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ADL6012SCPZN-R2 数据表(PDF) 22 Page - Analog Devices |
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ADL6012SCPZN-R2 数据表(HTML) 22 Page - Analog Devices |
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22 / 24 page ![]() ADL6012 Data Sheet Rev. 0 | Page 22 of 24 The following equations are used to calculate the slope and intercept of each device, which is used in calibration to improve the detection accuracy: Slope = (VOUT2 − VOUT1)/(VPEAK2 − VPEAK1) (1) Intercept = VOUT1 − (Slope × VPEAK1) (2) The error conformance is calculated as follows: Error = 20 × log((VOUT − Intercept)/(Slope × VPEAK)) (3) where: VOUT2 is the output voltage with VPEAK2 input. VOUT1 is the output voltage with VPEAK1 input. VOUT is the differential envelope output voltage at different input levels. VPEAK1 and VPEAK2 are input peak voltages at two different input levels. VPEAK is the peak voltage input. The ADL6012 offers extremely stable temperature performance across frequencies. See Figure 25 to Figure 35 for the temperature drift error from −55°C to +125°C. The typical temperature drift is less than 1 dB of error over the entire detection range of the device from 2 GHz to 67 GHz. This makes the device well suited for applications operating over a wide temperature range. Temperature drift error relative to 25°C is calculated as follows: Temperature Drift Error (dB) = (VOUT (TEMPERATURE) − VOUT (AT 25°C))/(dVOUT/dPIN) (4) where: VOUT is the differential envelope output. dVOUT/dPIN is the derivative of the transfer function of the differential VENV± output at 25°C vs. the input power. |
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