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AD820ARMZ-R7 Folha de dados(PDF) 17 Page - Analog Devices |
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AD820ARMZ-R7 Folha de dados(HTML) 17 Page - Analog Devices |
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17 / 24 page ![]() AD820 Rev. H | Page 17 of 24 OUTPUT CHARACTERISTICS The AD820 unique bipolar rail-to-rail output stage swings within 5 mV of the negative supply and 10 mV of the positive supply with no external resistive load. The approximate output saturation resistance of the AD820 is 40 Ω sourcing and 20 Ω sinking. This can be used to estimate output saturation voltage when driving heavier current loads. For instance, when sourcing 5 mA, the saturation voltage to the positive supply rail is 200 mV; when sinking 5 mA, the saturation voltage to the negative rail is 100 mV. The open-loop gain characteristic of the amplifier changes as a function of resistive load, as shown in Figure 10 through Figure 13. For load resistances over 20 kΩ, the AD820 input error voltage is virtually unchanged until the output voltage is driven to 180 mV of either supply. If the AD820 output is driven hard against the output saturation voltage, it recovers within 2 μs of the input returning to the linear operating region of the amplifier. Direct capacitive load interacts with the effective output imped- ance of the amplifier to form an additional pole in the amplifier feedback loop, which can cause excessive peaking on the pulse response or loss of stability. The worst case occurs when the amplifier is used as a unity-gain follower. Figure 40 shows AD820 pulse response as a unity-gain follower driving 350 pF. This amount of overshoot indicates approximately 20 degrees of phase margin—the system is stable, but is nearing the edge. Configurations with less loop gain, and as a result less loop bandwidth, are much less sensitive to capacitance load effects. Figure 41 is a plot of noise gain vs. the capacitive load that results in a 20 degree phase margin for the AD820. Noise gain is the inverse of the feedback attenuation factor provided by the feedback network in use. 20mV 2µs 100 90 10 0% Figure 40. Small Signal Response of AD820 as Unity-Gain Follower Driving 350 pF Capacitive Load 5 1 300 30k CAPACITIVE LOAD FOR 20º PHASE MARGIN (pF) 4 3 2 1k 3k 10k RF R1 Figure 41. Noise Gain vs. Capacitive Load Tolerance Figure 42 shows a possible configuration for extending capacitance load drive capability for a unity-gain follower. With these component values, the circuit drives 5000 pF with a 10% overshoot. AD820 – + – + +VS –VS 0.01µF 0.01µF 20pF 20kΩ 100Ω VOUT VIN 3 2 4 7 6 – + Figure 42. Extending Unity-Gain Follower Capacitive Load Capability Beyond 350 pF SINGLE-SUPPLY HALF-WAVE AND FULL-WAVE RECTIFIERS An AD820 configured as a unity-gain follower and operated with a single supply can be used as a simple half-wave rectifier. The AD820 inputs maintain picoamp level input currents even when driven well below the negative supply. The rectifier puts that behavior to good use, maintaining an input impedance of over 1011 Ω for input voltages from 1 V from the positive supply to 20 V below the negative supply. The full- and half-wave rectifier shown in Figure 43 operates as follows: when VIN is above ground, R1 is bootstrapped through the unity-gain follower, A1, and the loop of Amplifier A2. This forces the inputs of A2 to be equal; thus, no current flows through R1 or R2, and the circuit output tracks the input. When VIN is below ground, the output of A1 is forced to ground. The |
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