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AD9260ASZ датащи(PDF) 26 Page - Analog Devices |
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AD9260ASZ датащи(HTML) 26 Page - Analog Devices |
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26 / 45 page ![]() AD9260 Rev. C | Page 25 of 44 ANALOG MODULATOR VINA VINB SS1 SS2 CS1 CS2 SS3 SH1 SS4 SH2 SH3 SH4 CPB1 CPB2 CPA1 CPA2 Figure 61. Detailed Analog Input Structure Figure 61 illustrates the analog input structure of the AD9260. For the moment, ignore the presence of the parasitic capacitors CPA and CPB. The effects of these parasitic capacitors will be discussed near the end of this section. The switched capacitors, CS1 and CS2, sample the input voltages applied on pins VINA and VINB. These capacitors are connected to input pins VINA and VINB when CLK is low. When CLK rises, a sample of the input signal is taken on capacitors CS1 and CS2. When CLK is high, capacitors CS1 and CS2 are connected to the Analog Modulator. The modulator precharges capacitors CS1 and CS2 to minimize the amount of charge required from any circuit used in combination with the AD9260 to drive input pins VINA and VINB. This reduces the input drive requirements of the analog circuitry driving pins VINA and VINB. The Analog Modulator precharges the voltages across capacitors CS1 and CS2, approximately equal to a delayed version of the input signal. When capacitors CS1 and CS2 are connected to input pins VINA and VINB, the differential charge, Q(n), on these capacitors is given in the following equation, VCORE CS q q n Q × = − = 2 1 ) ( (6) where q1 and q2 are the individual charges stored on capacitors CS1 and CS2 respectively, and CS is the capacitance value of CS1 and CS2. When capacitors CS1 and CS2 are connected to the Analog Modulator during the preceding precharge clock phase, the capacitors are precharged equal to an approximation of a previous sample of the input signal. Consequently the differential charge on these capacitors while CLK is high is given in the following equation, () Vdelta CS delay VCORE CS n Q × + × = − ) 1 ( (7) where VCORE(delay) is the value of VCORE sampled during a previous period of CLK, and Vdelta is the sigma-delta error voltage left on the capacitors. Vdelta is a natural artifact of the sigma-delta feedback techniques utilized in the Analog Modulator of the AD9260. It is a small random voltage term that changes every clock period and varies from 0 to ±0.05 ×VREF. The analog circuitry used to drive the input pins of the AD9260 must respond to the charge glitch that occurs when capacitors CS1 and CS2 are connected to input pins VINA and VINB. This circuitry must provide additional charge, qdelta, to capacitors CS1 and CS2, which is the difference between the precharged value, Q(n–1), and the new value, Q(n), as given in the following equation, ( ) ( ) 1 − − = n Q n Q Qdelta (8) () [ ] Vdelta delay VCORE VCORE CS Qdelta + − × = (9) DRIVING THE INPUT Transient Response The charge glitch occurs once at the beginning of every period of the input CLK (falling edge), and the sample is taken on capacitors CS1 and CS2 exactly one-half period later (rising edge). Figure 62 presents a typical input waveform applied to input Pins VINA and VINB of the AD9260. CLOCK VINA-VINB TRACK SAMPLE TRACK SAMPLE TRACK SAMPLE TRACK SAMPLE Figure 62. Typical Input Waveform Figure 62 illustrates the effect of the charge glitch when a source with nonzero output impedance is used to drive the input pins. This source must be capable of settling from the charge glitch in one-half period of the CLK. Unfortunately, the MOS switches used in any CMOS-switched capacitor circuit (including those in the AD9260) include nonlinear parasitic junction capacitances connected to their terminals. Figure 61 also illustrates the parasitic capacitances, Cpa1, Cpb1, Cpa2, and Cpb2, associated with the input switches. Parasitic capacitor Cpa1 and Cpa2 are always connected to Pins VINA and VINB and therefore do not contribute to the glitch energy. Parasitic capacitors Cpb1 and Cpb2, on the other hand, cause a charge glitch that adds to that of input capacitors CS1 and CS2 when they are connected to input Pins VINA and VINB. The nonlinear junction capacitance of Cpb1 and Cpb2 cause charge glitch energy that is nonlinearily related to the input signal. Therefore, linear settling is difficult to achieve unless the input source completely settles during one-half period of CLK. A portion of the glitch impulse energy kicked back at the source is not linearly related to the input signal. Therefore, the best way to ensure that the input signal settles linearly is to use wide bandwidth circuitry, which settles as completely as possible from the glitch during one-half period of the CLK. The AD9260 utilizes a proprietary clock-boosted boot- strapping technique to reduce the nonlinear parasitic |
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