Phase modulation (PM) is a form of
modulation that represents information as variations in the instantaneous
phase of a
carrier wave.
Unlike its more popular counterpart, frequency modulation (FM), PM is not very widely used. This is because it tends to require more complex receiving hardware and there can be ambiguity problems in determining whether, for example, the signal has changed phase by +180° or -180°.
Theory
Suppose that the signal to be sent (called the modulating or message signal) is .
The carrier onto which the signal is to be modulated is
Then the modulated signal is
This shows how
modulates the phase. Clearly, it can also be viewed as a change of the frequency of the carrier signal. PM can thus be considered a special case of
FM in which the carrier frequency modulation is given by the time
derivative of the phase modulation.
The spectral behaviour of phase modulation is difficult to derive, but the mathematics reveals that there are two regions of particular interest:
- ,
- where and is the modulation index defined below. This is also known as Carson's Rule for PM.
Modulation index
As with other
modulation indices, this quantity indicates by how much the modulated variable varies around its unmodulated level. It relates to the variations in the phase of the carrier signal:
- ,
where
is the peak phase deviation. Compare to the modulation index for
frequency modulation.
See also