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LTC1966CMS8 数据表(PDF) 21 Page - Linear Technology |
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LTC1966CMS8 数据表(HTML) 21 Page - Linear Technology |
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21 / 32 page ![]() 21 LTC1966 sn1966 1966fas frequency. So with AC + DC waveforms, the required value for CAVE should be based on half of the lowest input frequency, using the same design curves presented in Figures 6, 8, 17 and 18. Crest factor, which is the peak to RMS ratio of a dynamic signal, also effects the required CAVE value. With a higher crest factor, more of the energy in the signal is concentrated into a smaller portion of the waveform, and the averaging has to ride out the long lull in signal activity. For busy waveforms, such as a sum of sine waves, ECG traces or SCR-chopped sine waves, the required value for CAVE should be based on the lowest fundamental input frequency divided as such: f f CF DESIGN INPUT MIN = () •– 32 APPLICATIO S I FOR ATIO using the same design curves presented in Figures 6, 8, 17 and 18. For the worst case of square top pulse trains, that are always either zero volts or the peak voltage, base the selection on the lowest fundamental input frequency divided by twice as much: f f CF DESIGN INPUT MIN = () •– 62 The effects of crest factor and DC offsets are cumulative. So for example, a 10% duty cycle pulse train from 0VPEAK to 1VPEAK (CF = √10 = 3.16) repeating at 16.67ms (60Hz) input is effectively only 30Hz due to the DC asymmetry and is effectively only: fHz DESIGN == 30 6 3 16 2 378 •. – . for the purposes of Figures 6, 8, 17 and 18. Figure 20. Settling Time with DC-Accurate Post Filter Figure 19. Settling Time with Buffered Post Filter SETTLING TIME (SEC) 0.01 0.1 1 10 1 0.1 10 100 1066 F14 C = 100 µF C = 47 µF C = 22 µF C = 10 µF C = 4.7 µF C = 2.2 µF C = 1.0 µF C = 0.47 µF C = 0.22 µF C = 0.1 µF SETTLING TIME (SEC) 0.01 0.1 1 10 1 0.1 10 100 1066 F20 C = 100 µF C = 47 µF C = 22 µF C = 10 µF C = 4.7 µF C = 2.2 µF C = 1.0 µF C = 0.47 µF C = 0.22 µF C = 0.1 µF |
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