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AD637JRZ-R7 数据表(PDF) 14 Page - Analog Devices |
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AD637JRZ-R7 数据表(HTML) 14 Page - Analog Devices |
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14 / 25 page ![]() AD637 Data Sheet Referring to Figure 8 for optional external gain and offset trim schematic. The following sections describe trimming for greater accuracy in detail. Offset Trim Ground the input signal (VIN) and adjust R1 until the output voltage at Pin 9 measures 0 V. Alternatively, apply the least expected value of VIN.at the input VIN and adjust R1 until the dc output voltage at Pin 9 measures the same value as the rms input. Scale Factor Trim Insert Resistor R4 in series with the input to decrease the range of the scale factor. Connect a precision source to Pin 13 and adjust the output for the desired full-scale input to VIN, using either a calibrated dc or 1 kHz ac voltage, and adjust Resistor R3 to give the correct output at Pin 9 (that is, 1 V rms at the input results in a dc output voltage of 1.000 V dc). A 2 V p-p sine wave input yields 0.707 V dc at the output. Remaining errors are due to the nonlinearity. 25kΩ –VS –VS –VS 1 25kΩ DEN INPUT CAV BUFF IN BUFF OUT CS dB OUTPUT 3 COMMON ABSOLUTE VALUE BIAS 2 NIC 4 OUTPUT OFFSET 4.7kΩ 5 6 7 8 9 10 11 12 NIC 13 14 NC VIN VIN R4 147Ω CAV + R3 1kΩ R2 1MΩ R1 50kΩ +VS +VS +VS +VS OUTPUT OFFSET TRIM SCALE FACTOR TRIM AD637 RMSOUT SQUARER/ DIVIDER – + – + RMS OUT – + NIC = NO INTERNAL CONNECTION Figure 8. Optional External Gain and Offset Trims CHOOSING THE AVERAGING TIME CONSTANT The AD637 computes the true rms value of both dc and ac input signals. For dc inputs, the output tracks the absolute value of the input exactly. However, when the voltage is ac, the converted dc output voltage asymptotically approaches the theoretical rms value of the input. The deviation from the ideal rms value is due to the implicit denominator inherent to averag- ing over an infinite time span. Because the error diminishes as the averaging period increases, it quickly becomes negligible. The remaining error components are the ac ripple and dc offset voltage, if any. The ac and averaging error components are both functions of the input-frequency (f) and the averaging time constant τ (τ: 25 ms/µF of averaging capacitance). Figure 9 shows the output errors, which are enlarged for clarity. The frequency of the ac component (ripple) is twice the frequency of the input, the dc error is the RSS sum of the average rectified error and any fixed value dc offset. The value of CAV and the 25 kΩ feedback resistor establish the averaging time constant, and solely determines the magnitude of the rms-to-dc conversion error. Furthermore, any post- conversion filtering does not improve the dc component composite result. Equation 1 defines the approximate peak value of the ac ripple component of the composite output. ) / 1 ( where reading of % in 3 . 6 50 f f > τ τ (1) DOUBLE-FREQUENCY RIPPLE EO TIME AVERAGE ERROR IDEAL EO DC ERROR = AVERAGE OF OUTPUT – IDEAL Figure 9. Enlarged Composite Conversion Result for a Sinusoidal Input Increasing the value of the averaging capacitor or adding a post- rms filter network reduces the ripple error. The dc error appears as a frequency dependent offset at the output of the AD637 and follows the relationship reading of % in 4 . 6 16 . 0 1 2 2 f τ + SINE WAVE INPUT FREQUENCY (Hz) 100 0.1 1.0 10 10k 1k 100 10 DC ERROR PEAK RIPPLE Figure 10. Comparison of Percent DC Error to the Percent Peak Ripple over Frequency Using the AD637 in the Standard RMS Connection with a 1 × µF CAV The ac ripple component of averaging error is greatly reduced by increasing the value of the averaging capacitor. However, the value of the averaging capacitor increases exponentially while the settling time increases directly proportion to the value of the averaging capacitor (TS = 115 ms/µF of averaging capacitance). Rev. L | Page 14 of 25 |
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