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ADF4377 Datasheet(PDF) 44 Page - Analog Devices |
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ADF4377 Datasheet(HTML) 44 Page - Analog Devices |
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44 / 79 page ![]() Data Sheet ADF4377 APPLICATIONS INFORMATION analog.com Rev. 0 | 44 of 79 Degradation of the SNR due to sample clock jitter only occurs if the analog input signal is slewing. If the analog input signal is stationary (dc), it does not matter when in time the sampling occurs. Additionally, a faster slewing input signal yields a greater error (more noise) than a slower slewing input signal. Figure 94 demonstrates this effect. Note how much larger the error term is with the fast slewing signal than with the slow slewing signal. To maintain the SNR performance of the data converter, digitization of high input frequency signals requires a clock with much less jitter than applications with lower frequency input signals. Figure 94. Fast and Slow Sine Wave Signals Sampled with a Jittery Clock It is important to note that the frequency of the analog input signal determines the jitter requirement of the sample clock. The actual sample clock frequency does not matter. Many ADC applications that under sample high frequency signals have especially challeng- ing sample clock jitter requirements. This information is useful for gaining an intuitive feel for the SNR degradation due to sampling clock jitter. Quantitatively, the actual sample clock jitter requirement for a given application is calculated as follows: tJTOTAL =10−SNRdB20 2×π×fSIG (27) where: tJ(TOTAL) is the total RMS jitter in seconds SNRdB is the SNR requirement in decibels fSIG is the highest frequency signal to be digitized, expressed in Hz The total jitter is the rms sum of the aperture jitter of the ADC and the sample clock jitter, calculated as follows: tJTOTAL = tJCLK2+tJADC2 (28) Alternatively, for a given total jitter, the attainable SNR is calculated as follows: SNRdB=−20×log 2×π×fSIG×tJTOTAL (29) These calculations assume a full-scale sine wave input signal. If the input signal is a complex, modulated signal with a moderate crest factor, the peak slew rate of the signal may be lower and the sample clock jitter requirement may be relaxed. These calculations are also theoretical. They assume a noiseless ADC with infinite resolution. All realistic ADCs have both added noise and a resolution limit. The limitations of the ADC must be accounted for to prevent overspecifying the sampling clock. Figure 95 plots the previous equations and provides a way to estimate the sampling clock jitter requirement for a given input signal or the expected SNR performance for a given sample clock jitter. Figure 95. SNR vs. Analog Input Frequency with Various Levels of Clock Jitter Measuring Clock Jitter Indirectly Using ADC SNR For some applications, integrating the phase noise of a clock generator within a defined offset frequency range (for example, 12 kHz to 20 MHz) is sufficient to calculate the impact of the clock on the overall system performance. In these situations, the rms jitter can be calculated from a phase noise measurement. However, other applications require knowledge of the phase noise of the clock at frequency offsets that exceed the capabilities of phase noise analyzers. This limitation makes it difficult to calculate jitter from a phase noise measurement. The rms jitter of an ADC clock source can be indirectly measured by comparing a jitter dominated SNR measurement to a non-jitter dominated SNR measurement. A jitter dominated SNR measure- ment (SNRJITTER) is created by applying a low jitter, high frequency full-scale sine wave to the ADC analog input. A non-jitter dominated SNR measurement (SNRBASE) is created by applying a very low amplitude (or low frequency) sine wave to the ADC analog input. The total clock jitter (tJ(TOTAL)) can be calculated using Equation 30. tJTOTAL =1012×log1010−SNRJITTER10−10−SNRBASE10 2×π×fSIG (30) |
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