|
Tuned
circuits
in
radios
have one
severe
limitation
-
bandwidth.
Without
going
into a
complex
explanation
let us
assume
that the
best
response
can be
about 2%
of the
signal
frequency.
In the
early
days of
a.m.
radio,
circuits
simply
tuned
straight
across
the
frequency
band of
interest.
Applying
our 2%
rule we
find at
say 540
Khz, the
bandwidth
is 10.8
Khz. We
would be
able to
receive
this
signal
without
a great
deal or
little
interference
from
adjacent
channels.
On the
downside
if we
wanted
to
receive
a signal
at say
1550 Khz
our
bandwidth
becomes
31 Khz
or
spanning
3
channels.
We would
have
little
hope of
satisfactorily
receiving
a signal
because
our
bandwidth
also now
includes
both
adjacent
channels.
A method
of
receiving
called
the 'superhetrodyne'
principle
evolved.
Here as
part of
our
receiver
we have
a 'local
oscillator'
or mini
transmitter
where
the
incoming
received
signal
is mixed
with the
local
oscillator.
As a
result 4
frequencies
become
available.
Firstly
the
original
signal,
(2) then
the
original
local
oscillator
signal,
(3) then
the
original
signal
plus the
local
oscillator
signal
and then
finally
(4) the
original
signal
minus
the
local
oscillator
signal.
Confused?.
Consider
this
practical
example
of your
little
transistor
a.m.
radio.
It is
designed
to
receive
about
540 -
1650 Khz.
The
local
oscillator
will
always
tune in
tandem
with the
input
section
to
produce
another
signal
at 995 -
2105 Khz.
At all
times
the
difference
frequency
is a
constant
455 Khz
or what
is
called
the
intermediate
frequency
or I.F.
All
other
frequencies
arising
from
this
process
are then
filtered
out.
When you
tune
your
radio
you are
actually
tuning
the
local
oscillator
which is
more
correctly
called
the 'V.F.O.'
or
variable
frequency
oscillator.
Because
we
always
have a
constant
difference
frequency
of 455
Khz it
is
relatively
easy to
design
and
construct
narrow
band
circuits
to suit
our
requirements.
It is in
these
circuits
(I.F.
Amplifier)
that the
greatest
amplification
occurs.
|