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AD8510ARM-R2 数据表(PDF) 17 Page - Analog Devices |
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AD8510ARM-R2 数据表(HTML) 17 Page - Analog Devices |
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17 / 20 page ![]() AD8510/AD8512/AD8513 Rev. E | Page 17 of 20 I-V CONVERSION APPLICATIONS Photodiode Circuits Common applications for I-V conversion include photodiode circuits, where the amplifier is used to convert a current emitted by a diode placed at the positive input terminal into an output voltage. The AD8510/AD8512/AD8513’s low input bias current, wide bandwidth, and low noise make them each an excellent choice for various photodiode applications, including fax machines, fiber optic controls, motion sensors, and bar code readers. The circuit shown in Figure 53 uses a silicon diode with zero bias voltage. This is known as a Photovoltaic Mode; this configuration limits the overall noise and is suitable for instrumentation applications. 4 7 3 6 2 AD8510 Cf R2 Rd Ct VEE VCC Figure 53. Equivalent Preamplifier Photodiode Circuit A larger signal bandwidth can be attained at the expense of additional output noise. The total input capacitance (Ct) consists of the sum of the diode capacitance (typically 3 pF to 4 pF) and the amplifier’s input capacitance (12 pF), which includes external parasitic capacitance. Ct creates a pole in the frequency response, which may lead to an unstable system. To ensure stability and optimize the bandwidth of the signal, a capacitor is placed in the feedback loop of the circuit shown in Figure 53. It creates a zero and yields a bandwidth whose corner frequency is 1/(2π(R2Cf)). The value of R2 can be determined by the ratio V/ID, where V is the desired output voltage of the op amp and ID is the diode current. For example, if ID is 100 µA and a 10 V output voltage is desired, R2 should be 100 kΩ. Rd is a junction resistance that drops typically by a factor of 2 for every 10°C increase in temperature. A typical value for Rd is 1000 MΩ. Since Rd >> R2, the circuit behavior is not impacted by the effect of the junction resistance. The maximum signal bandwidth is Ct R ft f MAX 2 2π = where ft is the unity gain frequency of the amplifier. Using the parameters above, Cf ≈ 1 pF, which yields a signal bandwidth of about 2.6 MHz. ft R Ct Cf 2 2π = where ft is the unity gain frequency of the op amp, achieves a phase margin, Φm, of approximately 45°. A higher phase margin can be obtained by increasing the value of Cf. Setting Cf to twice the previous value yields approximately Φm = 65° and a maximally flat frequency response, but reduces the maximum signal bandwidth by 50%. |
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