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AD823 Datasheet(PDF) 12 Page - Analog Devices |
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AD823 Datasheet(HTML) 12 Page - Analog Devices |
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12 / 16 page ![]() REV. 0 –12– AD823 The first pole in the denominator is the dominant pole of the amplifier, and occurs at about 18 Hz. This equals the input stage output impedance R1 multiplied by the Miller-multiplied value of C1. The second pole occurs at the unity-gain band- width of the output stage, which is 23 MHz. This type of archi- tecture allows more open loop gain and output drive to be obtained than a standard two-stage architecture would allow. OUTPUT IMPEDANCE The low frequency open loop output impedance of the common-emitter output stage used in this design is approxi- mately 30 k Ω. While this is significantly higher than a typical emitter follower output stage, when connected with feedback the output impedance is reduced by the open loop gain of the op amp. With 109 dB of open loop gain the output impedance is reduced to less than 0.2 Ω. At higher frequencies the output impedance will rise as the open loop gain of the op amp drops; however, the output also becomes capacitive due to the integra- tor capacitors C1 and C2. This prevents the output impedance from ever becoming excessively high (see Figure 17), which can cause stability problems when driving capacitive loads. In fact, the AD823 has excellent cap-load drive capability for a high fre- quency op amp. Figure 33 shows the AD823 connected as a fol- lower while driving 470 pF direct capacitive load. Under these conditions the phase margin is approximately 20 °. If greater phase margin is desired a small resistor can be used in series with the output to decouple the effect of the load capacitance from the op amp (see Figure 25). In addition, running the part at higher gains will also improve the capacitive load drive capa- bility of the op amp. VOUT S1N C1 S1P C5 R1 R1 gmVI gmVI gm2 C2 R2 Figure 36. Small Signal Schematic APPLICATION NOTES INPUT CHARACTERISTICS In the AD823, n-channel JFETs are used to provide a low offset, low noise, high impedance input stage. Minimum input common-mode voltage extends from 0.2 V below –VS to 1 V less than +VS. Driving the input voltage closer to the positive rail will cause a loss of amplifier bandwidth and increased common-mode voltage error. The AD823 does not exhibit phase reversal for input voltages up to and including +VS. Figure 37a shows the response of an AD823 voltage follower to a 0 V to +5 V (+VS) square wave input. The input and output are superimposed. The output polarity tracks the input polarity up to +VS—no phase reversal. The reduced bandwidth above a 4 V input causes the rounding of the output wave form. For input voltages greater than +VS, a resistor in series with the AD823’s plus input will prevent phase reversal, at the expense of greater input voltage noise. This is il- lustrated in Figure 37b. GND 10 90 100 0% 1V 2 µs 1V a. Response with RP = 0; VIN from 0 to VS +V S GND 10 90 100 0% 1V 1V 10µs 1V +5V V IN R P V OUT AD823 b. VIN = 0 to +VS + 200 mV; VOUT = 0 to +VS; RP = 49.9 kΩ Figure 37. AD823 Input Response |
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