Wrap the conductor wire around a former to create a coil and each turn of the
wire will lie adjacent to the turns around it. This sets up a complex
electromagnetic system - a combination of 'ordinary' resistance, self-inductance
and the capacity of the circuit, all of which acts as a 'brake' to the current, impeding its
progress. This is roughly where the term impedance comes from. Impedance is
measured in ohms although the symbol for impedance is Z.
With a loudspeaker, the coil is wrapped around a
thin former which slides freely over the pole of a permanent magnet. The
changing signal through the speech coil is translated into movement of the coil
due to magnetic attraction/repulsion (remember from schooldays - like poles
repel, opposites attract). The movement is linked to the loudspeaker cone to
create sound.
With the transformer, inductive coupling from
one winding (the primary) to another (the secondary) not electrically connected takes place, transferring the
AC current. Altering the primary-secondary turns ratio allows increases or
decreases in voltage obtained. This is known as step-up or step-down. 1-1
transformers are often called 'isolation' transformers as they give a measure of
protection due to the finite limit of current available from the secondary. AC
only sets mostly, but not entirely, use transformers both to step up and to
isolate from the mains.
IF transformers couple inductively but are tuned
circuits, the tuning being either capacitive across the coil or, far more
often, by metal or iron-dust core within the former.
Chokes act as low-ohms resistors to the
rectified mains power, working together with reservoir capacitors, limiting the
remaining AC ripple but allowing the DC component to flow virtually unimpeded.
Tuning coils have parallel capacitors to form
'tuned' circuits. In any tuned circuit, capacitive reactance falls as the frequency rises.
Inductive reactance rises as the frequency rises. The falling reactance of the
capacitor meets the rising reactance of the inductor at a frequency determined
by the values of both. At the coincident point the circuit is said to be in
resonance, resulting in the magnification of any transmitted signal at that frequency.
The magnification obtained by any given inductance is termed its 'Q' value.
Such
resonant points may be quite 'sharp' and excessively sharp resonance may result
in unwanted effects such as instability or severe sideband limiting, the latter
resulting in poor quality sound, lacking 'top'. Careful component design can
combat this problem but sometimes it is necessary to dampen the peak by fitting
a parallel resistance across the inductance, or by staggering the peak points
where two or more transformer stages are in use, for example the IF
circuitry in television receivers where there are several IF amplifying stages
in series.
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