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ADL5906SCPZN-R7 数据表(PDF) 24 Page - Analog Devices

部件名 ADL5906SCPZN-R7
功能描述  10 MHz to 10 GHz, 67 dB TruPwr Detector
PDF  30 Pages
Scroll/Zoom Zoom In 100%  Zoom Out
制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADL5906SCPZN-R7 数据表(HTML) 24 Page - Analog Devices

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Data Sheet
ADL5906
THEORY OF OPERATION
analog.com
Rev. B | 24 of 30
SYSTEM CALIBRATION AND ERROR
CALCULATION
The measured transfer function of the ADL5906 at 2.14 GHz is
shown in Figure 53, which contains plots of both output voltage vs.
input level and linearity error vs. input level. As the input level varies
from −65 dBm to +5 dBm, the output voltage varies from ~0.25 V to
~3.9 V.
Figure 53. 2.14 GHz VRMS and Log Conformance Error at +25°C, −40°C, and
+85°C Using Two-Point Calibration at 0 dBm and −40 dBm
Because slope and intercept vary from device to device, board
level calibration must be performed to achieve high accuracy. The
equation for the idealized output voltage can be written as
VRMS(IDEAL) = Slope × (PIN − Intercept)
(13)
where:
Slope is the change in output voltage divided by the change in input
power (dB).
Intercept is the calculated input power level at which the output
voltage is equal to 0 V (note that Intercept is an extrapolated
theoretical value and not a measured value).
In general, calibration is performed during equipment manufacture
by applying two or more known signal levels to the input of the
ADL5906 and measuring the corresponding output voltages. The
calibration points must be within the linear operating range of the
device.
With a two-point calibration, the slope and intercept are calculated
as follows:
Slope = (VRMS1 − VRMS2)/(PIN1 − PIN2)
(14)
Intercept = PIN1 − (VRMS1/Slope)
(15)
After the slope and intercept are calculated and stored in nonvola-
tile memory during equipment calibration, an equation can be used
to calculate an unknown input power based on the output voltage of
the detector.
PIN (Unknown) = (VRMS(MEASURED)/Slope) + Intercept
(16)
The log conformance error is the difference between this straight
line and the actual performance of the detector.
Error (dB) = (VRMS(MEASURED) − VRMS(IDEAL))/Slope
(17)
Figure 53 includes a plot of this error at +25°C, −40°C, and +85°C
when using a two-point calibration (calibration points are 0 dBm and
−40 dBm). The error at the calibration points at 25°C (in this case,
−40 dBm and 0 dBm) is equal to 0 dB by definition.
The residual nonlinearity of the transfer function that is apparent
in the two-point calibration error plot can be reduced by increasing
the number of calibration points. System Calibration and Error
Calculation shows the post-calibration error plots for a three-point
calibration. With a multipoint calibration, the transfer function is
segmented, with each segment having its own slope and intercept.
Multiple known power levels (three levels in this case) are applied,
and multiple voltages are measured. When the equipment is in
operation, the measured voltage from the detector is first used
to determine which of the stored slope and intercept calibration
coefficients are to be used. Then, the unknown power level is
calculated by inserting the appropriate slope and intercept values
into Equation 16.
When choosing calibration points, there is no requirement for, or
value in, equal spacing between the points. There is also no limit
to the number of calibration points used. However, when more
calibration points are used, calibration time increases.
Figure 54. 2.14 GHz VRMS and Log Conformance Error at +25°C, −40°C, and
+85°C Using Three-Point Calibration at 0 dBm, −40 dBm, and −55 dBm
The −40°C and +85°C error plots in Figure 54 are generated
using the +25°C slope and intercept values. This is consistent
with equipment calibration in a mass production environment where
calibration of multiple temperatures is not practical.
USING VTEMP TO IMPROVE INTERCEPT
TEMPERATURE DRIFT
In applications where VTEMP and VRMS are both being digitized by
an ADC, the VTEMP voltage can be used to further improve the
temperature drift of the ADL5906.



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