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ADL5513ACPZ-R7 数据表(PDF) 16 Page - Analog Devices |
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ADL5513ACPZ-R7 数据表(HTML) 16 Page - Analog Devices |
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16 / 25 page ![]() ADL5513 Data Sheet Rev. A | Page 16 of 25 ERROR CALCULATIONS The measured transfer function of the ADL5513 at 100 MHz is shown in Figure 31. The figure shows plots of measured output voltage, calculated error, and an ideal line. The input power and output voltage are used to calculate the slope and intercept values. The slope and intercept are calculated using linear regression over the input range from −40 dBm to −20 dBm. The slope and intercept terms are used to generate an ideal line. The error is the difference in measured output voltage compared to the ideal output line. 3.0 2.5 2.0 1.5 1.0 0.5 0 –0.5 –1.0 –1.5 –2.0 –2.5 –3.0 PIN (dBm) IDEAL LINE VOUT AND ERROR @ +25°C VOUT AND ERROR @ –40°C VOUT AND ERROR @ +85°C PIN2 PIN1 VOUT2 VOUT1 2.4 2.2 2.0 1.8 1.6 1.4 1.2 1.0 0.8 0.6 0.4 0.2 0 Figure 31. Typical Output Voltage vs. Input Signal The equation for output voltage can be written as VOUT = Slope × (PIN − Intercept) where: Slope is the change in output voltage divided by the change in input power, PIN. Slope is expressed in volts per decibel (V/dB). Intercept is the calculated power in decibels (dB) at which the output voltage is 0 V. Note that VOUT = 0 V can never be achieved. Calibration is performed by applying two known signal levels to the ADL 5513 and measuring the corresponding voltage outputs. The calibration points are in general chosen to be within the linear-in-dB range of the device. Calculation of the slope and intercept are accomplished by using the following equations: IN2 IN1 2 MEASURED OUT 1 MEASURED OUT P P V V Slope − − = ) ( ) ( Slope V P Intercept MEASURED OUT IN1 ) ( − = Once the slope and intercept are calculated, VOUT(IDEAL)can be calculated, and the error is determined using the following equation: Slope V V Error IDEAL OUT MEASURED OUT ) ( ) ( ) ( − = Figure 31 shows a plot of the error at 25°C, the temperature at which the device is calibrated. Error is not 0 dB over the full dynamic range. This is because the log amp does not perfectly follow the ideal VOUT vs. PIN equation, even within its operating range. The error at the calibrating points of −20 dBm and −40 dBm is equal to 0 dB by definition. Figure 31 also shows error plots for output voltages measured at −40°C and 85°C. These error plots are calculated using slope and intercept at 25°C, which is consistent in a mass-production environment, where calibration over temperature is not practical. This is a measure of the linearity of the device. Error from the linear response to the CW waveform is not a measure of absolute accuracy because it is calculated using the slope and intercept of each device. However, error verifies the linearity of the devices. Similarly, at temperature extremes, error represents the output voltage variations from the 25°C ideal line performance. Data presented in the graphs are the typical error distributions observed during characterization of the ADL5513. Device performance was optimized for operation at 85°C; this can be changed by changing the voltage at TADJ. ADJUSTING ACCURACY THROUGH CHOICE OF CALIBRATION POINTS Choose calibration points to suit the specific application, but usually they should be in the linear range of the log amp. In some applications, very high accuracy is required at a reduced input range; in other applications, good linearity is necessary over the full power input range. The linearity of the transfer function can be adjusted by choice of calibration points. Figure 32 and Figure 33 show plots for a typical device at 3600 MHz as an exam- ple of adjusting accuracy through choice of calibration points. 2.50 2.25 2.00 1.75 1.50 1.25 1.00 0.75 0.50 0.25 0 2.5 2.0 1.5 1.0 0.5 0 –0.5 –1.0 –1.5 –2.0 –2.5 –70 –65 –60 –55 –50 –45 –40 –35 –30 –25 –20 –15 –10 –5 0 5 10 PIN (dBm) +25°C –40°C +85°C +125°C Figure 32. Typical Device at 3600 MHz, Calibration Points at PIN = −20 dBm and −40 dBm |
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