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AD8551ARM-R2 数据表(PDF) 15 Page - Analog Devices |
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AD8551ARM-R2 数据表(HTML) 15 Page - Analog Devices |
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15 / 24 page ![]() AD8551/AD8552/AD8554 Rev. C | Page 15 of 24 + AB BB CM2 VIN+ VNB CM1 VOA –BA VNA ФB ФA AA VOSA ФB ФA VOUT VIN– Figure 50. Auto-Zero Phase of the AD855x Amplification Phase When the φB switches close and the φA switches open for the amplification phase, this offset voltage remains on CM1 and, essentially, corrects any error from the nulling amplifier. The voltage across CM1 is designated as VNA. Furthermore, VIN is designated as the potential difference between the two inputs to the primary amplifier, or VIN = (VIN+ − VIN−). Thus, the nulling amplifier can be expressed as [] [] ( ) [] t V B t V t V A t V NA A OSA IN A OA − − = ] [ (3) + AB BB CM2 VIN+ VNB CM1 VOA –BA VNA ФB ФA AA VOSA ФB ФA VOUT VIN– Figure 51. Output Phase of the Amplifier Because φA 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 φA was closed. If the period of the autocorrection switching frequency is labeled tS, then 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) 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, assume that the autocorrection frequency is much faster than any potential change in VOSA or VOSB. This is a valid 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 AD855x. This effectively renders V [] [ ] ( ) 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) From these equations, the auto-zeroing action becomes evident. Note the VOS term is reduced by a 1 + BA factor. This shows how the nulling amplifier has greatly reduced its own offset voltage error even before correcting the primary amplifier. This results in the primary amplifier output voltage becoming the voltage at the output of the AD855x amplifier. It is equal to [ ] [ ] ( ) NB B OSB IN B OUT V B V t V A t V + + = (8) In the amplification phase, VOA = VNB, so this can be rewritten as [] [] [] ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ + + + + = A OSB 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, [] [] () OSA B A OSA A A B B B IN OUT V A B V B A B A A t V t V + + + + = 1 (10) The AD855x architecture is optimized in such a way that AA = AB and BA B = B B OS time invariant; therefore, Equation 5 can be rearranged and rewritten as B B B and BA B >> 1 Also, the gain product of AAB B B is much greater than AB B . These allow Equation 10 to be simplified to [ ] [ ] ( ) OSB OSA A A A IN OUT V V A B A t V t V + + ≈ (11) Most obvious is the gain product of both the primary and nulling amplifiers. This AAB B A term is what gives the AD855x its extremely high open-loop gain. To understand how VOSA and VOSB B relate to the overall effective input offset voltage of the complete amplifier, establish the generic amplifier equation of ( ) EFF OS IN OUT V V k V , + × = (12) where k is the open-loop gain of an amplifier and VOS, EFF is its effective offset voltage. Putting Equation 12 into the form of Equation 11 gives [ ] [ ] A A EFF OS A A IN OUT B A V B A t V t V , + ≈ (13) Thus, it is evident that A OSB OSA EFF OS B V V V + ≈ , (14) The offset voltages of both the primary and nulling amplifiers are reduced by the Gain Factor BA. This takes a typical input offset voltage from several millivolts down to an effective input offset voltage of submicrovolts. This autocorrection scheme is the outstanding feature of the AD855x series that continues to |
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