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AD9632AR Datasheet(PDF) 13 Page - Analog Devices |
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AD9632AR Datasheet(HTML) 13 Page - Analog Devices |
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13 / 20 page ![]() REV. C AD9631/AD9632 –13– THEORY OF OPERATION General The AD9631 and AD9632 are wide bandwidth, voltage feedback amplifiers. Since their open-loop frequency response follows the conventional 6 dB/octave roll-off, their gain bandwidth product is basically constant. Increasing their closed-loop gain results in a corresponding decrease in small signal bandwidth. This can be observed by noting the bandwidth specification between the AD9631 (gain of +1) and AD9632 (gain of +2). The AD9631/ AD9632 typically maintain 65 degrees of phase margin. This high margin minimizes the effects of signal and noise peaking. Feedback Resistor Choice The value of the feedback resistor is critical for optimum perfor- mance on the AD9631 (gain of +1) and less critical as the gain increases. Therefore, this section is specifically targeted at the AD9631. At minimum stable gain (+1), the AD9631 provides optimum dynamic performance with RF = 140 W. This resistor acts as a parasitic suppressor only against damped RF oscillations that can occur due to lead (input, feedback) inductance and parasitic capacitance. This value of RF provides the best combination of wide bandwidth, low parasitic peaking, and fast settling time. In fact, for the same reasons, a 100 W–130 W resistor should be placed in series with the positive input for other AD9631 noninver- ting and all AD9631 inverting configurations. The correct connection is shown in Figures 3 and 4. AD9631/ AD9632 +VS –VS 100 –130 RTERM RIN VIN RG 0.1 F 10 F 0.1 F 10 F RF VOUT G = 1 + RF RG Figure 3. Noninverting Operation AD9631/ AD9632 +VS –VS 100 –130 RTERM RIN RG 0.1 F 10 F 0.1 F 10 F RF VOUT VIN G = – RF RG Figure 4. Inverting Operation When the AD9631 is used in the transimpedance (I to V) mode, such as in photodiode detection, the value of RF and diode capaci- tance (CI) are usually known. Generally, the value of RF selected will be in the k W range, and a shunt capacitor (CF) across RF will be required to maintain good amplifier stability. The value of CF required to maintain optimal flatness (<1 dB peaking) and settling time can be estimated as CC R R FO I F O F @ () [] 21 22 1 2 –/ where wO is equal to the unity gain bandwidth product of the amplifier in rad/sec, and CI is the equivalent total input capacitance at the inverting input. Typically wO = 800 106 rad/sec (see TPC 15). As an example, choosing RF = 10 k W and CI = 5 pF requires CF to be 1.1 pF (Note: CI includes both source and parasitic circuit capacitance). The bandwidth of the amplifier can be estimated using the CF calculated as f RC d FF 3 16 2 @ . AD9631 RF VOUT CI II CF Figure 5. Transimpedance Configuration For general voltage gain applications, the amplifier bandwidth can be closely estimated as f 21 R /R 3dB FG @ + () O This estimation loses accuracy for gains of +2/–1 or lower due to the amplifier’s damping factor. For these “low gain” cases, the bandwidth will actually extend beyond the calculated value (see TPCs 13 and 25). As a general rule, capacitor CF will not be required if RR C NG FG I () ¥£ 4 O where NG is the noise gain (1 + RF/RG) of the circuit. For most voltage gain applications, this should be the case. |
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