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ADA4817-1ARDZ-R7 数据表(PDF) 24 Page - Analog Devices |
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ADA4817-1ARDZ-R7 数据表(HTML) 24 Page - Analog Devices |
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24 / 29 page ![]() Data Sheet ADA4817-1/ADA4817-2 APPLICATIONS INFORMATION analog.com Rev. H | 24 of 29 LOW DISTORTION PINOUT The ADA4817-1/ADA4817-2 feature a low distortion pinout from Analog Devices. The new pinout provides two advantages over the traditional pinout. The first advantage is improved second harmonic distortion performance, which is accomplished by the physical sep- aration of the noninverting input pin and the negative power supply pin. The second advantage is the simplification of the layout due to the dedicated feedback pin and easy routing of the gain set resistor back to the inverting input pin. This pinout allows a compact layout, which helps to minimize parasitics and increase stability. The designer does not need to use the dedicated feedback pin to provide feedback for the ADA4817-1/ADA4817-2. The output pin of the ADA4817-1/ADA4817-2 can still be used to provide feedback to the inverting input of the ADA4817-1/ADA4817-2. WIDEBAND PHOTODIODE PREAMP The wide bandwidth and low noise of the ADA4817-1/ADA4817-2 make it an ideal choice for transimpedance amplifiers, such as those used for signal conditioning with high speed photo-diodes. Figure 63 shows a current to voltage converter with an electrical model of a photodiode. The basic transfer function is VOUT=IPHOTO×RF 1+sCFRF (12) where: IPHOTO is the output current of the photodiode. RF and CF are the parallel combination that sets the signal band- width. Figure 63. Wideband Photodiode Preamp The stable bandwidth attainable with this preamp is a function of RF, the gain bandwidth product of the amplifier, and the total capacitance at the summing junction of the amplifier, including the photodiode capacitance (CS) and the amplifier input capacitance. RF and the total capacitance produce a pole in the loop transmis- sion of the amplifier that can result in peaking and instability. Adding CF creates a zero in the loop transmission that compensates for the effect of the pole and reduces the signal bandwidth. It can be shown that the signal bandwidth obtained with a 45° phase margin (f(45)) is defined by f45 = fCR 2π×RF× CS+CM+CD (13) where: fCR is the amplifier crossover frequency. RF is the feedback resistor. CS is the source capacitance including the photodiode and the board parasitic. CM is the common-mode capacitance of the amplifier. CD is the differential capacitance of the amplifier. The CF value that produces f(45) is shown to be CF= CS+CM+CD 2π×RF×fCR (14) The frequency response shows less peaking if larger CF values are used. Figure 64 shows the preamplifier output noise over frequency. Figure 64. Photodiode Voltage Noise Contributions Figure 65. Photodiode Preamp Frequency Response The pole in the loop transmission translates to a zero in the noise gain of the amplifier, leading to an amplification of the input voltage noise over frequency. |
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