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OPA818 bảng dữ liệu(PDF) 10 Page - Texas Instruments |
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OPA818 bảng dữ liệu(HTML) 10 Page - Texas Instruments |
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10 / 27 page ![]() Frequency (Hz) 0 -180 8 -165 16 -150 24 -135 32 -120 40 -105 48 -90 56 -75 64 -60 72 -45 80 -30 88 -15 96 0 104 15 1k 10k 100k 1M 10M 100M 1G D027 AOL Magnitude (dB) AOL Phase (q) Frequency (Hz) 0 10 20 30 40 50 60 70 80 90 100 110 120 1k 10k 100k 1M 10M 100M 1G D106 TJ = 40qC TJ = 27qC TJ = 85qC 10 OPA818 SBOS940 – MAY 2019 www.ti.com Product Folder Links: OPA818 Submit Documentation Feedback Copyright © 2019, Texas Instruments Incorporated Feature Description (continued) indicating that the amplifier will not be stable in a gain of 1 V/V. Amplifiers like OPA818 that are not unity-gain stable are referred to as decompensated amplifiers. The decompensated architecture typically allows for higher GBWP, higher slew rate, and lower noise compared to a unity-gain stable amplifier with equivalent quiescent current. The additional advantage of the decompensated amplifier is better distortion performance at higher frequencies in high gain applications for comparable quiescent current to a unity-gain stable amplifier. OPA818 is stable in noise gain of 7 V/V (16.9 dB) or higher in conventional gain circuits as shown in Figure 6 and Figure 7. It has 790 MHz of SSBW in this gain configuration with approximately 50° phase margin. The high GBWP and low voltage and current noise of OPA818 make it a very suitable amplifier for wideband moderate to high transimpedance gain applications. Transimpedance gains of 50kΩ or higher benefit from the low current noise JFET input. In a typical transimpedance (TIA) circuit as shown in Figure 13, unity-gain stable amplifier is not a requirement. At low frequencies, the noise gain of TIA is 0 dB (1 V/V) and at high frequencies the noise gain is set by the ratio of the total input capacitance (CTOT) and the feedback capacitance (CF). To maximize TIA closed-loop bandwidth, the feedback capacitance is generally smaller than the total input capacitance. This results in the ratio of total input capacitance to the feedback capacitance to be greater than 1, which is ultimately the noise gain of the TIA at higher frequencies. The blog series, What you need to know about transimpedance amplifiers – part 1 and What you need to know about transimpedance amplifiers – part 2 describe TIA compensation techniques in greater detail. RL = 100 Ω Simulation Figure 10. Open-Loop Gain Magnitude and Phase Vs Frequency RL = 100 Ω Simulation Figure 11. Open-Loop Gain Magnitude vs Temperature 7.3.4 Low Input Capacitance Often two primary considerations for TIA applications are maximizing TIA closed-loop bandwidth and minimizing the total output noise to maximize Signal-to-Noise Ratio (SNR). The total input capacitance (CTOT) of TIA circuit causes a zero in the noise gain in combination with the transimpedance gain (feedback resistor, RF) at frequency 1/(2πRFCTOT). For a fixed RF, this zero is at a lower frequency for higher CTOT thus increasing the noise gain at lower frequency resulting in lower equivalent closed-loop bandwidth and higher total output noise compared to a lower CTOT. By choosing an amplifier like OPA818 that features a low input capacitance (2.4 pF combined common-mode and differential) for TIA application, the system designer can realize high closed-loop bandwidth at low total output noise or have the flexibility to choose a photodiode with relatively higher capacitance. The CTOT includes the input capacitance of the amplifier, the photodiode capacitance, and the PCB parasitic capacitance at the inverting input. |
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