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AD8132ARZ-R71 Folha de dados(PDF) 22 Page - Analog Devices |
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AD8132ARZ-R71 Folha de dados(HTML) 22 Page - Analog Devices |
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22 / 33 page ![]() AD8132 Rev. I | Page 21 of 32 OPERATIONAL DESCRIPTION DEFINITION OF TERMS Differential Voltage It is the difference between two node voltages. For example, the output differential voltage (or equivalently output differential mode voltage) is defined as VOUT, dm = (V+OUT − V−OUT) where V+OUT and V−OUT refer to the voltages at the +OUT and −OUT terminals with respect to a common reference. Common-Mode Voltage It is the average of two node voltages. The output common- mode voltage is defined as VOUT, cm = (V+OUT + V−OUT)/2 AD8132 CF +IN –IN RF CF RF RG RG +DIN VOCM –DIN RL, dm +OUT VOUT, dm –OUT Figure 64. Circuit Definitions BASIC CIRCUIT OPERATION One of the more useful and easy to understand ways to use the AD8132 is to provide two equal ratio feedback networks. To match the effect of parasitics, comprise these networks of two equal value feedback resistors (RF) and two equal value gain resistors (RG). This circuit is shown in Figure 64. Like a conventional op amp, the AD8132 has two differential inputs that can be driven with both differential mode input voltage (VIN, dm) and common-mode input voltage (VIN, cm). There is another input to consider (VOCM) on the AD8132 that is not present on conventional op amps. VOCM is completely separate from the previous inputs. There are two complementary outputs whose response can be defined by a differential mode output (VOUT, dm) and a common- mode output (VOUT, cm). Table 10 shows the gain from any type of input to either type of output. Table 10. Differential and Common-Mode Gains Input VOUT, dm VOUT, cm VIN, dm RF/RG 0 (by design) VIN, cm 0 0 (by design) VOCM 0 1 (by design) As listed in Table 10, the differential output (VOUT, dm) is equal to the differential input voltage (VIN, dm) times RF/RG. In this case, it does not matter if both differential inputs are driven, or only one output is driven and the other is tied to a reference voltage, such as ground. As seen from the two zero entries in the VOUT,dm column, neither of the common-mode inputs has any effect on this gain. The gain from VIN, dm to VOUT, cm is 0, and first-order, does not depend on the ratio matching of the feedback networks. The common-mode feedback loop within the AD8132 provides a corrective action to keep this gain term minimized. The term balance error describes the degree that this gain term differs from 0. The gain from VIN,cm to VOUT,dm directly depends on the matching of the feedback networks. The analogous term for this transfer function (used in conventional op amps) is common-mode rejection ratio (CMRR). Therefore, if it has a high CMRR, the feedback ratios must be well matched. The gain from VIN, cm to VOUT, cm is ideally 0 and is first-order independent of the feedback ratio matching. As in the case of VIN, dm to VOUT, cm, the common-mode feedback loop keeps this term minimized. The gain from VOCM to VOUT,dm is ideally 0 when the feedback ratios are matched only. The amount of differential output signal that is created by varying VOCM is related to the degree of mismatch in the feedback networks. VOCM controls the output common-mode voltage VOUT, cm with a unity-gain transfer function. With equal ratio feedback networks (as previously assumed), its effect on each output is the same, that is the gain from VOCM to VOUT, dm is 0. If not driven, the output common-mode voltage is set with an internal voltage divider to a level that is nominally midsupply. It is recommended that a 0.1 μF bypass capacitor be connected to VOCM. When unequal feedback ratios are used, the two gains associated with VOUT, dm become nonzero. This significantly complicates the mathematical analysis along with any intuitive understanding of how the part operates. |
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