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ADL5507ACBZ-R7 Folha de dados(PDF) 29 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) 29 Page - Analog Devices

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Data Sheet
ADL5507
APPLICATIONS INFORMATION
analog.com
Rev. 0 | 29 of 34
BASIC CONNECTIONS
Figure 82 shows the basic connections for measurement mode.
A supply voltage of 2.7 V to 3.45 V is required. Decouple the
supply to the VPOS pin with a low inductance 0.1 µF surface-mount
ceramic capacitor. A series resistor of about 10 Ω can be added;
this resistor slightly reduces the supply voltage to the ADL5507 and
depends on the load resistance at the output to ground. Avoid its
use in applications where the power supply voltage is very low. A
series inductor provides similar power supply filtering with minimal
drop in supply voltage.
Figure 82. Basic Connections
The ADL5507 has an internal input coupling capacitor. This elim-
inates the need for external AC coupling. In this example, a
broadband input match is achieved by connecting a 51 Ω resistor
between RFIN and ground. This resistance combines with the inter-
nal input impedance to give an overall broadband input resistance
of 50 Ω. Several other coupling methods are possible; these are
described in the Input Coupling Options section.
Figure 83 shows the typical logarithmic conformance at 3.6 GHz.
Figure 83. VVLOG and Log Conformance Error vs. Input Level at 3.6 GHz
TRANSFER FUNCTION IN TERMS OF SLOPE
AND INTERCEPT
The transfer function of the ADL5507 is characterized in terms of its
slope and intercept. The logarithmic slope is defined as the change
in the VLOG output voltage for a 1 dB change in RF power level at
the RF input. For the ADL5507, the slope is nominally 18.7 mV/dB
in positive slope response mode. Therefore, a 10 dB change at
the input results in a change at the output of approximately 187
mV. Figure 83 shows the range over which the device maintains
its constant slope. The dynamic range can be defined as the range
over which the error remains within a certain band, usually ±1 dB
or ±3 dB. In Figure 83 for example, the ±1 dB dynamic range is
approximately 55 dB (from −56 dBm to −1 dBm), and the ±3 dB
dynamic range is approximately 62 dB (from −60.5 dBm to +1.5
dBm).
The intercept is the point at which the extrapolated linear response
intersects the horizontal axis (see Figure 83). Using the slope and
intercept, calculate the output voltage for any input level within the
specified input range, or calculate the input level from the output
voltage by the following complementary equations:
VVLOG=SLOPE× PIN−INTERCEPT (1)
PIN=VVLOGSLOPE+INTERCEPT
(2)
where:
VVLOG is the power detector output voltage, in millivolts.
PIN is the input signal level, expressed in decibels relative to some
reference level (dBm in this case).
SLOPE is the logarithmic slope, expressed in mV/dB.
INTERCEPT is the logarithmic intercept, expressed in decibels
relative to the same reference level.
For example, at an input level of −25 dBm, the VLOG output
voltage is VVLOG = 18.7mV/dB × [−25 dBm −(−64.4 dBm)] = 737mV.
LOG CONFORMANCE ERROR CALCULATION
Log conformance error is expressed in terms of the deviation in
the output voltage between the measured VVLOG and the VVLOG
calculated with an ideal log transformation function. Ideally, the
measured VVLOG output at a particular input power, as plotted in
Figure 83, must not deviate from the calculated value of VVLOG at
that same input power. Setting the measured VVLOG to the right side
of the preceding equation and rearranging yields
VV LOG,  MEASURED PIN
SLOPE
− PIN + INTERCEPT = 0
(3)
In actuality, this does not always calculate to zero. The finite
calculation that results is the log conformance error, as follows:
Error PIN =
VV LOG,  MEASURED PIN
SLOPE
− PIN
+ INT ERCEPT
(4)
where Error is in dB.
The parameters SLOPE and INTERCEPT are best obtained from
the actual detector response using linear regression over a suitable
power range (where the detector response is close to linear). Better
accuracy/smaller errors are obtained if SLOPE and INTERCEPT
are determined for:
►
Each detector device individually
►
Each operating temperature



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