Data Sheet AD8315
Rev. D | Page 15 of 22
Now, the value of V
APC
is of interest, although it is a dependent
parameter, inside the loop. It depends on the characteristics of
the power amplifier, and the value of the carrier amplitude V
CW
.
Using the control values previously derived, that is, G
O
= 0.316
and V
GBC
= 1 V, and assuming the applied power is fixed at
−7 dBm (so V
CW
= 100 mV rms), the following is true using
Equation 11
V
APC
(max) = (V
SET
V
GBC
)/V
SLP
− log
10
kG
O
V
CW
/V
Z
= (1.44 × 1)/0.48 − log
10
(0.0316 × 0.316 × 0.1/316 µV)
= 3.0 − 0.5 = 2.5 V (15)
V
APC
(min) = (V
SET
V
GBC
)/V
SLP
− log
10
kG
O
V
CW
/V
Z
= (0.24 × 1)/0.48 − log
10
(0.0316 × 0.316 × 0.1/316 µV)
= 0.5 − 0.5 = 0 (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.
RF PA
DIRECTIONAL COUPLER
RF DRIVE: UP
TO 2.5GHz
AD8315
V
RF
V
CW
V
IN
= kV
RF
V
SET
V
APC
C
FLT
RESPONSE-SHAPING
OF OVERALL CONTROL-
LOOP (EXTERNAL CAP)
01520-034
Figure 35. 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
FLT
T
O
= (V
GBC
/V
SLP
) T
= (1/0.48)3.07 µs × 2 (nF) = 12.8 µs (17)
PRACTICAL LOOP
At 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)
varies with the setpoint because 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 vs. the APC voltage, draw a tangent at the
point on this curve where the slope is highest (see Figure 36).
Using this line, calculate the effective minimum value of the
variable V
GBC
and use it in Equation 17 to determine the time
constant. Note that the minimum in V
GBC
corresponds to the
maximum rate of change in the output power vs. V
APC
.
For example, suppose it is found that, for a given drive power,
the amplifier generates an output power of P
1
at V
APC
= V
1
and
P
2
at V
APC
= V
2
.
Then, it is readily shown that
V
GBC
= 20 (V
2
V
1
)/(P
2
P
1
) (18)
This must be used to calculate the filter capacitance. The
response time at high and low power levels (on the shoulders
of the curve shown in Figure 36) is slower. Note also that it is
sometimes useful to add a 0 in the closed-loop response by
placing a resistor in series with C
FLT
. For more information on
this, see the Transient Response section.
33
0
23
13
3
–7
V
2
, P
2
V
1
, P
1
P
RF
(dBm)
V
APC
(V)
0.5 1.0 1.5 2.0 2.5
01520-035
Figure 36. 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 Ω.
When this impedance is altered to 200 Ω, however, the same
voltage corresponds to a power level that is four times smaller
(P = V
2
/R) or −6 dBm. A dBV level can be converted to dBm in
the special case of a 50 Ω 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 often takes the form of
a simple resistor (52.3 Ω provides a net 50 Ω input), but more
elaborate matching networks can be used. The choice of impedance
determines the logarithmic intercept, that is, the input power
for which the V
SET
vs. P
IN
function crosses the baseline if that
relationship were continuous for all values of V
IN
.
This is never the case for a practical log amp; the intercept (so many
dBV) refers to the value obtained by the minimum error straight
line fit to the actual graph of V
SET
vs. P
IN
(more generally, V
IN
).
AD8315 Data Sheet
Rev. D | Page 16 of 22
Where the modulation is complex, as in CDMA, the calibration
of the power response must be adjusted; the intercept remains
stable for any given arbitrary waveform. When a true power
(waveform independent) response is needed, a mean-responding
detector, such as the AD8361, must be considered.
The logarithmic slope, V
SLP
in Equation 1, which is the amount
by which the setpoint voltage must 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
Figure 16).
BASIC CONNECTIONS
Figure 37 shows the basic connections for operating the
AD8315, and Figure 38 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 must be decoupled with a low
inductance 0.1 µF 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 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 plot of input impedance vs. frequency is shown
in Figure 12. Other coupling methods are also possible (see
Input Coupling Options section).
NC = NO CONNECT
RFIN
ENBL
VSET
VPOS
VAPC
NC
COMMFLTR
AD8315
1
2
3
54
6
7
8
RFIN
(2.7V TO 5.5V)
C1
0.1µF
R1
52.3
C
FLT
V
SET
+V
S
+V
S
+V
APC
01520-036
Figure 37. Basic Connections
RFIN
VSET
AD8315
VAPC
FLTR
DAC
RFIN
ATTENUATOR
52.3
POWER
AMP
DIRECTIONAL
COUPLER
GAIN
CONTROL
VOLTAGE
C
FLT
01520-037
Figure 38. Typical Application
In a power control loop, the AD8315 provides both the detector
and controller functions. A sample of the power amplifier (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 is a DAC). Any imbalance between the
RF input level and the level corresponding to the setpoint voltage is
corrected by the AD8315 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 tends to increase gain.
V
APC
can swing from 250 mV to within 100 mV of the supply
rail and can source up to 6 mA. If the control input of the PA
must 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 22.
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 5, Figure 6, Figure 8, and Figure 9). At 0.9 GHz, for
example, a voltage of 1 V on VSET indicates a demand for −30 dBV
(−17 dBm, re 50 Ω) 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 250 mV, V
APC
remains unconditionally at the minimum level of approximately
250 mV. This feature can prevent any spurious emissions during
power-up and power-down phases.
Above 250 mV, V
SET
has a linear control range up to 1.4 V,
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
FLT
is very
large, it dominates the time domain response, but the incremental
bandwidth of this loop still varies as V
APC
traverses the nonlinear
gain-control function of the PA, as shown in Figure 36.
Data Sheet AD8315
Rev. D | Page 17 of 22
This bandwidth is 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 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 the S-shaped form.
Using smaller values of C
FLT
, the loop bandwidth generally
increases in inverse proportion to the value. Eventually, however, a
secondary effect appears due to the inherent phase lag in the power
amplifier control path, some of which can 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
FLT
must be determined experimentally for a
particular amplifier. For GSM and DCS power amplifiers, C
FLT
typically ranges from 150 pF to 300 pF.
In many cases, some improvement in the worst-case response
time can be achieved by including a small resistance in series
with C
FLT
; this generates an additional 0 in the closed-loop transfer
function, that serves to cancel some of the higher order poles in
the overall loop. A combination of main capacitor C
FLT
shunted
by a second capacitor and resistor in series is also useful in
minimizing the settling time of the loop.
NC = NO CONNECT
RFIN
ENBL
VSET
VPOS
VAP C
NC
COMMFLTR
1
2
3
4
5
6
7
8
ENABLE
0V/2.7V
3
4
1
5
8
7
LDC15D190A0007A
2
6
AT T N
20dB
PF08107B
VCTL
VAPC
1000pF
3.5
V
1000pF
0.1µF
1.5k
150pF
R1
52.3
49.9
4.7µF 4.F
500
AD8315
BAND
SELECT
0V/2V
P
OUT
GSM
35dBm MAX
P
OUT
DCS
32dBm MAX
P
IN
GSM
3dBm
P
IN
DCS
3dBm
(OPTIONAL,
SEE TEXT)
+V
S
2.7V
R3
1
1k
R2
1
600
1
R2, R3 OPTIONAL,
SEE TEXT
8-BIT
RAMP DAC
0V TO 2.55V
TO
ANTENNA
01520-038
Figure 39. Dual-Mode (GSM/DCS) PA Control Example

AD8315ARMZ-RL

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
RF Detector 50dB GSM PA Cntlr
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union

Products related to this Datasheet