromagnetism is the effect resulting from the interaction between an electric current and a magnetic field. When a conductor is placed between the magnetic field or moved through the magnetic field it generates voltage i.e., electricity  . this resulting current is called induced current. This principle is called Electromagnetic Induction. The voltages generated will be based on the speed of the conductor moving through the magnetic field. Faster the speed of the conductor, the greater the induced electricity or voltage.

Experiments on electromagnetic induction

 Consider the following diagram

  When the wire is moved up the galvanometer deflects in one direction then the opposite direction when moved downwards.

When moved horizontally or held in a fixed position there is no deflection in the galvanometer.

This shows that e.m.f is induced due to the relative motion of the wire or the magnet

 Factors affecting the magnitude of the induced e.m.f

1. The rate of relative motion between the conductor and the field – if the velocity of the conductor is increased the deflection in the conductor increases.
2. The strength of the magnetic field – a stronger magnetic field creates a bigger deflection
3. The length of the conductor – if the length is increased in the magnetic field the deflection increases.

Faraday’s Law of Magnetic Induction

After considering the factors affecting the magnitude of the induced e.m.f, Michael Faraday came up with a law which states that “The induced e.m.f in a conductor in a magnetic field is proportional to the rate of change of the magnetic flux linking the conductor”.

 Lenz’s law of electromagnetic induction

This law is used to determine the direction of the induced current in a conductor. It states that “An induced current flows in such a direction that its magnetic effect opposes the change through which the current has been produced”.

It is applied similarly when a wire is been moved in magnetic field.

 Fleming’s right hand rule.

The law states that “The first finger, the second finger and the thumb of the right hand when placed mutually perpendicular to each other, the first finger points in the direction of the field and the thumb in the direction of motion then second finger points in the direction of the induced current”. This law is also called the generator rule.

• Applications of electromagnetic induction

1. A.c generator/alternator – a generator is a device which produces electricity on the basis of electromagnetic induction by continuous motion of either a solenoid or a magnet.

• It consists of an armature made of several turns of insulated wire wound on soft iron core and revolving freely on an axis between the poles of a powerful magnet.
• Two slip rings are connected to the ends of the armature with two carbon brushes rotating on the slip ring.
• ·
• In an external circuit the current is at maximum value at 900 and minimum value at2700.

This brings about alternating current and the corresponding voltage (e.m.f) is the alternating voltage. They are used in car alternators and H.E.P.

• 2. D.c generator/alternator – in this case the commutators replaces the slip rings to enable the output to move in one direction.
• After a rotation of 1800, instead of current reversing, the connections to the external circuit are reversed so that current direction flows in one direction.
• ·
• 3. Moving coil microphone – it consists of a coil wound on a cylindrical cardboard which opens into a diaphragm. The coil is placed between the poles of a magnet as shown.
• 
• As sound waves hit the diaphragm, they vibrate and move the coil which produces induced current into the coil and then it flows to the loudspeakers.

Eddy currents

• They are composed of loops of current which have a magnetic effect opposing the force producing them.
• When a copper plate with slits is used the loops are cut off and hence the effective currents are drastically reduced and so is the opposing force.

 Practically eddy currents are reduced by laminating metal plates. Armatures of electric generators and motors are wound on laminated soft iron cores.

The lamination slices, which are quite thin are glued together by a non-conducting glue and this reduces eddy currents to an almost negligible value.

Eddy currents are useful in moving coil meters to damp the oscillations of the armature when the current is switched off.

Mutual induction

Mutual induction is produced when two coils are placed close to each other and a changing current is passed through one of them which in turn produces an induced e.m.f in the second coil. Therefore mutual induction occurs when a changing magnetic flux in one coil links to another coil.

 Applications of mutual induction

1. The transformer – it converts an alternating voltage across one coil to a larger or smaller alternating voltage across the other. Since H.E.P is lost through transmission lines therefore it is stepped down before it being transmitted and stepped up again at the point of supply lines.

In a step up transformer the number of turns in the secondary coil (Ns) is higher than the number of turns in the primary coil (Np).

 In a step down transformer the primary coil has more turns than the secondary coil.

The relationship between the primary voltage and the secondary voltage is given by;

 Np / Ns = Vp / Vs.The efficiency of a transformer is the ratio of power in secondary coil (Ps) to power in primary coil (Pp), therefore efficiency = Ps / Pp × 100%.

Examples

1. A current of 0.6 A is passed through a step up transformer with a primary coil of 200 turns and a current of 0.1 A is obtained in the secondary coil. Determine the number of turns in the secondary coil and the voltage across if the primary coil is connected to a 240 V mains.

Solution

 Np / Ns = Vp / Vs = Ip / Is = Ns = (0.6 × 200) / 0.1 = 1200 turns

  Vp = 240 V hence Vs = (240 × 1200) / 200 = 1440 V

2. A step-up transformer has 10,000 turns in the secondary coil and 100 turns in the primary coil.

 An alternating current of 0.5 A flows in the primary circuit when connected to a 12.0 V a.c. supply.

1. a) Calculate the voltage across the secondary coil
2. b) If the transformer has an efficiency of 90%, what is the current in the secondary coil?

 Solution

1. a) Vs = (Ns / Np) × Vp = (10,000 × 12) / 100 = 1200 V
2. b) Power in primary = Pp = Ip × Vp= 5.0 × 12 = 60 W

 Efficiency = Ps / Pp × 100% but Ps = Is Vs

Is = (60 × 90) / (1200 × 100) = 0.045 A

Energy losses in a transformer.

 Loss of energy in a transformer is caused by;

1. i) Flux leakage– this may be due to poor transformer design
2. ii) Resistance in the windings–it is reduced by using copper wires which have very low resistance

iii) Hysteresis losses– caused by the reluctance of the domains to rotate as the magnetic field changes polarity. Reduced by using materials that magnetize and demagnetize easily like soft iron in the core of the transformer.

1. iv) Eddy currents– reduced by using a core made of thin, well insulated and laminated sections.

  Uses of transformers

1. Power stations – used to step up or down to curb power losses during transmission
2. Supplying low voltages for school laboratories
3. Low voltage supply in electronic goods like radios, TVs etc.
4. High voltage supply in cathode ray oscilloscope (CRO) for school laboratories.
5. Induction coil –was developed in 1851 by Heinrich Ruhmkortt. It has both secondary and primary coils with an adjustable spark gap.
6. Car ignition system – it is applied in petrol driven engines where a spark plug is used to ignite petrol vapour and air mixture to run the engine.