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Getting Started
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© 2014 Stanford Research Systems
When "THD+N" ratio is selected, the analyzer inserts a deep notch filter at the frequency of the
fundamental. In this case, because the notch filter is set to be tuned to the measured frequency, it is set
at the 1 kHz dominant frequency of our generator signal. The Time Domain detector then performs an
RMS integration of the remaining signal, which is distortion plus noise, and displays the ratio of that
signal to the total amplitude of the input Note that the measured THD+N ratio is -60 dB. (1 mV / 1 V =
60 dB).
To show how much more SR1 brings to a standard distortion measurement select the second analyzer
(A1) as the FFT1 analyzer. When the panel is displayed, change the source of the Analyzer to "Other
Analyzer". In this mode the FFT analyzer and the Time Domain Analyzer work as a team; the FFT
analyzer looking at the notch filtered signal from the Time Domain Detector. Take a look at the
information displayed on the FFT1 analyzer panel:
Like all analyzers the input source is displayed at the upper left. The analyzer sampling rate is displayed
at the upper right. Because we've connected the FFT analyzer to the output of the Time Domain Detector
Содержание SR1
Страница 5: ...Part I Getting Started Audio...
Страница 7: ...Getting Started 7 2014 Stanford Research Systems...
Страница 12: ...SR1 Operation Manual 12 2014 Stanford Research Systems...
Страница 27: ...Part II SR1 Operation Audio...
Страница 156: ...SR1 Operation Manual 156 2014 Stanford Research Systems Passband Group Delay of Elliptical Filter...
Страница 258: ...SR1 Operation Manual 258 2014 Stanford Research Systems...
Страница 272: ...SR1 Operation Manual 272 2014 Stanford Research Systems on the amplitude sweep...
Страница 289: ...SR1 Operation 289 2014 Stanford Research Systems...
Страница 290: ...Part III SR1 Reference Audio...