37.5 mV/dB Voltage Output
On-Chip Low-Pass Output Filter
Limiter Performance
ⴞ1 dB Output Flatness over 80 dB Range
ⴞ3ⴗ Phase Stability at 10.7 MHz over 80 dB Range
Adjustable Output Amplitude
Low Power
+5 V Single Supply Operation
65 mW Typical Power Consumption
CMOS-Compatible Power-Down to 325 W typ
<5 s Enable/Disable Time
APPLICATIONS
Ultrasound and Sonar Processing
Phase-Stable Limiting Amplifier to 100 MHz
Received Signal Strength Indicator (RSSI)
Wide Range Signal and Power Measurement
PRODUCT DESCRIPTION
The AD606 is a complete, monolithic logarithmic amplifier
using a 9-stage “successive-detection” technique. It provides
both logarithmic and limited outputs. The logarithmic output is
from a three-pole post-demodulation low-pass filter and provides
AD606
a loadable output voltage of +0.1 V dc to +4 V dc. The logarithmic scaling is such that the output is +0.5 V for a sinusoidal
input of –75 dBm and +3.5 V at an input of +5 dBm; over this
range the logarithmic linearity is typically within ±0.4 dB. All
scaling parameters are proportional to the supply voltage.
The AD606 can operate above and below these limits, with
reduced linearity, to provide as much as 90 dB of conversion
range. A second low-pass filter automatically nulls the input
offset of the first stage down to the submicrovolt level. Adding
external capacitors to both filters allows operation at input frequencies as low as a few hertz.
The AD606’s limiter output provides a hard-limited signal
output as a differential current of ±1.2 mA from open-collector
outputs. In a typical application, both of these outputs are
loaded by 200 Ω resistors to provide a voltage gain of more than
90 dB from the input. Transition times are 1.5 ns, and the
phase is stable to within ±3° at 10.7 MHz for signals from
–75 dBm to +5 dBm.
The logarithmic amplifier operates from a single +5 V supply
and typically consumes 65 mW. It is enabled by a CMOS logic
level voltage input, with a response time of <5 µs. When dis-
abled, the standby power is reduced to <1 mW within 5 µs.
The AD606J is specified for the commercial temperature range
of 0°C to +70°C and is available in 16-lead plastic DIPs or
SOICs. Consult the factory for other packages and temperature
ranges.
FUNCTIONAL BLOCK DIAGRAM
REFERENCE
AND POWER-UP
30kV30kV
1.5kV
250V
1.5kV
HIGH-END
DETECTORS
AD606
12345678
INLOCOMMISUMILOGBFINVLOGOPCMLMLO
12mA/dB
ONE-POLE
FILTER
2mA/dB
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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
Operating Temperature Range . . . . . . . . . . . . . 0°C to +70°C
Storage Temperature Range . . . . . . . . . . . . –65°C to +150°C
Lead Temperature Range (Soldering 60 sec) . . . . . . . . +300°C
NOTES
1
Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent damage to the device. This is a stress rating only; functional operation of the
device at these or any other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute maximum rating
conditions for extended periods may affect device reliability.
AD606JN0°C to +70°C 16-Lead Plastic DIPN-16
AD606JR0°C to +70°C 16-Lead Narrow-Body R-16A
SOIC
AD606JR-REEL 0°C to +70°C 13" Tape and ReelR-16A
AD606JR-REEL7 0°C to +70°C 7" Tape and ReelR-16A
AD606-EBEvaluation Board
AD606JCHIPS0°C to +70°C Die
PIN DESCRIPTION
Plastic DIP (N)
and
Small Outline (R)
Packages
1
INLOINHI
COMMCOMM
2
ISUMPRUP
3
ILOGVPOS
4
AD606
BFINFIL1
VLOGFIL2
OPCMLADJ
LMLOLMHI
TOP VIEW
5
(Not to Scale)
6
7
8
16
15
14
13
12
11
10
9
PIN FUNCTION DESCRIPTIONS
Pin Mnemonic Function
1INLODIFFERENTIAL RF INPUT
–75 dBm to +5 dBm, Inverting, AC Coupled.
2COMMPOWER SUPPLY COMMON
Connect to Ground.
3ISUMLOG DETECTOR SUMMING NODE
4ILOGLOG CURRENT OUTPUT
Normally No Connection; 2 µA/dB Output
Current.
5BFINBUFFER INPUT
Optionally Used to Realize Low Frequency
Post-Demodulation Filters.
6VLOGBUFFERED LOG OUTPUT
37.5 mV/dB (100 mV to 4.5 V).
7OPCMOUTPUT COMMON
Connect to Ground.
8LMLODIFFERENTIAL LIMITER OUTPUT
1.2 mA Full-Scale Output Current. Open
Collector Output Must Be “Pulled” Up to
VPOS with R ≤ 400 Ω.
9LMHIDIFFERENTIAL LIMITER OUTPUT
1.2 mA Full-Scale Output Current. Open
Collector Output Must Be “Pulled” Up to
VPOS with R ≤ 400 Ω.
10LADJLIMITER LEVEL ADJUSTMENT
Optionally Used to Adjust Limiter Output
Current.
11FIL1OFFSET LOOP LOW-PASS FILTER
Normally No Connection; a Capacitor Between
FIL1 and FIL2 May Be Added to Lower the
Filter Cutoff Frequency.
12FIL2OFFSET LOOP LOW-PASS FILTER
Normally No Connection; See Above.
13VPOSPOSITIVE SUPPLY
Connect to +5 V at 13 mA.
14PRUPPOWER UP
CMOS (5 V) Logical High = Device On
(≈ 65 mW).
CMOS (0 V) Logical Low = Device Off
(≈ 325 µW).
15COMMPOWER SUPPLY COMMON
Connect to Ground.
16INHIDIFFERENTIAL RF INPUT
–75 dBm to +5 dBm, Noninverting, AC-Coupled.
CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily
accumulate on the human body and test equipment and can discharge without detection.
Although the AD606 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–
AD606
INPUT LEVEL CONVENTIONS
RF logarithmic amplifiers usually have their input specified in
“dBm,” meaning “decibels with respect to 1 mW.” Unfortunately, this is not precise for several reasons.
1. Log amps respond not to power but to voltage. In this respect, it would be less ambiguous to use “dBV” (decibels
referred to 1 V) as the input metric. Also, power is dependent
on the rms (root mean-square) value of the signal, while log
amps are not inherently rms responding.
2. The response of a demodulating log amp depends on the
waveform. Convention assumes that the input is sinusoidal.
However, the AD606 is capable of accurately handling any
input waveform, including ac voltages, pulses and square
waves, Gaussian noise, and so on. See the AD640 data sheet,
which covers the effect of waveform on logarithmic intercept,
for more information.
3. The impedance in which the specified power is measured is
not always stated. In the log amp context it is invariably
assumed to be 50 Ω. Thus, 0 dBm means “1 mW rms in 50 Ω,”
and corresponds to an rms voltage of
224 mV.
(1 mW × 50 Ω),
or
Popular convention requires the use of dBm to simplify the
comparison of log amp specifications. Unless otherwise stated,
sinusoidal inputs expressed as dBm in 50 Ω are used to specify
the performance of the AD606 throughout this data sheet. We
will also show the corresponding rms voltages where it helps to
clarify the specification. Noise levels will likewise be given in
dBm; the response to Gaussian noise is 0.5 dB higher than for a
sinusoidal input of the same rms value.
Note that dynamic range, being a simple ratio, is always specified simply as “dB”, and the slope of the logarithmic transfer
function is correctly specified as “mV/dB,” NOT as “mV/dBm.”
LOGARITHMIC SLOPE AND INTERCEPT
A generalized logarithmic amplifier having an input voltage V
and output voltage V
must satisfy a transfer function of the
LOG
IN
form
VV VV
=log (/)
LOGYINX
10
where, in the case of the AD606, the voltage VIN is the difference between the voltages on pins INHI and INLO, and the
voltage V
V
are fixed voltages that determine the slope and intercept of
X
is that measured at the output pin VLOG. VY and
LOG
the logarithmic amplifier, respectively. These parameters are
inherent in the design of a particular logarithmic amplifier,
although may be adjustable, as in the AD606. When V
the logarithmic argument is one, hence the logarithm is zero. V
= VX,
IN
X
is, therefore, called the logarithmic intercept voltage because the
output voltage V
age V
is can also be interpreted as the “volts per decade” when
Y
crosses zero for this input. The slope volt-
LOG
using base-10 logarithms as shown here.
Note carefully that V
and VLOG in the above paragraph
LOG
(and elsewhere in this data sheet) are different. The first is a
voltage; the second is a pin designation.
This equation suggests that the input V
is positive, that VIN must likewise be positive, since the
if V
X
is a dc quantity, and,
IN
logarithm of a negative number has no simple meaning. In fact,
in the AD606, the response is independent of the sign of V
IN
because of the particular way in which the circuit is built. This
is part of the demodulating nature of the amplifier, which
–4–
results in an alternating input voltage being transformed into a
quasi-dc (rectified and filtered) output voltage.
The single supply nature of the AD606 results in common-mode
level of the inputs INHI and INLO being at about +2.5 V (using the recommended +5 V supply). In normal ac operation,
this bias level is developed internally and the input signal is
coupled in through dc blocking capacitors. Any residual dc
offset voltage in the first stage limits the logarithmic accuracy for
small inputs. In ac operation, this offset is automatically and
continuously nulled via a feedback path from the last stage, provided that the pins INHI and INLO are not shorted together, as
would be the case if transformer coupling were used for the signal.
While any logarithmic amplifier must eventually conform to the
basic equation shown above, which, with appropriate elaboration, can also fully account for the effect of the signal waveform
on the effective intercept,
1
it is more convenient in RF applications to use a simpler expression. This simplification results
from first, assuming that the input is always sinusoidal, and
second, using a decibel representation for the input level. The
standard representation of RF levels is (incorrectly, in a log amp
context) in terms of power, specifically, decibels above 1 milli-
watt (dBm) with a presumed impedance level of 50 Ω. That
being the case, we can rewrite the transfer function as
=(–)
VVPP
LOGYINX
where it must be understood that PIN means the sinusoidal input
power level in a 50 Ω system, expressed in dBm, and P
intercept, also expressed in dBm. In this case, P
simple, dimensionless numbers. (P
is sometimes called the
X
IN
is the
X
and PX are
“logarithmic offset,” for reasons which are obvious from the
above equation.) V
is still defined as the logarithmic slope,
Y
usually specified as so many millivolts per decibel, or mV/dB.
In the case of the AD606, the slope voltage, V
750 mV when operating at V
= 5 V. This can also be ex-
POS
, is nominally
Y
pressed as 37.5 mV/dB or 750 mV/decade; thus, the 80 dB
range equates to 3 V. Figure 1 shows the transfer function of the
AD606. The slope is closely proportional to V
generally be stated as V
= 0.15 × V
Y
Thus, in those applica-
POS.
, and can more
POS
tions where the scaling must be independent of supply voltage,
this must be stabilized to the required accuracy. In applications
where the output is applied to an A/D converter, the reference
4
3.5
3
2.5
2
1.5
VLOG – Volts DC
1
0.5
0
SLOPE = 37.5mV/dB
INTERCEPT
AT –88.33dBm
–80–100
INPUT SIGNAL – dBm
+20
0–20–40–60
Figure 1. Nominal Transfer Function
1
See, for example, the AD640 data sheet, which is published in Section 3 of
the Special Linear Reference Manual or Section 9.3 of the 1992 Amplifier
Applications Guide.
REV. B
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