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INA821 Datasheet(PDF) 19 Page - Texas Instruments |
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INA821 Datasheet(HTML) 19 Page - Texas Instruments |
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19 / 36 page ![]() 10 30 50 70 90 110 10M 100M 1G 10G Frequency (Hz) C001 10 30 50 70 90 110 10M 100M 1G 10G Frequency (Hz) C001 EMIRR (dB) 2 RF _ PEAK 20 OS P V V 10 100 mV § · ¨ ¸ © ¹ § · ¨ ¸ ' ˜ ¨ ¸ © ¹ 19 INA821 www.ti.com SBOS893 – AUGUST 2018 Product Folder Links: INA821 Submit Documentation Feedback Copyright © 2018, Texas Instruments Incorporated 8.3.1.1 Gain Drift The stability and temperature drift of the external gain setting resistor (RG) affects gain. The contribution of RG to gain accuracy and drift is determined from Equation 1. The best gain drift of 5 ppm/ ℃ (maximum) is achieved when the INA821 uses G = 1 without RG connected. In this case, gain drift is limited by the slight mismatch of the temperature coefficient of the integrated 10-kΩ resistors in the differential amplifier (A3). At gains greater than 1, gain drift increases as a result of the individual drift of the 24.7-kΩ resistors in the feedback of A1 and A2 relative to the drift of the external gain resistor (RG.) The low temperature coefficient of the internal feedback resistors significantly improves the overall temperature stability of applications using gains greater than 1 V/V over alternate options. Low resistor values required for high gain make wiring resistance important. Sockets add to the wiring resistance and contribute additional gain error (such as a possible unstable gain error) at gains of approximately 100 or greater. To ensure stability, avoid parasitic capacitance of more than a few picofarads at RG connections. Careful matching of any parasitics on the RG pins maintains optimal CMRR over frequency; see Figure 17. 8.3.2 EMI Rejection Texas Instruments developed a method to accurately measure the immunity of an amplifier over a broad frequency spectrum extending from 10 MHz to 6 GHz. This method uses an EMI rejection ratio (EMIRR) to quantify the ability of the INA821 to reject EMI. The offset resulting from an input EMI signal is calculated using Equation 2: where • VRF_PEAK is the peak amplitude of the input EMI signal. (2) Figure 52 and Figure 53 show the INA821 EMIRR graph for differential and common-mode EMI rejection across this frequency range. Table 2 shows the EMIRR values for the INA821 at frequencies encountered in real-world applications. Applications listed in Table 2 are centered on or operated near the particular frequency shown. Depending on the end-system requirements, additional EMI filters may be required near the signal inputs of the system, as well as incorporating known good practices such as using short traces, low-pass filters, and damping resistors combined with parallel and shielded signal routing. Figure 52. Common-Mode EMIRR Testing Figure 53. Differential Mode EMIRR Testing Table 2. INA821 EMIRR for Frequencies of Interest FREQUENCY APPLICATION OR ALLOCATION DIFFERENTIAL EMIRR COMMON-MODE EMIRR 400 MHz Mobile radio, mobile satellite, space operation, weather, radar, ultrahigh- frequency (UHF) applications 48 dB 87 dB |
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