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AD8571 Datasheet(PDF) 16 Page - Analog Devices |
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AD8571 Datasheet(HTML) 16 Page - Analog Devices |
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16 / 28 page ![]() AD8571/AD8572/AD8574 Data Sheet Rev. F | Page 16 of 28 AUTO-ZERO PHASE In this phase, all ΦAX switches are closed, and all ΦB switches are open. Here, the nulling amplifier is taken out of the gain loop by shorting its two inputs together. Of course, there is a degree of offset voltage, shown as VOSA, inherent in the nulling amplifier, that maintains a potential difference between the +IN and −IN inputs. The nulling amplifier feedback loop is closed through ΦA2, and VOSA appears at the output of the nulling amplifier and on CM1, an internal capacitor in the AD8571/ AD8572/AD8574. Mathematically, this can be expressed in the time domain as VOA[t] = AAVOSA[t] − BAVOA[t] (1) This can also be expressed as [ ] [ ] A OSA A OA B t V A t V + = 1 (2) The previous equations show that the offset voltage of the nulling amplifier times a gain factor appears at the output of the nulling amplifier and thus on the CM1 capacitor. AMPLIFICATION PHASE When the ΦB switches close and the ΦAX switches open for the amplification phase, the offset voltage remains on CM1 and essentially corrects any error from the nulling amplifier. The voltage across CM1 is designated as VNA. The potential difference between the two inputs to the primary amplifier is designated as VIN, or VIN = (VIN+ − VIN−). The output of the nulling amplifier can then be expressed as VOA[t] = AA(VIN[t] − VOSA[t]) − BAVNA[t] (3) Because ΦAX is now open and there is no place for CM1 to discharge, the voltage (VNA) at the present time (t) is equal to the voltage at the output of the nulling amp (VOA) at the time when ΦAX is closed. If the period of the autocorrection switching frequency is designated as TS, the amplifier switches between phases every 0.5 × TS. Therefore, in the amplification phase [ ] − = S NA NA T t V t V 2 1 (4) and substituting Equation 4 and Equation 2 into Equation 3 yields [ ] [ ] [ ] A S OSA A A OSA A IN A OA B T t V B A t V A t V A t V + − − + = 1 2 1 (5) For the sake of simplification, it can be assumed that the auto- correction frequency is much faster than any potential change in VOSA or VOSB. This is a good assumption because changes in offset voltage are a function of temperature variation or long- term wear time, both of which are much slower than the auto-zero clock frequency of the AD8571/AD8572/AD8574, which effectively makes the VOS time invariant, and Equation 5 can be rewritten as [ ] [ ] ( ) A OSA A A OSA A A IN A OA B V B A V B A t V A t V + − + + = 1 1 (6) or [ ] [ ] + + = A OSA IN A OA B V t V A t V 1 (7) Here, the auto-zeroing becomes apparent. Note that the VOS term is reduced by a factor of 1 + BA, which shows how the nulling amplifier has greatly reduced its own offset voltage error even before correcting the primary amplifier. Therefore, the primary amplifier output voltage is the voltage at the output of the AD8571/AD8572/AD8574 amplifier. It is equal to VOUT[t] = AB(VIN[t] + VOSB) + BBVNB (8) In the amplification phase, VOA = VNB, so this can be rewritten as [ ] [ ] [ ] + + + + = A OSA IN A B OSB B IN B OUT B V t V A B V A t V A t V 1 (9) Combining terms yield [ ] [ ] ( ) OSB B A OSA B A B A B IN OUT V A B V B A B A A t V t V + + + + = 1 (10) The AD8571/AD8572/AD8574 architecture is optimized in such a way that AA = AB, BA = BB, and BA >> 1. In addition, the gain product to AABB is much greater than AB. Therefore, Equation 10 can be simplified to VOUT[t] = VIN[t]AABA + AA(VOSA+ VOSB) (11) Most obvious is the gain product of both the primary and nulling amplifiers. This AABA term is what gives the AD8571/AD8572/ AD8574 extremely high open-loop gain. To understand how VOSA and VOSB relate to the overall effective input offset voltage of the complete amplifier, set up the generic amplifier equation of VOUT = k × (VIN + VOS, EFF) (12) where: k is the open-loop gain of an amplifier. VOS, EFF is its effective offset voltage. Putting Equation 12 into the form of Equation 11 gives VOUT[t] = VIN[t]AABA + VOS, EFFAABA (13) |
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