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AD823AARMZ-R7 Datasheet(PDF) 16 Page - Analog Devices |
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AD823AARMZ-R7 Datasheet(HTML) 16 Page - Analog Devices |
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16 / 20 page ![]() AD823A Data Sheet Rev. | Page 16 of 20 WIDEBAND PHOTODIODE PREAMP – + VOUT VB CD CM CM AD823A RSH = 10 11 Ω CS IPHOTO CF RF Figure 42. Wideband Photodiode Preamp The AD823A is an excellent choice for photodiode preamp application. Its low input bias current minimizes the DC error at the preamp output. In addition, its high gain bandwidth product and low input capacitance maximizes the signal bandwidth of the photodiode preamp. Figure 42 shows the AD823A as a current-to-voltage (I/V) converter with an electrical model of a photodiode. The transimpedance gain of the photodiode preamp can be described by the basic transfer function: F F F PHOTO OUT R sC R I V + × = 1 (1) where IPHOTO is the output current of the photodiode, and the parallel combination of RF and CF sets the signal bandwidth (see the I to V gain curve in Figure 43). Note that one should set RF such that the maximum attainable output voltage corresponds to the maximum diode current IPHOTO. This allows one to utilize the full output swing. The signal bandwidth that is attainable with this preamp is a function of RF, the gain bandwidth product (fu) of the amplifier, and the total capacitance at the amplifier summing junction, including CS and the amplifier input capacitance CD and CM. RF and the total capacitance produce a pole with loop frequency (fp). S F p C R f π 2 1 = (2) With the additional pole from the amplifier’s open loop response, the two-pole system results in peaking and instability due to an insufficient phase margin (Figure 43(A), Without Compensation). Adding CF creates a zero in the loop transmission that compensates for the effect of the input pole. This stabilizes the photodiode preamp design because of the increased phase margin. It also sets the signal bandwidth (Figure 43(B), With Compensation). The signal bandwidth and the zero frequency are determined by F F z C R f π 2 1 = (3) Setting the zero at the frequency fx maximizes the signal bandwidth with a 45° phase margin. Since fx is the geometric mean of fp and fu, it can be calculated by u p x f f f × = (4) Combining Equation 2, Equation 3 and Equation 4, the value of CF that produces fx is defined by u F S F f R C C × × = π 2 (5) The frequency response in this case shows about 2 dB of peaking and 15% overshoot. Doubling CF and cutting the bandwidth in half results in a flat frequency response with about 5% transient overshoot. B |
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