The carrier wave is a sine wave for almost
any communication system. A sine wave, of course, exists at only one frequency
and therefore occupies zero bandwidth.
As soon as the signal is modulated to
transmit information, however, the bandwidth increases. A detailed knowledge of
the bandwidth of various types of modulated signals is essential to the
understanding of the communication systems.
Thorough study of signal bandwidths will
have to wait until we know more about the modulation schemes referred to above.
However, at this time it would be well to look at the concept of bandwidth in
more general terms.
First, bandwidth in radio systems is always
a scarce resource. Not all frequencies are useful for a given communication
system, and there is often competition among users for the same part of the
spectrum.
In addition, as we have seen, the degrading
effect of noise on signals increases with bandwidth. Therefore, in most
communication systems it is important to conserve bandwidth to the extent
possible.
There is a general rule known as Hartley’s
Law which relates bandwidth, time, and information content. We will not yet be
able to use it for actual calculations, but it would be well to note it for
future reference, as Hartley’s Law applies to the operation of all
communication systems.
Here it is:
I = ktB; where
I = amount of information to be transmitted
in bits
k = a constant that depends on the modulation
scheme and the signal-to-noise ratio
t = time in seconds
B = bandwidth in hertz
Our problem thus far is that we do not have
precise ways of quantifying either the amount of information I or the constant
k. However, the general form of the equation is instructive.
It tells us that the rate at which
information is transmitted is proportional to the bandwidth occupied by a
communication system. To transmit more information in a given time requires
more bandwidth (or a more efficient modulation scheme).
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