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Automotive mechanics (volume i)(part 6, chapter36) effects and applications of electric currents

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Nội dung

Effects and applications of electric currents 635 Effects of an electric current 636 Heating effect of a current 636 Chemical effect of a current 637 Magnetic effect of a current 638 Theory of magnetism 638 Electromagnetism 640 Solenoids and electromagnets 641 Electromagnetic switches (relays) 643 Electrical measuring instruments 644 Electromagnetic induction 645 Electric motors 648 Direct and alternating current 649 Technical terms 649 Review questions 649

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Effects and applications

of electric currents

Chapter 36

Effects of an electric current

Heating effect of a current

Chemical effect of a current

Magnetic effect of a current

Theory of magnetism

Electromagnetism

Solenoids and electromagnets

Electromagnetic switches (relays)

Electrical measuring instruments

Electromagnetic induction

Electric motors

Direct and alternating current

Technical terms

Review questions

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This chapter deals with the effects that are produced by

an electric current and shows how these apply to

various electrical components of a motor vehicle.

One of these is magnetism This has applications in

many parts of the electrical system, so an appreciation

of magnetism is particularly helpful in understanding

the operation of various electrical components and

devices.

Effects of an electric current

Three different effects can be produced by an electric

current, and all three of these have automotive

applications Generally, the effects are used to

advantage, but sometimes they are unwanted and

have to be removed, or precautions are taken to

prevent them from becoming excessive The three

effects are:

1 heating

2 chemical

3 magnetic.

Of these three effects, the magnetic effect is the

most extensively used in automotive electrical

systems.

Heating effect of a current

Any conductor that carries an electric current will

become heated as a result of the current flow.

The heat produced and the temperature rise in the

conductor will depend on the material of which the

con-ductor is made, the size of the concon-ductor and the rate at

which current flows in the conductor.

The conductors in an automotive electrical system

do not normally produce enough heat to cause

problems This is because the system is designed with

conductors (cables) of a suitable size for the particular

current that they will have to carry.

However, problems can arise if part of the system is

overloaded or if connections and terminals are not

clean and tight A loose or dirty electrical connection

can cause a high resistance, which will produce

unwanted heat and also cause voltage drop.

Figure 36.1 shows a number of cables Where large

currents are used, such as in starter motor circuits,

large cables are required These prevent excessive

voltage drop and are able to carry the starter current

without overheating In other circuits, which have

much lower currents, small cables are adequate.

Applications of heating effect

Applications of the heating effect of a current are outlined under the headings that follow.

Lamps

The heating effect of an electric current is used in light bulbs Current passing through the bulb filament causes it to become white hot and this produces light.

Fuses

Excess current passing through a fuse will cause it to overheat to the extent that it ‘blows’ by melting the fuse wire Fuses and fusible links are used as protec-tive devices to prevent overheating of circuits There are a number of designs of fuses; one type is shown in Figure 36.2.

figure 36.1 A range of electrical cables – heavy cables

are used for high currents to prevent over-heating and voltage drop

figure 36.2 A fuse provides protection by melting when it

is overheated by excess current

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Glow plugs

In some diesel engines, glow plugs and heater plugs

are used as starting aids These contain elements that

are electrically heated by passing a current through

them In turn, they heat the air or fuel mixture around

them.

Switches

Heat-operated controls and switches function by means

of the heating effect of the current that they carry.

Switches of this type have one of their contacts

mounted on a bimetal blade which normally holds the

contacts closed (Figure 36.3) The contacts are opened

by the heating effect of the current passing through the

blade which causes it to distort This occurs whenever

the blade reaches a predetermined temperature As the

blade cools, it resumes its normal shape and this closes

the contacts.

Switches and controls of this type, which are

sensitive to heat and current flow, are used as circuit

breakers to protect circuits from excessive current The

principle is also used in some flasher lights where an

intermittent current is required.

positive ions move through the electrolyte to the cathode, which is the negative electrode, and the negative ions move to the anode, which is the positive electrode.

Action of electrolysis

The action of electrolysis not only enables current to flow in a liquid, but it can also deposit material from the anode onto the cathode The extent to which this occurs will depend on the material of the electrodes and the type of electrolyte.

The process of electroplating uses this principle to deposit plating material from the anode onto the article being plated, which is arranged as the cathode In this process, the material of the anode gradually erodes away as it is being deposited on the cathode.

Electroplating is a controlled process, but electrolysis can exist where it is not wanted, taking place wherever there are two dissimilar metals and moisture or impure water The dissimilar metals have different electrical potential, so one becomes the anode and the other the cathode The moisture acts as an electrolyte, and over a period of time, material is gradually removed from the anode.

Electrolysis and cooling systems

The conditions outlined above exist in an engine’s cooling system, where cast iron of the cylinder block, aluminium alloy of the cylinder head, and water are present Electrolysis can occur in the cooling system and cause corrosion of the water-jackets and passages.

For this reason, distilled or deionised water, which

is practically free of chemicals, is used in cooling systems, together with special chemical additives.

figure 36.3 Thermal switch with a bimetal arm

figure 36.4 Electrolysis – a chemical effect of an electric

current

Chemical effect of a current

Some liquids, such as water with a small quantity of

acid, will conduct an electric current, and this will

produce a chemical action The conductors that are in

contact with the liquid are known as electrodes, and

the liquid is known as an electrolyte The chemical

action that occurs is called electrolysis (Figure 36.4).

With electrolysis, conduction in the electrolyte is

by movement of ions, which are atoms carrying

positive or negative charges When a current flows, the

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The chemical effect of current flow can also be related

to batteries Automotive batteries consist of a number

of cells These are referred to as lead-acid cells

because they consist basically of lead plates immersed

in an acid solution (electrolyte) The cells store

electrical energy in chemical form.

When current is flowing from the battery, chemical

energy is being converted to electrical energy When

current is supplied to the battery, the battery is being

charged and electrical energy is being converted to

chemical energy.

Batteries are covered separately in Chapter 38: The

battery.

Magnetic effect of a current

Current flowing in any conductor produces a magnetic

effect and this is used in many ways in automotive

components In fact, magnetism is so closely

associated with electricity that a knowledge of the

principles of magnetism is essential in order to

understand the operation of many of the electrical

devices which are fitted to motor vehicles.

Some of the electrical components that involve

magnetism in their operation are the starter motor,

alternator, ignition, horn, windscreen wipers, and

instruments.

Magnets

A permanent magnet is a piece of special alloy steel

that has the property of attracting other magnetic

materials Magnets can be made in a variety of shapes,

the common types being bar magnets and horseshoe

magnets (Figure 36.5).

Magnetic materials are those containing iron.

Metals such as aluminium and copper are

non-magnetic.

Magnetic polarity

The compass needle is a familiar example of a magnet.

This is a small permanent magnet, lightly suspended

on a pivot, which always locates itself in a direction N

and S, being attracted in this direction by the magnetic

north pole of the earth Because of this, the end of the

magnetic needle pointing to the north is referred to as

the north pole and the other end as the south pole.

The attractive force of a magnet is concentrated at

its ends This can be seen by dipping the magnet in iron filings The filings will be attracted to the ends, and not to the other parts of the magnet (see Figure 36.5) This demonstrates the magnetic force at the poles.

Attraction and repulsion

Magnets not only attract other magnetic materials, but they will also attract and repel other magnets If two magnets are placed with their unlike poles opposite (N facing S), then they will be attracted to each other as shown in Figure 36.6 When magnets are placed with like poles opposite (N facing N, or S facing S) they will repel each other.

The rule for magnetic attraction is – unlike poles attract, like poles repel.

figure 36.5 The poles at the ends of the magnets attract

iron filings

figure 36.6 Unlike poles of a magnet attract each other

whereas like poles repel

Theory of magnetism

A suitable theory for magnetism supposes that every magnet is made up of a number of minute magnetic particles In an unmagnetised piece of iron or steel, these particles are arranged in such a way that their

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poles form closed magnetic loops, thereby neutralising

one another, so that no magnetic effect is evident

(Figure 36.7).

When a piece of steel is magnetised, the magnetic

particles are rearranged, so that their poles are all

aligned in the same direction to produce the effect of

N and S poles at the ends of the bar, which becomes a

magnet.

To continue this idea a little further, it can also be

presumed that the particles are easy to arrange in some

materials and more difficult in others Iron and mild

steel are easy to magnetise because their particles will

arrange easily, while hard and special steels are

difficult to magnetise because their particles are hard

to disturb.

On the other hand, iron and mild steel, which

magnetise easily, also lose their magnetism quickly.

Hard steels, once magnetised, will retain their

magnetism.

A material that can be easily magnetised is referred

to as being susceptible to magnetism, while a material

which, once magnetised, retains its magnetism is said

to have the property of retentivity.

A material cannot have both these properties Iron

has the property of susceptibility which makes it most

useful as an electromagnet, or as a temporary magnet,

while special steels have the property of retentivity

which makes them suitable for permanent magnets.

If a piece of unmagnetised steel is brought within the influence of the magnetic field, it also will become magnetised, but not as readily as the soft iron.

Residual magnetism

When the piece of soft iron or steel is removed from the influence of the magnet, it becomes demagnetised, but there is a very weak magnetic effect that remains This is called residual magnetism Almost every magnetic material has the property of residual magnetism to some degree and it is made use of in some electrical devices.

Magnetic field

The magnetic field is the space surrounding the magnet

in which a magnetic force may be detected It is considered to be made up of a number of magnetic lines of force, which represent the field by showing the direction in which a north pole would move if it were free to do so.

The magnetic field can be demonstrated in various ways, such as by plotting the positions of the north end

of a compass needle as it is moved within the field, and also by the use of iron filings scattered over a sheet of glass or paper placed on top of a magnet.

From various experiments, the magnetic lines of force are found to have the following properties (Figure 36.9):

1 They go from the north to south outside the magnet, and from south to north within the magnet.

2 They repel each other sideways, and do not cross.

3 They tend to crowd through magnetic materials placed in the field.

4 They are not affected if non-magnetic materials are placed in the field.

Magnetic flux is a term that can be used instead of lines of force It is used to represent all the lines

of force in a magnetic field.

figure 36.7 Arrangement of magnetic particles in a steel

bar

figure 36.8 Magnetic induction – a piece of soft iron

becomes an induced magnet only while it is within the magnetic field of the permanent magnet

Magnetic induction

Magnetism can be induced from a magnet into an

unmagnetised piece of soft iron to make a temporary

magnet This is called magnetic induction.

If a piece of soft iron is brought close to a magnet,

it will become an induced magnet, as long as it

remains within the influence of the magnetic field of

the magnet It will lose its magnetism the instant that it

is removed from the magnetic field (Figure 36.8).

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Whenever a current flows in a conductor, a magnetic

field is set up around the conductor This effect is

known as electromagnetism.

This means that any wire, or conductor of any type,

will have a magnetic field if current is flowing through

it In most cases, this is only a weak field and is of

little importance, but when a strong magnetic field is

required, the wire can be wound into a coil with many

turns to concentrate the effect and so produce a very

strong magnetic field.

To demonstrate this basic principle, on which

further principles depend, a small experiment can be

used If a piece of wire is connected to a battery (with

a resistance in series to prevent excessive current), the

current flow will produce magnetic lines of force

around the wire as shown in Figure 36.10.

If a compass is brought close to the wire, the

compass needle will be deflected by the lines of force, and will assume a position at right angles to the wire as shown in Figure 36.11 From this, it can be concluded that magnetic lines of force do exist and that they are

in a circular direction around the wire.

figure 36.9 Magnetic fields of a bar magnet

figure 36.10 Magnetic lines of force around a conductor

figure 36.11 Compass needles are deflected by lines of

force – this is the basic principle of electrical measuring instruments

magnetic needle turns at right angles to wire when current flows.

magnetic needle

Simple measuring instrument

The arrangement of a compass needle, in conjunction with a conductor carrying a current, is the basic principle of electrical measuring instruments When the current flows, the needle deflects; when the current

is stopped, the needle returns to its original position This indicates that the magnetic field is present only when the current is flowing.

If the compass needle was provided with a spring

to limit its deflection, then it could also be used to indicate the strength of the magnetic field It would be found that the field strength would increase and decrease in proportion to current flow.

Current flow therefore provides a means of varying the strength of an electromagnet and this can be summarised as follows:

1 No current – no magnetic field.

2 Small current – weak magnetic field.

3 Large current – strong magnetic field.

Effect of current direction

The direction of current flow in a conductor will affect the lines of force With the current flowing from left to right, as shown in Figure 36.10, the lines of force will

be clockwise around the conductor.

The north end (shaded end) of the compass needle

in Figure 36.11 also indicates this by pointing in the direction in which a north pole of the field would move.

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If the direction of the current in the conductor was

reversed, then the lines of force would also reverse

their direction around the conductor The compass

needle would swing around and point in the opposite

direction.

Figure 36.12 shows two conductors with current

flowing in opposite directions In Figure 36.12(a), the

direction of current is shown by a cross, representing

current flowing away from us to produce a clockwise

field In Figure 36.12(b), the direction of current is

shown by a dot, representing current flowing towards

us to produce an anticlockwise field.

The current direction is shown by an arrow The

cross (x) represents its tail and the dot (•)

represents its point.

Magnetic field of a coil

The field around a wire can be concentrated by

winding the wire into a coil The small fields

surrounding each part of the wire will then combine to

form a strong field which can serve a useful purpose.

Coils are used in many practical electrical devices.

A section through a coil is shown in Figure 36.13.

The direction of current flow in the parts of the coil is

shown by crosses and dots The lines of force that

circle the wire are in opposite directions on each side

of the coil.

On the left-hand side, the current is flowing away

from us to produce a field in a clockwise direction On

the right-hand side, the current is flowing towards us,

so that the field is in an anticlockwise direction.

The fields on each side of the loop will combine because their lines of force are moving in the same direction Figure 36.14 shows this for the two loops

of the right-hand side of the coil, and how the fields of the two conductors have combined to form a stronger field.

If a number of loops of wire are used in the coil, then the fields of all these will combine in a similar manner to produce a strong field similar to a permanent bar magnet The lines of force will be in

a direction from N to S outside the coil, and S to N inside the coil (Figure 36.15).

If the direction of current in the coil is reversed, then the polarity of the electromagnet will also be reversed.

figure 36.12 Field surrounding two conductors

(a) current flowing away, field is clockwise (b) current flowing towards, field is anticlockwise

figure 36.13 Section through a coil showing the field

around each conductor

figure 36.14 Parallel conductors with the current in the

same direction have a combined field (this is the right-hand side of the coil of the previous figure)

figure 36.15 Field of a coil shown with iron filings – this is

similar to the field of a bar magnet

Solenoids and electromagnets Solenoids

A solenoid is a particular arrangement of an electro-magnet It is a coil consisting of a series of turns of

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insulated wire wound on a hollow cylindrical former

made of non-magnetic material.

When current passes through the solenoid, it

produces a magnetic field as previously described,

with a north and south pole at its ends.

The strength of the magnetic field of a solenoid can

be increased by:

1 Increasing the number of turns of the wire.

2 Increasing the current flowing through the wire.

This means that, to produce a magnetic field strong

enough for practical use, either a large number of turns

of wire are used or a heavy current is required In

practice, both these methods are used.

Electromagnets

If a coil is wound around a piece of soft iron, or a piece

of iron is placed in a solenoid, then the soft iron will

become a magnet while the current is flowing The

windings produce a magnetic field, and also arrange

the magnetic particles of the soft iron to form a

magnet.

When the current flow is stopped, the field around

the coil will collapse and the iron core will be

demagnetised because the magnetic particles will no

longer be under the influence of the electromagnetic

field.

Electromagnets can be found in various forms in

many parts of the motor vehicle and the starter,

alternator, ignition, and instruments are some of the

components that make use of the principle of an

electromagnet.

Where the coil is wound directly on to a soft-iron

core, this is known as an electromagnet Where the

coil is hollow, it is referred to as a solenoid.

Figure 36.16 shows a practical application of

electromagnetism This is a simplified arrangement

of an alternator rotor, which consists of a field coil

mounted inside a pair of claw-shaped iron poles The

coil has a large number of turns of wire and is able to

produce a strong magnetic field.

Because one end of the coil is a north pole and the

other a south pole, the rotor becomes an electromagnet

and the claws become alternate north and south poles

as shown.

The strength of the magnetic field can be varied by

altering the current flowing in the coil, and this is the

method that is used to control the output voltage of

the alternator.

Coils of electromagnets

Figure 36.17 illustrates two electromagnets of the type used in switches and relays The coil in Figure 36.17(a) has a few turns of heavy-gauge wire, while the coil in Figure 36.17(b) has many turns of light-gauge wire It is necessary to consider the manner in which these become electromagnets.

The strength of an electromagnet depends on the ampere-turns This is the product of the current (in amperes) and the number of turns in the coil There-fore, the two coils referred to above may be different

in design, but could still have the same number of ampere-turns, and the same field strength.

figure 36.16 Simplified alternator rotor – the field coil is

an electromagnet which magnetises the field poles

figure 36.17 Coils of electromagnets

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Series coil

The coil in Figure 36.17(a) has a few turns of heavy

wire As a result of the short length of wire and

comparatively large cross-section of the wire, this coil

has a very low resistance.

Such a coil cannot be connected directly across the

battery or alternator, as damage would be caused by

the excessively high currents that would result.

This coil requires some form of load or resistance

connected in series with it to limit the current, and is

therefore referred to as a series coil Because of its few

turns, a high current is needed to produce a useful

electromagnetic field.

Shunt coil

The coil in Figure 36.17(b) has many turns of fine wire

(more than shown) As a result of the long length of

wire and its small cross-sectional area, this coil will

have a comparatively high resistance.

Because of its high resistance, this coil can be

connected directly across a battery or alternator It will

not burn out, as its resistance allows only a low current

flow However, because of the large number of turns

of wire and the fact that each turn provides some

magnetic lines of force, this coil will produce a strong

field It is often referred to as a voltage coil or a shunt

coil because it is connected in parallel with the

alternator or battery.

Being connected in this way makes the coil

responsive to any variation in voltage An increase in

the voltage applied to the coil will cause an increase

in current through the windings and a corresponding

increase in the strength of the electromagnet Any

decrease in the voltage will have the opposite effect.

Some voltage regulators use a coil in this way to

regulate the alternator voltage.

Electromagnetic switches (relays)

Figure 36.18 illustrates the principle of an

electro-magnetic switch This is also referred to as an

electromechanical switch, but is usually called a relay.

A relay consists of an electromagnet, with a

soft-iron armature pivoted to open and close a set of contact

points When a control switch is closed to connect the

battery to the coil, current energises the coil windings.

The magnetised core attracts the armature and the

contact points close When the control switch is open,

the coil is no longer energised and the contact points

are opened by the spring.

This arrangement could be used to operate the

headlamps The contact points are used to connect the headlamp to the battery by a much more direct circuit than through the headlamp switch on the steering column The relay is mounted close to the headlamps, with heavier and shorter wire, which reduces voltage drop The headlamp switch is used only to control a low current to operate the relay.

There are many relays used on a motor vehicle They are used in the circuits for horns, lights, fans and many other components.

Some relays are designed to close their points when energised, others are designed to open their points when energised.

Solenoid switch

The basic principle of a starter solenoid switch is illustrated in Figure 36.19 The coil is energised when the driver turns the ignition switch to the start position and this attracts the soft-iron plunger further into the hollow solenoid The copper disc bridges across the contacts to complete the starter circuit and operate the starter motor.

The solenoid switch is mounted on the starter (Figure 36.20) and a small current from the start switch closes the large switch contacts of the solenoid This provides a remote control where a small switch is able

to operate the starter.

The starter solenoid actually performs two functions As well as switching, it operates a lever that

figure 36.18 Diagram of an electromagnetic switch or

relay

control switch

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moves the starter pinion into mesh with the ring gear

on the flywheel.

Electrical measuring instruments

A compass needle placed in the magnetic field of a

conductor represents the basic principle of most

measuring instruments This was previously discussed

in relation to Figure 36.11 Now, the basic construction

of a workshop measuring instrument is illustrated in

Figure 36.21.

Ammeters and voltmeters both operate on the same

principle and their construction is basically the same as

far as the working parts of the instrument are

concerned The basic instrument is known as a

galvanometer and it is used to detect the flow of an

electric current The manner in which the

galvano-meter is arranged determines whether it will be a

voltmeter or an ammeter.

Moving-coil meter

The instrument shown (see Figure 36.21) is known as a moving-coil meter It has a permanent horseshoe magnet, with a small coil of fine wire suspended lightly between the poles of the magnet on two fine spiral springs A needle, or pointer, is attached to the coil, and a suitable scale is provided on the face of the instrument to show the deflection of the needle.

Operation

When there is no current passing through the coil, the spiral springs locate the coil so that the pointer registers with the zero on the scale.

When current passes through the coil, an electro-magnetic field is produced by the coil, which reacts with the field of the permanent magnet This causes the coil to rotate a few degrees against the tension of the springs, moving the pointer across the scale The amount of deflection will depend on the strength of the field of the coil The field, in turn, will depend on current flow The scale is graduated to suit this so that the pointer shows the current flow.

A galvanometer such as this will read only very small currents, and so cannot be used as a workshop instrument in this basic form.

Instruments with pointers operate magnetically and are known as analog meters, but there are digital meters which operate electronically.

Ammeter

An ammeter (Figure 36.22(a)) consists of a galvano-meter with a shunt The shunt, which has a very low resistance, is connected in parallel with the moving coil of the meter, so that most of the current being measured bypasses the moving coil via the shunt This

is a simple parallel circuit.

The current being measured will branch in the instrument and only a small current will pass through

figure 36.19 Principle of a solenoid switch

figure 36.20 The starter solenoid is mounted on top of the

starter motor where it acts as a switch and also moves the pinion into mesh

figure 36.21 Basic construction of an electrical measuring

instrument

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