Angle encoded signals have the general form
For phase modulation (PM), in generalso that, in particular, for
the signal becomes
For frequency modulation (FM), things are quite a bit more complicated and calculus rears its head. To be quite specific

so that, in particular and most simply, for

FM Signal with b =5 FM Signal with b =5 (includes an overlay of modulation) (without overlay)
The spectral representation of angular modulation signals is a bit more complicated the representations of amplitude modulated signals discussed previously. The equation above may be rewritten as
So that in the limit of small modulation [1] -- i.e. for a narrowband signal [2]
PHASOR REPRESENTATIONS OF AM AND FM SIGNALS A DSB-AM Signal A narrowband FM Signal
[1] When the argument of a sinusoidal function, say A, is small
[2] For the more mathematically inclined, it may be noted that going beyond the narrowband limitation, it can be shown that
where the
is the so called nth order Bessel function of the first kind. Thus,
is the value of the relative amplitude of the nth sideband. For example,