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ADA4927-2YCPZ-R2 数据表(PDF) 17 Page - Analog Devices |
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ADA4927-2YCPZ-R2 数据表(HTML) 17 Page - Analog Devices |
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17 / 24 page ![]() ADA4927-1/ADA4927-2 Rev. 0 | Page 17 of 24 APPLICATIONS INFORMATION ANALYZING AN APPLICATION CIRCUIT The ADA4927 uses high open-loop transimpedance and negative current feedback to control its differential output voltage in such a way as to minimize the differential error currents. The differential error currents are defined as the currents that flow in and out of the differential inputs labeled +IN and −IN (see Figure 46). For most purposes, these currents can be assumed to be zero. The voltage between the +IN and −IN inputs is internally bootstrapped to 0 V; therefore, the voltages at the amplifier inputs are equal, and external analysis can be carried out in a similar fashion to that of voltage feedback amplifiers. Similarly, the difference between the actual output common- mode voltage and the voltage applied to VOCM can also be assumed to be zero. Starting from these principles, any application circuit can be analyzed. SETTING THE CLOSED-LOOP GAIN Using the approach previously described, the differential gain of the circuit in Figure 46 can be determined by G F dm IN dm OUT R R V V = , , This presumes that the input resistors (RG) and feedback resistors (RF) on each side are of equal value. ESTIMATING THE OUTPUT NOISE VOLTAGE The differential output noise of the ADA4927 can be estimated using the noise model in Figure 47. The input-referred noise voltage density, vnIN, is modeled as a differential input, and the noise currents, inIN− and inIN+, appear between each input and ground. The output voltage due to vnIN is obtained by multiplying vnIN by the noise gain, GN (defined in the GN equation). The noise currents are uncorrelated with the same mean-square value, and each produces an output voltage that is equal to the noise current multiplied by the associated feedback resistance. The noise voltage density at the VOCM pin is vnCM. When the feedback networks have the same feedback factor, as in most cases, the output noise due to vnCM is common mode. Each of the four resistors contributes (4kTRxx)1/2. The noise from the feedback resistors appears directly at the output, and the noise from each gain resistor appears at the output multiplied by RF/RG. Table 11 summarizes the input noise sources, the multiplication factors, and the output-referred noise density terms. ADA4927 + RF2 VnOD VnCM VOCM VnIN RF1 RG2 RG1 VnRF1 VnRF2 VnRG1 VnRG2 inIN+ inIN– Figure 47. Noise Model Table 11. Output Noise Voltage Density Calculations for Matched Feedback Networks Input Noise Contribution Input Noise Term Input Noise Voltage Density Output Multiplication Factor Differential Output Noise Voltage Density Term Differential Input vnIN vnIN GN vnO1 = GN(vnIN) Inverting Input inIN inIN × (RF2) 1 vnO2 = (inIN)(RF2) Noninverting Input inIN inIN × (RF1) 1 vnO3 = (inIN)(RF1) VOCM Input vnCM vnCM 0 vnO4 = 0 Gain Resistor, RG1 vnRG1 (4kTRG1)1/2 RF1/RG1 vnO5 = (RF1/RG1)(4kTRG1)1/2 Gain Resistor, RG2 vnRG2 (4kTRG2)1/2 RF2/RG2 vnO6 = (RF2/RG2)(4kTRG2)1/2 Feedback Resistor, RF1 vnRF1 (4kTRF1)1/2 1 vnO7 = (4kTRF1)1/2 Feedback Resistor, RF2 vnRF2 (4kTRF2)1/2 1 vnO8 = (4kTRF2)1/2 |
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