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AD8318 Datasheet(PDF) 16 Page - Analog Devices

Part # AD8318
Description  1 MHz to 8 GHz, 60 dB Logarithmic Detector/Controller
PDF  24 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

AD8318 Datasheet(HTML) 16 Page - Analog Devices

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AD8318
Rev. A | Page 16 of 24
Using the equation for the ideal output voltage (7) as a reference, the
log conformance error of the measured data can be calculated
Error(dB) = (VOUT(MEASURED) − VOUT(IDEAL))/Slope
(12)
Figure 31 includes a plot of the error at 25°C, the temperature at
which the log amp is calibrated. Note that the error is not zero. This
is because the log amp does not perfectly follow the ideal VOUT vs. PIN
equation, even within its operating region. The error at the calibra-
tion points (−12 dBm and −52 dBm, in this case) is, however, equal
to zero by definition.
Figure 31 includes error plots for the output voltage at −40°C and
+85°C. These error plots are calculated using the slope and intercept
at 25°C. This method is consistent with a mass-production environ-
ment where calibration at temperature is not practical.
SELECTING CALIBRATION POINTS TO IMPROVE
ACCURACY OVER A REDUCED RANGE
In some applications, very high accuracy is required at just one
power level or over a reduced input range. For example, in a wireless
transmitter, the accuracy of the high power amplifier (HPA) is most
critical at, or close to, full power.
Figure 32 shows the same measured data as Figure 31. Note that
accuracy is very high from −10 dBm to −30 dBm. Below −30 dBm,
the error increases to about −1 dB. This is because the calibration
points have changed to −14 dBm and −26 dBm.
2.2
2.0
1.8
1.6
1.4
1.2
1.0
0.6
0.4
0.2
2.5
2.0
1.5
1.0
0.5
0
–0.5
–1.0
–1.5
–2.0
–2.5
–65 –60 –55 –50 –45 –40 –35 –30
–20
–10
–5
0
5
PIN (dBm)
PIN1
PIN2
ERROR +25
°C
ERROR –40
°C
ERROR +85
°C
VOUT +25°C
VOUT –40°C
VOUT +85°C
VOUT2
VOUT1
Figure 32. Output Voltage and Error vs. PIN with 2-Point Calibration at
−10 dBm and −30 dBm
Calibration points are chosen to suit the application at hand. In
general, the calibration points are never chosen in the nonlinear
portion of the transfer function of the log amp (above −5 dBm or
below −60 dBm, in this case).
Figure 33 shows how calibration points can be adjusted to
increase dynamic range, but at the expense of linearity. In this
case, the calibration points for slope and intercept are set at
−4 dBm and −60 dBm. These points are at the end of the linear
range of the device.
Once again, at 25°C, an error of 0 dB is seen at the calibration
points. Note also that the range over which the AD8318
maintains an error of < ±1 dB is extended to 60 dB at 25°C and
58 dB over temperature. The disadvantage of this approach is
that linearity suffers, especially at the top end of the input range.
2.2
2.0
1.8
1.6
1.4
1.2
1.0
0.8
0.6
0.4
0.2
–65 –60 –55 –50 –45 –40 –35 –30 –25 –20 –15 –10 –5
0
5
PIN (dBm)
2.5
–2.5
–2.0
–1.5
–1.0
–0.5
0
0.5
1.0
1.5
2.0
VOUT +25°C
VOUT –40°C
VOUT +85°C
ERROR +25
°C
ERROR –40
°C
ERROR +85
°C
58dB DYNAMIC RANGE (
±1dB ERROR)
Figure 33. Dynamic Range Extension by Choosing Calibration Points
Close to the End of the Linear Range
Another way of presenting the error function of a log amp
detector is shown in Figure 34. In this case, the dB error at hot
and cold temperatures is calculated with respect to the output
voltage at ambient. This is a key difference in comparison to the
plots in Figure 32 and Figure 33. Previously, all errors were
calculated with respect to the ideal transfer function at ambient.
When this alternative technique is used, the error at ambient
becomes, by definition, equal to 0 (see Figure 34)
. This is valid
if the device transfer function perfectly follows the ideal
VOUT = Slope × (Pin - Intercept) equation. However, because a
log amp in practice never perfectly follows this equation
(especially outside of its linear operating range), this plot tends
to artificially improve linearity and extend the dynamic range.
This plot is a useful tool for estimating temperature drift at a
particular power level with respect to the (nonideal) output
voltage at ambient. However, to achieve this level of accuracy in
an end application requires calibration at multiple points in the
operating range of the device.



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