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ADL5507ACBZ-R7 Folha de dados(PDF) 28 Page - Analog Devices

Nome de Peças ADL5507ACBZ-R7
Descrição Electrónicos  10 MHz to 12 GHz, 55 dB Logarithmic RF Power Detector
PDF  34 Pages
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Fabricante Electrônico  AD [Analog Devices]
Página de início  http://www.analog.com
Logo AD - Analog Devices

ADL5507ACBZ-R7 Folha de dados(HTML) 28 Page - Analog Devices

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Data Sheet
ADL5507
THEORY OF OPERATION
analog.com
Rev. 0 | 28 of 34
The ADL5507 is a logarithmic detector (log amp), based on
the principle of successive compression. It is fabricated on an
advanced BiCMOS process. It comes in a smaller 0.8 mm × 1.2
mm WLCSP package and offers 12 GHz RF bandwidth. Functional
Block Diagram shows the main features of the ADL5507 in block
schematic form.
The ADL5507 combines two key functions needed for the measure-
ment of signal level over a moderately wide dynamic range. First,
it provides the amplification needed to respond to small signals in
a chain of four amplifier/limiter cells, each having a small signal
gain of 13 dB and a bandwidth of approximately 12 GHz. At the
output of each amplifier stage is a full wave rectifier, essentially a
square law detector cell that converts the RF signal voltages to a
fluctuating current with an average value that increases with signal
level. A further passive detector stage is added preceding the first
stage. Therefore, there are five detectors, each separated by 13
dB, giving about 52 dB of total gain and approximately 55 dB of
dynamic range. The overall accuracy at the extremes of this total
range, viewed as the deviation from an ideal logarithmic response,
that is, the log conformance error, can be judged by referencing
the figure in the Typical Performance Characteristics section, which
show that errors across the central 55 dB are moderate. These
figures show how the conformance to an ideal logarithmic function
varies with temperature, frequency, and supply voltage.
The output of these detector cells is in the form of a differential
current, making their summation a simple matter. It can easily be
shown that such summation closely approximates a logarithmic
function. The summed differential current polarity can be swapped
(thereby changing the slope polarity) by setting the ENBL pin
voltage to VPOS/2 (or floating) for negative slope or VPOS for
positive slope. This result is then converted to a voltage at the
VLOG pin through a high gain stage. This output is connected back
to a voltage-to-current (V-to-I) stage, in such a manner that VVLOG
is a logarithmic measure of the RF input voltage with a slope and
intercept controlled by the design. For a fixed termination resistance
at the input of the ADL5507, a given voltage corresponds to a
certain power level.
The external termination added before the ADL5507 determines the
effective power scaling. This often takes the form of a simple resis-
tor (51 Ω provides a net 50 Ω input), but more elaborate matching
networks can be used. This impedance determines the logarithmic
intercept, the input power for which the output crosses the baseline
(VVLOG = 0 V) if the function were continuous for all values of input.
Because this is never the case for a practical log amp, the intercept
refers to the value obtained by the minimum error, straight line fit
to the actual graph of VVLOG vs. input power. The quoted values
in Specifications assume a sinusoidal (CW) signal. In the place
of complex modulation, as in 5G-NR, the calibration of the power
response needs to be adjusted accordingly. Where a true power
(waveform independent) response is needed, consider the use of
an rms responding detector, such as the ADL5906.
However, in terms of the logarithmic slope, the amount by which
the output VVLOG changes for each decibel of input change (voltage
or power), is, in principle, independent of waveform or termination
impedance. In practice, it usually falls off at higher frequencies
because of the declining gain of the amplifier stages and other
effects in the detector cells. The ADL5507, at 3.6 GHz, has a typical
slope of 18.7 mV/dB in Positive Slope mode, and −18.7 mV/dB in
Negative Slope mode. These values are sensibly independent of
temperature and almost completely unaffected by supply voltages
of 2.7 V to 3.45 V.



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