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LAB MANUAL/EMIT
EXPERIMENT NO. 5
TITLE: Study of Spectrum Analyzer
AIM: Study of Spectrum Analyzer
Perform harmonic analysis and Total Harmonic Distortion (THD) measurement for sine
and square waves.
Analyse Spectrum of AM & FM and to measure percent modulation and bandwidth.
APPARATUS:
Sr. No. Instrument Specifications
1. Arbitrary Waveform generator
2. Spectrum analyzer
Technical Specifications:
I/p Freq.
Frequency Range
50Ω
Specifications
9kHz to 1.5GHz
Frequency Reference
Aging
Temperature Stability
±2*10-6 /year
±5*10-6
Frequency Readout Accuracy
(Start,Stop,Center,Marker)
±(frequency readout*frequency reference error3
+span accuracy+20% of RBW)
Frequency Span
Range
Resolution
Accuracy
0Hz (zero span),100 Hz to 1.5GHz
Four digits or 2Hz,whichever is greater
±1% of span
Sweep Time
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Range
Accuracy
Sweep Trigger
5ms to 2000s
±1%
Free Run,Single,Line,video,External
Measurement Range
50 Ω
Input Attenuator Range
-120 dBm to +30dBm
0 to 60dB,in 5 dB steps
Frequency Response
50 Ω,9kHz to 1.5GHz
20 to 30 C
0 to 55C
±0.75 dB
±1.0 dB
THEORY:
The most common way of observing a signal is to display it on an oscilloscope, with time as x-
axis. This is a view of the signal in time domain. It is also very useful to display signals in
frequency domain. The instrument providing this frequency domain view is the spectrum
analyzer. On its CRT, the spectrum analyzer provides a calibrated graphical display with
frequency on horizontal axis and voltage on vertical axis.
There are two types of spectrum analyzers:
Scanning types, which can scan the frequency and non-scanning types also called real-time
spectrum analyzer. The scanning types are essentially swept receivers, both superhetrodyne and
tuned rf (Trf) whose tuning is electrically swept over the frequency range of observation by a
scanning signal that also controls the horizontal position of the spot on the CRT ray tube. There
are two kinds of real-time non-scanning spectrum analyzers: The multichannel spectrum
analyzer or Fourier analyzer. These real-time analyzers “lock” over all parts of their frequency
display range simultaneously and so present the spectrum of an electrical event as soon as it
happens. The scanning spectrum analyzer can only “lock” at a single frequency at a given
instant. The spectrum analyzer that we are using in the laboratory is the swept spectrum analyzer.
Fig 1 shows the basic block diagram of a spectrum analyzer covering the range of 500 kHz to 1
GHz which is representative of super heterodyne type. the input signal is fed into the diode mixer
which is driven to saturation by a strong signal from the local oscillator, which is linearly tunable
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electrically over the range of 2 to 3ghz.the input mixer multiplies (heterodynes) the input signal
and the local oscillator signal together and so provides two signals at its output that are
proportional in amplitude to the input signal but of frequencies that are the sum and difference
between the frequencies of input signal and the local oscillator signal.
The intermediate frequency amplifier is tuned to a narrowband around 2ghz.as the local
oscillator is tuned over the range from 2 to 3 GHz, only input signals that are expected from the
local oscillator frequency by 2 GHz will be converted into the intermediate frequency band pass
through the intermediate frequency amplifier, be rectified in the detector and produce a vertical
deflection on the CRT.The spectrum analyzer will also be sensitive to signals from 4 to 5 GHz. a
LPF with a cutoff a little above 1 GHz at the input suppresses these spurious signals.
Fig.1: Swept Heterodyne Spectrum Analyzer
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Fig.2 Block Diagram of Spectrum Analyzer
Fig 2 is a more detailed block diagram of the spectrum analyzer. The frequency of the first local
oscillator is controlled with the select ably attenuated signal from the scan generated combined
with an adjustable bias level from the center frequency control in a voltage control block. The
attenuator controls the frequency axis calibration of the display by controlling the frequency
range over which the first local oscillator is scanned. The adjustable bias level sets the frequency
about which the local oscillator is scanned and thus the center frequency of the display.
Several conversions are used in the intermediate frequency amplifier chain, which ultimately
gets down to a 3 MHz intermediate frequency amplifier having a B.W.of a few 100 Hz to
provide this high selectivity over the whole range of the instrument. the high first IF is necessary
for wide image separation, the low cost IF is necessary for narrowband filtering unobtainable at
the 1st IF.
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Frequency Resolution and Bandwidth:
Frequency resolution is the ability of the spectrum analyzer to separate signals closely spaced in
the frequency. The scanning action in the spectrum analyzer slides the input spectrum past the IF
amplifier filter. Because of this, the magnified display of a single frequency CW signal is a plot
of sensitivity char. of the IF amplifier filter.The other factors determining resolution are the
frequency stability of the spectrum analyzer, local oscillator.
Sweep Desensitization:
Sweep desensitization is an effect caused by scanning a spectrum analyzer too fast which results
in loss of amplitude, sensitivity and resolution.The scan velocity in Hz must not exceed the
square of 3 dB B.W.of the IF filter in Hz.
Sensitivity:
The ability of the swept super heterodyne spectrum analyzer to measure small signals is
determined by its own internally generated be noise. Typical noise fig. varies from 24 dB at low
frequency to 40 dB at 12 GHz. Noise power is proportional to B.W. and so the highest sensitivity
to CW signals is obtained by the narrowest B.W.s
Dynamic Range:
The dynamic range of the spectrum analyzer expresses its ability to display the true spectra of
large and small signals simultaneously with signal levels within the dynamic range of the
instrument.
Harmonic Mixing:
Harmonic mixing is used to extend the frequency range of the swept super heterodyne spectrum
analyzer.
PROCEDURE:
1. Capture 98.3MHz radio Mirchi signal by giving appropriate START and STOP
frequency.
2. Generate AM waveform using arbitrary waveform generator. Observe fc-fm, fc, fc+fm
frequencies on spectrum analyzer and calculate modulation index.
%m = Em/Ec
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3. Generate FM waveform using arbitrary waveform generator and calculate modulation
index. %m = ∆f/frequency of modulating signal(fm)
4. Using markers measure bandwidth of FM
For m=0.5, no of side bands = 4
For m= 1,no of side bands = 6
For m= 2,no of side bands = 8
For m= 5,no of side bands = 16
Bandwidth= fm* no. of sidebands
5. For sine and square wave input measure total harmonic distortion.
THD = sqrt[(v22+v32+v42+…..)]/V1, where V1 = amplitude of fundamental frequency
V2 = amplitude of second harmonic
V3 = amplitude of third harmonic and so on.
CONCLUSIO
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