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AS1419AF-SPACE Datasheet(PDF) 10 Page - Austin Semiconductor |
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AS1419AF-SPACE Datasheet(HTML) 10 Page - Austin Semiconductor |
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10 / 20 page ![]() ADC ADC ADC ADC ADC AS1419 AS1419A AS1419 & AS1419A Rev. 1.5 08/09 Austin Semiconductor, Inc. reserves the right to change products or specifications without notice. 10 Austin Semiconductor, Inc. Intermodulation Distortion If the ADC input signal consists of more than one spectral component, the ADC transfer function nonlinearity can pro- duce intermodulation distortion (IMD) in addition to THD. IMD is the change in one sinusoidal input caused by the presence of another sinusoidal input at a different frequency. If two pure sine waves of frequencies fa and fb are applied to the ADC input, nonlinearities in the ADC transfer function can create distortion products at the sum and difference frequencies of mfa ±nfb, where m and n = 0, 1, 2, 3, etc. For example, the 2nd order IMD terms include (fa + fb). If the two input sine waves are equal in magnitude, the value (in decibels) of the 2nd order IMD products can be expressed by the following formula: Peak Harmonic or Spurious Noise The peak harmonic or spurious noise is the largest spectral component excluding the input signal and DC. This value is expressed in decibels relative to the RMS value of a full-scale input signal. Full-Power and Full-Linear Bandwidth The full-power bandwidth is that input frequency at which the amplitude of the reconstructed fundamental is reduced by 3dB for a full-scale input signal. The full-linear bandwidth is the input frequency at which the S/(N + D) has dropped to 77dB (12.5 effective bits). The AS1419 has been designed to optimize input bandwidth, allowing the ADC to undersample input signals with frequencies above the converter’s Nyquist Frequency. The noise floor stays very low at high frequencies; S/(N + D) becomes dominated by distortion at frequencies far beyond Nyquist. Driving the Analog Input The differential analog inputs of the AS1419 are easy to drive. The inputs may be driven differentially or as a singleended input (i.e., the –A IN input is grounded). The +A IN and –A IN inputs are sampled at the same instant. Any unwanted signal that is common mode to both inputs will be reduced by the common mode rejection of the sample-and-hold circuit. The inputs draw only one small current spike while charging the sample-and-hold capacitors at the end of conversion. During conversion, the analog inputs draw only a small leakage current. If the source impedance of the driving circuit is low, then the AS1419 inputs can be driven directly. As source impedance increases so will acquisition time (see Figure 6). For minimum acquisition time with high source impedance, a buffer amplifier should be used. The only requirement is that the amplifier driving the analog input(s) must settle after the small current spike before the next conversion starts (settling time must be 200ns for full throughput rate). FIGURE 6: t ACQ vs. Source Resistance Input Filtering The noise and the distortion of the input amplifier and other circuitry must be considered since they will add to the AS1419 noise and distortion. The small-signal bandwidth of the sample-and-hold circuit is 20MHz. Any noise or distortion products that are present at the analog inputs will be summed over this entire bandwidth. Noisy input circuitry should be filtered prior to the analog inputs to minimize noise. A simple 1-pole RC filter is sufficient for many applications. For example, Figure 7 shows a 1000pF capacitor from +A IN to ground and a FIGURE 7: RC Input Filter |
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