FEATURES
Complete RF Detector/Controller Function
>50 dB Range at 0.9 GHz (–49 dBm to +2 dBm re 50 )
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, 38 mW at 5 V
Power Down to 10.8 W
APPLICATIONS
Single, Dual, and Triple Band Mobile Handset
(GSM, DCS, EDGE)
Transmitter Power Control
PRODUCT DESCRIPTION
The AD8315 is a complete low cost subsystem for the precise
control of RF power amplifiers operating in the frequency range
0.1 GHz–2.5 GHz and over a typical dynamic range of 50 dB. It is
intended for use in cellular handsets and other battery-operated
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 –30∞C to +85∞C.
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
may be dc grounded.
The AD8315 provides a voltage output, VAPC, that has the
voltage range and current drive to directly connect to most handset power amplifiers’ gain control pin. VAPC can swing from 250
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–1.4 V. The associated circuit determines the slope and intercept of the linear-in-dB measurement
system; these are nominally 23 mV/dB and –60 dBm for a 50 W
termination (–73 dBV) at 0.9 GHz. Further simplifying the
application of the AD8315, the input resistance of the setpoint
interface is over 100 MW, and the bias current is typically 0.5 mA.
The AD8315 is available in MSOP and lead frame chip scale
(LFCSP) packages and consumes 8.5 mA from a 2.7 V to 5.5 V
supply. When powered down, the sleep current is 4 mA.
FUNCTIONAL BLOCK DIAGRAM
RFIN
COMM
VPOS
ENBL
LOW NOISE
GAIN BIAS
OFFSET
COMP’N
LOW NOISE
BAND GAP
REFERENCE
10dB10dB10dB
REV. B
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. 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 companies.
*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.
PIN CONFIGURATION
1
RFIN
2
ENBL
3
VSET
(Not to Scale)
4
NC = NO CONNECT
AD8315
TOP VIEW
8
7
6
5
VPOS
VAPC
NC
COMMFLTR
PIN FUNCTION DESCRIPTIONS
Pin
No.MnemonicFunction
1RFINRF Input
2ENBLConnect to VPOS for Normal Operation
Connect pin to ground for Disable Mode
3VSETSetpoint Input. Nominal input range
0.25 V to 1.4 V.
4FLTRIntegrator Capacitor. Connect between
FLTR and COMM.
5COMMDevice Common (Ground)
6NCNo Connection
7VAPCOutput. Control voltage for gain control
element.
8VPOSPositive Supply Voltage: 2.7 V to 5.5 V
ORDERING GUIDE
ModelTemperature RangePackage DescriptionsPackage OptionBranding Information
AD8315ARM–30∞C to +85∞CTube, 8-Lead MSOPRM-8J7A
AD8315ARM-REEL13" Tape and Reel
AD8315ARM-REEL77" Tape and Reel
AD8315-EVALMSOP Evaluation Board
AD8315ACP-REEL–30∞C to +85∞C13" Tape and Reel,CP-8J7A
8-Lead LFCSP
AD8315ACP-REEL77" Tape and Reel
AD8315ACP-EVALLFCSP Evaluation Board
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
WARNING!
the AD8315 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.
REV. B
–3–
ESD SENSITIVE DEVICE
Page 4
AD8315
–Typical Performance Characteristics
1
0
–10
–20
–30
–40
0.9GHz
–50
RF INPUT AMPLITUDE – dBV
–60
–70
–80
0.2
10
0
(+3dBm)
–10
–20
–30
RF INPUT
–40
AMPLITUDE – dBV
–50
(–47dBm)
–60
–70
0.1
0.40.60.81.01.21.4
TPC 1. Input Amplitude vs. V
+25C
0.30.50.70.91.11.31.5
1.9GHz
0.1GHz
2.5GHz
V
– V
SET
SET
–30C
+25C
+85C
–30C
ERROR AT +85C AND –30C
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
V
– V
SET
+85C
TPC 2. Input Amplitude and Log Conformance vs. V
0.1 GHz
23
13
3
–7
–17
–27
–37
–47
RF INPUT AMPLITUDE – dBm
–57
–67
4
3
2
1
0
ERROR – dB
–1
–2
(–47dBm)
TPC 5. Input Amplitude and Log Conformance vs. V
SET
–3
–4
at
1.9 GHz
ERROR – dB
(+3dBm)
–10
–20
–30
RF INPUT
–40
AMPLITUDE – dBV
–50
–60
–70
4
3
2
1
0
–1
–2
–3
–4
0.2
0.1GHz
0.40.60.81.01.21.41.6
V
– V
SET
TPC 4. Log Conformance vs. V
10
0
+85C
+25C
+85C
0.1
–30C
0.30.50.70.91.11.31.5
–30C
+25C
ERROR AT +85C AND –30C
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
V
– V
SET
1.9GHz
2.5GHz
SET
0.9GHz
4
3
2
1
0
–1
–2
–3
–4
SET
ERROR – dB
at
(+3dBm)
RF INPUT
(–47dBm)
10
0
–10
–20
–30
–40
AMPLITUDE – dBV
–50
–60
–70
0.30.50.70.91.11.31.5
0.1
–30C
+25C
–30C
+85C
+25C
ERROR AT +85C AND –30C
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
V
– V
SET
+85C
TPC 3. Input Amplitude and Log Conformance vs. V
0.9 GHz
SET
4
3
2
1
0
ERROR – dB
–1
–2
–3
–4
at
10
0
(+3dBm)
–10
–30C
+85C
ERROR AT +85C AND –30C
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
V
– V
SET
RF INPUT
(–47dBm)
–20
–30
–40
AMPLITUDE – dBV
–50
+25C
–60
–70
0.1
0.30.50.70.91.11.31.5
+25C
–30C+85C
TPC 6. Input Amplitude and Log Conformance vs. V
2.5 GHz
–4–
4
3
2
1
0
ERROR – dB
–1
–2
–3
–4
at
SET
REV. B
Page 5
AD8315
(
)(
)
(
)(
)
(
)(
)
4
3
2
1
0
ERROR – dB
–1
–2
–3
–4
–800–70
+85C
ERROR AT +85C AND –30C
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
–60
RF INPUT AMPLITUDE – dBV
–47dBm
–50–40–30–20–10
–30C
+3dBm
TPC 7. Distribution of Error at Temperature after Ambient
Normalization vs. Input Amplitude, 3 Sigma to Either Side
of Mean, 0.1 GHz
4
3
2
30C
4
3
2
1
0
ERROR – dB
–1
–2
ERROR AT +85C AND –30C
–3
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
–4
–800–70
–30C
+85C
–50–40–30–20–10
–60
RF INPUT AMPLITUDE – dBV
–47dBm
+3dBm
TPC 10. Distribution of Error at Temperature after Ambient
Normalization vs. Input Amplitude, 3 Sigma to Either Side of
Mean, 1.9 GHz
4
3
2
–30C
1
0
ERROR – dB
–1
–2
ERROR AT +85C AND –30C
–3
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
–4
–800–70
85C
–60
–50–40–30–20–10
RF INPUT AMPLITUDE – dBV
(+3dBm)(–47dBm)
TPC 8. Distribution of Error at Temperature after Ambient
Normalization vs. Input Amplitude, 3 Sigma to Either Side
of Mean, 0.9 GHz
jX
j1500
j220
j130
j110
0
–200
–400
–600
–800
–1000
–1200
X
–1400
–1600
–1800
–2000
3000
2700
2400
2100
1800
X (LFCSP)
1500
1200
RESISTANCE –
900
600
300
0
02.50.511.52
X (MSOP)
FREQUENCY
(GHz)
0.1
0.9
1.9
2.5
FREQUENCY – GHz
2900 –
R (LFCSP)
R (MSOP)
R –
700 –
130 –
170 –
Chip Scale (LFCSP)
MSOP
jX
j1900
j240
j80
j70
R –
2700 –
730 –
460 –
440 –
R
TPC 9. Input Impedance
1
0
ERROR – dB
–1
–2
ERROR AT +85C AND –30C
–3
BASED ON DEVIATION FROM
SLOPE AND INTERCEPT AT +25C
–4
–800–70
–50–40–30–20–10
–60
RF INPUT AMPLITUDE – dBV
–47dBm
+85C
+3dBm
TPC 11. Distribution of Error at Temperature after Ambient
Normalization vs. Input Amplitude, 3 Sigma to Either Side of
Mean, 2.5 GHz
10
8
REACTANCE –
6
4
DECREASING
SUPPLY CURRENT – mA
2
0
1.3
V
ENBL
1.41.51.61.7
V
ENBL
TPC 12. Supply Current vs. V
– V
INCREASING
V
ENBL
ENBL
REV. B
–5–
Page 6
AD8315
g
25
24
23
22
SLOPE – mV/dB
21
20
0
–30 C
0.51.01.52.02.5
FREQUENCY – GHz
+85 C
+25 C
TPC 13. Slope vs. Frequency; –30∞C, +25∞C, and +85∞C
24
23
SLOPE – mV/dB
22
0.1GHz
0.9GHz
1.9GHz
–66
–68
+85 C
–70
–72
+25 C
–74
INTERCEPT – dBV
–76
–78
–80
0
–30C
0.51.01.52.02.5
FREQUENCY – GHz
TPC 16. Intercept vs. Frequency; –30∞C, +25∞C, and +85∞C
TPC 27. Power-On and -Off Response with V
ENBL Grounded
R AND S
SMT03
SIGNAL
GENERATOR
52.3
220pF
10MHz REF
OUTPUT
RF OUT
1
2
3
4
NC = NO CONNECT
AD8315
RFIN
ENBL
VSET
VPOS
VA PC
COMMFLTR
NC
8
7
6
5
EXT TRIG
TEK P6205
FET PROBE
TEK P6205
FET PROBE
STANFORD DS345
PULSE
GENERATOR
AD811
732
PULSE OUT
49.9
TEK TDS694C
and
SET
TRIG
SCOPE
TRIG
OUT
TPC 26. Test Setup for Power-On and -Off Response with
VSET Grounded
GENERAL DESCRIPTION AND THEORY
The AD8315 is a wideband logarithmic amplifier (log amp)
similar in design to the AD8313 and AD8314. However, it is
strictly optimized for use in power control applications rather
than as a measurement device. Figure 1 shows the main features
in block schematic form. The output (Pin 7, 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
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
VV
=log
OUTSLP
Here V
because when V
is the input voltage, VZ is called the intercept (voltage)
IN
IN
and thus the result is zero, and V
IN
10
V
Z
(1)
= VZ the argument of the logarithm is unity
is called the slope (voltage),
SLP
which is the amount by which the output changes for a certain
change in the ratio (V
denoted by the function log
and since a decade corresponds to 20 dB, V
). When BASE-10 logarithms are used,
IN/VZ
, V
represents the “volts/decade,”
10
SLP
/20 represents the
SLP
“volts/dB.” For the AD8315, a nominal (low frequency) slope
–8–
TPC 28. Test Setup for Power-On and -Off Response with
VSET and ENBL Grounded
of 24 mV/dB was chosen, and the intercept VZ was placed at the
equivalent of –70 dBV for a sine wave input (316 mV rms). This
corresponds to a power level of –57 dBm when the net resistive
part of the input impedance of the log amp is 50 W. However,
both the slope and the intercept are dependent on frequency (see
TPC 13 and TPC 16).
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:
VVPP
=(–)
OUTDBINZ
where the input power P
and the equivalent intercept PZ are
IN
(2)
both expressed in dBm (thus, the quantity in parentheses is
simply a number of decibels), and V
so many mV/dB. For a log amp having a slope V
is the slope expressed as
DB
of 24 mV/dB
DB
and an intercept at –57 dBm, the output voltage for an input
power of –30 dBm is 0.024 [–30 – (–57)] = 0.648 V.
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 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.
REV. B
Page 9
AD8315
RFIN
COMM
(PADDLE)
VPOS
ENBL
(PRECISE GAIN
CONTROL)
LOW NOISE
GAIN BIAS
OFFSET
COMP’N
(WEAK GM STAGE)
(PRECISE SLOPE
CONTROL)
LOW NOISE
BAND GAP
REFERENCE
10dB10dB10dB
INTERCEPT
POSITIONING
Figure 1. Block Schematic
The intercept need not correspond to a physically realizable part
of the signal range for the log amp. Thus, the specified intercept
is –70 dBV, at 0.1 GHz, whereas the smallest input for accurate
measurement (a +1 dB error, see Table I) at this frequency is
higher, being about –58 dBV. At 2.5 GHz, the +1 dB error point
shifts to –64 dBV. This positioning of the intercept is deliberate
and ensures that the V
voltage is within the capabilities of cer-
SET
tain DACs, whose outputs cannot swing below 200 mV. Figure 2
shows the 100 MHz response of the AD8315; the vertical axis
represents not the output (at pin VAPC) but the value required
at the power control pin VSET to null the control loop. This
will be explained next.
1.5
1.0
SET
V
0.5
0
100V
–80dBV
–67dBm
–70dBV
0.288V @ –58dBV
IDEAL
1mV
–60dBV
–47dBm
V
P
O
L
S
10mV
–40dBV
–27dBm
, dBVIN, P
IN
1.416V @ –11dBV
B
/d
V
m
= 24
E
ACTUAL
IN
100mV
–20dBV
–7dBm
1V (RMS)
0dBV
+13dBm (RE 50)
Figure 2. Basic Calibration of the AD8315 at 0.1 GHz
Controller-Mode Log Amps
The AD8315 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 1), 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-
(ELIMINATES
GLITCH)
OUTPUT
ENABLE
DELAY
(CURRENT-MODE SIGNAL)
DETDETDETDETDET
10dB
(CURRENT-
NULLING
MODE)
HI-Z
LOW NOISE (25nV/ Hz)
RAIL-TO-RAIL BUFFER
(CURRENT-MODE
FEEDBACK)
(SMALL INTERNAL
FILTER CAPACITOR
FOR GHz RIPPLE)
1.35
V- I
VA PC
FLTR
VSET
23mV/dB
250mV to
1.4V = 50dB
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 overall accuracy at the
extremes of this total range, viewed as the deviation from an
ideal logarithmic response, that is, the log conformance error, can
be judged by reference to TPC 4, which shows that errors across
the central 40 dB are moderate. Other performance curves show
how conformance to an ideal logarithmic function varies with
supply voltage, temperature, and frequency.
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 the
log(V
IN
AD8315 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 time-integral of the error
between the actual input V
and a dc voltage V
IN
(applied to
SET
Pin 3, VSET) which defines the setpoint, that is, a target value
for the power level, typically generated by a D/A converter.
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 current-mode
SET
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 AD8315 and the setpoint
voltage. Finally, the voltage developed across the ground-referenced
filter capacitor C
is buffered by a special low noise amplifier
FLT
of low voltage gain (¥1.35) and presented at Pin 7 (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: The RF power is assumed
to increase monotonically with an increasingly positive delivered
by the amplifier under control of the AD8315 voltage on its
APC control pin.
REV. B
–9–
Page 10
AD8315
Control Loop Dynamics
In order to understand how the AD8315 behaves in a complete
control loop, an expression for the current in the integration
capacitor as a function of the input V
must be developed. Refer to Figure 3.
V
SET
V
SET
3
RFIN
1
V
SET
V
IN
SETPOINT
INTERFACE
LOGARITHMIC
RF DETECTION
SUBSYSTEM
I
= I
DET
SLP
I
SET
I
DET
LOG10 (VIN/VZ)
and the setpoint voltage
IN
= V
/4.15k
SET
FLTR
I
ERR
4
1.35
C
FLT
VAPC
7
Figure 3. Behavioral Model of the AD8315
First, the summed detector currents are written as a function of
the input:
IIVV
=log (/)
DETSLPINZ
where I
is the partially filtered demodulated signal, whose
DET
10
(3)
exact average value will be extracted through the subsequent
integration step; I
of 115 mA per decade (that is, 5.75 mA/dB); V
volts-rms; and V
is the current-mode slope and has a value
SLP
is the effective intercept voltage, which, as
Z
is the input in
IN
previously noted, is dependent on waveform but is 316 mV rms
(–70 dBV) for a sine wave input. Now the current generated by
the setpoint interface is simply:
IVk
=W/.415
SETSET
The difference between this current and I
loop filter capacitor C
this capacitor, V
VsI I sC
FLTSETDETFLT
SETSLPINZ
=
FLT
() (–)/=
/.–log(/)415
The control output V
. It follows that the voltage appearing on
FLT
, is the time integral of the difference current:
WVkI VV
sC
is slightly greater than this, since the
APC
10
FLT
DET
is applied to the
(4)
(5)
(6)
gain of the output buffer is ¥1.35. Also, an offset voltage is
deliberately introduced in this stage; this is inconsequential
since the integration function implicitly allows for an arbitrary
constant to be added to the form of Equation 6. The polarity is
such that V
greater than the equivalent value of VIN. In practice, the
V
SET
V
output will rail to the positive supply under this condition
APC
will rise to its maximum value for any value of
APC
unless the control loop through the power amplifier is present.
In other words, the AD8315 seeks to drive the RF power to its
maximum value whenever it falls below the setpoint. The use
of exact integration results in a final 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 will depend on the power level, and this effect can
strongly influence the design of the control loop.
Equation 6 can be restated as:
Vs
()
=
APC
VVVV
SETSLPIN Z
-
log (/)
10
sT
(7)
–10–
where V
is the volts-per-decade slope from Equation 1, having
SLP
a value of 480 mV/decade, and T is an effective time constant for
the integration, being equal to 4.15 kW ¥ C
/1.35; the resistor
FLT
value comes from the setpoint interface scaling Equation 4 and
the factor 1.35 arises because of the voltage gain of the buffer.
So the integration time constant can be written as:
TCin s when C isin nF
= 307.,mexpressed
FLT
(8)
To simplify our understanding of the control loop dynamics,
begin by assuming that the power amplifier gain function actually is linear-in-dB. Also use voltages to express the signals at
the power amplifier input and output, for the moment. Let the
RF output voltage be V
and its input be VCW. Further, to
PA
characterize the gain control function, this form is used:
(/)
VV
VGV
=10
PAO CW
where G
V
GBC
is the gain of the power amplifier when V
O
is the gain-scaling. While few amplifiers will conform so
APC GBC
APC
(9)
= 0 and
conveniently to this law, it provides a clearer starting point for
understanding the more complex situation that arises when the
gain control law is less ideal.
This idealized control loop is shown in Figure 4. With some
manipulation, it is found that the characteristic equation of this
system is:
Vs
()
APC
()/–log/
SET GBCSLPGBCO CWZ
=
sT
+101
()
O
(10)
VV V VkGV V
where k is the coupling factor from the output of the power
amplifier to the input of the AD8315 (e.g., ¥ 0.1 for a “20 dB
coupler”), and T
is a modified time constant (V
O
GBC/VSLP
)T.
This is quite easy to interpret. First, it shows that a system of
this sort will exhibit a simple single-pole response, for any power
level, with the customary exponential time domain form for
either increasing or decreasing step polarities in the demand
level V
final value of the control voltage V
or the carrier input VCW. Second, it reveals that the
SET
will be determined by
APC
several fixed factors:
VtVV VkGVV
=•
=
()
APCSET GBCSLPO CWZ
()()
/–log/
10
(11)
Example
Assume that the gain magnitude of the power amplifier runs
from a minimum value of ¥0.316 (–10 dB) at V
(40 dB) at V
V
= 1 V. Using a coupling factor of k = 0.0316 (that is, a
GBC
= 2.5 V. Applying Equation 9, GO = 0.316 and
APC
= 0 to ¥100
APC
30 dB directional coupler) and recalling that the nominal value of
is 480 mV and VZ = 316 V for the AD8315, first calculate
V
SLP
the range of values needed for V
to control an output range
SET
of 33 dBm to –17 dBm. This can be found by noting that, in
the steady state, the numerator of Equation 7 must be zero,
that is:
VVkVV
=log (/)
SETSLPPAZ
when V
is expanded to kVPA, the fractional voltage sample of
IN
10
the power amplifier output. Now, for +33 dBm, V
= 10 V rms,
PA
(12)
this evaluates to:
VmVVV
().log (/).max ==0483163161 44
SET
10
For a delivered power of –17 dBm, V
VmVVV
().log (/).min ==0481316024
SET
10
m
= 31.6 mV rms:
PA
m
(13)
(14)
REV. B
Page 11
AD8315
Check: The power range is 50 dB, which should correspond
to a voltage change in V
of 50 dB¥ 24 mV/dB = 1.2 V,
SET
which agrees.
Now, the value of V
is of interest, although it is a dependent
APC
parameter, inside the loop. It depends on the characteristics of
the power amplifier, and the value of the carrier amplitude V
Using the control values derived above, that is, G
= 1 V, and assuming the applied power is fixed at –7 dBm
V
GBC
= 0.316 and
O
CW
.
(so VCW = 100 mV rms), the following is true using Equation 11:
VVVVkGVV
()( )/ –log/
max =
APCSET GBCSLPO CW Z
(.)/ . –log(.../)
=¥¥ ¥
144104800316 0 316 0 1 316
.–..
==
VVVVkGVV
APCSET GBCSLPO CWZ
30 05 25
()()/ –log/
min =
(.)/ . –log (... /)
=¥¥ ¥
024104800316 0 316 0 1 316
.–.
==
05 05
zero
10
V
10
V
10
10
m
(15)
V
m
(16)
both of which results are consistent with the assumptions made
about the amplifier control function. Note that the second term
is independent of the delivered power and a fixed function of
the drive power.
DIRECTIONAL COUPLER
V
= kV
IN
RF
V
SET
RESPONSE-SHAPING
OF OVERALL CONTROL-
LOOP (EXTERNAL CAP)
V
RF
AD8315
RF PA
C
FLT
V
RF DRIVE: UP
TO 2.5GHz
V
APC
CW
Figure 4. Idealized Control Loop for Analysis
Finally, using the loop time constant for these parameters and
an illustrative value of 2 nF for the filter capacitor C
TVVT
=
(/)
OGBCSLP
=¥=
(/ . ) .( ).1048 3072 128mm
snFs
FLT
:
(17)
Practical Loop
At the present time, power amplifiers, or VGAs preceding such
amplifiers, do not provide an exponential gain characteristic. It
follows that the loop dynamics (the effective time constant) will
vary with the setpoint, since the exponential function is unique
in providing constant dynamics. The procedure must, therefore,
be as follows. Beginning with the curve usually provided for the
power output versus the APC voltage, draw a tangent at the
point on this curve where the slope is highest (see Figure 5).
Using this line, calculate the effective minimum value of the
variable V
constant. Note that the minimum in V
maximum rate of change in the output power versus V
and use it in Equation 17 to determine the time
GBC
corresponds to the
GBC
APC
.
For example, suppose it is found that, for a given drive power,
the amplifier generates an output power of P
at V
P
2
VVVPP
GBC
= V2. Then, it is readily shown that:
APC
= 20
(–)/(–)
21 2 1
at V
1
= V1 and
APC
(18)
This should be used to calculate the filter capacitance. The
response time at high and low power levels (on the “shoulders”
REV. B
–11–
of the curve shown in Figure 5) will be slower. Note also that it
is sometimes useful to add a zero in the closed-loop response by
placing a resistor in series with C
. For more about these
FLT
matters, refer to the Applications section.
V2, P
33
23
13
– dBm
RF
P
3
–7
0
0.51.01.52.02.5
V1, P
1
V
– V
APC
2
Figure 5. Typical Power-Control Curve
A Note About Power Equivalency
In using the AD8315, it must be understood that log amps do not
fundamentally respond to power. It is for this reason that dBV
(decibels above 1 V rms) are used rather than the commonly used
metric of dBm. The dBV scaling is fixed, independent of termination impedance, while the corresponding power level is not.
For example, 224 mV rms is always –13 dBV (with one further
condition of an assumed sinusoidal waveform; see the AD640
data sheet for more information about the effect of waveform on
logarithmic intercept), and this corresponds to a power of 0 dBm
when the net impedance at the input is 50 W. When this impedance
is altered to 200 W, however, the same voltage corresponds to a
power level that is four times smaller (P = V
2
/R) or –6 dBm. A
dBV level may be converted to dBm in the special case of a 50 W
system and a sinusoidal signal by simply adding 13 dB (0 dBV
is then, and only then, equivalent to 13 dBm).
Therefore, the external termination added ahead of the AD8315
determines the effective power scaling. This will often take the
form of a simple resistor (52.3 W will provide a net 50 W input),
but more elaborate matching networks may be used. The choice
of impedance determines the logarithmic intercept, that is, the
input power for which the V
versus PIN function would
SET
cross the baseline if that relationship were continuous for all
values of V
. This is never the case for a practical log amp; the
IN
intercept (so many dBV) refers to the value obtained by the
minimum error straight line fit to the actual graph of V
(more generally, VIN). Where the modulation is complex, as
P
IN
SET
versus
in CDMA, the calibration of the power response needs to be
adjusted; the intercept will remain stable for any given arbitrary
waveform. When a true power (waveform independent) response is
needed, a mean-responding detector, such as the AD8361,
should be considered.
The logarithmic slope, V
in Equation 1, which is the amount
SLP
by which the setpoint voltage needs to be changed for each decibel
of input change (voltage or power), is, in principle, independent
of waveform or termination impedance. In practice, it usually
falls off somewhat at higher frequencies, due to the declining
gain of the amplifier stages and other effects in the detector
cells (see TPC 13).
Page 12
AD8315
Basic Connections
Figure 6 shows the basic connections for operating the AD8315,
and Figure 7 shows a block diagram of a typical application.
The AD8315 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 AD8315.
The supply to the VPOS pin should be decoupled with a low
inductance 0.1 mF surface-mount ceramic capacitor, close to the
device. The AD8315 has an internal input coupling capacitor.
This negates the need for external ac-coupling. This capacitor,
along with the low frequency input impedance of the device of
approximately 2.8 kW, sets the minimum usable input frequency
to around 0.016 GHz. A broadband 50 W input match is achieved
in this example by connecting a 52.3 W resistor between RFIN
and ground. A plot of input impedance versus frequency is
shown in TPC 9. Other coupling methods are also possible (see
Input Coupling Options section).
NC
0.1F
8
7
6
C1
+V
S
(2.7V TO 5.5V)
+V
APC
RFIN
+V
V
SET
R1
52.3
S
C
FLT
AD8315
1
2
3
45
NC = NO CONNECT
RFIN
ENBL
VSET
VPOS
VAPC
COMMFLTR
Figure 6. Basic Connections
DIRECTIONAL
COUPLER
ATTENUATOR
52.3
RFIN
POWER
AMP
GAIN
CONTROL
VOLTAGE
VAPC
AD8315
FLTR
C
VSET
FLT
RFIN
DAC
Figure 7. Typical Application
In a power control loop, the AD8315 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 AD8315, 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 AD8315.
A setpoint voltage is applied to VSET from the controlling
source (generally this will be a DAC). Any imbalance between
the RF input level and the level corresponding to the setpoint
voltage will be corrected by the AD8315’s VAPC output that
drives the gain control terminal of the PA. This restores a balance
between the actual power level sensed at the input of the AD8315
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 will tend to increase gain.
can swing from 250 mV to within 100 mV of the supply
V
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 TPC 19.
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 TPCs 2, 3, 5, and 6). At 0.9 GHz, for example, a voltage of
1 V on VSET indicates a demand for –30 dBV (–17 dBm re 50 W)
at RFIN. The corresponding power level at the output of the
power amplifier will be greater than this amount due to the
attenuation through the directional coupler.
For setpoint voltages of less than approximately 250 mV, V
APC
will remain unconditionally at its minimum level of approximately
250 mV. This feature can be used to prevent any spurious emissions
during power-up and power-down phases.
Above 250 mV, V
will have 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 mV/dB or approximately 43.5 dB/V.
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 which, in the case of the AD8315, 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
is very large, it will dominate the time domain
FLT
response, but the incremental bandwidth of this loop will still
vary as V
traverses the nonlinear gain-control function of the
APC
PA, as sketched in Figure 5. This bandwidth will be highest at
the point where the slope of the tangent drawn on this curve is
greatest—that is, for power outputs near the center of the PA’s
range—and will be 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
, the loop bandwidth will generally
FLT
increase, in inverse proportion to its value. Eventually, however,
a secondary effect will appear, due to the inherent phase lag in
the power amplifier’s control path, some of which may be due to
parasitic or deliberately added capacitance at the VAPC pin.
This 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
will typically range 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 resistance in series
with C
; this generates an additional zero in the closed-loop
FLT
transfer function, that will serve to cancel some of the higher
order poles in the overall loop. A combination of main capacitor
shunted by a second capacitor and resistor in series will
C
FLT
also be useful in minimizing the settling time of the loop.
Mobile Handset Power Control Example
Figure 8 shows a complete power amplifier control circuit for a
dual mode handset. The PF08107B (Hitachi), a dual mode
(GSM, DCS) PA, is driven by a nominal power level of 3 dBm.
–12–
REV. B
Page 13
3.5V
4.7F4.7F
AD8315
TO
ANTENNA
8-BIT
RAMP DAC
0V–2.55V
BAND
SELECT
0V/2V
VCTL
VAPC
0.1F
8
7
6
5
1000pF
(OPTIONAL,
SEE TEXT)
+V
S
2.7V
500
LDC15D190A0007A
7
8
5
ATTN
20dB
R2*
600
R3*
1k
*R2, R3 OPTIONAL,
*SEE TEXT
2
ENABLE
0V/2.7V
6
52.3
150pF
1.5k
1
49.9
4
3
R1
1
2
3
4
NC = NO CONNECT
GSM
P
OUT
35dBm MAX
P
DCS
OUT
32dBm MAX
AD8315
RFIN
ENBL
VSET
1000pF
PF08107B
VPOS
VA PC
NC
COMMFLTR
Figure 8. Dual Mode (GSM/DCS) PA Control Example
PIN GSM
3dBm
DCS
P
IN
3dBm
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.
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 AD8315.
This results in peak input levels to the AD8315 of –4 dBm
(GSM) and –2 dBm (DCS). While the AD8315 gives a linear
response for input levels up to +2 dBm, for highly temperaturestable performance at maximum PA output power, the maximum input level should be limited to approximately –2 dBm
(see TPC 3 and TPC 5). This does, however, reduce the sensitivity of the circuit at the low end.
The operational setpoint voltage, in the range 250 mV to 1.4 V, is
applied to the VSET Pin of the AD8315. This will typically be
supplied by a digital-to-analog converter (DAC). The AD8315’s
VAPC output drives the level control pin of the power amplifier
directly. V
reaches a maximum value of approximately 2.5 V
APC
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,
VAPC should be held at its minimum level of 250 mV by keeping
VSET below 200 mV.
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 VSET to 0.4 dB/bit (0.04 dB/mV times
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
will depend 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 may be necessary.
In this example, a 150 pF capacitor is used and a 1.5 kW 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 will work with the input impedance of the
PA to create a resistor divider and will reduce the loop gain. The
size of the resistor divider ratio depends upon the available
output swing of V
and the required control voltage on the PA.
APC
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 (i.e., VAPC goes to its maximum value in an effort to balance the loop), the quiescent current
of the AD8315 will increase somewhat, particularly at supply
voltages greater than 3 V.
REV. B
–13–
Page 14
AD8315
Figure 9 shows the relationship between V
power (P
) at 0.9 GHz . The overall gain control function is
OUT
linear in dB for a dynamic range of over 40 dB. Note that for V
and output
SET
SET
voltages below 300 mV, the output power drops off steeply as
VAPC drops toward its minimum level of 250 mV.
1.6
4
3
2
1
0
–1
–2
–3
–4
ERROR – dB
40
30
20
10
0
– dBm
OUT
P
–10
–20
–30
–40
0
Figure 9. P
+85 C
+25 C
+25 C
–30 C
–30 C
0.20.40.60.81.01.21.4
vs. V
OUT
SET
V
– V
SET
at 0.9 GHz for Dual Mode Handset
+85 C
Power Amplifier Application; –30∞C, +25∞C, and +85∞C
Enable and Power-On
The AD8315 may be disabled by pulling the ENBL pin to ground.
This reduces the supply current from its nominal level of 7.4 mA
to 4 mA. The logic threshold for turning on the device is at 1.5 V
with 2.7 V supply voltage. A plot of the enable glitch is shown in
TPC 20. Alternatively, the device can be completely disabled by
pulling the supply voltage to ground. To minimize glitch in this
mode, ENBL and VPOS should be tied together. If VPOS is
applied before the device is enabled, a narrow 750 mV glitch will
result (see TPC 27).
In both situations, the voltage on VSET should be kept below
200 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 AD8315, along with
the low frequency input impedance of 2.8 kW, give a high-pass
input corner frequency of approximately 16 MHz. This sets the
minimum operating frequency. Figure 10 shows three options for
input coupling. A broadband resistive match can be implemented
by connecting a shunt resistor to ground at RFIN (Figure 10a).
This 52.3 W resistor (other values can also be used to select different overall input impedances) combines with the input impedance
of the AD8315 to give a broadband input impedance of 50 W.
While the input resistance and capacitance (C
and RIN) of the
IN
AD8315 will vary from device to device by approximately ±20%,
and over frequency (TPC 9), the dominance of the external shunt
resistor means that the variation in the overall input impedance
will be close to the 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 10b.
This is not recommended at low frequencies as device tolerances
will dramatically vary the quality of the match because of the large
input resistance. For low frequencies, Option 10a or Option 10c
is recommended.
In Figure 10b, 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 will be 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.
AD8315
C
C
RFIN
R
SHUNT
52.3
R
C
IN
IN
a. Broadband Resistive
AD8315
C
RFIN
C
R
C
IN
IN
X1
X2
b. Narrow Band Reactive
ANTENNA
AD8315
C
C
STRIPLINE
PA
R
ATTN
RFIN
R
C
IN
IN
c. Series Attenuation
Figure 10. Input Coupling Options
Figure 10c shows a third method for coupling the input signal
into the AD8315. A series resistor, connected to the RF source,
combines with the input impedance of the AD8315 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.
–14–
REV. B
Page 15
AD8315
Using the Chip Scale Package
On the underside of the chip scale package, there is an exposed
paddle. This paddle is internally connected to the chip’s ground.
There is no thermal requirement to solder the paddle down to the
printed circuit board’s ground plane. However, soldering down
the paddle has been shown to increase the stability over frequency
of the AD8315 ACP’s response at low input power levels (i.e., at
around –45 dBm) in the DCS and PCS bands
.
Evaluation Board
Figure 11 shows the schematic of the AD8315 MSOP evaluation
board. The layout and silkscreen of the component side are
shown in Figures 12 and 13. An evaluation board is also available
for the LFCSP package (for exact part numbers, see Ordering
Guide). Apart from the slightly smaller device footprint, the
LFCSP evaluation board is identical to the MSOP board. 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 single 0.1 F capacitor.
Table II details the various configuration options of the
evaluation board.
RFIN
VSET
R2
52.3
R1
J1
0
VPOS
SW1
J3
C4
(OPEN)
0.1F
AD8315
1
RFIN
2
ENBL
3
VSET
4
FLTR
NC = NO CONNECT
V
POS
C3
0.1F
C5
16.2k
AD8031
R5
10k
R7
VPOS
VAPC
COMM
NC
0.1F
8
7
6
5
R8
10k
R6
17.8k
C1
TP2
TP1
R3
0
R4
(OPEN)C2(OPEN)
LK2LK1
V
POS
Figure 11. Evaluation Board Schematic
Table II. Evaluation Board Configuration Options
ComponentFunctionDefault Condition
TP1, TP2Supply and Ground Vector PinsNot Applicable
SW1Device Enable: When in Position A, the ENBL pin is connected to VPOS andSW1 = A
the AD8315 is in operating mode. In Position B, the ENBL pin is grounded
putting the device in power-down mode.
R1, R2Input Interface: The 52.3 W resistor in Position R2 combines with theR2 = 52.3 W (Size 0603)
AD8315’s internal input impedance to give a broadband input impedanceR1 = 0 W (Size 0402)
of around 50 W. A reactive match can be implemented by replacing R2 with
an inductor and R1 (0 W) with a capacitor. Note that the AD8315’s RF input
is internally ac-coupled.
R3, R4, C2Output Interface: R4 and C2 can be used to check the response of V
capacitive and resistive loading. R3/R4 can be used to reduce the slope of V
toR4 = C2 = Open (Size 0603)
APC
.R3 = 0 W (Size 0603)
APC
C1Power Supply Decoupling: The nominal supply decoupling consists of aC1 = 0.1 mF (Size 0603)
0.1 mF capacitor.
C4Filter Capacitor: The response time of V
can be modified by placing aC4 = Open (Size 0603)
APC
capacitor between FLTR (Pin 4) and ground.
LK1, LK2Measurement Mode: A quasi-measurement mode can be implemented byLK1, LK2 = Installed
installing LK1 and LK2 (connecting an inverted V
nominal relationship between RFIN and V
. In this mode, a large capacitor
SET
APC
to V
) to yield the
SET
(0.01 mF or greater) must be installed in C4.
J2
VAPC
REV. B
–15–
Page 16
AD8315
Figure 12. Layout of Component Side (MSOP)
For operation in controller mode, both jumpers, LK1 and LK2,
should be removed. The setpoint voltage is applied to V
SET
,
RFIN is connected to the RF source (PA output or directional
coupler), and V
is connected to the gain control pin of the
APC
PA. When used in controller mode, a capacitor must be installed in
for loop stability. For GSM/DCS handset power amplifiers,
C
4
this capacitor should typically range from 150 pF to 300 pF.
A quasi-measurement mode (where the AD8315 delivers an
output voltage that is proportional to the log of the input signal)
can be implemented, to establish the relationship between V
SET
and RFIN, by installing the two jumpers, LK1 and LK2. This
mimics an AGC loop. To establish the transfer function of the
log amp, the RF input should be swept while the voltage on
is measured, that is, the SMA connector labeled VSET
V
SET
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 mF or greater) must be installed in C4
(filter capacitor) to ensure loop stability.