4.1 VOLTS AND AMPS
In Figure 1.4 the electron flow was maintained by a
‘pump’ or generator in an anti-clockwise direction, but, because of a
historical mistake, current was deemed to flow in a clockwise direction.
In an equivalent water circuit, the pump delivers a pressure
(measured in psi, kgf/cm2 or bars), and the water flow is measured
in gal/min, or m3/s or other unit.
So for an electric circuit. Pressure is measured in VOLTS (after Volta,
the early Italian experimenter) and current in AMPERES (after an early French
pioneer). Instruments are made which
indicate pressures in volts and currents in amperes - all switchboards have
voltmeters and ammeters.
On platforms and large installations pressures tend to
be very high, involving thousands or tens of thousands of volts. In those cases the ‘kilovolt’ (equals one
thousand volts) is usually taken as the unit of pressure. Thus on most platforms the main generation
pressure is 6.6kV, or 6.6 thousand volts.
For domestic appliances and small services 440 or 250 volts is usual on
platforms and 415 or 240 volts ashore.
4.2 CURRENT FLOW - OHM’S LAW
Once the units of pressure and current flow were
established, a German experimenter named Georg Simon Ohm discovered a very
important relationship between them.
It has already been seen that some materials (mainly
metals) allow electrons to move freely (but not all as freely as each other),
whereas others do not do so and tend to resist such movement - again some more
so than others.
Ohm discovered that, for a given
sample of material, the current flowing I
(in amperes) was directly proportional to the pressure applied V (in volts). In other words, for that given sample, the
ratio of voltage to current was constant:
V
|
= const
|
I
|
This was true for any one sample, but the constant itself differed
from sample to sample. The ratio is
called the ‘resistance’ of that sample, symbol R. It can be considered as
opposition to the flow of electrons - like friction.
Ohm’s Law can then be stated:
V
|
=
|
R
|
|
I
|
|||
or
|
V
|
=
|
IR
|
where R is the resistance of the sample and differs from sample to
sample. If V is measured in volts and I
in amperes, R is measured in ‘ohms’.
4.3 HEATING
An important result stems from this. Since the resistance R of a conductor is akin to friction in the mechanical equivalent,
it might be expected that loss of energy by heating might result from a current
flow.
This indeed is so.
Whenever current is forced by pressure of voltage to flow through a
conductor which has resistance (and all conductors do, even metals), heat is
generated in that conductor. The rate of
heat generation is proportional to the resistance (in ohms) and to the square of the current (in amperes
squared). That is to say, the heat
generated is I2R, and, since
it represents a continuing loss of energy, it is expressed in the energy-rate
unit ‘watts’ (W).
It is important to remember that current flowing in any conductor, be it cable, generator,
motor or transformer, gives rise to heat, which must be conducted away if the
temperature is not to rise to a level which can damage the insulation and
possibly lead to flashover or breakdown and severe damage, or even danger to
life.
To reduce heat generation either the current (I) or the resistance (R) must be reduced (for example, by
increasing the cross-section of the conductor).
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