Complete RF detector/controller function
>50 dB range at 0.9 GHz (−48 dBm to +3 dBm re 50 Ω)
Accurate scaling from 0.1 GHz to 2.5 GHz
Temperature-stable linear-in-dB response
Log slope of 23 mV/dB, intercept at −60 dBm at 0.9 GHz
True integration function in control loop
Low power: 20 mW at 2.7 V
APPLICATIONS
Single, dual, and triple band mobile handset (GSM, DCS,
EDGE)
Transmitter power control
GENERAL DESCRIPTION
The AD8311 is a complete low cost subsystem for the precise
control of RF power amplifiers operating in the frequency range
0.1 GHz to 2.5 GHz and over a typical dynamic range of 50 dB.
It is intended for use in cellular handsets and other batteryoperated wireless devices. The log amp technique provides a
much wider measurement range and better accuracy than
controllers using diode detectors. In particular, its temperature
stability is excellent over a specified range of −40°C to +85°C.
50 dB GSM PA Controller
AD8311
Its high sensitivity allows control at low signal levels, thus
reducing the amount of power that needs to be coupled to the
detector. For convenience, the signal is internally ac-coupled.
This high-pass coupling, with a corner at approximately
0.016 GHz, determines the lowest operating frequency. Thus,
the source can be dc-grounded.
The AD8311 provides a voltage output, VAPC, which has the
voltage range and current drive to directly connect to the gain
control pin of most handset power amplifiers. VAPC can swing
from 300 mV above ground to within 200 mV below the supply
voltage. Load currents of up to 6 mA can be supported.
The setpoint control input is applied to pin VSET and has an
operating range of 0.25 V to 1.4 V. The associated circuit
determines the slope and intercept of the linear-in-dB
measurement system; these are nominally 23.6 mV/dB and
−59.7 dBm at 0.9 GHz. Further simplifying the application of
the AD8311, the input resistance of the setpoint interface is over
35 MΩ, and the bias current is typically 0.26 µA.
The AD8311 is available in a 6-ball wafer-level chip scale
package (WLCSP), 1.0 mm × 1.5 mm, and consumes 7.6 mA
from a 2.7 V to 5.5 V supply.
FUNCTIONAL BLOCK DIAGRAM
VPOS
RFIN
10dB
OFFSET
COMPENSATION
COMM
Rev. 0
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.
VPOS = 2.7 V, Frequency = 0.1 GHz, TA = 25°C, 52.3 Ω termination on RFIN, light condition = 600 lux, unless otherwise noted.
Table 1.
Parameter Conditions Min Typ Max Unit
SPECIFIED FREQUENCY RANGE RFIN (Pin 6) 0.1 2.5 GHz
MEASUREMENT MODE1 (f = 0.1 GHz)
Input Impedance No termination resistor on RFIN 2140 || 1.97 Ω || pF
±1 dB Dynamic Range TA = +25°C
Maximum Input Level
Minimum Input Level
2
Slope
−40°C < T
±1 dB error
±1 dB error
21.5 23.8 25.5 mV/dB
< +85°C
A
Intercept2 −66 −58.9 −51 dBm
VSET Voltage—High Power In PIN = –10 dBm 1.16 V
VSET Voltage—Low Power In PIN = –40 dBm 0.45 V
Temperature Sensitivity PIN = –10 dBm
25°C ≤ T
−40°C ≤ T
≤ +85°C
A
≤ +25°C
A
MEASUREMENT MODE (f = 0.9 GHz)
Input Impedance No termination resistor on RFIN 370 || 1.58 Ω || pF
±1 dB Dynamic Range TA = +25°C
Maximum Input Level
Minimum Input Level
−40°C < T
±1 dB error
±1 dB error
< +85°C
A
Slope2 23.6 mV/dB
Intercept2 −59.7 dBm
VSET Voltage—High Power In PIN = –10 dBm 1.17 V
VSET Voltage—Low Power In PIN = –40 dBm 0.46 V
Temperature Sensitivity PIN = –10 dBm
25°C ≤ T
−40°C ≤ T
≤ +85°C
A
≤ +25°C
A
MEASUREMENT MODE (f = 1.9 GHz)
Input Impedance No termination resistor on RFIN 180 || 1.67 Ω || pF
±1 dB Dynamic Range TA = +25°C
Maximum Input Level
Minimum Input Level
−40°C < T
±1 dB error
±1 dB error
< +85°C
A
Slope2 22.7 mV/dB
Intercept2 −60.8 dBm
VSET Voltage—High Power In PIN = –10 dBm 1.15 V
VSET Voltage—Low Power In PIN = –40 dBm 0.47 V
Temperature Sensitivity PIN = –10 dBm
25°C ≤ T
−40°C ≤ T
≤ +85°C
A
≤ +25°C
A
47 dB
46 dB
+2 +2.6 dBm
−44.5 −44 dBm
−0.0020
+0.0121
dB/°C
dB/°C
51 dB
50 dB
+2.8 dBm
−47.9 dBm
0.0015
0.0094
dB/°C
dB/°C
42 dB
41 dB
−5.6 dBm
−48.0 dBm
0.0056
0.0077
dB/°C
dB/°C
Rev. 0 | Page 3 of 24
AD8311
Parameter Conditions Min Typ Max Unit
MEASUREMENT MODE (f = 2.5 GHz)
Input Impedance No termination resistor on RFIN 164 || 1.55 Ω || pF
±1 dB Dynamic Range TA = +25°C
Maximum Input Level
Minimum Input Level
−40°C < T
±1 dB error
±1 dB error
< +85°C
A
Slope2 22.5 mV/dB
Intercept2 −60.6 dBm
VSET Voltage—High Power In PIN = –10 dBm 1.14 V
VSET Voltage—Low Power In PIN = –40 dBm 0.46 V
Temperature Sensitivity PIN = –10 dBm
25°C ≤ T
−40°C ≤ T
≤ 85°C
A
≤ +25°C
A
OUTPUT INTERFACE VAPC (Pin 2)
Minimum Output Voltage V
Maximum Output Voltage I
R
vs. Temperature 85°C, V
≤ 150mV 0.2 0.3 0.4 V
SET
= 3 mA 2.3 2.55 V
OUT
= ∞ 2.4 2.65 V
L
POS
= 3 V, I
= 6 mA 2.54 V
OUT
General Limit 2.7 V ≤ VPOS ≤ 5.5 V, RL = ∞ VPOS – 0.1 V
Output Current Drive V
Output Noise RF Input = 2 GHz, 0 dBm, f
= 1.5 V, RFIN = –50 dBm, source/sink 5/200 mA/µA
SET
= 100 kHz, C
NOISE
= 220 pF 170 nV/√Hz
FLT
Small Signal Bandwidth RFIN = −10 dBm; from FLTR to VAPC 30 MHz
Fall Time Input level = off to 0 dBm, 90% to 10% 120 ns
Rise Time Input level = 0 dBm to off, 10% to 90% 270 ns
Slew Rate 90% – 10%, V
= 0.3 V, open loop 15 V/µs
SET
Response Time FLTR = Open 130 ns
VSET INTERFACE VSET (Pin 3)
Nominal Input Range RFIN = 0 dBm; measurement mode
RFIN = −50 dBm; measurement mode
Logarithmic Scale Factor 0.04 dB/mV
Bias Current Source RFIN = −10 dBm; V
= 1.4 V 0.26
SET
Input Resistance 36 MΩ
Slew Rate 14 V/µs
POWER INTERFACE VPOS (Pin 1)
Supply Voltage 2.7 5.5 V
Quiescent Current 5 7.6 10.7 mA
vs. Temperature
Power-On Time
Power-Off Time
1
VAPC (Pin 2) to VSET (Pin 3) with inversion stage, sinusoidal input signal.
2
Mean and standard deviation specifications are available in . Table 4
–40°C ≤ T
Time from VPOS high to V
V
SET
Time from VPOS low to V
V
SET
≤ +85°C
A
≤ 200 mV
≤ 200 mV
within 1% of final value,
APC
within 1% of final value,
APC
42 dB
41 dB
−6.2 dBm
−47.7 dBm
−0.0004
+0.0090
dB/°C
dB/°C
1.4 V
0.27 V
µA
8.2 12.9 mA
3 10 µs
100 2000 ns
Rev. 0 | Page 4 of 24
AD8311
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameters Ratings
Supply Voltage VPOS 5.5 V
VAPC, VSET 0 V, VPOS
RFIN 17 dBm
Equivalent Voltage 1.6 V rms
Internal Power Dissipation 60 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
ESD 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 this product 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.
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.
Rev. 0 | Page 5 of 24
AD8311
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
BUMP 1
INDICATOR
VPOSRFIN
VAPC
VSETFLTR
6
1
5
2
4
3
TOP VIEW
Not to Scale
COMM
05545-002
Figure 2. Pin Configuration
Table 3. Pin Function Descriptions
Pin No. Mnemonic Function
1 VPOS Positive Supply Voltage: 2.7 V to 5.5 V.
2 VAPC Output. Control voltage for gain control element.
3 VSET Setpoint Input. Nominal input range 0.25 V to 1.4 V.
4 FLTR Integrator Capacitor. Connect between FLTR and COMM.
5 COMM Device Common (Ground).
6 RFIN RF Input.
Response Time, Full-Scale Amplitude Change, Open-Loop
Figure 19. Test Setup for V
0dBm
1V PER
VERTICAL
DIVISION
RF
INPUT
PULSED RF
0.1GHz, 0dBm
100ns PER
HORIZONTAL
DIVISION
10MHz REF
OUTPUT
PULSE MODE INOUT
1
VPOS
2
VAPC
3
VSET
NC = NO CONNECT
AD8311
RFIN
COMM
FLTR
EXT TRIG
6
5
4
TEK P6205
FET PROBE
APC
PICOSECOND
PULSE LABS
GENERATO R
SPLITTER
–3dB
NC
Response Time
C
= 220pF, RF INPUT = 2GHz
FLT
–50dBm
–20dBm
–10dBm
1k10k100k1M
Figure 20. V
FREQUENCY (Hz)
Noise Spectral Density
APC
PULSE
RF
52.3Ω
–40dBm
TRIG
OUT
–3dB
TEK TDS694C
SCOPE
–38dBm
–35dBm
–30dBm
TRIG
10M
05545-032
05545-034
05545-033
Rev. 0 | Page 9 of 24
AD8311
25
–55
23
–40°C
23
SLOPE (mV/dB)
22
21
0
0.51.01.52.0
FREQUENCY (GHz)
+25°C
+85°C
2.5
05545-035
Figure 21. Slope vs. Frequency
−40°C, +25°C, and +85°C
25
23
0.1GHz
0.9GHz
23
1.9GHz
SLOPE (mV/dB)
2.5GHz
22
–57
–59
–61
INTERCEPT (dBm)
–63
–65
–58
–59
–60
–61
INTERCEPT (dBm)
–62
+25°C
–40°C
0
0.51.01.52.0
FREQUENCY (GHz)
+85°C
2.5
05545-037
Figure 23. Intercept vs. Frequency
−40°C, +25°C, and +85°C
0.1GHz
0.9GHz
1.9GHz
2.5GHz
21
2.5
3.03.54.04.5
V
(V)
POS
5.0
Figure 22. Slope vs. Supply Voltage
5.5
05545-036
–63
2.55.5
3.03.54.04.5
V
(V)
POS
5.0
Figure 24. Intercept vs. Supply Voltage
05545-038
Table 4. Typical Specifications at Selected Frequencies at 25°C (Mean and Sigma)
Slope (mV/dB) Intercept (dBm) Low Point (dBm) High Point (dBm)
±1 dB Dynamic Range
Frequency (GHz) Mean Sigma Mean Sigma Mean Sigma Mean Sigma
0.1 23.8 0.1 −58.9 0.4 −44.5 0.8 +2.6 0.3
0.9 23.6 0.1 −59.7 0.4 −47.9 0.3 +2.8 0.1
1.9 22.7 0.1 −60.8 0.5 −48.0 0.6 −5.6 0.6
2.5 22.5 0.1 −60.6 0.5 −47.7 0.6 −6.2 0.5
Rev. 0 | Page 10 of 24
AD8311
(
)
THEORY OF OPERATION
The AD8311 is a wideband logarithmic amplifier (log amp)
similar in design to the AD8313, AD8314, and AD8315. Like
the AD8315, it is strictly optimized for use in power control
applications rather than as a measurement device. Figure 25
shows the main features in block schematic form. The output
(Pin 2, VAPC) is intended to be applied directly to the
automatic power-control (APC) pin of a power amplifier
module.
BASIC THEORY
Logarithmic amplifiers provide a type of compression in which
a signal having a large range of amplitudes is converted to one
of a smaller range. The use of the logarithmic function uniquely
results in the output representing the decibel value of the input.
The fundamental mathematical form is
V
IN
log=
OUT
VV
SLP
(1)
10
V
Z
corresponds to 20 dB, V
AD8311, a nominal (low frequency) slope of 24 mV/dB was
chosen, and the intercept V
wave input (251 µV rms). However, both the slope and the
intercept are dependent on frequency.
Keeping in mind that log amps do not respond to power but
only to voltages and that the calibration of the intercept is
waveform dependent and is only quoted for a sine wave signal,
the equivalent power response can be written as
OUT
where the input power
both expressed in dBm (thus, the quantity in parentheses is
simply a number of decibels), and
mV/dB. For a log amp having a slope V
intercept at −59 dBm, the output voltage for an input power of –
30 dBm is 0.024 [−30 − (−57)] = 0.696 V.
/20 represents the volts/dB. For the
SLP
was placed at −59 dBm for a sine
Z
PPVV−= (2)
INDB
Z
P
and the equivalent intercept PZ are
IN
V
is the slope expressed in
DB
of 24 mV/dB and an
DB
where:
V
is the input voltage.
IN
is called the intercept (voltage) because when VIN = VZ the
V
Z
argument of the logarithm is unity and thus the result is zero.
is called the slope (voltage), which is the amount by which
V
SLP
the output changes for a certain change in the ratio (V
IN/VZ
When BASE-10 logarithms are used, denoted by the function
, V
log
represents the volts/decade, and since a decade
10
SLP
(PRECISE G AIN
CONTROL)
LOW NOISE
GAIN BIAS
10dB10dB
Figure 25. Block Schematic
RFIN
COM
VPOS
10dB
OFFSET
COMPENSATION
(WEAK GM STAGE)
).
(PRECISE SLOPE
INTERCEPT
POSITIONING
Further details about the structure and function of log amps can
be found in data sheets for other log amps produced by Analog
Devices. Refer to the data sheets for the AD640 and AD8307,
both of which include a detailed discussion of the basic
principles of operation and explain why the intercept depends
on waveform, an important consideration when complex
modulation is imposed on an RF carrier.
CONTROL)
LOW NOISE
BAND GAP
REFERENCE
(CURRENT-MODE S IGNAL)
DETDETDETDETDET
10dB
(CURRENT-
NULLING
MODE)
⋅ 1.35
HI-Z
LOW NOISE
RAIL-TO- RAIL BUFFER
(CURRENT-MODE
FEEDBACK)
(SMALL INTERNAL
FILTE R CAPACITOR
FOR GHz RIPPLE)
V I
VAPC
FLTR
VSET
23mV/dB
250mV TO
1.4V = 50dB
05545-003
Rev. 0 | Page 11 of 24
AD8311
The intercept need not correspond to a physically realizable
part of the signal range for the log amp. Thus, the specified
intercept is −58.9 dBm at 0.1 GHz, whereas the smallest input
for accurate measurement (a +1 dB error) at this frequency is
higher, about −44.5 dBm. At 2.5 GHz, the +1 dB error point
shifts to −47.7 dBm. This positioning of the intercept is
deliberate and ensures that the V
capabilities of certain digital-to-analog converters (DACs),
whose outputs cannot swing below 200 mV. Figure 26 shows the
100 MHz response of the AD8311; the vertical axis represents
not the output (at the VAPC pin) but the value required at the
power control pin (VSET) to null the control loop. This is
explained in the Controller-Mode Log Amps section.
1.5
1.0
SLOPE = 23.8mV/dB
VSET (V)
0.5
0
100µV
–67dBm
–58.9dBm
1mV
–47dBm
448mV @ –40dBm
IDEAL
Figure 26. Basic Calibration of the AD8311 at 0.1 GHz
CONTROLLER-MODE LOG AMPS
The AD8311 combines the two key functions required for the
measurement and control of the power 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 (see Figure 25), each having a small signal gain of 10 dB
and a bandwidth of approximately 3.5 GHz. At the output of
each of these amplifier stages is a full-wave rectifier, essentially a
square law detector cell that converts the RF signal voltages to a
fluctuating current having an average value that increases with
signal level. A further passive detector stage is added before the
first stage. These five detectors are separated by 10 dB, spanning
some 50 dB of dynamic range. Their outputs are each in the
form of a differential current, making summation a simple
matter. It is readily shown that the summed output can closely
approximate a logarithmic function. The log conformance
error, which is the overall accuracy at the extremes of this total
range viewed as the deviation from an ideal logarithmic
response, can be judged by reference to Figure 6, which shows
that errors across the central 40 dB are moderate.
voltage is within the
SET
1.211V @ –8dBm
ACTUAL
10mV
–27dBm
VIN, PIN
100mV
–7dBm
05545-040
1V (RMS)
13dBm (RE 50Ω)
In a device intended for measurement applications, this current
would then be converted to an equivalent voltage, to provide the
) function shown in Equation 1. However, the design of
log(V
IN
the AD8311 differs from standard practice in that its output
needs to be a low noise control voltage for an RF power
amplifier, not a direct measure of the input level. Further, it is
highly desirable that this voltage be proportional to the timeintegral of the error between the actual input V
voltage V
(applied to Pin 3, VSET). V
SET
SET
and a dc
IN
defines the setpoint,
a target value for the power level typically generated by a DAC.
This is achieved by converting the difference between the sum
of the detector outputs (still in current form) and an internally
generated current proportional to V
to a single-sided
SET
current-mode signal. This, in turn, is converted to a voltage (at
Pin 4, FLTR, the low-pass filter capacitor node) to provide a
close approximation to an exact integration of the error
between the power present in the termination at the input of the
AD8311 and the setpoint voltage. Finally, the voltage developed
across the ground-referenced filter capacitor C
is buffered by
FLT
a special low noise amplifier of low voltage gain (×1.35) and
presented at Pin 2 (VAPC) for use as the control voltage for the
RF power amplifier. This buffer can provide rail-to-rail swings
and can drive a substantial load current, including large
capacitors. Note that the RF power amplifier is assumed to have
a positive slope with RF power increasing monotonically with
an increasing APC control voltage.
CONTROL LOOP DYNAMICS
In order to understand how the AD8311 behaves in a complete
control loop, an expression for the current in the integration
capacitor as a function of the input P
must be developed. Refer to Figure 27.
V
SET
DIRECTIONAL
COUPLER
I
= I
SLPPIN
+ I
INT
I
DET
I
= V
SET
RFIN
6
VSET
3
DET
LOGARITHMIC
RF DETECTION
V
SUBSYSTEM
IN
SETPOINT
INTERFACE
V
SET
Figure 27. Behavioral Model of the AD8311
and the setpoint voltage
IN
P
OUT
FLTR
4
I
ERR
C
FLT
SET/RSET
VAPC
1.35
2
RF PA
P
CW
RF DRIVE:
UP TO
2.5GHz
05545-047
Rev. 0 | Page 12 of 24
AD8311
T
P
[
]
(
)
First, the summed detector currents are written as a function of
the input power.
DET
SLP
INT
IPII+×= (3)
IN
where:
I
is the partially filtered demodulated signal, whose steady-
DET
state average value is extracted through the subsequent
integration step.
I
is the slope, which has a value of 5.75 µA/dB.
SLP
P
is the input power in dBm (assuming 50 Ω input match).
IN
I
is the current intercept which, as previously noted, is
INT
dependent on the RF waveform (not the envelope). Assuming
I
a sinusoidal input,
is 350 µA.
INT
The current generated by the setpoint interface is simply
RVI= (4)
SETSETSET
where the
current and I
this point note that the inclusion of a filter resistor, R
R
resistor is 4.1 kΩ. The difference between this
SET
is applied to the loop filter capacitor C
DET
FLT
, can be
FLT
. At
helpful in improving the phase margin at low powers where the
/∂V
PA control gain (that is, ∂P
OUT
later in this section. For now assume that R
that the voltage appearing on this capacitor,
) is large, as is described
APC
is zero. It follows
FLT
V
, is the time-
FLT
integral of the difference current.
() ()
sCIIsV−= (5)
FLTDETSETFLT
Equation 6 can be restated as
V
−×−
IN
INT
(7)
APC
()
sV
=
s
VV
SLP
SET
where:
V
is I
× R
SLP
SLP
V
is the voltage intercept given by I
INT
, which has a value of 24 mV/dB.
SET
× R
INT
, which has a
SET
value of 1.44 V.
T is the effective time constant for the integration and is equal
to R
× C
SET
/1.35. The factor of 1.35 arises because of the
FLT
voltage gain of the buffer.
So the open-loop integration time constant can be written as
OpenLoop
CRT×=
FLTSET
(8)
35.1
To assess the closed-loop performance, refer to the block
diagram in Figure 28 and calculate the loop transfer function.
In general, the buffer time constant (τ
time constant (τ
) can be neglected, except in the case of
LOGAMP
) and the log amp
BUFFER
very high PA control function gains (> than 500 dB/V) and/or
very wide PA control port bandwidths. Assuming that the
frequency response of the output buffer and the log amp can be
neglected, the overall transfer function can be expressed as
P
=
OUT
SET
()
SLP
INT
[]
()
()
135.11
PAPA
sCsGI
τ+××+
PAPASLP
FLT
sCsGIII
FLT
)1(135.130
(9)
×τ+××−×+
IPIRV−×−
INTINSLPSETSET
=
The control output V
sC
FLT
is slightly greater than this, since the gain
APC
(6)
of the output buffer is ×1.35, plus a slight offset voltage. The
polarity is such that V
greater than the equivalent value of PIN. That is, the
of V
SET
rises to its maximum value for any value
APC
AD8311 seeks to drive the RF power to its maximum value
whenever it falls below the setpoint. The use of exact integration
results in a dc error that is theoretically zero, and the logarithmic
detection law would ideally result in a constant response time
following a step change of either the setpoint or the power level if
the power-amplifier control function were likewise linear-in-dB.
This latter condition is rarely true, however, and it follows that in
practice the loop response time depends on the power level. This
effect can strongly influence the design of the control loop.
I
_
DET
I
ERR
1
sC
FLT
Figure 28. Control Loop Block Diagram
V
R
+
FLT
I
SLP PIN
1 + s
τ
I
SET
+
FLT
+ I
LOGAMP
Here, G
is the PA control function gain ∂P
PA
OUT
dB/V, and the factor of −30 is due to the coupler.
The input power to the log amp, P
therefore is simply P
typically −30 dB, or P
of the PA minus the coupler value,
OUT
= P
IN
OUT
, is given in dBm and
IN
− 30.
Equation 9 assumes that the next parasitic pole in the control
loop comes from the PA. For a typical PA, a 1 MHz pole is not
unusual, making this a good assumption. Therefore, except for
in the case of a very wide bandwidth on the PA control port
(>10 MHz), the response time and stability of the control loop is mainly determined by the characteristics of the PA. This is true
for both the gain and the phase response. It is essential to
understand both the magnitude and frequency response of the
power amplifier control port.
P
OUT
PA
05545-048
INT
1 +
1.35
s
τ
BUFFER
P
IN
V
APC
–30dB
COUPLER
GPA (dB/V)
1 + s
τ
/∂V
given in
APC
Rev. 0 | Page 13 of 24
AD8311
(
)
Continuing with the stability analysis, the gain of the control
loop can be expressed as
P
∂
OUT
I
∂
SET
where:
=
k
The effect of the zero resistor, R
replacing (1/sC
stability can be derived by setting the denominator of
Equation 10 equal to 0, giving
10
From Equation 13, the closed-loop integration time constant is
given by
ClosedLoop
The gain and phase margins of the control loop can be deduced
from the Bode plots of Equation 13.
BASIC CONNECTIONS
Figure 29 shows the basic connections for operating the
AD8311, and Figure 30 shows a block diagram of a typical
application. The AD8311 is typically used in the RF power
control loop of a mobile handset.
A supply voltage of 2.7 V to 5.5 V is required for the AD8311.
The supply to the VPOS pin should be decoupled with a low
inductance 0.1 µF surface-mount ceramic capacitor, close to the
device. The AD8311 has an internal input coupling capacitor,
which negates the need for external ac-coupling. This capacitor,
along with the low frequency input impedance of the device of
approximately 2.14 kΩ, sets the minimum usable input
frequency to around 0.016 GHz. A broadband 50 Ω input
match is achieved in this example by connecting a 52.3 Ω
resistor between RFIN and ground. A Smith chart plot of input
impedance vs. frequency is shown in Figure 14. Other coupling
methods are also possible (see the Input Coupling Options
section).
k
=
IA = (A/dB) (12)
SLP
+=
()
1
+V
S
(2.7V TO 5.5V)
V
APC
V
SET
(10)
kA
+
1
sCG
××
PA
s
τ+
1
PA
) with (R
FLT
()
PA
FLT
C1
0.1µF
Figure 29. Basic Connections
)1(35.1
FLT
(dB/A) (11)
, can be easily included by
FLT
+ 1/sC
FLT
+×
135.1
FLT
IGCT
AD8311
1
VPOS
2
VAPC
34
VSET
). The criteria for loop
FLT
CsR
FLTFLT
()
SLPPA
RFIN
COMM
FLTR
(13)
IGsCs
××τ+
SLPPA
(14)
35.1××=
R1
52.3Ω
6
5
RFIN
C
FLT
05545-007
DIRECTIONAL
COUPLER
ATTENUATOR
52.3Ω
Figure 30. Typical Application
RFIN
POWER
AMP
GAIN
CONTROL
VOLTAGE
VAPC
AD8311
FLTR
R
RFIN
VSET
C
FLT
FLT
DAC
05545-008
In a power control loop, the AD8311 provides both the detector
and controller functions. A sample of the power amplifier’s (PA)
output power is coupled to the RF input of the AD8311, usually
via a directional coupler. In dual mode applications, where there
are two PAs and two directional couplers, the outputs of the
directional couplers can be passively combined (both PAs will
never be turned on simultaneously) before being applied to the
AD8311.
A setpoint voltage is applied to VSET from the controlling
source (generally this is a DAC). Any imbalance between the RF
input level and the level corresponding to the setpoint voltage is
corrected by the AD8311’s V
output that drives the gain
APC
control terminal of the PA. This restores a balance between the
actual power level sensed at the input of the AD8311 and the
value determined by the setpoint. This assumes that the gain
control sense of the variable gain element is positive, that is, an
increasing voltage from VAPC tends to increase gain.
V
can swing from 200 mV to within 100 mV of the supply
APC
rail and can source up to 6 mA. If the control input of the PA
needs to source current, a suitable load resistor can be
connected between VAPC and COMM. The output swing and
current sourcing capability of VAPC is shown in Figure 11.
RANGE ON VSET AND RFIN
The relationship between the RF input level and the setpoint
voltage follows from the nominal transfer function of the device
(see Figure 4, Figure 5, Figure 7, and Figure 8). At 0.9 GHz, for
example, a voltage of 1 V on VSET indicates a demand for
−18 dBm at RFIN. The corresponding power level at the output
of the power amplifier is greater than this amount due to the
attenuation through the directional coupler.
For setpoint voltages of less than approximately 150 mV, V
unconditionally remains at its minimum level of approximately
300 mV. This feature can be used to prevent any spurious
emissions during power-up and power-down phases.
Above 250 mV, V
has a linear control range up to 1.4 V,
SET
corresponding to a dynamic range of 50 dB. This results in a
slope of 23.8 mV/dB, or approximately 42.0 dB/V.
APC
Rev. 0 | Page 14 of 24
AD8311
TRANSIENT RESPONSE
The time domain response of power amplifier control loops,
using any kind of controller, is only partially determined by the
choice of filter. In the case of the AD8311, the filter has a true
integrator form 1/sT as shown in Equation 7, with a time
constant given by Equation 8. The large signal step response is
also strongly dependent on the form of the gain-control law.
Nevertheless, some simple rules can be applied. When the filter
capacitor C
response, but the incremental bandwidth of this loop still varies
as V
APC
This bandwidth is highest at the point where the slope of the
tangent drawn on the PA power-control curve is greatest—that
is, for power outputs near the center of the PA’s range—and is
much reduced at both the minimum and the maximum power
levels, where the slope of the gain control curve is lowest due to
its S-shaped form.
Using smaller values of C
increases in inverse proportion to its value. Eventually, however,
a secondary effect appears due to the inherent phase lag in the
power amplifier’s control path, some of which can be due to
parasitic or deliberately added capacitance at the VAPC pin. This
is very large it dominates the time domain
FLT
traverses the nonlinear gain-control function of the PA.
, the loop bandwidth generally
FLT
3.5V
results in the characteristic poles in the ac loop equation moving
off the real axis and thus becoming complex (and somewhat
resonant). This is a classic aspect of control loop design. The
lowest permissible value of C
needs to be determined
FLT
experimentally for a particular amplifier. For GSM and DCS
power amplifiers, C
typically ranges from 150 pF to 300 pF.
FLT
In many cases, some improvement in the worst-case response
time can be achieved by including a small resistor in series with
C
; this generates an additional zero in the closed-loop
FLT
transfer function, which serves to cancel a higher order pole in
the overall loop. A more complex filter network can be used to
minimize the settling time of the loop—for example, a
combination of the main capacitor, C
, shunted by a second
FLT
capacitor and resistor series.
MOBILE HANDSET POWER CONTROL EXAMPLE
Figure 31 shows a complete power amplifier control circuit for a
dual mode handset. The PF08123B (Hitachi), a dual mode
(GSM, DCS) PA, is driven by a nominal power level of +3 dBm.
The PA has a single gain control line; the band to be used is
selected by applying either 0 V or 2 V to the PA’s VCTL input.
PIN GSM
3dBm
DCS
P
IN
3dBm
8-BIT
RAMP DAC
0V–2.55V
4.7 F
1000pF
500Ω
(OPTIONAL,
SEE TEXT)
1
R2
600
Ω
1
R3
1kΩ
µ
1000pF
BAND
SELECT
0V/+2V
VCTL
PF08123B
VAPC
+V
S
2.7V
1
R2, R3 OPTIONAL, SEE TEXT
0.1
µF
1
2
3
µ
4.7 F
1000pF
P
35dBm MAX
32dBm MAX
AD8311
VPOS
VAPC
VSET
P
OUT
OUT
GSM
DCS
RFIN
COMM
FLTR
49.9
6
5
4
Figure 31. Dual Mode (GSM/DCS) PA Control Example
LDC15D190A0007A
1
Ω
4
3
6
2
R1
52.3
Ω
150pF
1.5kΩ
TO
7
8
5
TO ANTENNA
ATTN
20dB
05545-049
Rev. 0 | Page 15 of 24
AD8311
Some of the output power from the PA is coupled off using a
dual-band directional coupler (Murata part number
LDC15D190A0007A). This has a coupling factor of
approximately +19 dB for the GSM band and +14 dB for DCS
and an insertion loss of 0.38 dB and 0.45 dB, respectively.
Because the PF08107B transmits a maximum power level of
+35 dBm for GSM and +32 dBm for DCS, additional
attenuation of 20 dB is required before the coupled signal is
applied to the AD8311. This results in peak input levels to the
AD8311 of −4 dBm (GSM) and −2 dBm (DCS). While the
AD8311 gives a linear response for input levels up to +2 dBm,
for highly temperature-stable performance at maximum PA
output power the maximum input level should be limited to
approximately −2 dBm (see Figure 5 and Figure 7). This does,
however, reduce the sensitivity of the circuit at the low end.
This technique can also be used to limit the control voltage in
situations where the PA cannot deliver the power level being
demanded by VAPC. Overdrive of the control input of some
PAs causes increased distortion. It should be noted, however,
that if the control loop opens (that is, V
goes to its maximum
APC
value in an effort to balance the loop), the quiescent current of
the AD8311 increases somewhat, particularly at supply voltages
greater than 3 V.
Figure 32 shows the relationship between V
power (P
) at 0.9 GHz. The overall gain control function is
OUT
and output
SET
linear in dB for a dynamic range of over 40 dB. Note that for
V
voltages below 300 mV, the output power drops off steeply
SET
drops toward its minimum level of 300 mV.
as V
APC
40
–40°C
3
The operational setpoint voltage, in the range 250 mV to 1.4 V,
is applied to the VSET pin of the AD8311. This typically is
supplied by a DAC. The AD8311’s VAPC output drives the level
control pin of the power amplifier directly. V
reaches a
APC
maximum value of approximately 2.5 V on a 2.7 V supply while
delivering the 3 mA required by the level control input of the
PA. This is more than sufficient to exercise the gain control
range of the PA.
During initialization and completion of the transmit sequence,
V
should be held at its minimum level of 300 mV by keeping
APC
below 150 mV.
V
SET
In this example, V
is supplied by an 8-bit DAC that has an
SET
output range from 0 V to 2.55 V or 10 mV per bit. This sets the
control resolution of V
to 0.4 dB/bit (0.04 dB/mV times
SET
10 mV). If finer resolution is required, the DAC’s output voltage
can be scaled using two resistors as shown. This converts the
DAC’s maximum voltage of 2.55 V down to 1.6 V and increases
the control resolution to 0.25 dB/bit.
A filter capacitor (C
choice of C
depends to a large degree on the gain control
FLT
) must be used to stabilize the loop. The
FLT
dynamics of the power amplifier, something that is frequently
poorly characterized, so some trial and error might be
necessary.
In this example, a 150 pF capacitor is used and a 1.5 kΩ series
resistor is included. This adds a zero to the control loop and
increases the phase margin, which helps to make the step
response of the circuit more stable when the PA output power is
low and the slope of the PA’s power control function is the
steepest.
A smaller filter capacitor can be used by inserting a series
resistor between VAPC and the control input of the PA. A series
resistor works with the input impedance of the PA to create a
resistor divider, which reduces the loop gain. The size of the
resistor divider ratio depends on the available output swing of
V
and the required control voltage on the PA.
APC
30
20
10
0
OUTPUT POWER (dBm)
–10
–20
–40°C
+25°C
+85°C
+25°C
0
0.20.40.60.81.01.21.4
Figure 32. P
SETPOINT VOLTAGE (V)
vs. V
OUT
at 0.9 GHz for Dual Mode Handset
SET
Power Amplifier Application;
−40°C, +25°C, and +85°C
+85°C
1.6
2
1
0
ERROR (dB)
–1
–2
–3
POWER-ON AND POWER-OFF
The AD8311 can be completely disabled by pulling the supply
voltage to ground. The voltage on VSET should be kept below
150 mV during power-on and power-off to prevent any
unwanted transients on VAPC.
INPUT COUPLING OPTIONS
The internal 5 pF coupling capacitor of the AD8311 and the low
frequency input impedance of 2.14 kΩ give a high-pass input
corner frequency of approximately 16 MHz. This sets the
minimum operating frequency. Figure 33, Figure 34, and
Figure 35 shows three options for input coupling. A broadband
resistive match can be implemented by connecting a shunt
resistor to ground at RFIN (Figure 33). This 52.3 Ω resistor
(other values can also be used to select different overall input
impedances) combines with the input impedance of the
AD8311 to give a broadband input impedance of 50 Ω. While
the input resistance and capacitance (C
AD8311 vary from device to device by approximately ±20%, as
well as in the same device over a range of frequencies
(Figure 14), the dominance of the external shunt resistor means
that the variation in the overall input impedance is close to the
and RIN) of the
IN
05545-041
Rev. 0 | Page 16 of 24
AD8311
tolerance of the external resistor. This method of matching is
most useful in wideband applications or in multiband systems
where there is more than one operating frequency.
A reactive match can also be implemented as shown in
Figure 34. This is not recommended at low frequencies because
device tolerances dramatically vary the quality of the match due
to the large input resistance. For low frequencies, Figure 33 or
Figure 35 is recommended.
In Figure 34, the matching components are drawn as generic
reactances. Depending on the frequency, the input impedance,
and the availability of standard value components either a
capacitor or an inductor is used. As in the previous case, the
input impedance at a particular frequency is plotted on a Smith
Chart and matching components are chosen (shunt or series L,
shunt or series C) to move the impedance to the center of the
chart.
TEMPERATURE DRIFT
Figure 36 shows the log slope and error over temperature for a
0.9 GHz input signal. Error due to drift over temperature
consistently remains within ±1 dB and only begins to exceed
this limit when the ambient temperature goes above +65 °C and
below −20 °C. For all frequencies using a reduced temperature
range, higher measurement accuracy is achievable.
Figure 34. Narrow Band Reactive Input Coupling Option
ANTENNA
AD8311
C
C
STRIPLINE
PA
R
ATTN
RFIN
R
C
IN
IN
05545-011
Figure 35. Series Attention Input Coupling Option
Figure 35 shows a third method for coupling the input signal
into the AD8311. A series resistor connected to the RF source
combines with the input impedance of the AD8311 to
resistively divide the input signal being applied to the input.
This has the advantage of very little power being tapped off in
RF power transmission applications.
1.6
–2
–3
05545-042
–50
–60
0.2
0.40.60.81.01.21.4
VSET (V)
Figure 36. Typical Drift at 900 GHz for Various Temperatures
DEVICE CALIBRATION AND ERROR CALCULATION
The measured transfer function of the AD8311 at 0.9 GHz is
shown in Figure 37. The figure shows plots of both input power
and calculated error vs. setpoint voltage.
The vertical axis represents the input power required at the RFIN
pin to null the control loop when a VSET voltage is applied. As
the setpoint voltage varies from about 0.2 V to 1.5 V, the
corresponding input power varies from −60 dBm to +10 dBm.
PIN
= (VSET1/ SLOPE) + INTERCEPT
IDEAL
ERROR (dB) = (PIN
SLOPE = (VSET
INTERCEPT = PIN
10
0
–10
–20
–30
RFIN (dBm)
–40
INTERCEPT
–50
–60
0
+85°C
PIN
1
0.20.40.60.81.01.21.4
Figure 37. Transfer Function of AD8311 at 0.9 GHz
Because slope and intercept vary from device to device, boardlevel calibration must be performed to achieve high accuracy.
– PIN)
IDEAL
– VSET1)/(PIN1– PIN2)
2
– (VSET1 / SLOPE)
1
–40°C
VSET
1
VSET (V)
–40°C
+25°C
PIN
4
3
2
VSET
+25°C
2
+85°C
1.6
2
1
0
–1
–2
–3
ERROR (dB)
05545-043
Rev. 0 | Page 17 of 24
AD8311
In a control loop, calibration is performed by applying two
levels to the AD8311’s setpoint voltage and measuring the
corresponding power. The calibration points are generally
chosen to be within the linear-in-dB operating range of the
device (see Figure 37). Calculation of slope and intercept is
done using the equations
)/()(
PPVVSLOPE−−=
(15)
1SET2SET
−=
1IN
1SET
1IN2IN
(16)
)/(SLOPEVPINTERCEPT
Once slope and intercept have been calculated, an equation can
be written which allows calculation of an (unknown) power
based on the setpoint voltage.
INTERCEPTSLOPEVP
IN
SET
+=)/(
(17)
Using Equation 17 as a reference for the ideal input power, the
log conformance error of the measured data can be calculated:
PPdBERROR−= (18)
)()(
DIN,MEASUREIN,IDEAL
Figure 37 includes a plot of the error at 25°C, the temperature at
which the AD8311 is calibrated. Note that the error is not zero.
This is because the AD8311 does not perfectly follow the ideal
V
vs. PIN equation, even within its operating region. The error
SET
at the calibration points (0.45 V and 1.15 V in this case) is,
however, equal to zero by definition.
Figure 37 also includes error plots for the output voltage at
−40°C and +85 °C. These error plots are calculated using the
slope and intercept at +25°C. This is consistent with calibration
in a mass-production environment where calibration at
temperature is not practical.
SELECTING CALIBRATION POINTS TO IMPROVE
ACCURACY OVER A REDUCED RANGE
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.
Figure 38 shows the same measured data as Figure 37. Notice
that accuracy is very high from −15 dBm to 0 dBm. Below
−15 dBm the error increases to about −2 dB. This is because the
calibration points have been changed to approximately 0.975 V
and 1.3 V.
2
+85°C
1.6
4
3
2
1
0
–1
–2
–3
ERROR (dB)
05545-044
10
0
–10
–20
–30
RFIN (dBm)
–40
–50
–60
0
–40°C
0.20.40.60.81.01.21.4
VSET (V)
Figure 38. Output Voltage and Error vs. P
+85°C
+25°C
–40°C
PIN
PIN
2
1
VSET
1
+25°C
with 2-Point Calibration at
IN
VSET
Approximately 0.975 V and 1.3 V
Calibration points should be chosen to suit the application at
hand. In general, though, the calibration points should never be
chosen in the nonlinear portion of the log amp’s transfer
function (above 1.4 V or below 0.35 V in this case).
Figure 39 shows how calibration points can be adjusted to
increase dynamic range, but at the expense of linearity. In this
case the calibration points for slope and intercept are set at
0.37 V and 1.37 V. These points are at the end of the device’s
linear range. Once again at 25°C we see an error of 0 dB at the
calibration points. Note also that the range over which the
AD8311 maintains an error of less than ±0.5 dB is extended to
more than 45 dB at 25°C and more than 40 dB over
temperature. The disadvantage of this approach is that linearity
suffers, especially in the middle of the range.
VSET
+85°C
4
3
2
2
1
0
ERROR (dB)
–1
–2
–3
1.6
05545-045
10
0
–10
–20
–30
RFIN (dBm)
–40
–50
–60
0
PIN
1
VSET
1
0.20.40.60.81.01.21.4
+25°C
VSET (V)
+85°C
+25°C
–40°C
–40°C
PIN
2
Figure 39. Dynamic Range Extension by Choosing Calibration Points that are
Close to the End of the AD8311’s Linear Range
Rev. 0 | Page 18 of 24
AD8311
Another way of presenting the error function of a log amp
detector is shown in Figure 40. In this case, the dB error at hot
and cold temperatures is calculated with respect to the transfer
function at ambient. This is a key difference in comparison to
the previous plots. Up to now, all errors have been calculated
with respect to the ideal transfer function at ambient.
When we use this alternative technique, the error at ambient
becomes by definition equal to 0 (see Figure 40).
This would be valid if the device transfer function perfectly
followed the ideal P
IN
= V
/ SLOPE + INTERCEPT equation.
SET
However since a log amp in practice never perfectly follows this
equation (especially outside of its linear operating range), this
plot tends to artificially improve linearity and extend the
dynamic range. This plot is a useful tool for estimating
temperature drift at a particular power level with respect to the
(nonideal) response at ambient. However, achieving this level of
accuracy in an end application requires calibration at multiple
points in the device’s operating range.
1.6
4
3
2
1
0
–1
–2
–3
ERROR (dB)
05545-046
10
0
–10
–20
–30
RFIN (dBm)
–40
–50
–60
0
+85°C
+25°C
–40°C
+85°C
–40°C
+25°C
DOES NOT TAKE INTO ACCOUNT TRANSFER
FUNCTIONS’ NONLINEARITIES AT +25°C
0.20.40.60.81.01.21.4
VSET (V)
Figure 40. Error vs. Temperature with respect to Output Voltage at 25 °C
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 package 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
additional information. WLCSP devices are bumped die, and
exposed die can be sensitive to light condition, which can
influence specified limits.
AN-617 application note for
Rev. 0 | Page 19 of 24
AD8311
EVALUATION BOARD
Figure 41 shows the schematic of the AD8311 WLCSP
evaluation board. The layout and silkscreen of the component
and circuit sides are shown in Figure 42 to Figure 45. The board
is powered by a single supply in the range 2.7 V to 5.5 V. The
power supply is decoupled by a 0.1 µF capacitor. A 100 pF
capacitor provides additional supply decoupling, but is not
necessary for basic operation.
Table 5 details the various configuration options of the
evaluation board.
For operation in controller mode, both jumpers J1 and J2
should be removed. The setpoint voltage is applied to VSET,
RFIN is connected to the RF source (PA output or directional
coupler), and VAPC is connected to the gain control pin of the
PA. When used in controller mode, a capacitor must be
installed in C4 for loop stability (R2 must also be installed, 0 Ω
by default). For GSM/DCS handset power amplifiers, this
capacitor should typically range from 150 pF to 300 pF.
A quasi-measurement mode (where the AD8311 delivers an
output voltage that is proportional to the log of the input signal)
can be implemented, to establish the relationship between VSET
and RFIN, by installing the two jumpers J1 and J2. This mimics
an AGC loop. To establish the transfer function of the log amp,
the RF input should be swept while the voltage on VSET is
measured, that is, the SMA connector labeled VSET now acts as
an output. This is the simplest method to validate operation of
the evaluation board. When operated in this mode, a large
capacitor (0.01 µF or greater) must be installed in C4 (filter
capacitor) to ensure loop stability. The op amp must be powered
with a nominal voltage of 2.7 V to 5.5 V with the VS supply.
Alternately, J3 can be installed to power the op amp with the
AD8311’s VPOS power supply.
6
5
4
R9
(OPEN)
52.3Ω
R1
C4
(OPEN)
R2
0Ω
RFIN
05545-012
VAPC
(OPEN)
VSET
C1
100pF
R3
0Ω
J2
R10
TO EDGE
CONNECTOR
C2
R6
10kΩ
17.8kΩ
AD8311
1
VPOS
2
VAPC
3
VSET
VPOS
C6
0.1µF
R7
16.2kΩ
R8
R5
10kΩ
C7
(OPEN)
J3
VS
C5
0.1µF
COMM
RFIN
FTLR
J1
TO EDGE
CONNECTOR
0.1µF
VPOS
R4
C3
(OPEN)
(OPEN)
Figure 41. Evaluation Board Schematic
Rev. 0 | Page 20 of 24
AD8311
05545-015
Figure 42. Layout of Component Side (WLCSP)
05545-013
Figure 44. Silkscreen of Component Side (WLCSP)
05545-013
Figure 43. Layout of Circuit Side (WLCSP)
Figure 45. Silkscreen of Circuit Side (WLCSP)
Table 5. Evaluation Board Configuration Options
Component Function Default Condition
VPOS, GND Supply and Ground Vector Pins. Not Applicable
R1
Input Interface. The 52.3 Ω resistor in Position R1 combines with the AD8311’s internal
R1 = 52.3 Ω (Size 0402)
input impedance to give a broadband input impedance of around 50 Ω. Note that the
AD8311’s RF input is internally ac-coupled.
R3, R4, C3
C1, C2
C4, R2
Output Interface. R4 and C3 can be used to check the response of V
resistive loading. R3/R4 can be used to reduce the slope of V
APC
to capacitive and
APC
.
Power Supply Decoupling. The nominal supply decoupling consists of a 0.1 µF capacitor at
C1. C2 can be used for additional supply decoupling.
Filter Capacitor. The response time of V
can be modified by placing a capacitor between
APC
FLTR (Pin 4) and ground. The control loop phase margin can be increased by adding a series
R3 = 0 Ω (Size 0402)
R4 = C3 = open (Size 0402)
C1 = 0.1 µF (Size 0402)
C2 = 100 pF (Size 0402)
C4 = open (Size 0402)
R2 = 0 Ω (Size 0402)
resistor.
J1, J2, J3
Measurement Mode. A quasi-measurement mode can be implemented by installing J1 and
to V
J2 (connecting an inverted V
APC
) to yield the nominal relationship between RFIN and
SET
J1, J2 = installed
J3 = installed
VSET. In this mode, a large capacitor (0.01 µF or greater) must be installed in C4. J3 can be
installed to power the op-amp with the VPOS power supply. Alternately, the op-amp can be
powered with the VS supply pin.
R9, R10
Alternate Interface. R5 and R6 allow for VOUT and VSET to be accessible from the edge
connector, which is only used for characterization.