T«fr til f i
*
* rtt
-, lYiVr^Vftii ^itirifaifl§l
Operating Instructions— Type H 3 0
/ :
(A ) Narrow band FM.
Note the resemblance to AM.
CARRIER
100 KHz/CM
DISPERSION
2 GHz
h'/. ■ ■
f>:
(C) Carrier almost at a null.
(D )* Carrier at null.
Fig. 2-15. Frequency modulated display. At first carrier null, index o f modulation is 2.4; so ratio of deviation to rate is 2.4. Rate is 0.8
cm X 100 kHz/cm = 80 kHz. Deviation 2.4 X 80 kHz = 192 kHz.
Pulse Modulated Signal Spectra
W hen a C W signal is pulse modulated, the carrier is
periodically turned on and off. The on period is determined
by the modulating pulse width; the off time is related to
the pulse repetition time or frequency. The carrier is usually
modulated by a rectangular-shaped pulse.
A symmetrical square wave is composed of its fundamental
frequency plus the odd harmonics. If the relative amplitudes
and phase of the harmonics are changed, a number of wave
shapes are produced; rectangular, trapezoidal, sawtooth,
etc. The spectrum of the square wave or any pulse shape,
therefore, is displayed according to its frequency compo
nents and their amplitudes on a spectrum analyzer. Com
mon pulse forms and their spectra are described in Ref
erence Data for Radio Engineers, 4th edition. Chapter 35.
ITT 1956.
Fig. 2-16A illustrates a theoretical voltage spectrum of
a rectangulary-pulse, pulse-modulated oscillator The main
lobe and the side lobes are shown as groups of spectral lines
extending above and below the baseline. The number of
these side lobes for a truly rectangular pulse approaches
infinity. Any two adjacent side lobes are separated on the
frequency scale by a distance equal to the inverse of the
modulating pulse width.
Fourier theory shows that adjacent lobes are 180° out
of phase; however, since the spectrum analyzer is insensitive
to phase, only the absolute value of the spectrum is dis
played and appears as illustrated in Fig. 2-16B.
Fig. 2-17 illustrates the relative effects the pulse width
and pulse repetition frequency have on a pulsed RF spec
trum.
Since the spacing between the spectral lines of the pulsed
RF spectrum is a function of the PRF (pulse repetition fre
quency), the spectrum analyzer resolution bandwidth should
be less than the PRF to respond to one frequency compo
nent. In most instances this is impractical. The spectrum
£■
t
I:
t- ■
fe
iT
2-15
Summary of Contents for 1L30
Page 48: ...si L i y n Maintenance Type 1L30 Fig 4 15 Honeycomb assembly drcui a n d component layout 4 n ...
Page 59: ...Fig 6 1 A Test equipment required for calibration ...
Page 60: ... Calibration Type 1130 ...
Page 120: ...T Y P E I L 3 0 S P E C T R U M A N A L Y Z E R ib i IF SYSTEM BLOCK DIAGRAM 9 1 9 2 ...
Page 127: ......