Phase
Modulation Review
As shown in the previous section, the
general signal with phase noise can be represented by s(t)
= A sin(wct + f(t)) f(t)
is a noise-like signal that phase modulates the carrier.
Before analyzing the case of modulation by noise, we will first
review sinusoidal phase modulation. A
signal consisting of a carrier of frequency wc phase
modulated by a sinusoidal signal of frequency wm
is given by s(t) = A sin(wct
+ qpksin(wmt)) ..
(1.4) where
qpk is the peak phase
deviation (in radians) The
time-domain waveform in (1.4) is quite simple, the signal has a phase
offset that varies according to the modulation signal.
Large-level phase modulation is easily observed on an oscilloscope as
jitter in the zero crossings. The
spectrum of the waveform in (1.4) is anything but simple, consisting
of a sidebands around the carrier wc
offset by ±wm and (theoretically)
an infinite number of harmonics of wm
. The result is an infinite series of sidebands with amplitudes
given by Bessel functions. The following table shows the
spectrum of an 0dBm, 100MHz carrier phase modulated by a 100kHz
sinusoid, with varying phase deviations:
|

qpk =
0.1 radian (5.7 degrees)
|

qpk =
0.5 radian (28 degrees)
|
|

qpk =
1 radian (5.7 degrees)
|

qpk =5
radians (280 degrees)
|
Phase Modulation is a
non-linear modulation. This means that if we want to know what
happens if the signal is phase modulated by a signal that is a sum of
other signals, we cannot work it out by adding up the
modulation responses to each signal individually. This is fairly
clear from the spectra above, increasing the modulation index does
not just increase the levels of the spectral lines in a linear
manner, a whole lot of new spectral lines become important. The
non-linearity is potentially a problem for when we analyze noise
modulation, as one of the main techniques for treating noise is to
consider it as a sum of sine waves, and to consider the response to
each sine wave separately. Luckily,
for low levels of phase modulation, the modulation behaves in a
linear manner, allowing phase noise to be treated using conventional
linear techniques.
|