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ADL5502 Datasheet(PDF) 16 Page - Analog Devices

Part # ADL5502
Description  450 MHz to 6000 MHz Crest Factor Detector
PDF  28 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

ADL5502 Datasheet(HTML) 16 Page - Analog Devices

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ADL5502
Rev. A | Page 16 of 28
APPLICATIONS INFORMATION
BASIC CONNECTIONS
Figure 44 shows the basic connections for the ADL5502. The
device is powered by a single supply between 2.5 V and 3.3 V,
with a quiescent current of 3 mA. The VPOS pin is decoupled
using 100 pF and 0.1 μF capacitors.
Placing a single 75 Ω resistor at the RF input provides a
broadband match of 50 Ω. More precise resistive or reactive
matches can be applied for narrow frequency band use (see the
RF Input Interfacing section).
The rms averaging can be augmented by placing additional
capacitance at CFLTR. The ac residual can be reduced further by
increasing the output capacitance, COUT. The combination of the
internal 100 Ω output resistance and COUT produce a low-pass
filter to reduce output ripple of the VRMS output (see the
Selecting the Square-Domain Filter and Output Low-Pass Filter
section for more details).
RFIN
CFLTR
+VS 2.5V TO 3.3V
CONTROL
(HIGH RESET;
LOW PEAK HOLD)
VPEAK
VRMS
ROUT
0.1µF
0.1pF
COUT
FLTR
VPOS
RFIN
VRMS
PEAK
CNTL
COMM
ENBL
ADL5502
8
4
1
2
3
7
6
5
R10
75Ω
Figure 44. Basic Connections for ADL5502
To measure the peak of a waveform, the control line (CNTL)
must be temporally set to high (reset mode for >1 μs) and then set
back to low (peak-hold mode). This allows the ADL5502 to be
initialized to a known state. When setting the device to measure
peak, peak-hold mode should be toggled for a period in which
the input rms power and CF is not likely to change.
If the ADL5502 is in peak-hold mode and the CF changes from
high to low or the input power changes from high to low, a
faulty peak measurement is reported. The ADL5502 simply
keeps reporting the highest peak that occurred when the peak-
hold mode was activated and the input power or the CF was
high. Unless CNTL is reset, the PEAK output does not reflect
the new peak in the signal.
RF INPUT INTERFACING
The input impedance of the ADL5502 decreases with increasing
frequency in both its resistive and capacitive components (see
Figure 34). The resistive component varies from 330 Ω at 900 MHz
to about 240 Ω at 1900 MHz.
A number of options exist for input matching. For operation
at multiple frequencies, a 75 Ω shunt to ground, as shown in
Figure 45, provides the best overall match. For use at a single
frequency, a resistive or a reactive match can be used. By plotting
the input impedance on a Smith Chart, the best value for a
resistive match can be calculated. (Both input impedance and
input capacitance can vary by up to ±20% around their nominal
values.) Where VSWR is critical, the match can be improved
with a series inductor prior to the shunt component.
ADL5502
RFIN
RF TRANSMISSION LINE
50Ω
DIRECTIONAL
COUPLER
75Ω
ATTN
Figure 45. Input Interfacing to Directional Coupler
Resistive Tap RF Input
Figure 46 shows a technique for coupling the input signal into
the ADL5502 that can be applicable where the input signal is
much larger than the input range of the ADL5502. A series
resistor combines with the input impedance of the ADL5502
to attenuate the input signal. Because this series resistor forms
a divider with the frequency dependent input impedance, the
apparent gain changes greatly with frequency. However, this
method has the advantage of very little power being tapped off
in RF power transmission applications. If the resistor is large
compared to impedance of the transmission line, the VSWR of
the system is relatively unaffected.
ADL5502
RFIN
RF TRANSMISSION LINE
RSERIES
Figure 46. Attenuating the Input Signal
The resistive tap or series resistance, RSERIES, can be expressed as
RSERIES
= RIN (1 − 10ATTN/20)/(10ATTN/20)
(1)
where:
RIN
is the input impedance of RFIN.
ATTN
is the desired attenuation factor in dB.
For example, if a power amplifier with a maximum output power
of 28 dBm is matched to the ADL5502 input at 5 dBm, then a
−23 dB attenuation factor is required. At 900 MHz, the input
resistance, RIN, is 330 Ω.
RSERIES
= (330 Ω)(1 − 10−23/20)/(10−23/20) = 4330 Ω
(2)
Thus, for an attenuation of −23 dB, a series resistance of
approximately 4.33 kΩ is needed.



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