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The procedures for conducting lab experiments using a spectrum analyzer and oscilloscope to measure the frequency and amplitude of signals from a signal generator. The lab involves connecting the signal generator to the spectrum analyzer and oscilloscope using various cables and settings, and recording the observed frequencies and amplitudes. The document also includes observations and exercises for measuring noisy signals and comparing the measurements from the two instruments.
Typology: Cheat Sheet
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Note: Do not use the very short SMA cables for this lab such as for the connection between T-Junction and SA in- put. It is recommended that longer SMA or BNC cables be used for this lab. DO NOT FORGET TO USE DC BLOCK WITH SPECTRUM ANALYZER (SA).
Part I: SA Measurement of two signals close in frequency
(What you should see: The ability to clearly identify two signals that are close in frequency as separate signals depends strongly on the measurement settings on the spectrum analyzer. You will explore the effect of the span and resolution bandwidth settings on this type of measurement. The resolution bandwidth is really the key in this case, but the two set- tings are linked within the SA.)
We will use two SIGNAL GENERATORS in this lab and combine the signals using a combiner/splitter provided to you as shown in Fig. 1. The combined signal will be then observed in the SA to determine the frequency contents of the signal and to visualize the resolution bandwidth of two signals close in frequency.
Figure 1: SA Measurement of two signals close in frequency
Figure 2: Test configuration for measurement of SIGNAL GENERATOR as a single frequency source
Table 2: Observed frequency and amplitudes for varied SIGNAL GENERATOR CW test signals
Source test Frequency (MHz)
Source Power Level Setting (dBm)
SA Measured Peak Frequency (MHz)
SA Measured Amplitude (dBm)
Comments
By how much does the SA measured signal amplitude drop at 25 MHz and 300 MHz when the SIGNAL GENERATOR power level setting is reduced by 3 dB?
Other comments and observations:
Part III: Oscilloscope Measurement of the SIGNAL GENERATOR signal at varied frequency and amplitude
(What you should see: you will measure the same signals in the time domain on an Oscilloscope that you measured above on the SA. You should see agreement between the O-Scope and SA frequency measurements at low frequency, but will see differences at higher frequencies. Amplitude correlation between the two instruments requires you to properly understand and calculate powers in dBm from voltages across a 50 ohm load and vice-versa. The 1 MΩ vs 50 Ω coupling setting is critical to getting this right.)
The test configuration for this part is shown below. You should read the reference guide for the oscilloscope provided in handout material before completing this part.
Figure 3: Configuration for time domain measure- ment of SIGNAL GENER- ATOR test signal using os- cilloscope
OBSERVATIONS: T= s f= Hz
OBSERVATIONS: Vpp (1MΩ coupling) = mV Vpp(50Ω coupling) = mV
Table 3: Summary of Oscilloscope Amplitude and Frequency Measurements
Signal gen. Test Fre- quency (MHz)
Signal gen. Power Level (dBm)
OSCOPE Meas. Frequency (MHz) fo +/-∆
Measured Vpp Z: 1MΩ
Measured Vpp Z: 50Ω
Comments
Observations: What values do you estimate for A 0 and A 1 for your measurement configuration? A 0 = A 1 =
Enter these values into the Matlab file, and compare to the O-Scope display.
Observations: Printout the Matlab file with plots that are closest to what you can measure for the two signals on the O-scope.
(Optional) See if you can capture the digital waveform from the scope and obtain a plot to compare to your Matlab file.
Hint: You may have to vary the time scale (ns/division) on the scope and the total time span of the Matlab file in looking for similar waveform representations. By increasing the total time span of the screen you should definitely see a repetitive “beat signal” pattern that repeats on both the scope and on the Matlab representations. By varying the phase you should be able to get the O-scope screen view to look similar to the Matlab view.
Part V: Simulations and additional analysis
(What you should see: if done properly you should see reasonable agreement between SA and oscilloscope measure- ments of frequency and power – i.e. powers calculated from voltage for OSCOPE – for lower frequencies. You will see problems at higher frequencies with this agreement.)
Convert your peak-to-peak voltage values from part IV for the 50 ohm coupling case to power in dBm and compare to the results obtained with the spectrum analyzer in Table 4 below. Also summarize the frequency results from the SA and OSCOPE. The following equation may be used to convert the 50 ohm voltages to power in dBm.
P (dBm) = 10 log
(Vpp)^2 400 × 10 −^3
where Vpp is the peak-to-peak voltage in volts measured on the OSCOPE. Use of Matlab or a spreadsheet facilitates these calculations.
Table 4: : Comparison of Spectrum Analyzer and Oscilloscope Measurements
Signal gen. Test Freq. (MHz)
Signal gen. Power Level (dBm)
OSCOPE Meas. Freq. (MHz) fo+/
Measured Vpp Z: 1MΩ
Measured Vpp Z: 50Ω
Comments
How well do the SA and OSCOPE frequency measurements compare?
How well to the SA and OSCOPE amplitude measurements compare?
Other comments:
Part VII (Optional) : Oscilloscope Measurement of Noisy Signal.
(This part is required for graduate students, but optional for undergraduates.)
(What you should see: you will measure a very low level signal sent through a “wireless link” and observe the dif- ferent measurement requirements that such “noisy” signals may require. You will be receiving your signal as well some other signals.)
In this portion of the lab you will construct a simple wireless link and note the effect of link losses and noise on time- domain and frequency-domain measurements. The test configuration is shown below.
Figure 5: Configuration to observe the effect of link losses and noise on Time-Domain and Frequency - Domain mea- surements using OSCOPE and SA respectively.