AD606
REV. B
–6–
Offset-Control Loop
The offset-control loop nulls the input offset voltage, and sets
up the bias voltages at the input pins INHI and INLO. A full
understanding of this offset-control loop is useful, particularly
when using larger input coupling capacitors and an external
filter capacitor to lower the minimum acceptable operating
frequency. The loop’s primary purpose is to extend the lower
end of the dynamic range in the case where the offset voltage of
the first stage should be high enough to cause later stages to
prematurely enter limiting, because of the high dc gain (about
8000) of the main amplifier system. For example, an offset
voltage of only 20 µV would become 160 mV at the output of
the last stage in the main amplifier (before the final limiter sec-
tion), driving the last stage well into limiting. In the absence of
noise, this limiting would simply result in the logarithmic output
ceasing to become any lower below a certain signal level at the
input. The offset would also degrade the logarithmic conform-
ance in this region. In practice, the finite noise of the first stage
also plays a role in this regard, even if the dc offset were zero.
Figure 3 shows a representation of this loop, reduced to essen-
tials. The figure closely corresponds to the internal circuitry,
and correctly shows the input resistance. Thus, the forward gain
of the main amplifier section is 7 × 11.15 dB, but the loop gain
is lowered because of the attenuation in the network formed by
RB1 and RB2 and the input resistance RA. The connection
polarity is such as to result in negative feedback, which reduces
the input offset voltage by the dc loop gain, here about 50 dB,
that is, by a factor of about 316. We use a differential representa-
tion, because later we will examine the consequences to the
power-up response time in the event that the ac coupling capaci-
tors C
C1
and C
C2
do not exactly match. Note that these capaci-
tors, as well as forming a high-pass filter to the signal in the
forward path, also introduce a pole in the feedback path.
TO FINAL
LIMITER
STAGE
+1
+1
RB1
30kV
RB2
30kV
RA
2.5kV
CF2
30pF
CF1
30pF
0V
RF2
360kV
RF1
360kV
FIL2
FIL1
C
Z
R
Z
C
C1
C
C2
78dB
Figure 3. Offset Control Loop
Internal resistors RF1 and RF2 in conjunction with grounded
capacitors CF1 and CF2 form a low-pass filter at 15 kHz. This
frequency can optionally be lowered by the addition of an exter-
nal capacitor C
Z
, and in some cases a series resistor R
Z
. This, in
conjunction with the low-pass section formed at the input cou-
pling, results in a two-pole high-pass response, falling of at
40 dB/decade below the corner frequency. The damping factor
of this filter depends on the ratio C
Z
/C
C
(when C
Z
>>C
F
) and
also on the value of R
Z
.
The inclusion of this control loop has no effect on the high frequency
response of the AD606. Nor does it have any effect on the low fre-
quency response when the input amplitude is substantially above the
input offset voltage.
The loop’s effect is felt only at the lower end of the dynamic
range, that is, from about 80 dBm to –70 dBm, and when the
signal frequency is near the lower edge of the passband. Thus,
the small signal results which are obtained using the suggested
model are not indicative of the ac response at moderate to high
signal levels. Figure 4 shows the response of this model for the
default case (using C
C
= 100 pF and C
Z
= 0) and with C
Z
=
150 pF. In general, a maximally flat ac response occurs when C
Z
is roughly twice C
C
(making due allowance for the internal
30 pF capacitors). Thus, for audio applications, one can use
C
C
= 2.7 µF and C
Z
= 4.7 µF to achieve a high-pass corner
(–3 dB) at 25 Hz.
90
70
–20
100k 100M10M1M10k
80
60
40
50
20
30
10
–10
0
INPUT FREQUENCY – Hz
RELATIVE OUTPUT – dB
C
Z
= 150pF
C
Z
= 0pF
Figure 4. Frequency Response of Offset Control Loop for
C
Z
= 0 pF and C
Z
= 150 pF (C
C
= 100 pF)
However, the maximally flat ac response is not optimal in two
special cases. First, where the RF input level is rapidly pulsed,
the fast edges will cause the loop filter to ring. Second, ringing
can also occur when using the power-up feature, and the ac
coupling capacitors do not exactly match in value. We will ex-
amine the latter case in a moment. Ringing in a linear amplifier
is annoying, but in a log amp, with its much enhanced sensitiv-
ity to near zero signals, it can be very disruptive.
To optimize the low level accuracy, that is, achieve a highly
damped pulse response in this filter, it is recommended to in-
clude a resistor R
Z
in series with an increased value of C
Z
. Some
experimentation may be necessary, but for operation in the
range 3 MHz to 70 MHz, values of C
C
= 100 pF, C
Z
= 1 nF
and R
Z
= 2 k are near optimal. For operation down to 100 kHz
use C
C
= 10 nF, C
Z
= 0.1 µF and R
Z
= 13 k. Figure 5 shows
typical connections for the AD606 with these filter components
added.
INHI
COMM
PRUP
VPOS
FIL1
FIL2
LADJ
LMHI
INLO
COMM
ISUM
ILOG
BFIN
VLOG
OPCM
LMLO
AD606JN
R
Z
C
Z
Figure 5. Use of C
Z
and R
Z
for Offset Control Loop
Compensation
AD606
REV. B
–7–
For operation above 10 MHz, it is not necessary to add the
external capacitors CF1, CF2, and C
Z
, although an improve-
ment in low frequency noise can be achieved by so doing (see
APPLICATIONS). Note that the offset control loop does not
materially affect the low-frequency cutoff at high input levels,
when the offset voltage is swamped by the signal.
Power-Up Interface
The AD606 features a power-saving mode, controlled by the
logic level at Pin 14 (PRUP). When powered down, the quies-
cent current is typically 65 µA, or about 325 µW. A CMOS
logical HIGH applied to PRUP activates both internal refer-
ences, and the system becomes fully functional within about
3.5 µs. When this input is a CMOS logical LOW, the system
shuts down to the quiescent level within about 5 µs.
The power-up time is somewhat dependent on the signal level
and can be degraded by mismatch of the input coupling capaci-
tors. The explanation is as follows. When the AD606 makes the
transition from powered-down to fully active, the dc bias voltage
at the input nodes INHI and INLO (about +2.5 V) inevitably
changes slightly, as base current in the input transistors flows in
the bias resistors. In fact, first-order correction for this is in-
cluded in the specially designed offset buffer amplifier, but even
a few millivolts of change at these inputs represents a significant
equivalent “dBm” level.
Now, if the coupling capacitors do not match exactly, some
fractional part of this residual voltage step becomes coupled into
the amplifier. For example, if there is a 10% capacitor mis-
match, and INHI and INLO jump 20 mV at power-up, there is
a 2 mV pulse input to the system, which may cause the offset
control loop to ring. Note that 2 mV is roughly 40 times greater
than the amplitude of a sinusoidal input at –75 dBm. As long as
the ringing persists, the AD606 will be “blind” to the actual
input, and V
LOG
will show major disturbances.
The solution to this problem is first, to ensure that the loop
filter does not ring, and second, to use well-matched capacitors
at the signal input. Use the component values suggested above
to minimize ringing.
APPLICATIONS
Note that the AD606 has more than 70 MHz of input band-
width and 90 dB of gain! Careful shielding is needed to realize
its full dynamic range, since nearly all application sites will be
pervaded by many kinds of interference, radio and TV stations,
etc., all of which the AD606 faithfully hears. In bench evalua-
tion, we recommend placing all of the components in a shielded
box and using feedthrough decoupling networks for the supply
voltage. In many applications, the AD606’s low power drain
allows the use of a 6 V battery inside the box.
Basic RSSI Application
Figure 6 shows the basic RSSI (Receiver Signal Strength Indica-
tor) application circuit, including the calibration adjustments,
either or both of which may be omitted in noncritical applica-
tions. This circuit may be used “as is” in such measurement
applications as the log/IF strip in a spectrum or network ana-
lyzer or, with the addition of an FM or QPSK demodulator fed
by the limiter outputs, as an IF strip in such communications
applications as a GSM digital mobile radio or FM receiver.
The slope adjustment works in this way: the buffer amplifier
(which forms part of a Sallen-Key two-pole filter, see Figure 2)
has a dc gain of plus two, and the resistance from BFIN (buffer
in) to OPCM (output common) is nominally 9.375 k. This
resistance is driven from the logarithmic detector sections with a
current scaled 2 µA/dB, generating 18.75 mV/dB at BFIN,
hence 37.5 mV/dB at V
LOG
Now, a resistor (R4 in Figure 6)
connected directly between BFIN and VLOG would form a
controlled positive-feedback network with the internal 9.375 k
resistor which would raise the gain, and thus increase the slope
voltage, while the same external resistor connected between
BFIN and ground would form a shunt across the internal resis-
tor and reduce the slope voltage. By connecting R4 to a potenti-
ometer R2 across the output, the slope may be adjusted either
way; the value for R4 shown in Figure 6 provides approximately
±10% range, with essentially no effect on the slope at the
midposition.
The intercept may be adjusted by adding a small current into
BFIN via R1 and R3. The AD606 is designed to have the nomi-
nal intercept value of –88 dBm when R1 is centered using this
network, which provides a range of ±5 dB.
51.1V
100pF
100pF
RF INPUT
NC
R5
200V
LIMITER OUTPUT
LOGARITHMIC
OUTPUT
R3
412kV
R4
174kV
R1
200kV
INTERCEPT
ADJUSTMENT
65dB
R2
50kV
SLOPE
ADJUSTMENT
610%
+5V
+5V
INHI
COMM
PRUP
VPOS
FIL1
FIL2
LADJ
LMHI
INLO
COMM
ISUM
ILOG
BFIN
VLOG
OPCM
LMLO
AD606
NC
0.1mF
NC = NO CONNECT
Figure 6. Basic Application Circuit Showing Optional Slope and Intercept Adjustments
AD606
REV. B
–8–
Adjustment Procedure
The slope and intercept adjustments interact; this can be mini-
mized by reducing the resistance of R1 and R2, chosen here to
minimize power drain. Calibration can be achieved in several
ways: The simplest is to apply an RF input at the desired oper-
ating frequency which is amplitude modulated at a relatively
low frequency (say 1 kHz to 10 kHz) to a known modulation
index. Thus, one might choose a ratio of 2 between the maxi-
mum and minimum levels of the RF amplitude, corresponding
to a 6 dB (strictly, 6.02 dB) change in input level. The average
RF level should be set to about –35 dBm (the midpoint of the
AD606’s range). R2 is then adjusted so that the 6 dB input
change results in the desired output voltage change, for ex-
ample, 226 mV at 37.5 mV/dB.
A better choice would be a 4:1 ratio (12.04 dB), to spread the
residual error out over a larger segment of the whole transfer
function. If a pulsed RF generator is available, the decibel incre-
ment might be enlarged to 20 dB or more. Using just a fixed-
level RF generator, the procedure is more time consuming, but
is carried out in just the same way: manually change the level by
a known number of decibels and adjust R2 until V
LOG
varies by
the corresponding voltage.
Having adjusted the slope, the intercept may now be simply ad-
justed using a known input level. A value of –35 dBm (397.6 mV
rms, or 400 mV to within 0.05 dB) is recommended, and if the
standard scaling is used (P
X
= –88.33 dBm, V
Y
= 37.5 mV/dB),
then V
LOG
should be set to +2 V at this input level.
A Low Cost Audio Through RF Power Meter
Figure 7 shows a simple power meter that uses the AD606 and
an ICL7136 3-1/2 digit DMM IC driving an LCD readout. The
circuit operates from a single +5 V supply and provides direct
readout in dBm, with a resolution of 0.1 dBm.
In contrast to the limited dynamic range of the diode and
thermistor-styled sensors used in power meters, the AD606 can
measure signals from below –80 dBm to over +10 dBm. An
optional 50 termination is included in the figure; this could
form the lower arm of an external attenuator to accommodate
larger signal levels. By the simple expedient of using a 13 dB
attenuator, the LCD reading now becomes dBV (decibels above
1 V rms). This requires a series resistor of 174 , presenting an
input resistance of 224 . Alternatively, the input resistance can
be raised to 600 using 464 and 133 . It is important to
note that the AD606 inputs must be ac coupled. To extend the
low frequency range, use larger coupling capacitors and an
external loop filter, as outlined earlier.
The nominal 0.5 V to 3.5 V output of the AD606 (for a –75 dBm
to +5 dBm input) must be scaled and level shifted to fit within
the +1 V to +4.5 V common-mode range of the ICL7136 for
the +5 V supply used. This is achieved by the passive resistor
network of R1, R2, and R3 in conjunction with the bias net-
works of R4 through R7, which provide the ICL7136 with its
reference voltage, and R9 through R11, which set the intercept.
The ICL7136 measures the differential voltage between INHI
and INLO, which ranges from –75 mV to +5 mV for a
–75 dBm to +5 dBm input.
To calibrate the power meter, first adjust R6 for 100 mV be-
tween REF HI and REF LO. This sets the initial slope. Then
adjust R10 to set INLO 80 mV higher than INHI. This sets the
initial intercept. The slope and intercept may now be adjusted
using a calibrated signal generator as outlined in the previous
section.
To extend the low frequency limit of the system to audio fre-
quencies, simply change C1, C2, and C3 to 4.7 µF.
The limiter output of the AD606 may be used to drive the high-
impedance input of a frequency counter.
51.1V
C1*
100pF
dBm
INPUT
NC
200V
+5V
INHI
COMM
PRUP
VPOS
FIL1
FIL2
LADJ
LMHI
INLO
COMM
ISUM
ILOG
BFIN
VLOG
OPCM
LMLO
AD606JN
NC
0.1mF
OPTIONAL
DRIVE TO
FREQUENCY
COUNTER
C3*
150pF
dBV
INPUT
174V
C2*
100pF
NC
+5V
FOR AUDIO MEASUREMENTS CHANGE
C1, C2, AND C3 TO 4.7mF; POSITIVE POLARITY
CONNECT TO PINS 1, 16
*
NC = NO CONNECT
+5V
2.513V NOM
R8
100kV
R9
5kV
R10
100kV
C4
1mF
+5V
R2
54.9kV
R1
1MV
R3
54.9kV
2.433V NOM
80mV
FOR
0dBm
SIGNAL
INPUT
R5
4.32kV
R6
500V
R7
162V
R4
4.99kV
+5V
100mV
+5V
0.1mF
DISPLAY
–75.0
32
35
31
36
40
39
38
34
33
180kV
50pF
0.1mF
1.8MV
0.1mF
0.047mF
V–
INHI
INLO
REF HI
COMM
REF LO
ICL7136CPL
Figure 7. A Low Cost RF Power Meter

AD606JNZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Logarithmic Amplifiers 50 MHz 80dB DEMODULATING AMP
Lifecycle:
New from this manufacturer.
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