FEATURES
Calibrated RMS Response
Excellent Temperature Stability
Up to 30 dB Input Range at 2.5 GHz
700 mV rms, 10 dBm re 50 ⍀ Maximum Input
ⴞ0.25 dB Linear Response Up to 2.5 GHz
Single Supply Operation: 2.7 V to 5.5 V
Low Power: 3.3 mW at 3 V Supply
Rapid Power-Down to Less than 1 A
APPLICATIONS
Measurement of CDMA, W-CDMA, QAM, Other
Complex Modulation Waveforms
RF Transmitter or Receiver Power Measurement
PRODUCT DESCRIPTION
The AD8361 is a mean-responding power detector for use in highfrequency receiver and transmitter signal chains, up to 2.5 GHz.
It is very easy to apply. It requires only a single supply between
2.7 V and 5.5 V, power supply decoupling capacitor and an
input coupling capacitor in most applications. The output is a
linear-responding dc voltage with a conversion gain of 7.5 V/V rms.
An external filter capacitor can be added to increase the averaging time constant.
RFIN
PWDN
RFIN
™
TruPwr
Detector
AD8361
FUNCTIONAL BLOCK DIAGRAMS
micro_SOIC
2
TRANSCONDUCTANCE
CELLS
TRANSCONDUCTANCE
CELLS
2
2
2
i
i
BAND-GAP
REFERENCE
SOT-23-6L
i
i
ERROR
AMP
ERROR
AMP
INTERNAL FILTER
AD8361
IREF
INTERNAL FILTER
AD8361
ⴛ 7.5
BUFFER
OFFSET
ⴛ 7.5
BUFFER
VPOS
FLTR
VRMS
ADD
SREF
COMM
VPOS
FLTR
VRMS
3.0
2.8
2.6
2.4
2.2
2.0
1.8
1.6
1.4
1.2
V rms – Volts
1.0
0.8
0.6
0.4
0.2
0.0
0
SUPPLY
REFERENCE MODE
INTERNAL
REFERENCE MODE
REFERENCE MODE
RFIN – V rms
GROUND
0.50.10.20.30.4
Figure 1. Output in the Three Reference Modes, Supply 3 V,
Frequency 1.9 GHz (SOT-23-6L Package Ground Reference
Mode Only)
TruPwr is a trademark of Analog Devices, Inc.
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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
PWDN
BAND-GAP
REFERENCE
COMM
The AD8361 is intended for true power measurement of simple
and complex waveforms. The device is particularly useful for
measuring high crest-factor (high peak-to-rms ratio) signals, such
as CDMA and W-CDMA.
The AD8361 has three operating modes to accommodate a
variety of analog-to-digital converter requirements:
1. Ground referenced mode, in which the origin is zero;
2. Internal reference mode, which offsets the output 350 mV
above ground;
3. Supply reference mode, which offsets the output to V
/7.5.
S
The AD8361 is specified for operation from –40°C to +85°C and
is available in 8-lead micro_SOIC and 6-lead SOT packages.
It is fabricated on a proprietary high f
Operating Temperature Range . . . . . . . . . . . –40°C to +85°C
Storage Temperature Range . . . . . . . . . . . . –65°C to +150°C
Lead Temperature Range (Soldering 60 sec) . . . . . . . . . 300°C
NOTES
1
Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent 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.
nal reference mode enabled when pin
is left open. Otherwise, this pin should
be tied to VPOS. DO NOT ground this
pin.
35RFINSignal Input Pin. Must be driven from
an ac-coupled source. The low frequency
real input impedance is 225 Ω.
44PWDNPower-Down Pin. For the device to
operate as a detector it needs a logical
low input (less than 100 mV). When
a logic high (greater than V
– 0.5 V)
S
is applied, the device is turned off and
the supply current goes to nearly zero
(ground and internal reference mode
less than 1 µA, supply reference mode
divided by 100 kΩ).
V
S
52COMM Device Ground Pin.
63FLTRBy placing a capacitor between this pin
and VPOS, the corner frequency of the
modulation filter is lowered. The onchip filter is formed with 27 pF储2 kΩ
for small input signals.
71VRMSOutput Pin. Near-rail-to-rail voltage
output with limited current drive capabilities. Expected load >10 kΩ to ground.
8SREFSupply Reference Control Pin. To en-
able supply reference mode this pin
must be connected to VPOS, otherwise it should be connected to COMM
(ground).
AD8361ARM*–40°C to +85°CTube, 8-Lead micro_SOICRM-8
AD8361ARM-REEL13" Tape and Reel
AD8361ARM-REEL77" Tape and Reel
AD8361ART-REEL13" Tape and ReelRT-6
AD8361ART-REEL77" Tape and Reel
AD8361-EVALEvaluation Board micro_SOIC
AD8361ART-EVALEvaluation Board SOT-23-6L
*Device branded as J3A.
CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily
accumulate on the human body and test equipment and can discharge without detection. Although
the AD8361 features proprietary ESD protection circuitry, permanent damage may occur on
devices subjected to high-energy electrostatic discharges. Therefore, proper ESD precautions are
recommended to avoid performance degradation or loss of functionality.
Figure 3. Output vs. Input Level, Supply 2.7 V, 3.0 V, 5.0 V,
and 5.5 V, Frequency 900 MHz
3.0
2.5
2.0
1.5
1.0
0.5
0
–0.5
ERROR – dB
–1.0
–1.5
–2.0
–2.5
–3.0
0.01
0.02
(–21dBm)
MEAN ⴞ3 SIGMA
0.1
(–7dBm)
INPUT – V rms
0.4
(+5dBm)
Figure 5. Error from Linear Reference vs. Input Level,
3 Sigma to Either Side of Mean, Sine Wave, Supply 3.0 V,
Frequency 900 MHz
3.0
2.5
2.0
1.5
1.0
0.5
0
–0.5
ERROR – dB
–1.0
–1.5
–2.0
–2.5
–3.0
0.01
0.02
(–21dBm)
MEAN ⴞ3 SIGMA
0.1
(–7dBm)
INPUT – V rms
0.6
(+8.6dBm)
Figure 6. Error from Linear Reference vs. Input Level,
3 Sigma to Either Side of Mean, Sine-Wave, Supply 5.0 V,
Frequency 900 MHz
5.0
4.5
4.0
3.5
3.0
2.5
2.0
OUTPUT – Volts
1.5
1.0
0.5
0.0
IS95
REVERSE LINK
0
INPUT – V rms
CW
WCDMA
4- AND 15-CHANNEL
0.50.10.20.30.4
0.60.70.8
Figure 4. Output vs. Input Level with Different Waveforms
Sine Wave (CW), IS95 Reverse Link, W-CDMA 4-Channel
and W-CDMA 15-Channel, Supply 5.0 V
3.0
2.5
2.0
ERROR – dB
1.5
1.0
0.5
0.0
–0.5
–1.0
–1.5
–2.0
–2.5
–3.0
CW
4-CHANNEL
15-CHANNEL
0.020.6
INPUT – V rms
0.2
IS95
REVERSE LINK
Figure 7. Error from CW Linear Reference vs. Input with
Different Waveforms Sine Wave (CW), IS95 Reverse Link,
W-CDMA 4-Channel and W-CDMA 15-Channel, Supply
3.0 V, Frequency 900 MHz
–4–
1.00.010.1
REV. A
Page 5
AD8361
3.0
2.5
2.0
1.5
1.0
0.5
0
–0.5
ERROR – dB
–1.0
–1.5
–2.0
–2.5
–3.0
0.01
0.02
(–21dBm)
MEAN ⴞ3 SIGMA
0.1
(–7dBm)
INPUT – V rms
0.4
(+5dBm)
Figure 8. Error from CW Linear Reference vs. Input,
3 Sigma to Either Side of Mean, IS95 Reverse Link Signal,
Supply 3.0 V, Frequency 900 MHz
3.0
2.5
2.0
1.5
1.0
0.5
0
–0.5
ERROR – dB
–1.0
–1.5
–2.0
–2.5
–3.0
0.01
0.02
(–21dBm)
MEAN ⴞ3 SIGMA
0.1
(–7dBm)
INPUT – V rms
0.6
(+8.6dBm)
Figure 9. Error from CW Linear Reference vs. Input Level,
3 Sigma to Either Side of Mean, IS95 Reverse Link Signal,
Supply 5.0 V, Frequency 900 MHz
3.0
2.5
2.0
ERROR – dB
1.5
1.0
0.5
–0.5
–1.0
–1.5
–2.0
–2.5
–3.0
0
0.01
0.02
(–21dBm)
INPUT – V rms
0.1
(–7dBm)
+85ⴗC
–40ⴗC
0.4
(+5dBm)
Figure 11. Output Delta from +25°C vs. Input Level,
3 Sigma to Either Side of Mean Sine Wave, Supply 3.0 V,
Frequency 1900 MHz, Temperature –40°C to +85°C
SUPPLY CURRENT – mA
11
10
9
8
+25ⴗC
VS = 3V
INPUT OUT
OF RANGE
–40ⴗC
7
6
5
4
+85ⴗC
3
2
1
0
0
VS = 5V
INPUT OUT
OF RANGE
–40ⴗC
INPUT – V rms
+25ⴗC
0.50.10.20.30.4
0.60.70.8
+85ⴗC
Figure 12. Supply Current vs. Input Level, Supplies 3.0 V,
°
and 5.0 V, Temperatures –40
C, +25°C, and +85°C
3.0
2.5
2.0
ERROR – dB
1.5
1.0
0.5
–0.5
–1.0
–1.5
–2.0
–2.5
–3.0
0
0.01
0.02
(–21dBm)
INPUT – V rms
0.1
(–7dBm)
+85ⴗC
–40ⴗC
0.4
(+5dBm)
Figure 10. Output Delta from +25°C vs. Input Level,
3 Sigma to Either Side of Mean Sine Wave, Supply 3.0 V,
Frequency 900 MHz, Temperature –40°C to +85°C
REV. A
250
+25
ⴗ
C
ⴗ
C
+85
200
–40
ⴗ
C
+85
ⴗ
C
150
100
+25
ⴗ
C
SHUNT RESISTANCE – ⍀
50
0
05001000
–40
ⴗ
C
FREQUENCY – MHz
1500
20002500
Figure 13. Input Impedance vs. Frequency, Supply 3 V,
The AD8361 is an rms-responding (mean power) detector providing an approach to the exact measurement of RF power that
is basically independent of waveform. It achieves this function
through the use of a proprietary technique in which the outputs
of two identical squaring cells are balanced by the action of a
high-gain error amplifier.
The signal to be measured is applied to the input of the first
squaring cell, which presents a nominal (LF) resistance of 225 Ω
between the pin RFIN and COMM (connected to the ground
plane). Since the input pin is at a bias voltage of about 0.8 V
above ground, a coupling capacitor is required. By making this
an external component, the measurement range may be extended
to arbitrarily low frequencies.
The AD8361 responds to the voltage, V
this voltage to generate a current proportional to V
, at its input, by squaring
IN
squared.
IN
This is applied to an internal load resistor, across which is connected a capacitor. These form a low-pass filter, which extracts
the mean of V
squared. Although essentially voltage-responding,
IN
the associated input impedance calibrates this port in terms of
equivalent power. Thus 1 mW corresponds to a voltage input of
447 mV rms. In the Application section it is shown how to match
this input to 50 Ω.
The voltage across the low-pass filter, whose frequency may
be arbitrarily low, is applied to one input of an error-sensing
amplifier. A second identical voltage-squaring cell is used to
close a negative feedback loop around this error amplifier.
This second cell is driven by a fraction of the quasi-dc output
voltage of the AD8361. When the voltage at the input of the
second squaring cell is equal to the rms value of V
, the loop
IN
is in a stable state, and the output then represents the rms value of
the input. The feedback ratio is nominally 0.133, making the
rms-dc conversion gain ×7.5, that is
V
= 7.5 × VIN rms
OUT
By completing the feedback path through a second squaring cell,
identical to the one receiving the signal to be measured, several
benefits arise. First, scaling effects in these cells cancel; thus, the
overall calibration may be accurate, even though the open-loop
response of the squaring cells taken separately need not be.
Note that in implementing rms-dc conversion, no reference
voltage enters into the closed-loop scaling. Second, the tracking
in the responses of the dual cells remains very close over temperature, leading to excellent stability of calibration.
The squaring cells have very wide bandwidth with an intrinsic
response from dc to microwave. However, the dynamic range
of such a system is fairly small, due in part to the much larger
dynamic range at the output of the squaring cells. There are
practical limitations to the accuracy with which very small error
signals can be sensed at the bottom end of the dynamic range,
arising from small random offsets; these set the limit to the
attainable accuracy at small inputs.
On the other hand, the squaring cells in the AD8361 have
a “Class-AB” aspect; the peak input is not limited by their
quiescent bias condition, but is determined mainly by the
eventual loss of square-law conformance. Consequently, the top
end of their response range occurs at a fairly large input level
(about 700 mV rms) while preserving a reasonably accurate
square-law response. The maximum usable range is, in practice,
limited by the output swing. The rail-to-rail output stage can
swing from a few millivolts above ground to less than 100 mV
below the supply. An example of the output induced limit: given
a gain of 7.5 and assuming a maximum output of 2.9 V with a 3 V
supply; the maximum input is (2.9 V rms)/7.5 or 390 mV rms.
Filtering
An important aspect of rms-dc conversion is the need for
averaging (the function is root-MEAN-square). For complex RF
waveforms such as occur in CDMA, the filtering provided by
the on-chip low-pass filter, while satisfactory for CW signals above
100 MHz, will be inadequate when the signal has modulation
components that extend down into the kilohertz region. For this
reason, the FLTR pin is provided: a capacitor attached between
this pin and VPOS can extend the averaging time to very low
frequencies.
Offset
An offset voltage can be added to the output (when using the
micro_SOIC version) to allow the use of A/D converters whose
range does not extend down to ground. However, accuracy at
the low end will be degraded because of the inherent error in this
added voltage. This requires that the pin IREF (internal reference)
should be tied to VPOS and SREF (supply reference) to ground.
In the IREF mode, the intercept is generated by an internal
reference cell, and is a fixed 350 mV, independent of the supply
voltage. To enable this intercept, IREF should be open-circuited,
and SREF should be grounded.
In the SREF mode, the voltage is provided by the supply. To
implement this mode, tie IREF to VPOS and SREF to VPOS. The
offset is then proportional to the supply voltage, and is 400 mV
for a 3 V supply and 667 mV for a 5 V supply.
USING THE AD8361
Basic Connections
Figures 32, 33, and 34 show the basic connections for the
micro_SOIC version AD8361 in its three operating modes. In all
modes, the device is powered by a single supply of between 2.7 V
and 5.5 V. The VPOS pin is decoupled using 100 pF and 0.01 µF
capacitors. The quiescent current of 1.1 mA in operating mode
can be reduced to 1 µA by pulling the PWDN pin up to VPOS.
A 75 Ω external shunt resistance combines with the ac-coupled
input to give an overall broadband input impedance near 50 Ω.
Note that the coupling capacitor must be placed between the input and the shunt impedance. Input impedance and input coupling
are discussed in more detail below.
The input coupling capacitor combines with the internal input
resistance (Figure 13) to give a high-pass corner frequency
given by the equation
f
dB
3
2=××π
1
CR
CIN
REV. A
–9–
Page 10
AD8361
With the 100 pF capacitor shown in Figures 32–34, the highpass corner frequency is about 8 MHz.
2.7 – 5.5V
+V
S
100pF
RFIN
0.01F
R1
75⍀
C
C
100pF
AD8361
1
VPOS
2
IREF
3
RFIN
45
PWDN
SREF
VRMS
FLTR
COMM
8
7
6
V rms
CFLTR
Figure 32. Basic Connections for Ground Referenced Mode
2.7 – 5.5V
+V
S
100pF
RFIN
0.01F
R1
75⍀
C
C
100pF
AD8361
1
VPOS
2
IREF
3
RFIN
45
PWDN
SREF
VRMS
FLTR
COMM
8
7
6
V rms
CFLTR
Figure 33. Basic Connections for Internal Reference Mode
2.7 – 5.5V
+V
S
100pF
RFIN
0.01F
R1
75⍀
C
C
100pF
AD8361
1
VPOS
2
IREF
3
RFIN
45
PWDN
SREF
VRMS
FLTR
COMM
8
7
6
V rms
CFLTR
Figure 34. Basic Connections for Supply Referenced Mode
The output voltage is nominally 7.5 times the input rms voltage
(a conversion gain of 7.5 V/V rms). Three different modes of
operation are set by the pins SREF and IREF. In addition to the
ground referenced mode shown in Figure 32, where the output
voltage swings from around near ground to 4.9 V on a 5.0 V
supply, two additional modes allow an offset voltage to be added to
the output. In the internal reference mode, (Figure 33), the
output voltage swing is shifted upward by an internal reference
voltage of 350 mV. In supply referenced mode (Figure 34), an
offset voltage of V
/7.5 is added to the output voltage. Table I
S
summarizes the connections, output transfer function and minimum output voltage (i.e., zero signal) for each mode.
Output Swing
Figure 35 shows the output swing of the AD8361 for a 5 V supply
voltage for each of the three modes. It is clear from Figure 35,
that operating the device in either internal reference mode or
supply referenced mode, will reduce the effective dynamic range as
the output headroom decreases. The response for lower supply
voltages is similar (in the supply referenced mode, the offset is
smaller), but the dynamic range will be reduced further, as headroom decreases. Figure 36 shows the response of the AD8361 to
a CW input for various supply voltages.
5.0
4.5
4.0
3.5
3.0
2.5
2.0
OUTPUT – Volts
1.5
1.0
0.5
0.0
INTERNAL REF
0
SUPPLY REF
GROUND REF
INPUT – V rms
0.50.10.20.30.4
0.60.70.8
Figure 35. Output Swing for Ground, Internal and Supply
Referenced Mode. VPOS = 5 V (micro_SOIC Only)
5.5
5.0
4.5
4.0
3.5
3.0
2.5
2.0
OUTPUT – Volts
1.5
1.0
0.5
0.0
0
INPUT – V rms
5.5V
2.7V
0.60.70.8
0.50.10.20.30.4
5.0V
3.0V
Figure 36. Output Swing for Supply Voltages of 2.7 V,
3.0 V, 5.0 V and 5.5 V (micro_SOIC Only)
Dynamic Range
Because the AD8361 is a linear responding device with a nominal transfer function of 7.5 V/V rms, the dynamic range in dB is
not clear from plots such as Figure 35. As the input level is
increased in constant dB steps, the output step size (per dB)
will also increase. Figure 37 shows the relationship between the
output step size (i.e., mV/dB) and input voltage for a nominal
transfer function of 7.5 V/V rms.
Table I. Connections and Nominal Transfer Function for
Ground, Internal, and Supply Reference Modes
InternalOPENCOMM0.350 V7.5 VIN + 0.350 V
SupplyVPOSVPOSVS/7.57.5 VIN + VS/7.5
–10–
REV. A
Page 11
AD8361
700
600
500
400
mV/dB
300
200
100
0
0
INPUT – mV
500100200300400
600700800
Figure 37. Idealized Output Step Size as Function of Input
Voltage
Plots of output voltage vs. input voltage result in a straight line. It
may sometimes be more useful to plot the error on a logarithmic scale, as shown in Figure 38. The deviation of the plot for
the ideal straight line characteristic is caused by output clipping
at the high end and by signal offsets at the low end. It should
however be noted that offsets at the low end can be either positive or negative, so that this plot could also trend upwards at the
low end. Figures 5, 6, 8, and 9 show a ±3 sigma distribution of
device error for a large population of devices.
2.0
1.5
1.0
2.5GHz
1.9GHz
0.4
(+5dBm)
1.0
ERROR – dB
0.5
0.0
–0.5
–1.0
–1.5
–2.0
0.01
100MHz
0.02
(–21dBm)
100MHz
0.1
(–7dBm)
INPUT – V rms
900MHz
Figure 38. Representative Unit, Error in dB vs. Input Level,
= 2.7 V
V
S
It is also apparent in Figure 38 that the error plot tends to
shift to the right with increasing frequency. Because the input
impedance decreases with frequency, the voltage actually applied
to the input will also tend to decrease (assuming a constant source
impedance over frequency). The dynamic range is almost constant over frequency, but with a small decrease in conversion gain
at high frequency.
Input Coupling and Matching
The input impedance of the AD8361 decreases with increasing
frequency in both its resistive and capacitive components (Figure
13). The resistive component varies from 225 Ω at 100 MHz
down to about 95 Ω at 2.5 GHz.
A number of options exist for input matching. For operation at
multiple frequencies, a 75 Ω shunt to ground, as shown in Figure
39a, will provide 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. The VSWR can be held below
1.5 at frequencies up to 1 GHz, even as the input impedance
varies from part to part. (Both input impedance and input
capacitance can vary by up to ±20% around their nominal values.)
At very high frequencies (i.e., 1.8 GHz to 2.5 GHz), a shunt
resistor will not be sufficient to reduce the VSWR below 1.5.
Where VSWR is critical, remove shunt component and insert
an inductor in series with the coupling capacitor as shown in
Figure 39b.
Table II gives recommended shunt resistor values for various
frequencies and series inductor values for high frequencies. The
coupling capacitor, C
, essentially acts as an ac-short and plays
C
no intentional part in the matching.
C
C
RFIN
R
SH
RFIN
AD8361
a. Broadband Resistor Match
RFIN
L
M
C
C
RFIN
AD8361
b. Series Inductor Match
RFIN
C
M
C
C
RFIN
L
M
AD8361
c. Narrowband Reactive Match
RFIN
R
SERIES
C
C
RFIN
AD8361
d. Attenuating the Input Signal
Figure 39. Input Coupling/Matching Options
Table II. Recommended Component Values for Resistive or
Inductive Input Matching (Figures 39a and 39b)
FrequencyMatching Component
100 MHz63.4 Ω Shunt
800 MHz75 Ω Shunt
900 MHz75 Ω Shunt
1800 MHz150 Ω Shunt or 4.7 nH Series
1900 MHz150 Ω Shunt or 4.7 nH Series
2500 MHz150 Ω Shunt or 2.7 nH Series
REV. A
–11–
Page 12
AD8361
Alternatively, a reactive match can be implemented using a shunt
inductor to ground and a series capacitor as shown in Figure
39c. A method for hand calculating the appropriate matching
components is shown on page 12 of the AD8306 data sheet.
Matching in this manner results in very small values for C
,
M
especially at high frequencies. As a result, a stray capacitance as
small as 1 pF can significantly degrade the quality of the match.
The main advantage of a reactive match is the increase in sensitivity that results from the input voltage being “gained up” (by
the square root of the impedance ratio) by the matching network.
Table III shows recommended values for reactive matching.
Table III. Recommended Values for a Reactive Input Match
(Figure 39c)
Figure 39d shows a technique for coupling the input signal
into the AD8361, which may be applicable where the input signal
is much larger than the input range of the AD8361. A series
resistor combines with the input impedance of the AD8361 to
attenuate the input signal. Since 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 the transmission line’s impedance then the VSWR of
the system is relatively unaffected.
250
200
1.7
1.4
provides adequate filtering for all frequencies above 240 MHz
(i.e., ten times the frequency at the output of the squarer, which
is twice the input frequency). However, signals with high peakto-average ratios, such as CDMA or W-CDMA signals, and
with low frequency components, require additional filtering.
TDMA signals, such as GSM, PDC, or PHS have a peak-toaverage ratio that is close to that of a sinusoid, and the internal
filter is adequate.
The filter capacitance of the AD8361 can be augmented by
connecting a capacitor between Pin 6 (FLTR) and VPOS.
Table IV shows the effect of several capacitor values for various
communications standards with high peak-to-average ratios along
with the residual ripple at the output, in peak-to-peak and rms
volts. Note that large filter capacitors will increase the enable
and pulse response times, as discussed below.
Table IV. Effect of Waveform and C
on Residual AC
FILT
Output Residual AC
WaveformC
FILT
V dcmV p-p mV rms
IS95 Reverse LinkOpen0.5550100
1.01000180
2.02000360
0.01 µF0.5406
1.016020
2.043060
0.1 µF0.5203
1.0406
2.011018
IS95 8-Channel0.01 µF0.529040
Forward Link1.0975150
2.02600430
0.1 µF0.5507
1.019030
2.067095
W-CDMA 150.01 µF0.522535
Channel1.0940135
2.02500390
0.1 µF0.5456
1.016525
2.055080
150
100
RESISTANCE – ⍀
50
0
0
100015002000250030003500
500
FREQUENCY – MHz
1.1
0.8
CAPACITANCE – pF
0.5
0.2
Figure 40. Input Impedance vs. Frequency, Supply 3 V,
SOT-23-6L
Selecting the Filter Capacitor
The AD8361’s internal 27 pF filter capacitor is connected in
parallel with an internal resistance that varies with signal level
from 2 kΩ for small signals to 500 Ω for large signals. The
resulting low-pass corner frequency between 3 MHz and 12 MHz
–12–
Operation at Low Frequencies
Although the AD8361 is specified for operation up to 2.5 GHz,
there is no lower limit on the operating frequency. It is only necessary to increase the input coupling capacitor to reduce the
corner frequency of the input high-pass filter (use an input resistance of 225 Ω for frequencies below 100 MHz). It is also
necessary to increase the filter capacitor so that the signal at the
output of the squaring circuit is free of ripple. The corner frequency will be set by the combination of the internal resistance of
2 kΩ and the external filter capacitance.
Power Consumption, Enable and Power-On
The quiescent current consumption of the AD8361 varies with
the size of the input signal from about 1 mA for no signal up to
7 mA at an input level of 0.66 V rms (9.4 dBm re 50 Ω). If the
input is driven beyond this point, the supply current increases
steeply (see Figure 12). There is little variation in quiescent
current with power supply voltage.
REV. A
Page 13
AD8361
The AD8361 can be disabled either by pulling the PWDN (Pin 4)
to VPOS or by simply turning off the power to the device. While
turning off the device obviously eliminates the current consumption, disabling the device reduces the leakage current to less
than 1 µA. Figures 23 and 24 show the response of the output of
the AD8361 to a pulse on the PWDN pin, with no capacitance and
with a filter capacitance of 0.01 µF respectively; the turn-on time is
a function of the filter capacitor. Figure 27 shows a plot of the
output response to the supply being turned on (i.e., PWDN is
grounded and VPOS is pulsed) with a filter capacitor of 0.01 µF
Again, the turn-on time is strongly influenced by the size of the
filter capacitor.
If the input of the AD8361 is driven while the device is disabled
(PWDN = VPOS), the leakage current of less than 1 µA will
increase as a function of input level. When the device is disabled, the output impedance increases to around 16 kΩ.
Volts to dBm Conversion
In many of the plots, the horizontal axis is scaled in both rms
volts and dBm. In all cases, dBm are calculated relative to an
impedance of 50 Ω. To convert between dBm and volts in a
50 Ω. system, the following equations can be used. Figure 40
shows this conversion in graphical form.
2
50
Ω
=
1020
log (() )
W
dBm
–
Ω
1
10
=
2
V rms
–
1
dBm
log/
(
20
10
)
V rms
()
Power dBm
()log
=
=××
V rmsW
0 00150
.log
10
0 001
.
current is required (>10 mA), the AD8051, which also has railto-rail capability, can be used, down to a supply voltage of 3 V. It
can deliver up to 45 mA of output current.
0.01F
VPOS
AD8361
COMM PWDN
100pF
0.01F
VOUT
AD8031
5k⍀
5k⍀
5V
15V/V rms
a. Slope of 15 V/V rms
0.01F
VPOS
AD8361
COMM PWDN
100pF
VOUT
5k⍀
5k⍀
10k⍀
0.01F
AD8031
5V
3.75V/V rms
b. Slope of 3.75 V/V rms
5V
VPOS
AD8361
100pF
VOUT
AD8031
0.01F
7.5V/V rms
0.01F
V rmsdBm
1
0.1
0.01
0.001
+20
+10
0
–10
–20
–30
–40
Figure 41. Conversion from dBm to rms Volts
Output Drive Capability and Buffering
The AD8361 is capable of sourcing an output current of approximately 3 mA. If additional current is required, a simple buffering
circuit can be used as shown in Figure 42c. Similar circuits
can be used to increase or decrease the nominal conversion gain of
7.5 V/V rms (Figure 42a and 42b). In Figure 42b, the AD8031
buffers a resistive divider to give a slope of 3.75 V/V rms. In Figure
42a, the op amp’s gain of two increases the slope to 15 V/V rms.
Using other resistor values, the slope can be changed to an
arbitrary value. The AD8031 rail-to-rail op amp, used in these
examples can swing from 50 mV to 4.95 V on a single 5 V supply
and operate at supply voltages down to 2.7 V. If high output
COMM PWDN
c. Slope of 7.5 V/V rms
Figure 42. Output Buffering Options
OUTPUT REFERENCE TEMPERATURE DRIFT
COMPENSATION
The error due to low temperature drift of the AD8361 can be
reduced if the temperature is known. Many systems incorporate
a temperature sensor; the output of the sensor is typically digitized, facilitating a software correction. Using this information,
only a two-point calibration at ambient is required.
The output voltage of the AD8361 at ambient (25°C) can be
expressed by the equation:
VGAIN VV
=×
OUTINOS
()
+
where GAIN is the conversion gain in V/V rms and VOS is the
extrapolated output voltage for an input level of 0 V. GAIN and
(also referred to as Intercept and Output Reference) can be
V
OS
calculated at ambient using a simple two-point calibration;
that is, by measuring the output voltages for two specific input
levels. Calibration at roughly 35 mV rms (–16 dBm) and
250 mV rms (+1 dBm) is recommended for maximum linear
dynamic range. However, alternative levels and ranges can be
REV. A
–13–
Page 14
AD8361
chosen to suit the application. GAIN and VOS are then calculated
using the equations:
VV
−
OUTOUT
21
GAIN
VVGAIN V
OSOUTIN
Both GAIN and VOS drift over temperature. However, the drift
has a bigger influence on the error relative to the output.
of V
OS
This can be seen by inserting data from Figures 14 and 17 (conversion gain and intercept drift) into the equation for V
plots are consistent with Figures 10 and 11 which show that the
error due to temperature drift decreases with increasing input
level. This results from the offset error having a diminishing
influence with increasing level on the overall measurement error.
From Figure 14, the average Intercept drift is 0.43 mV/°C from
–40°C to +25°C and 0.17 mV/°C from +25°C to +85°C. For a
less rigorous compensation scheme, the average drift over the
complete temperature range can be calculated:
DRIFTV C
With the drift of V
()
VOS
included, the equation for V
OS
()
=
VV
−
ININ
21
()
=− ×
11
()
. These
OUT
VV
..
/
°
= 0.000304 V/°C
0 0100 028
=
+°−−°
8540
−−
()
CC
()
becomes:
OUT
VGAIN VVDRIFTTEMPC
=×
OUTINOSVOS
The equation can be rewritten to yield a temperature compensated value for V
EVALUATION BOARD
Figures 43 and 46 show the schematic of the AD8361 evaluation board. Note that uninstalled components are drawn in as
dashed. The layout and silkscreen of the component side are
shown in Figures 44, 45, 47, and 48. The board is powered by a
single supply in the range, 2.7 V to 5.5 V. The power supply
is decoupled by 100 pF and 0.01 µF capacitors. Additional
decoupling, in the form of a series resistor or inductor in R6,
can also be added. Table V details the various configuration
options of the evaluation board.
()
IN
VVDRIFTTEMPC
OUTOSVOS
()
V
=
IN
++×−°
.
−−×−°
GAIN
()
()
25
25
Table V. Evaluation Board Configuration Options
ComponentFunctionDefault Condition
TP1, TP2Ground and Supply Vector Pins.Not Applicable
SW1Device Enable. When in Position A, the PWDN pin is connected to +V
the AD8361 is in power-down mode. In Position B, the PWDN pin is grounded,
putting the device in operating mode.
SW2/SW3Operating Mode. Selects either Ground Referenced Mode, Internal ReferenceSW2 = A, SW3 = B
Mode or Supply Reference Mode. See Table I for more details.(Ground Reference Mode)
C1, R2Input Coupling. The 75 Ω resistor in position R2 combines with the AD8361’sR2 = 75 Ω (Size 0402)
internal input impedance to give a broadband input impedance of around 50 Ω.C1 = 100 pF (Size 0402)
For more precise matching at a particular frequency, R2 can be replaced by a
different value (see Input Matching and Figure 39).
Capacitor C1 ac-couples the input signal and creates a high-pass input filter
whose corner frequency is equal to approximately 8 MHz. C1 can be increased
for operation at lower frequencies. If resistive attenuation is desired at the input,
series resistor R1, which is nominally 0 Ω, can be replaced by an appropriate value.
C2, C3, R6Power Supply Decoupling. The nominal supply decoupling of 0.01 µF andC2 = 0.01 µF (Size 0402)
100 pF. A series inductor or small resistor can be placed in R6 for additionalC3 = 100 pF (Size 0402)
decoupling.R6 = 0 Ω (Size 0402)
C5Filter Capacitor. The internal 50 pF averaging capacitor can be augmentedC5 = 1 nF (Size 0603)
by placing a capacitance in C5.
C4, R5Output Loading. Resistors and capacitors can be placed in C4 and R5 toC4 = R5 = Open
load test V rms.(Size 0603)
andSW1 = B
S
–14–
REV. A
Page 15
RFIN
C5
1nF
C3
100pF
C2
0.01F
J2
J3
J1
R2
75⍀
TP2
R4
0⍀
C4
OPEN
R5
OPEN
AD8361
VPOS
RFIN
PWDN
VRMS
FLTR
COMM
1
2
3
4
5
6
TP1
C1
100pF
SW1
1
2
3
R7
50⍀
VPOS
TP2
0⍀
V
A
B
VPOS
A
B
VPOS
R6
S
SW2
75⍀
R2
SW1
0.01F
100pF
C2
C3
100pF
AD8361
VPOS
IREF
RFIN
PWDN
SREF
VRMS
FLTR
COMM
8
7
6
1
C1
2
3
45
1nF
AD8361
V
S
SW3
A
B
VPOS
TP1
R5
(OPEN
C5
R4
0⍀
V
C4
)
(OPEN
rms
)
Figure 43. Evaluation Board Schematic micro_SOIC
Figure 44. Layout of Component Side micro_SOIC
Figure 46. Evaluation Board Schematic, SOT-23-6L
Figure 47. Layout of the Component Side, SOT-23-6L
Figure 45. Silkscreen of Component Side micro_SOIC
REV. A
Figure 48. Silkscreen of the Component Side, SOT-23-6L
–15–
Page 16
AD8361
0.122 (3.10)
0.106 (2.70)
PIN 1
0.118 (3.00)
0.098 (2.50)
0.075 (1.90)
BSC
0.037 (0.95) BSC
1
3
4 5 6
2
0.071 (1.80)
0.059 (1.50)
0.009 (0.23)
0.003 (0.08)
0.022 (0.55)
0.014 (0.35)
10ⴗ
0ⴗ
0.020 (0.50)
0.010 (0.25)
0.006 (0.15)
0.000 (0.00)
0.051 (1.30)
0.035 (0.90)
SEATING
PLANE
0.057 (1.45)
0.035 (0.90)
Problems caused by impedance mismatch may arise using the
evaluation board to examine the AD8361 performance. One
way to reduce these problems is to put a coaxial 3 dB attenuator
on the RFIN SMA connector. Mismatches at the source, cable,
and cable interconnection, as well as those occurring on the
evaluation board can cause these problems.
A simple (and common) example of such problem is triple travel
due to mismatch at both the source and the evaluation board.
Here the signal from the source reaches the evaluation board
and mismatch causes a reflection. When that reflection reaches
the source mismatch, it causes a new reflection, which travels
back to the evaluation board adding to the original signal incident at the board. The resultant voltage will vary with both
cable length and frequency dependent upon the relative phase of
the initial and reflected signals. Placing the 3 dB pad at the
input of the board improves the match at the board and thus
reduces the sensitivity to mismatches at the source. When such
precautions are taken, measurements will be less sensitive to
cable length and other fixturing issues. In an actual application
when the distance between AD8361 and source is short and well
defined, this 3 dB attenuator is not needed.
CHARACTERIZATION SETUPS
Equipment
The primary characterization setup is shown in Figure 50. The
signal source used was a Rohde & Schwarz SMIQ03B, version
3.90HX. The modulated waveforms used for IS95 reverse link,
IS95 nine active channels forward (Forward Link 18 setting),
W-CDMA 4- and 15-channel were generated using the default
settings coding and filtering. Signal levels were calibrated into a
50 Ω impedance.
Analysis
The conversion gain and output reference are derived using the
coefficients of a linear regression performed on data collected in
its central operating range (35 mV rms to 250 mV rms). This
range was chosen to avoid areas of operation where offset distorts
the linear response. Error is stated in two forms Error from Linear
°
Response to CW waveform and Output Delta from 25
C performance.
The Error from Linear Response to CW waveform is the difference
in output from the ideal output defined by the conversion gain
and output reference. This is a measure of both the linearity of
the device response to both CW and modulated waveforms. The
error in dB uses the conversion gain multiplied times the input
as its reference. Error from Linear Response to CW waveform is not a
measure of absolute accuracy, since it is calculated using the
gain and output reference of each device. But it does show the
linearity and effect of modulation on the device response.
Error from 25°C performance uses the performance of a given
device and waveform type as the reference; it is predominantly a measure of output variation with temperature.
C4
0.1FC2100pF
AD8361
VPOS
IREF
RFIN
PWDN
R1
75⍀
Figure 49. Characterization Board
SMIQ038B
RF SOURCE
IEEE BUS
PC CONTROLLER
1
VPOS
2
IREF
3
C1
0.1F
RF SIGNAL
RFIN
45
PWDN
RFIN
3dB
ATTENUATOR
DC SOURCES
PRUP +V
Figure 50. Characterization Setup
8
SREF
7
VRMS
FLTR
COMM
CHARACTERIZATION
DC MATRIX / DC SUPPLIES / DMM
C3
6
AD8361
BOARD
SREF IREF
S
VRMS
SREF
VRMS
DC OUTPUT
C3716a–2–6/00 (rev. A) 01088
0.122 (3.10)
0.114 (2.90)
0.006 (0.15)
0.002 (0.05)
8-Lead micro_SOIC Package
(RM-8)
0.122 (3.10)
0.114 (2.90)
85
1
PIN 1
0.0256 (0.65) BSC
0.016 (0.40)
0.010 (0.25)
4
SEATING
PLANE
0.193
(4.90)
BSC
0.043
(1.10)
MAX
0.009 (0.23)
0.005 (0.13)
6ⴗ
0ⴗ
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
0.037 (0.95)
0.030 (0.75)
0.028 (0.70)
0.016 (0.40)
–16–
6-Lead SOT-23-6L Package
(RT-6)
PRINTED IN U.S.A.
REV. A
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