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Programme 19: Circuits
Background Information
Meaning of Electricity
It is unfortunate that when scientists first realised that
electricity was a flow of charges they accepted a model in which
positive charges travelled from the positive terminal of a power
supply to the negative terminal. When the charge-carrying particle,
the electron, was eventually discovered it was found to have a
negative charge and to travel from the negative terminal of the
power supply to the positive terminal. This is why the direction of
conventional current flow is opposite to the actual flow of
electrons. Students sometimes ask why this was not corrected at the
time. By the time electrons were discovered electricity had moved
out of the laboratory and into everyday life. It would have been
difficult to get people to change, and would have been potentially
dangerous if machines were connected the wrong way round.
Differences in Series and Parallel Circuits
There are three main differences between series and parallel
circuits:
- Adding more components in series reduces the current in the
circuit. Adding more components in parallel draws more current from
the supply so that the current through each one is unchanged.
- If one component fails in a series circuit there is no current
through any of the components. In a parallel circuit the other
components are unaffected.
- Components must all be switched on and off together in series,
but can be switched on and off individually in parallel.
Note that when adding more components in parallel if the power
supply is current limited (has a maximum current which can be
drawn), once the maximum is reached then adding more components
will lead to a reduction in current through each component.
Ohm’s Law
Ohm’s Law says that voltage (V) is directly
proportional to current (I) for a conductor provided that its
temperature remains constant. If V is directly proportional
to I, a graph of V (in volts), against I (in
amps), will be a straight line through the origin. Resistance
increases with temperature, and if the conductor warms up, due to
the current flowing through it, the graph will not be a straight
line. The constant of proportionality is called resistance
R, so V = RI where R is the gradient of
the graph. R is a measure of how difficult it is for
electrons to flow through the material. It is measured in ohms
(W).
It is usual to plot the dependent variable (in this case
I) against the independent variable (in this case V).
In the case of Ohm’s Law, graphs are plotted of V
against I so that the gradient gives R and not
1/R. Some devices and materials do not obey Ohm’s law,
for example, thermistors.
Filament lamps are designed to heat up even at low voltages, so
that the filament gives out light. The filament wire would follow
Ohm’s law if the temperature was constant. At very low
voltages the lamp may start off with V proportional to
I, but it quickly heats up. Since it can’t be kept at
constant temperature and is designed to heat up, we refer to
filament lamps as non-ohmic.
Resistance
Resistance is shown to depend on the type of metal. The metal is
shown to be a lattice of positive metal ions surrounded by a sea of
free electrons. One reason why different metals do not have the
same resistance is that they contain a different number of free
electrons. There are other reasons, such that the positive ions
vibrate with different amplitude or frequency for different
metals.
Resistance is proportional to the length of the wire –
doubling the length doubles the resistance.
Resistance also depends on the thickness of the wire. It is
actually inversely proportional to the cross-sectional area of the
wire: as the area doubles the resistance halves. This is
demonstrated by using two wires to double the area (doubling the
diameter of a circular cross-section wire would give four times the
area and so one quarter of the resistance).
Temperature
Temperature affects resistance because it changes the vibration
of the positive ions in the lattice. It is more difficult for the
electrons to flow through a wire if the ions are vibrating more.
This means that resistance increases with temperature. The
demonstration shows that resistance decreases when materials are
cooled. The superconductor is a ceramic which becomes
superconducting at liquid nitrogen temperatures
(–196°C). When a magnet is moved close to the
superconductor, currents will be induced in the superconductor (by
induction), to oppose the movement of the magnet. These currents
will not die away due to resistance as they do in most materials,
because the superconductor has no resistance. They will continue to
provide a magnetic field which repels the magnet.
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