True rms response detector
Envelope peak hold output
Excellent temperature stability
±0.25 dB rms detection accuracy vs. temperature
±0.25 dB envelope detection accuracy vs. temperature;
over the top 25 dB of the input range
Over 35 dB input power dynamic range, inclusive of crest factor
RF bandwidths from 450 MHz to 6 GHz
Envelope bandwidths of 10 MHz
500 Ω input impedance
Single-supply operation: 2.5 V to 3.3 V
Low power: 3 mA at 3 V supply
RoHS-compliant part
APPLICATIONS
Power and envelope measurement of W-CDMA, CDMA2000,
and QPSK-/QAM-based OFDM, and other complex
modulation waveforms
RF transmitter or receiver power and envelope measurement
RFIN
ENBL
Crest Factor Detector
ADL5502
FUNCTIONAL BLOCK DIAGRAM
POS
ADL5502
1kΩ
RMS CORE
PEAK/
ENVELOPE
COMM
Figure 1.
VRMS
4nF
BUFFERS
RF INPUT
INTERNAL
FILTERING
100Ω
100Ω
PEAK
FLTR
VRMS
PEAK
CNTL
07631-001
GENERAL DESCRIPTION
The ADL5502 is a mean-responding (true rms) power detector
in combination with an envelope detector to accurately determine
the crest factor of a modulated signal. It can be used in high
frequency receiver and transmitter signal chains from 450 MHz
to 6 GHz with envelope bandwidths over 10 MHz. Requiring
only a single supply between 2.5 V and 3.3 V, the detector draws
less than 3 mA. The input is internally ac-coupled and has a
nominal input impedance of 500 Ω.
The rms output is a linear-responding dc voltage with a conversion
gain of 1.8 V/V rms at 900 MHz. The peak envelope output with a
conversion gain of 1.2 V/V is toggled for peak hold with less
than 1% output voltage droop in over 1 ms.
CNTL
PEAK HOLDENV TRACK
1µs/DIV
Figure 2.
07631-002
The ADL5502 is a highly accurate, easy to use means of
determining the rms and peak to the average value of complex
waveforms. It can be used for crest factor measurements of both
simple and complex waveforms but is particularly useful for
measuring high crest factor (high peak-to-rms ratio) signals,
such as W-CDMA, CDMA2000, and QPSK-/QAM-based
OFDM waveforms. The peak hold function allows the capture
of short peaks in the envelope with lower sampling rate ADCs.
The crest factor detector operates from −40°C to +85°C and is
available in an 8-ball, 1.5 mm × 1.5 mm wafer-level chip scale
package. It is fabricated on a high f
silicon BiCMOS process.
T
Rev. A
Information furnished by Analog Devices is believed to be accurate and reliable. However, no
responsibility is assumed by Analog Devices for its use, nor for any infringements of patents or other
rights of third parties that may result from its use. Specifications subject to change without notice. No
license is granted by implication or otherwise under any patent or patent rights of Analog Devices.
Trademarks and registered trademarks are the property of their respective owners.
RF INPUT (f = 1900 MHz) Input RFIN to output VRMS and PEAK
Input Impedance No termination 238||0.90 Ω||pF
RMS CONVERSION Input RFIN to output VRMS
Dynamic Range CW input, −40°C < TA < +85°C
±0.25 dB Error 1 27 dB
±1 dB Error1 32 dB
±2 dB Error2 30 dB
Maximum Input Level
Minimum Input Level
±0.25 dB error
±1 dB error
2
2
Conversion Gain VRMS = (Gain × VIN) + Intercept 1.75 V/V rms
Output Intercept3 0.010 V
Output Voltage, High Power In PIN = 5 dBm, 400 mV rms 0.700 V
Output Voltage, Low Power In PIN = −15 dBm, 40 mV rms 0.079 V
ENVELOPE CONVERSION Input RFIN to output PEAK
Dynamic Range CW input, −40°C < TA < +85°C
±0.25 dB Error1 26 dB
±1 dB Error1 32 dB
±2 dB Error2 30 dB
Maximum Input Level
Minimum Input Level
±0.25 dB error
±1 dB error
2
2
Conversion Gain PEAK = (Gain × VIN) + Intercept 1.17 V/V rms
Output Intercept3 0.011 V
Output Voltage, High Power In PIN = 5 dBm, 400 mV rms 0.472 V
Output Voltage, Low Power In PIN = −15 dBm, 40 mV rms 0.057 V
RF INPUT (f = 3500 MHz) Input RFIN to output VRMS and PEAK
Input Impedance No termination 232||0.39 Ω||pF
RMS CONVERSION Input RFIN to output VRMS
Dynamic Range CW input, −40°C < TA < +85°C
±1 dB Error1 32 dB
±2 dB Error2 30 dB
Maximum Input Level
Minimum Input Level
±0.25 dB error
±1 dB error
2
2
Conversion Gain VRMS = (Gain × VIN) + Intercept 1.52 V/V rms
Output Intercept3 0.002 V
Output Voltage, High Power In PIN = 5 dBm, 400 mV rms 0.594 V
Output Voltage, Low Power In PIN = −15 dBm, 40 mV rms 0.065 V
ENVELOPE CONVERSION Input RFIN to output PEAK
Dynamic Range CW input, −40°C < TA < +85°C
±1 dB Error1 32 dB
±2 dB Error2 31 dB
Maximum Input Level
Minimum Input Level
±0.25 dB error
±1 dB error
2
2
Conversion Gain PEAK = (Gain × VIN) + Intercept 1.02 V/V rms
Output Intercept3 0.005 V
Output Voltage, High Power In PIN = 5 dBm, 400 mV rms 0.403 V
Output Voltage, Low Power In PIN = −15 dBm, 40 mV rms 0.049 V
12 dBm
−15 dBm
12 dBm
−16 dBm
7 dBm
−16 dBm
7 dBm
−16 dBm
Rev. A | Page 4 of 28
Page 5
ADL5502
Parameter Test Conditions Min Typ Max Unit
VRMS OUTPUT Pin VRMS
Maximum Output Voltage VS = 3.0 V, R
Output Offset No signal at RFIN 15 100 mV
Pulse Response Time
10 dB step, 10% to 90% of settling level, no filter
capacitor
Available Output Current 3 mA
PEAK OUTPUT Pin PEAK
Maximum Output Voltage VS = 3.0 V, R
Output Offset No signal at RFIN 14 100 mV
Available Output Current 3 mA
Envelope Modulation Bandwidth 5 10 MHz
Peak Hold Time 1% voltage drop from last peak, CNTL = high 600 μs
CONTROL INTERFACE
Logic Level to Track Envelope, High 2.5 V ≤ VS ≤ 3.3 V, −40°C < TA < +85°C 1.8 V
Input Current when High 2.5 V at CNTL, –40°C ≤ TA ≤ +85°C 0.05 0.1 μA
Logic Level for Peak Hold Condition, Low 2.5 V ≤ VS ≤ 3.3 V, −40°C < TA < +85°C −0.5 +0.5 V
Enable Time 0 dBm at RFIN, CNTL held high for >1 μs <0.1 μs
ENABLE INTERFACE Pin ENBL
Logic Level to Enable Power, High Condition 2.5 V ≤ VS ≤ 3.3 V, −40°C < TA < +85°C 1.8 V
Input Current when High 2.5 V at ENBL, –40°C ≤ TA ≤ +85°C 0.05 0.1 μA
Logic Level to Disable Power, Low Condition 2.5 V ≤ VS ≤ 3.3 V, −40°C < TA < +85°C −0.5 +0.5 V
Power-Up Response Time4 C
C
= open, 0 dBm at RFIN 12 μs
FLTR
= 10 nF, 0 dBm at RFIN 10 μs
FLTR
POWER SUPPLIES
Operating Range −40°C < TA < +85°C 2.5 3.3 V
Quiescent Current No signal at RFIN,5 ENBL high input condition 3.0 mA
Disable Current6 ENBL input low condition, CNTL in high condition <1 1 μA
1
Error referred to delta from 25°C response, see Figure 10, Figure 11, and Figure 12 for VRMS and Figure 16, Figure 17, and Figure 18 for PEAK.
2
Error referred to best-fit line at 25°C, see Figure 13, Figure 14, and Figure 15 for VRMS and Figure 19, Figure 20, and Figure 21 for PEAK.
3
Calculated using linear regression.
4
The response time is measured from 10% to 90% of settling level, see Figure 41, Figure 42, and Figure 43.
5
Supply current is input level dependant, see Figure 37.
6
Guaranteed but not tested; limits are specified at six sigma levels.
≥ 10 kΩ 2.4 V
LOAD
15 μs
≥ 10 kΩ 1.5 V
LOAD
V
POS
V
POS
Rev. A | Page 5 of 28
Page 6
ADL5502
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Rating
Supply Voltage, VS 3.5 V
VRMS, PEAK, ENBL, CNTL 0 V, VS
RFIN 1.25 V rms
Equivalent Power, re: 50 Ω 15 dBm
Internal Power Dissipation 200 mW
θJA (WLCSP) 200°C/W
Maximum Junction Temperature 125°C
Operating Temperature Range −40°C to +85°C
Storage Temperature Range −65°C to +150°C
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only; functional operation of the device at these or any
other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect
device reliability.
ESD CAUTION
Rev. A | Page 6 of 28
Page 7
ADL5502
V
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
BALLA1
CORNER
ENBL
ADL5502
1
FLTR
2
POS
3
RFIN
COMM
TOP VIEW
(BALL SIDE DO WN)
Figure 3. Pin Configuration
Table 3. Pin Function Descriptions
Pin No. Mnemonic Description
1 FLTR Modulation Filter Pin. Connection for an external capacitor to lower the corner frequency of the modulation filter.
2 VPOS Supply Voltage Pin. Operational range 2.5 V to 3.3 V.
3 RFIN Signal Input Pin. Internally ac-coupled after internal termination resistance. Nominal 500 Ω input impedance.
4 COMM Device Ground Pin.
5 CNTL
Control Pin. Connect pin to ground for peak-hold mode. Connect pin to V
To measure the peak of a waveform, the control pin must be briefly set to high (reset mode for >1 μs) to start at a
known state.
6 PEAK
Envelope Peak Output. Voltage output for peak-hold function, with limited current drive capability. The output
has an internal 100 Ω series resistance. Low capacitance loads are recommended to allow for envelope tracking
and fast response time.
7 VRMS
RMS Output Pin. Rail-to-rail voltage output with limited current drive capability. The output has an internal 100 Ω
series resistance. High resistive loads and low capacitance loads are recommended to preserve output swing and
allow fast response.
8 ENBL Enable Pin. Connect pin to VS for normal operation. Connect pin to ground for disable mode.
7
8
4
VRMS
PEAK
6
CNTL
5
07631-003
for reset mode (tracking envelope).
S
Rev. A | Page 7 of 28
Page 8
ADL5502
TYPICAL PERFORMANCE CHARACTERISTICS
TA = 25°C, VS = 3.0 V, C
−40°C, red = +85°C, unless otherwise noted.
= 10 nF, C
FLTR
= open, light condition ≤ 600 lux, 75 Ω input termination resistor, colors: black = +25°C, blue =
Figure 26. Error from CW Linear Reference vs. Input with Various
CDMA2000 Reverse Link Waveforms at 1900 MHz, C
3
= 10 nF, C
FLTR
= Open
OUT
2
1
0
ERROR (d B)
–1
–2
–3
–25–20–15–10–5051015
CW
TEST MO DEL 1 WIT H 16 DPCH, 1 CARRIER
TEST MO DEL 1 WIT H 32 DPCH, 1 CARRIER
TEST MO DEL 1 WIT H 64 DPCH, 1 CARRIER
TEST MO DEL 1 WIT H 64 DPCH, 2 CARRIERS
TEST MO DEL 1 WIT H 64 DPCH, 3 CARRIERS
TEST MO DEL 1 WIT H 64 DPCH, 4 CARRIERS
INPUT (dBm)
Figure 24. Error from CW Linear Reference vs. Input with Various
Figure 34. Input Impedance vs. Frequency, Supply 3 V,
Temperatures −40°C, +25°C, and +85°C
3.5
3.0
2.5
2.0
1.5
1.0
0.5
0
15
14
13
12
11
10
9
8
7
6
5
4
SHUNT CAPACITACE (p F)
07631-034
SUPPLY CURRENT (mA)
3
2
1
0
00.10.20.30.40.50.60.70.80.9
INPUT (V rms)
2.5V
07631-037
Figure 37. Supply Current vs. Input Level; 2.5 V, 3.0 V, and 3.3 V Supply;
900 MHz Frequency, Temperatures −40°C, +25°C, and +85°C
PULSED RFIN
OSCILLOSCOPE
7
6
5
FET PROBE
POWER
SUPPLY
100pF
RF SIGNAL
GENERATOR
8
ENBL
1
0.1µF
2
3
FLTR
VPOS
RFIN
C
R
F
L
T
75Ω
ADL5502
COMM
4
VRMS
PEAK
CNTL
Figure 35. Hardware Configuration for Output Response to RF Input Pulse
PULSED RFIN
400mV rms RF INPUT
160mV rms
VRMS, PEAK (400mV /DIV)
400mV rms
160mV rms
10μs/DIV
PEAK
VRMS
07631-036
Figure 36. Output Response to Various RF Input Pulse Levels, Supply 3 V,
900 MHz Frequency, C
= Open, C
FLTR
= Open
OUT
400mV rms RF INPUT
160mV rms
VRMS, PEAK (400mV/DIV)
07631-035
400mV rms
160mV rms
20μs/DIV
PEAK
VRMS
07631-038
Figure 38. Output Response to Various RF Input Pulse Levels, Supply 3 V,
900 MHz Frequency, C
VRMS, PEAK (400mV/ DIV)
= 10 nF, C
FLTR
400mV rms RF INPUT
160mV rms
400mV rms
160mV rms
40μs/DIV
= Open
OUT
PULSED RFIN
PEAK
VRMS
07631-039
Figure 39. Output Response to Various RF Input Pulse Levels, Supply 3 V,
900 MHz Frequency, C
= 22 nF, C
FLTR
= Open
OUT
Rev. A | Page 13 of 28
Page 14
ADL5502
PULSE
GENERATOR
50Ω
AD811
ENBL
732Ω
POWER
SUPPLY
100pF
RF SIGNAL
GENERATOR
8
ENBL
1
C
T
R
F
L
0.1µF
75Ω
FLTR
VPOS
2
RFIN
3
VRMS
ADL5502
PEAK
CNTL
COMM
4
OSCILLOSCOPE
7
6
5
FET PROBE
Figure 40. Hardware Configuration for Output Response to
Enable Gating Measurements
ENBL
400mV rms RF INPUT
160mV rms
VRMS, PEAK (400mV/DIV)
400mV rms
160mV rms
10μs/DIV
PEAK
VRMS
07631-041
Figure 41. Output Response to Enable Gating at Various RF Input Levels,
Supply 3 V, 900 MHz Frequency, C
= Open, C
FLTR
= Open
OUT
400mV rms RF INPUT
160mV rms
VRMS, PEAK (400mV/DIV)
07631-040
400mV rms
160mV rms
10μs/DIV
PEAK
VRMS
07631-042
Figure 42. Output Response to Enable Gating at Various RF Input Levels,
Supply 3 V, 900 MHz Frequency, C
400mV rms RF INPUT
160mV rms
VRMS, PEAK (400mV/DIV)
400mV rms
160mV rms
10μs/DIV
= 10 nF, C
FLTR
= Open
OUT
ENBL
PEAK
VRMS
07631-043
Figure 43. Output Response to Enable Gating at Various RF Input Levels,
Supply 3 V, 900 MHz Frequency, C
= 22 nF, C
FLTR
= Open
OUT
Rev. A | Page 14 of 28
Page 15
ADL5502
[
CIRCUIT DESCRIPTION
The ADL5502 employs two-stage detection. The critical aspect
of this technical approach is the concept of first stripping the
carrier to reveal the envelope and then performing the required
analog computation of rms and peak or any other aspect of the
envelope. An on-chip, 2-pole, passive low-pass filter preserves
the envelope frequencies up to 10 MHz and filters out the carrier.
This carrier filtering ensures that the carrier does not introduce
an error in the peak measurement.
The extracted envelope is further processed in two parallel
channels, one computing the rms value of the envelope and the
other transferring the envelope with appropriate scaling to the
output buffer.
RMS CIRCUIT DESCRIPTION AND FILTERING
The rms processing is done using a proprietary translinear
technique. This method is a mathematically accurate rms
computing approach and allows achieving unprecedented rms
accuracies for complex modulation signals irrespective of the
crest factor of the input signal. An integrating filter capacitor
does the square-domain averaging. The VRMS output can be
expressed as
T
2
2
dtV
×
∫
IN
T
1
AVRMS
×=
T1T2
−
Note that A is a scaling parameter that is decided on by the on-chip
resistor ratio, and there are no other scaling parameters involved in
this computation, which means that the rms output is inherently
free from any sources of error due to temperature, supply, and
process variation.
FILTERING
The on-chip rms filtering is sufficient for most common handset
applications, but an external filter capacitor can be connected
if additional filtering is required; however, this increases the
averaging time (see the Selecting the Square-Domain Filter and
Output Low-Pass Filter section). The on-chip rms filter has a
nominal corner frequency of 40 kHz. Any external capacitor
acts on a 1 kΩ resistor to yield a new corner frequency for the
rms filter (see Figure 1).
ENVELOPE PEAK-HOLD CIRCUIT
The envelope signal is processed through a peak-hold circuit,
using the gate of an NMOS device with a charge holding capacitor
connected to ground, driven by a one way charging path. This
low leakage node allows peak-hold times of >1 ms without
practically any drop in voltage. This circuit has the option of either
transferring the envelope in real-time or in the peak-hold mode
by toggling a control logic pin (CNTL). In the peak-hold mode,
the output only is updated when a peak bigger than the previous
biggest peak occurs. The PEAK output can be expressed as
2
T
T
max
1
2
T
()
]
VenvelopeBPEAK×=
IN
1
T
where:
T1 is the time at which CNTL goes from high to low which is
followed by a time where CNTL stays low.
T2 is the time at which the PEAK measurement is taken, while
CNTL is still low. Here again the only scaling parameter involved is
a Scalar B, which is also decided on by the on-chip resistor ratio.
OUTPUT BUFFERS
A dual buffer takes in internal rms and envelope/peak signals
and gains these up accordingly before these are brought out on
the VRMS and PEAK pins. The output stage of the rms buffer is
a common source PMOS with a resistive load to provide a railto-rail output. However, output stage of the PEAK buffer is an
emitter-follower NPN stage with a resistive load to provide high
speed characteristics for this output. This however limits the
maximum voltage on the PEAK output to about 1.2 V below
supply, resulting in a lower scaling factor for the PEAK signal
path. Such a stage allows fast tracking of a rising transition when a
very narrow peak is to be followed in the 10 MHz signal bandwidth. It is highly recommended that capacitive loads greater
than 2 pF are avoided on the PEAK output to realize the full
bandwidth potential of the device.
Both the buffers have 100 Ω on-chip series resistances on the
output. This allows for easy low-pass filtering of the two outputs.
MEASURING THE CREST FACTOR
After proper calibration of the rms and envelope channels, the
ratio of the two outputs gives the crest factor of the signal, when
envelope output is in peak-hold mode (see the Calculation of
Crest Factor (CF) section for more details). The envelope
extraction that precedes rms and peak/envelope measurement is
common to both channels. In addition, the rms and envelope
channels share bias lines and other critical devices that are matched
between the two channels, wherever possible. This ensures that the
relative measurement between the two channels or the crest
factor measurement of the signal is more accurate than the
individual measurements of the rms value and the peak value,
although these measurements in themselves are very accurate
over temperature, supply, and process variations as well.
Rev. A | Page 15 of 28
Page 16
ADL5502
O
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 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 C
increasing the output capacitance, C
internal 100 Ω output resistance and C
. The ac residual can be reduced further by
FLTR
. The combination of the
OUT
produce a low-pass
OUT
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).
+VS 2.5V
T
0.1µF0.1pF
RFIN
3.3V
8
1
2
3
FLTR
ADL5502
VPOS
RFIN
COMM
ENBL
VRMS
PEAK
CNTL
4
C
FLTR
R10
75Ω
R
OUT
7
6
5
V
PEAK
CONTROL
(HIGH RESET;
LOW PEAK HO LD)
C
VRMS
OUT
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 peakhold 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 at 900 MHz
to about 240 at 1900 MHz.
07631-044
A number of options exist for input matching. For operation
at multiple frequencies, a 75 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.
RF TRANSMISSI ON LINE
DIRECTIONAL
COUPLE R
50Ω
ATTN
75Ω
RFIN
ADL5502
07631-045
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.
RF TRANSMISS ION LINE
R
SERIES
RFIN
ADL5502
07631-046
Figure 46. Attenuating the Input Signal
The resistive tap or series resistance, R
R
SERIES
= RIN (1 − 10
ATTN/20
)/(10
ATTN/20
, can be expressed as
SERIES
) (1)
where:
R
is the input impedance of RFIN.
IN
AT TN 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, R
R
, is 330 Ω.
IN
= (330 Ω)(1 − 10
SERIES
−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.
Rev. A | Page 16 of 28
Page 17
ADL5502
Multiple RF Inputs
Figure 47 shows a technique for combining multiple RF input
signals to the ADL5502. Some applications can share a single
detector for multiple bands. Three 16.5 Ω resistors in a T-network
combine the three 50 Ω terminations (including the ADL5502
with the shunt 75 Ω matching component). The broadband
resistive combiner ensures each port of the T-network sees a
50 Ω termination. Because there are only 6 dB of isolation from
one port of the combiner to the other ports, only one band
should be active at a time.
BAND 1
DIRECTIONAL
COUPLER
DIRECTIONAL
COUPLER
Figure 47. Combining Multiple RF Input Signals
BAND 2
50Ω
50Ω
16.5Ω
16.5Ω
16.5Ω
75Ω
RFIN
ADL5502
07631-047
LINEARITY
Because the ADL5502 is a linear responding device, plots of
output voltage vs. input voltage result in a straight line (see
Figure 4, Figure 5, and Figure 7) and the dynamic range in
dB is not clearly visible. It is more useful to plot the error on
a logarithmic scale, as shown in Figure 6 and Figure 8. The
deviation of the plot for the ideal straight line characteristic is
caused by input stage clipping at the high end and by signal
offsets at the low end. However, offsets at the low end can be
either positive or negative; therefore, the linearity error vs. input
level plots could also trend upwards at the low end. Figure 10,
Figure 11, Figure 12, Figure 16, Figure 17, and Figure 18 show
error distributions for a large population of devices at specific
frequencies over temperature.
It is also apparent in Figure 6 that the error at the lower portion
of the dynamic range tends to shift up as frequency is increased
This is due to the calibration points chosen, 0 dBm and 9 dBm
(see the Device Calibration and Error Calculation section).
The absolute value cell has an input impedance that varies with
frequency. The result is a decrease in the actual voltage across the
squaring cell as the frequency increases, reducing the conversion
gain. Similarly, conversion gain is less at frequencies near 450 MHz
because of the small on-chip coupling capacitor. The dynamic
range is near constant over frequency, but with a decrease in
conversion gain as frequency is increased.
Output Swing
At 900 MHz, the VRMS output voltage is nominally 1.89 times the
input rms voltage (a conversion gain of 1.89 V/V rms). Similarly,
the PEAK output voltage is nominally 1.27 times the input rms
voltage (a conversion gain of 1.27 V/V rms). The rms output
voltage swings from near ground to 2.4 V on a 3.0 V supply.
Figure 9 shows the output swings of the ADL5502 to a CW input
for various supply voltages. Only at the lowest supply voltage
(2.5 V) is there a reduction in the dynamic range as the input
headroom decreases.
VRMS Output Offset
The ADL5502 has a ±1 dB error detection range of about 30 dB,
as shown in Figure 10 to Figure 12 and Figure 16 to Figure 18. The
error is referred to the best-fit line defined in the linear region of
the output response (see the Device Calibration and Error
Calculation section for more details). Below an input power of
−18 dBm, the response is no longer linear and begins to lose
accuracy. In addition, depending on the supply voltage,
saturation may limit the detection accuracy above 12 dBm.
Calibration points should be chosen in the linear region,
avoiding the nonlinear ranges at the high and low extremes.
1k
100
VRMS (mV)
10
1
–30 –25–20 –15–10–505
INPUT (dBm)
Figure 48. VRMS Output vs. Input Level Distribution of 50 Devices,
1k
100
PEAK (mV)
10
1
–30 –25–20 –15–10–5051015
Figure 49. PEAK Output vs. Input Level Distribution of 50 Devices,
900 MHz Frequency, Supply 3.0 V
INPUT (dBm)
900 MHz Frequency, Supply 3.0 V
10
15
07631-048
7631-049
Figure 48 and Figure 49 show distributions of VRMS and PEAK
output responses vs. the input power for multiple devices. The
ADL5502 loses accuracy at low input powers as the output
response begins to fanout. As the input power is reduced, the
spread of the output response increases along with the error.
Rev. A | Page 17 of 28
Page 18
ADL5502
Although some devices follow the ideal linear response at very
low input powers, not all devices continue the ideal linear
regression to a near 0 V y-intercept. Some devices exhibit
output responses that rapidly decrease and some flatten out.
With no RF signal applied, the ADL5502 has a typical output
offset of 15 mV (with a maximum of 100 mV) on VRMS and an
offset of 14 mV (with a maximum of 100 mV) on PEAK.
OUTPUT DRIVE CAPABILITY AND BUFFERING
The ADL5502 is capable of sourcing a VRMS output current of
approximately 3 mA. The output current is sourced through the
on-chip, 100 Ω series resistor; therefore, any load resistor forms
a voltage divider with this on-chip resistance. It is
recommended that the ADL5502 VRMS output drive high
resistive loads to preserve output swing. If an application requires
driving a low resistance load (as well as, in cases where increasing
the nominal conversion gain is desired), a buffering circuit is
necessary.
The PEAK output is designed to drive 2 pF loads. It is
recommended that the ADL5502 PEAK output drive low
capacitive loads to achieve a full output response time. The
effects of larger capacitive loads are particularly visible when
tracking envelopes during the falling transitions. When the
envelope is in a fall transition, the load capacitor discharges
through the on-chip load resistance of 1.9 kΩ. If the larger
capacitive load is unavoidable, the additional capacitance
can be counteracted by putting a shunt resistor to ground on
the PEAK output to allow for fast discharge. Such a shunt
resistor also makes the ADL5502 run higher current, and it
should not be reduced beyond 500 Ω.
When viewing the PEAK output on an oscilloscope, a low
capacitive FET probe should be used to interface with the
PEAK output. This reduces the capacitance presented to the
PEAK output and avoids the corresponding effects of larger
capacitive loads.
SELECTING THE SQUARE-DOMAIN FILTER AND
OUTPUT LOW-PASS FILTER
The internal filter capacitor of the ADL5502 provides averaging
in the square domain but leaves some residual ac on the output.
Signals with high peak-to-average ratios, such as W-CDMA or
CDMA2000, can produce ac residual levels on the ADL5502
VRMS dc output. To reduce the effects of these low frequency
components in the waveforms, some additional filtering is
required.
The square-domain filter capacitance of the ADL5502 can be
augmented by connecting a capacitor between Pin 1 (FLTR) and
Pin 2 (VPOS). In addition, the VRMS output of the ADL5502 can
be filtered directly by placing a capacitor between VRMS (Pin 7)
and ground. The PEAK output can be filtered by placing a
capacitor between Pin 6 (PEAK) and ground. The combination
of the on-chip, 100 Ω output series resistance and the external
shunt capacitor forms a low-pass filter to reduce the residual ac.
Figure 50 and Figure 51 show the effects on the residual ripple
vs. the output and square-domain filter capacitor values at two
communication standards with high peak-to-average ratios.
Note that there is a tradeoff between ac residual and response
time. Large filter capacitances increase the turn-on and pulse
response times (see Figure 36, Figure 38, Figure 39, Figure 41,
Figure 42, and Figure 43). Figure 52 shows the effect of the two
filtering options, the output filter and the square-domain filter
capacitor, on the pulse response time of the ADL5502. For more
information on the effects of the filter capacitances on the
response, see the Power Consumption, Enable, and PowerOn/Power-Off Response Time section.
60
50
C
40
30
20
AC RESIDUAL (V p- p)
10
0
1101001000
Figure 50. AC Residual vs. C
W-CDMA Forward Link (4.6 dB CF) Waveform
400
350
300
250
200
150
AC RESIDUAL (V p -p)
100
OUT
C
FLTR
CAPACITANCE (nF )
FLTR
C
OUT
C
FLTR
and C
OUT
7631-050
,
Rev. A | Page 18 of 28
50
0
1101001000
CAPACITANCE (nF )
Figure 51. AC Residual vs. C
W-CDMA Reverse Link (11.7 dB CF) Waveform
FLTR
and C
OUT
,
07631-051
Page 19
ADL5502
1000
900
800
700
600
500
400
RESPONSE T IME (µs)
300
FLTR
C
200
100
0
1101001000
CAPACITANCE (nF )
Figure 52. Response Time vs. C
FLTR
and C
C
OUT
C
FLTR
OUT
200
180
160
140
120
100
80
RESPONSE TIME (µs)
60
C
40
20
0
POWER CONSUMPTION, ENABLE, AND POWERON/POWER-OFF RESPONSE TIME
The quiescent current consumption of the ADL5502 varies
linearly with the size of the input signal from approximately
3 mA for no signal up to 11 mA at an input level of 0.7 V rms
(10 dBm, re: 50 Ω). There is little variation in quiescent current
across power supply voltage or temperature, as shown in Figure 37.
The ADL5502 can be disabled either by pulling the ENBL (Pin 8)
to COMM (Pin 4) or by removing the supply power to the device.
Disabling the device via the ENBL function reduces the leakage
current to less than 1 µA. When the device is disabled, the output
impedance increases to approximately 5.5 kΩ on VRMS and
1.9 kΩ on PEAK.
The turn-on time and pulse response is strongly influenced by
the size of the square-domain filter and output shunt capacitor.
Figure 53 shows a plot of the output response to an RF pulse on
the RFIN pin, with a 0.1 µF output filter capacitor and no squaredomain filter capacitor. The falling edge is particularly dependent
on the output shunt capacitance, as shown in Figure 53.
PULSED RFIN
400mV rms RF INPUT
250mV rms
160mV rms
VRMS (250mV/DIV)
Figure 53. Output Response to Various RF Input Pulse Levels, Supply 3 V,
To improve the falling edge of the enable and pulse responses, a
resistor can be placed in parallel with the output shunt capacitor.
The added resistance helps to discharge the output filter capacitor.
Although this method reduces the power-off time, the added
load resistor also attenuates the output (see the Output Drive
Capability and Buffering section).
PULSED RFIN
OUT
07631-052
VRMS (250mV/ DIV)
400mV rms RF INPUT
250mV rms
160mV rms
70mV rms
1ms/DIV
VRMS
07631-054
Figure 54. Output Response to Various RF Input Pulse Levels,
Supply 3 V, 900 MHz Frequency, Square-Domain Filter Open,
Output Filter 0.1 μF with Parallel 1 kΩ
The square-domain filter improves the rms accuracy for high
crest factors (see the Selecting the Square-Domain Filter and
Output Low-Pass Filter section), but it can hinder the response
time. For optimum response time and low ac residual, both the
square-domain filter and the output filter should be used. The
square-domain filter at FLTR can be reduced to improve response
time, and the remaining ac residual can be decreased by using
the output filter, which has a smaller time constant.
DEVICE CALIBRATION AND ERROR CALCULATION
Because slope and intercept vary from device to device, boardlevel calibration must be performed to achieve high accuracy.
In general, calibration is performed by applying two input power
levels to the ADL5502 and measuring the corresponding output
voltages. The calibration points are generally chosen to be within
the linear operating range of the device. The best-fit line is
characterized by calculating the conversion gain (or slope) and
intercept using the following equations:
Gain = (V
Intercept = V
where:
V
is the rms input voltage to RFIN.
IN
V
is the voltage output at VRMS.
VRMS
Once gain and intercept are calculated, an equation can be
written that allows calculation of an (unknown) input power
based on the measured output voltage.
V
= (V
IN
− V
VRMS2
VRMS1
− Intercept)/Gain (5)
VRMS
)/(V
VRMS1
IN2
− (Gain × V
− V
) (3)
IN1
) (4)
IN1
Rev. A | Page 19 of 28
Page 20
ADL5502
For an ideal (known) input power, the law conformance error of
the measured data can be calculated as
ERROR (dB) =
20 × log [(
V
VRMS, MEASURED
− Intercept)/(Gain × V
IN, IDEAL
)] (6)
Figure 55 includes a plot of the error at 25°C, the temperature
at which the ADL5502 is calibrated. Note that the error is not
zero; this is because the ADL5502 does not perfectly follow the
ideal linear equation, even within its operating region. The error
at the calibration points is, however, equal to 0 by definition.
3
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. The ADL5502
offers a tight error distribution in the high input power range,
as shown in Figure 56. The high accuracy range, beginning
around 4 dBm at 1900 MHz, offers 8 dB of ±0.15 dB detection
error over temperature. Multiple point calibration at ambient
temperature in the reduced range offers precise power
measurement with near 0 dB error from −40°C to +85°C.
3
2
1
0
ERROR (dB)
–1
–2
–3
–25–20–15–10–5051015
Figure 55. VRM S Error from Linear Reference vs. Input at −40°C , +25°C, a nd
+85°C vs. +25°C Linear Reference, Frequency 1900 MHz, Supply 3.0 V
+85ºC
+25ºC
–40ºC
INPUT (dBm)
07631-055
Figure 55 also includes error plots for the output voltage at
−40°C and +85°C. These error plots are calculated using the
gain and intercept at 25°C. This is consistent with calibration in
a mass production environment where calibration at temperature is
not practical.
The same procedure should be followed to calculate the linearity
error for the PEAK output. In this case, replace V
in the preceding equations.
V
PEAK
VRMS
with
CALIBRATION FOR IMPROVED ACCURACY
Another way of presenting the error function of the ADL5502 is
shown in Figure 56. In this case, the dB error at hot and cold
temperatures is calculated with respect to the transfer function
at ambient temperature. This is a key difference in comparison to
the previous plots. Up until now, the errors were calculated with
respect to the ideal linear transfer function at ambient temperature.
When this alternative technique is used, the error at ambient
temperature becomes equal to zero by definition (see Figure 56).
This plot is a useful tool for estimating temperature drift at a
particular power level with respect to the (nonideal) response at
ambient. The linearity and dynamic range tend to be improved
artificially with this type of plot because the ADL5502 does not
perfectly follow the ideal linear equation (especially outside of
its linear operating range). Achieving this level of accuracy in
an end application requires calibration at multiple points in the
operating range of the device.
2
1
0
ERROR (d B)
–1
–2
–3
–25–20–15–10–5051015
Figure 56. VRMS Error from +25°C Output Voltage at −40°C, +25°C, and
+85°C After Ambient Normalization, Frequency 1900 MHz, Supply 3.0 V
+25ºC
+85ºC
–40ºC
INPUT (dBm)
07631-056
Note that the high accuracy range center varies over frequency
(see Figure 13, Figure 14, Figure 15, Figure 19, Figure 20, and
Figure 21).
CALCULATION OF CREST FACTOR (CF)
The ADL5502 is a true rms power detector in combination with
an envelope detector that accurately determines the crest factor
of a modulated signal. The device has two outputs, VRMS and
PEAK, which respectively provide the rms and envelope peak of
the RF waveform present at RFIN. Therefore, these two outputs can
be used to accurately calculate the crest factor of the waveform.
Before CF can be measured and calculated, both of the ADL5502
outputs must be calibrated (see the Device Calibration and Error
Calculation section for the calibration procedure for VRMS and
PEAK). It is suggested that the calibration step be completed by
applying at least two input power levels with a CW signal. The
CW signal (with a CF of 0 dB) serves as the reference for the CF
calculation. When the characteristics (slope and intercept) of
the VRMS and PEAK outputs are known, the calibration for the
CF calculation is complete.
Rev. A | Page 20 of 28
Page 21
ADL5502
A three-stage process must be taken to measure and calculate
the crest factor of any waveform. First, the unknown signal
must be applied to the RF input and the corresponding VRMS
level is measured. This level is indicated in Figure 57 as
V
VRMS-UNKNOWN
V
VRMS-UNKNOWN
V
PEAK-UNKNOW N
V
VRMS-UNKNO WN
V
Next, the CW reference level of PEAK, V
using
. The RF input, VIN, is calculated using
andEquation 5.
PEAK OF
UNKNOWN WAVEFO RM
VRMS OF
OUTPUT (V)
3
PEAK-CW
2
1
0
V
IN
Figure 57. Procedure for Crest Factor Calculation
V
(that is, the output voltage that would be seen if the
IN
UNKNOWN WAVEFO RM
(RESULT INDEP ENDENT
OF WAVEFORM)
INPUT (V rms)
PEAK OF
CW, CF = 0d B
PEAK-CW
, is calculated
07631-057
incoming waveform was a CW signal).
V
Finally, the actual level of PEAK,
PEAK-CW
= (VIN Gain
) + Intercept
PEAK
V
PEAK-UNKNOWN
(7)
PEAK
, is measured and
the CF can be calculated as
CF = 20·log
V
where
V
PEAK-UNKNOWN
PEAK-CW
(V
10
PEAK-UNKNOWN/VPEAK-CW
) (8)
, is used as a reference point to compare
,. If both V
values are equal, then the CF is 0 dB,
PEAK
as shown in Figure 58 with the CW signal. Across the dynamic
range, the calculated CF hovers about the 0 dB line. Likewise, for
complex waveforms of 3 dB, 6 dB, and 9 dB CFs, the calculations
accurately hover about the corresponding CF levels.
10
9
8
7
6
5
4
3
CREST FACTOR (dB)
2
1
0
–1
–25–20–15–10–5051015
Figure 58. Reported Crest Factor of Various Waveforms
8-TONE WAVEFORM, 9d B CF
4-TONE WAV EFORM, 6d B CF
2-TONE WAV EFORM, 3dB CF
CW, 0dB CF
INPUT (dBm)
07631-058
DRIFT OVER A REDUCED TEMPERATURE RANGE
Figure 59 and Figure 60 shows the error over temperature for a
1.9 GHz input signal. RMS error due to drift over temperature
consistently remains within ±0.25 dB and only begins to exceed
this limit when the ambient temperature rises above +65°C and
drops below −30°C. For all frequencies using a reduced
temperature range, higher measurement accuracy is achievable.
1.00
+25°C
–40°C
–20°C
+5°C
+45°C
+75°C
–10°C
+15°C
+55°C
+85°C
0.75
0.50
0.25
0
ERROR (dB)
–0.25
–0.50
–0.75
–1.00
–25–20–15–10–5051015
Figure 59. VRMS Typical Drift at 1.9 GHz for Various Temperatures
1.00
+25°C
–40°C
–20°C
+5°C
+45°C
+75°C
–10°C
+15°C
+55°C
+85°C
0.75
0.50
0.25
0
ERROR (dB)
–0.25
–0.50
–0.75
–1.00
–25–20–15–10–5051015
Figure 60. PEAK Typical Drift at 1.9 GHz for Various Temperatures
–30°C
0°C
+35°C
+65°C
INPUT (dBm)
–30°C
0°C
+35°C
+65°C
INPUT (dBm)
07631-059
07631-060
Rev. A | Page 21 of 28
Page 22
ADL5502
OPERATION AT HIGH FREQUENCIES
The ADL5502 works at high frequencies but exhibits slightly
higher linearity error. Figure 61 and Figure 62 show the linearity
error distributions for VRMS and PEAK of 50 devices at 6000 MHz
over temperature. The typical slopes at 6000 MHz are 0.87 V/V rms
and 0.58 V/V rms for VRMS and PEAK, respectively. The intercepts
at 6000 MHz are 0.002 V and 0.005 V for each respective output.
3
2
1
0
ERROR (dB)
–1
–2
–3
–25–20–15–10–505
INPUT (dBm)
Figure 61. VRMS Output Temperature Drift from +25°C Linear Reference
for 50 Devices at −40°C, +25°C, and +85°C, 6000 MHz, Supply 3.0 V
3
10
15
07631-061
3
2
1
0
ERROR (dB)
–1
–2
–3
–25–20–15–10–505
INPUT (dBm)
10
15
Figure 63. VRMS Output Delta from +25°C Output Voltage for
50 Devices at −40°C and +85°C, Frequency 6000 MHz, Supply 3.0 V
3
2
1
0
ERROR (d B)
–1
07631-063
2
1
0
ERROR (dB)
–1
–2
–3
–25–20–15–10–505
INPUT (dBm)
10
15
07631-062
Figure 62. PEAK Output Temperature Drift from +25°C Linear Reference
for 50 Devices at −40°C, +25°C, and +85°C, 6000 MHz, Supply 3.0 V
Due to the repeatability of the performance from part to part,
compensation can be applied to reduce the effects of temperature
drift and linearity error. To detect larger dynamic ranges at
higher frequencies, the transfer function at ambient temperature
can be calibrated, thus eliminating the linearity error. This
technique is discussed in detail in the Calibration for Improved
Accuracy section. Figure 63 and Figure 64 show the temperature
drift distributions for both outputs of 50 devices at 6000 MHz.
–2
–3
–25–20–15–10–505
INPUT (dBm)
10
15
07631-064
Figure 64. PEAK Output Delta from +25°C Output Voltage for
50 Devices at −40°C and +85°C, Frequency 6000 MHz, Supply 3.0 V
DEVICE HANDLING
The wafer-level chip scale package consists of solder bumps
connected to the active side of the die. The part is lead-free with
95.5% tin, 4.0% silver, and 0.5% copper solder bump composition.
The WLCSP can be mounted on printed circuit boards using
standard surface-mount assembly techniques; however, caution
should be taken to avoid damaging the die. See the AN-617
Application Note,
additional information. WLCSP devices are bumped die; therefore,
the exposed die can be sensitive to light, which can influence
specified limits. Lighting in excess of 600 lux can degrade
performance.
MicroCSP Wafer Level Chip Scale Package, for
Rev. A | Page 22 of 28
Page 23
ADL5502
EVALUATION BOARD
Figure 65 shows the schematic of the ADL5502 evaluation board.
The board is powered by a single supply in the 2.5 V to 3.3 V
range. The power supply is decoupled by 100 pF and 0.1 µF
capacitors.
Tabl e 4 details the various configuration options of the evaluation
board. Figure 66 and Figure 67 show the component and circuit
layouts of the evaluation board.
The RF input has a broadband match of 50 Ω using a single
75 resistor at R10. More precise matching at spot frequencies
is possible using the pads for C15, C16, and R10 (see the RF
Input Interfacing section).
The two outputs, accessible via the SMAs labeled VRMS and
VENV, provide the rms response and the envelope/peak-hold
measurement of the RF input power level. The device must be
enabled by switching SW1 to high (setting the switch to the
position opposite that of the SW1 label).
RFIN
VPOS
(P1 – 8)
ENBL
C17
10nF
C
1
4
1
0
0
F
p
R10
C15C16
75Ω
VPOS
R2
0Ω
1
2
3
1
C
F
µ
1
.
0
3
VPOS(P1 – 1)
SW1
8
ENBL
FLTR
VRMS
ADL5502
1
p
2
F
COMM
4
PEAK
CNTL
1
C
1
.
0
1
F
µ
VPOS
RFIN
C
0
0
1
Figure 65. Evaluation Board Schematic
R1
0Ω
7
6
5
The device is placed in peak-hold mode by placing the switch
SW2 in the position closes to the SW2 label. Envelope-tracking
mode is possible by setting SW2 in the opposite switch position
(away from the SW2 label). A signal generator can drive the control
mode via the SMA labeled CNTL (see Tab l e 4 for more details).
Operating in Peak-Hold Mode
To operate the device in peak-hold mode, the control line must be
temporally set to high (reset mode for >1 s) and then set back to
low (peak-hold mode). This allows the ADL5502 initialize to a
known state.
Land Pattern and Soldering Information
Pad diameters of 0.28 mm are recommended with a solder paste
mask opening of 0.38 mm. For the RF input trace, a trace width
of 0.30 mm is used, which corresponds to a 50 characteristic
impedance for the dielectric material being used (FR4). All traces
going to the pads are tapered down to 0.15 mm. For the RFIN
line, the length of the tapered section is 0.20 mm.
(P1 – 4)
R11
(OPEN)
R12
(OPEN)
R4
0Ω
(P1 – 6)
R5
0Ω
(P1 – 6)
R9
0Ω
R7
10kΩ
VPOS
VRMS
VENV
CNTL
07631-065
R3
0Ω
C18
(OPEN)
R6
0Ω
C19
(OPEN)
R13
0Ω
C20
(OPEN)
R8
10kΩ
SW2
Figure 66. Layout of Evaluation Board, Component Side
7631-066
Rev. A | Page 23 of 28
07631-067
Figure 67. Layout of Evaluation Board, Circuit Side
Page 24
ADL5502
Table 4. Evaluation Board Configuration Options
Component Description Default Condition
VPOS, GND Ground and Supply Vector Pins. Not applicable
C13, C14 Power Supply Decoupling. Nominal supply decoupling of 0.01 μF and 100 pF.
C17
R10, C15, C16
R3, R6, R11,
R12, C18, C19
R1, SW1
R7, R8, R13,
C20, SW2
R2, R4, R5,
R9, C11, C12
Filter Capacitor. The internal rms averaging capacitor can be augmented by placing
additional capacitance in C17.
RF Input interface. The 75 Ω resistor at R10 combines with the ADL5502 internal input
impedance to give a broadband input impedance of around 50 Ω. The pads for components
C15, C16, and R10 can be used for more precise matching at a particular frequency.
Output Filtering. The combination of the internal 100 Ω output resistance and C18 produce
a low-pass filter to reduce output ripple of the VRMS output. Similarly, C19 and the internal
100 Ω output resistance form a low-pass filter at the PEAK output. Either output can be
scaled down using the resistor divider pads, R3, R11, R6, and R12.
Device Enable. When the switch is set toward the SW1 label, the ENBL pin is grounded
(through the 0 Ω resistor) putting the device in power-down mode. In the opposite switch
position, the ENBL pin is connected to VPOS and the ADL5502 is in enable mode. While the
switch is in the disabled position, the ENBL pin can be driven by a signal generator via the
SMA labeled ENBL. In this case, R1 must be removed or changed to provide a 50 Ω match.
Control Interface. When the switch is set toward the SW2 label, the CNTL pin is grounded
(through a 10 kΩ resistor) putting the device in peak-hold mode. In the opposite switch
position, the pin is connected to VPOS (through a 10 kΩ resistor) and the ADL5502 is in
reset mode. While the switch is in the peak-hold position, the CNTL pin can be driven by
a signal generator via the SMA labeled CNTL. In this case, R8 may be removed or changed to
provide a 50 Ω match. R13 and C20 allow for a low-pass filter design for the control pin.
Alternate Interface. The end connector, P1, allows access to various ADL5502 signals.
These signal paths are only used during factory test and characterization.
C13 = 0.1 μF (Size 0402)
C14 = 100 pF (Size 0402)
C17 = 10 nF (Size 0402)
R10 = 75 Ω (Size 0402)
C15, C16 = 0 Ω (Size 0402)
R3, R6 = 0 Ω (Size 0402)
R11, R12 = open (Size 0402)
C18, C19 = open (Size 0402)