True rms value
Average rectified value
Absolute value
Provides:
200 mV full-scale input range
(larger inputs with input attenuator)
High input impedance of 1012 V
Low input bias current: 25 pA max
High accuracy: ±0.3 mV ±0.3% of reading
RMS conversion with signal crest factors up to 5
Wide power supply range: +2.8 V, –3.2 V to ±16.5 V
Low power: 200 mA max supply current
Buffered voltage output
No external trims needed for specified accuracy
AD737—an unbuffered voltage output version with chip
power-down also available
GENERAL DESCRIPTION
The AD736 is a low power, precision, monolithic true rms-to-dc
converter. It is laser trimmed to provide a maximum error of
±0.3 mV ± 0.3% of reading with sine wave inputs. Furthermore,
it maintains high accuracy while measuring a wide range of
input waveforms, including variable duty cycle pulses and triac
(phase) controlled sine waves. The low cost and small size of
this converter make it suitable for upgrading the performance
of non-rms precision rectifiers in many applications. Compared
to these circuits, the AD736 offers higher accuracy at an equal
or lower cost.
The AD736 can compute the rms value of both ac and dc input
voltages. It can also be operated ac-coupled by adding one external capacitor. In this mode, the AD736 can resolve input signal
levels of 100 µV rms or less, despite variations in temperature or
supply voltage. High accuracy is also maintained for input
waveforms with crest factors of 1 to 3. In addition, crest factors
as high as 5 can be measured (while introducing only 2.5%
additional error) at the 200 mV full-scale input level.
The AD736 has its own output buffer amplifier, thereby providing a great deal of design flexibility. Requiring only 200 µA
of power supply current, the AD736 is optimized for use in
portable multimeters and other battery-powered applications.
Rev. F
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.
True RMS-to-DC Converter
FUNCTIONAL BLOCK DIAGRAM
8kΩ
1
C
C
FULL
WAVE
V
2
IN
AMPLIFIER
C
3
F
–V
S
4
BIAS
SECTION
INPUT
RECTIFIER
RMS CORE
Figure 1.
AD736
8kΩ
OUTPUT
AMPLIFIER
The AD736 allows the choice of two signal input terminals: a
high impedance FET input (10
12
Ω) that directly interfaces with
high Z input attenuators and a low impedance input (8 kΩ) that
allows the measurement of 300 mV input levels while operating
from the minimum power supply voltage of +2.8 V, −3.2 V. The
two inputs may be used either single-ended or differentially.
The AD736 has a 1% reading error bandwidth that exceeds
10 kHz for the input amplitudes from 20 mV rms to 200 mV
rms while consuming only 1 mW.
The AD736 is available in four performance grades. The
AD736J and AD736K grades are rated over the 0°C to +70°C
and −20°C to +85°C commercial temperature ranges. The
AD736A and AD736B grades are rated over the −40°C to +85°C
industrial temperature range. The AD736 is available in three
low c ost, 8-lead packages: PDIP, SOIC, and CERDIP.
PRODUCT HIGHLIGHTS
The AD736 is capable of computing the average rectified value,
absolute value, or true rms value of various input signals.
Only one external component, an averaging capacitor, is
required for the AD736 to perform true rms measurement.
The low power consumption of 1 mW makes the AD736
suitable for many battery-powered applications.
12
A high input impedance of 10
external buffer when interfacing with input attenuators.
A low impedance input is available for those applications that
require an input signal up to 300 mV rms operating from low
power supply voltages.
Table 1. @25°C ±5 V supplies, ac-coupled with 1 kHz sine wave input applied, unless otherwise noted. Specifications in bold are
tested on all production units at final electrical test. Results from those tests are used to calculate outgoing quality levels.
AD736J/AD736A AD736K/AD736B
Parameter Conditions Min Typ Max Min Typ Max Unit
TRANSFER FUNCTION
= √
V
OUT
CONVERSION ACCURACY 1 kHz sine wave
Tot al E rror, Inter nal Trim
All Grades 0 mV rms–200 mV rms 0.3/0.3
200 mV to 1 V rms −1.2
T
to T
MIN
MAX
A and B Grades @ 200 mV rms
J and K Grades @ 200 mV rms 0.007
vs. Supply Voltage
@ 200 mV rms Input VS = ±5 V to ±16.5 V
V
DC Reversal Error, DC-Coupled @ 600 mV dc
Nonlinearity2, 0 mV–200 mV @ 100 mV rms
1
Using C
C
0.5/0.5
±2.0
0.7/0.7
+0.06
−0.18
+0.1 0
−0.3 0
1.3 2.5
0.25
0.35 0
= ±5 V to ±3 V
S
0
0
0
Total Error, External Trim 0 mV rms–200 mV rms 0.1/0.5 0.1/0.3 ±mV/±% of Reading
Input Bias Current VS = ±3 V to ±16.5 V 1 25 1 25 pA
Low Impedance Input (Pin 1)
Signal Range
Continuous rms Level VS = +2.8 V, –3.2 V 300 300 mV rms
V
= ±5 V to ±16.5 V 1 1 V rms
S
Peak Transient Input VS = +2.8 V, −3.2 V ±1.7 ±1.7 V
V
V
= ±5 V ±3.8 ±3.8 V
S
= ±16.5 V ±11 ±11 V
S
Input Resistance 6.4 8 9.6 6.4 8 9.6 kΩ
Maximum Continuous
All supply voltages ±12 ±12 V p-p
Nondestructive Input
Input Offset Voltage
J and K Grades
A and B Grades
4
±3
±3
vs. Temperature 8 30 8 30 µV/°C
vs. Supply VS = ±5 V to ±16.5 V 50
V
= ±5 V to ±3 V 80 80 µV/V
S
150
1
Accuracy is specified with the AD736 connected as shown in Figure 18 with capacitor CC.
2
Nonlinearity is defined as the maximum deviation (in percent error) from a straight line connecting the readings at 0 mV rms and 200 mV rms. Output offset voltage is
adjusted to zero.
3
Error versus crest factor is specified as additional error for a 200 mV rms signal. Crest factor = V
4
DC offset does not limit ac resolution.
PEAK
/V rms.
2
Avg(V
)
IN
0.2/0.2
−1.2
0.007
+0.06
−0.18
1.3 2.5 % of Reading
0.25
±0.9
±4.0
V
±2.7 V
V
12
50
0.3/0.3
±2.0
0.5/0.5
+0.1
−0.3
0.35
200
1
±mV/±% of Reading
% of Reading
±mV/±% of Reading
±% of Reading/°C
%/V
%/V
% of Reading
mV rms
V rms
Ω
±3
±3
150
mV
mV
µV/V
Rev. F | Page 3 of 16
AD736
AD736J/AD736A AD736K/AD736B
Parameter Conditions Min Typ Max Min Typ Max Unit
OUTPUT CHARACTERISTICS
Output Offset Voltage
J and K Grades ±0.1
A and B Grades
±0.5
±0.5
vs.Temperature 1 20 1 20 µV/°C
vs. Supply VS = ±5 V to ±16.5 V 50
V
= ±5 V to ±3 V 50 50 µV/V
S
130
Output Voltage Swing
2 kΩ Load VS = +2.8 V, −3.2 V 0–1.6 1.7 0–1.6 1.7 V
V
V
No Load VS = ±16.5 V
= ±5 V 0–3.6 3.8 0–3.6 3.8 V
S
= ±16.5 V
S
0–4
0–4
5
12
Output Current 2 2 mA
Short-Circuit Current 3 3 mA
Output Resistance @ dc 0.2 0.2 Ω
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
8kΩ
FULL
WAVE
RECTIFIER
INPUT
AMPLIFIER
BIAS
SECTION
RMS CORE
and 8-Lead CERDIP (Q-8) Packages
AD736
8kΩ
OUTPUT
AMPLIFIER
8
COM
+V
7
6
OUTPUT
C
5
S
AV
00834-F-001
5
8-Lead PDIP Package: θJA = 165°C/W
8-Lead CERDIP Package: θ
8-Lead SOIC Package: θ
= 110°C/W
JA
= 155°C/W
JA
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.
Rev. F | Page 5 of 16
AD736
TYPICAL PERFORMANCE CHARACTERISTICS
0.7
VIN = 200mV rms
1kHz SINE WAVE
C
0.5
0.3
0.1
–0.1
–0.3
ADDITIONAL ERROR (% OF READING)
= 100µF
AV
C
= 22µF
F
0
10V
SINEWAVE INPUT,VS=±5V,
= 22µF, CF = 4.7µF, CC = 22µF
C
AV
1V
100mV
10mV
INPUT LEVEL (rms)
1mV
1% ERROR
–3dB
10% ERROR
–0.5
0428612141016
SUPPLY VOLTAGE (±V)
Figure 3. Additional Error vs. Supply Voltage
16
DC-COUPLED
14
12
10
8
6
4
PEAK INPUT BEFORE CLIPPING (V)
2
0
0428612141016
PIN 1
PIN 2
SUPPLY VOLTAGE (±V)
Figure 4. Maximum Input Level vs. Supply Voltage
16
1kHz SINE WAVE INPUT
14
12
10
00834-F-002
100µV
0.11100101000
–3dB FREQUENCY (kHz)
00834-F-005
Figure 6. Frequency Response Driving Pin 1
10V
SINEWAVE INPUT,VS=±5V,
= 22µF, CF = 4.7µF, CC = 22µF
C
AV
1V
100mV
10mV
INPUT LEVEL (rms)
1mV
00834-F-003
100µV
0.11100101000
1% ERROR
–3dB FREQUENCY (kHz)
10% ERROR
–3dB
00834-F-006
Figure 7. Frequency Response Driving Pin 2
6
3ms BURST OF 1kHz =
3 CYCLES
200mV rms SIGNAL
5
= ±5V
V
S
C
= 22µF
C
C
= 100µF
F
4
CAV = 10µF
CAV = 33µF
8
6
4
PEAK BUFFER OUTPUT (V)
2
0
02461081214
SUPPLY VOLTAGE (±V)
Figure 5. Peak Buffer Output vs. Supply Voltage
00834-F-004
16
Rev. F | Page 6 of 16
3
2
1
ADDITIONAL ERROR (% OF READING)
0
1234
CREST FACTOR (V
CAV = 250µF
/V rms)
PEAK
Figure 8. Additional Error vs. Crest Factor vs. C
CAV = 100µF
AV
00834-F-007
5
AD736
0.8
VIN = 200mV rms
1kHz SINE WAVE
0.6
C
= 100µF
AV
C
= 22µF
F
0.4
V
= ±5V
S
0.2
0
–0.2
–0.4
ADDITIONAL ERROR (% OF READING)
–0.6
–0.8
–60–20–402006080100 12040140
TEMPERATURE (°C)
Figure 9. Additional Error vs. Temperature
00834-F-008
1.0
0.5
0
–0.5
–1.0
–1.5
ERROR (% OF READING)
VIN = SINE WAVE @ 1kHz
–2.0
C
= 22µF, CC = 47µF,
AV
= 4.7µF, VS = ±5V
C
F
–2.5
10mV100mV1V2V
INPUT LEVEL (rms)
Figure 12. Error vs. RMS Input Voltage (Pin 2),
Output Buffer Offset Is Adjusted to Zero
00834-F-011
600
VIN = 200mV rms
1kHz SINE WAVE
= 100µF
C
AV
500
= 22µF
C
F
V
= ±5V
S
400
300
DC SUPPLY CURRENT (µA)
200
100
00.20.40.60.81.0
rms INPUT LEVEL (V)
Figure 10. DC Supply Current vs. RMS Input Level
10mV
VIN = 1kHz
SINE WAVE INPUT
AC-COUPLED
= ±5V
V
S
1mV
100
(µF)
10
AV
C
00834-F-009
1
101001k
Figure 13. C
AV
FREQUENCY (Hz)
vs. Frequency for Specified Averaging Error
–0.5%
–1%
= 200mV rms
V
IN
C
= 47µF
C
C
= 47µF
F
VS = ±5V
00834-F-012
1V
–1%
100mV
–0.5%
INPUT LEVEL (rms)
100µV
10µV
1001k10k100k
–3dB FREQUENCY (Hz)
Figure 11. –3 dB Frequency vs. RMS Input Level (Pin 2)
00834-F-010
Rev. F | Page 7 of 16
10mV
INPUT LEVEL (rms)
VIN SINE WAVE
AC-COUPLED
= 10µF, CC = 47µF,
C
AV
= 47µF, VS = ±5V
C
1mV
1101001k
FREQUENCY (Hz)
F
Figure 14. RMS Input Level vs. Frequency for Specified Averaging Error
00834-F-013
AD736
4.0
3.5
3.0
2.5
2.0
INPUT BIAS CURRENT (pA)
1.5
1.0
1V
100mV
0246812141016
SUPPLY VOLTAGE (±V)
Figure 15. Pin 2 Input Bias Current vs. Supply Voltage
VS = 5V
C
= 22µF
C
C
= 0µF
F
CALCULATING SETTLING TIME USING FIGURE 16
Figure 16 may be used to closely approximate the time required
for the AD736 to settle when its input level is reduced in
amplitude. The net time required for the rms converter to settle
is the difference between two times extracted from the graph—
the initial time minus the final settling time. As an example,
consider the following conditions: a 33 µF averaging capacitor, a
100 mV initial rms input level, and a final (reduced) 1 mV input
level. From Figure 16, the initial settling time (where the
100 mV line intersects the 33 µF line) is approximately 80 ms.
00834-F-014
The settling time corresponding to the new or final input level
of 1 mV is approximately 8 seconds. Therefore, the net time for
the circuit to settle to its new value is 8 seconds minus 80 ms,
which is 7.92 seconds. Note that because of the smooth decay
characteristic inherent with a capacitor/diode combination, this
is the total settling time to the final value (i.e., not the settling
time to 1%, 0.1%, and so on, of the final value). Als o, this g raph
provides the worst-case settling time since the AD736 settles
very quickly with increasing input levels.
CAV = 10µF
10mV
INPUT LEVEL (rms)
1mV
100µV
1ms10ms100ms1s10s100s
CAV = 33µF
SETTLING TIME
CAV = 100µF
Figure 16. Settling Time vs. RMS Input Level for Various Values of C
10nA
1nA
100pA
10pA
INPUT BIAS CURRENT
1pA
00834-F-015
AV
100fA
–55 –35 –15525658510545125
TEMPERATURE (°C)
00834-F-016
Figure 17. Pin 2 Input Bias Current vs. Temperature
Rev. F | Page 8 of 16
AD736
TYPES OF AC MEASUREMENT
The AD736 is capable of measuring ac signals by operating as
either an average responding converter or a true rms-to-dc
converter. As its name implies, an average responding converter
computes the average absolute value of an ac (or ac and dc)
voltage or current by full-wave rectifying and low-pass filtering
the input signal; this approximates the average. The resulting
output, a dc average level, is then scaled by adding (or reducing)
gain; this scale factor converts the dc average reading to an rms
equivalent value for the waveform being measured. For
example, the average absolute value of a sine wave voltage is
0.636 times that of V
times V
. Therefore, for sine wave voltages, the required scale
PEAK
; the corresponding rms value is 0.707
PEAK
factor is 1.11 (0.707 divided by 0.636).
In contrast to measuring the average value, true rms measurement is a universal language among waveforms, allowing the
magnitudes of all types of voltage (or current) waveforms to be
compared to one another and to dc. RMS is a direct measure of
the power or heating value of an ac voltage compared to that of
a dc voltage; an ac signal of 1 V rms produces the same amount
of heat in a resistor as a 1 V dc signal.
Mathematically, the rms value of a voltage is defined (using a
simplified equation) as
)(2VAvgrmsV=
This involves squaring the signal, taking the average, and then
obtaining the square root. True rms converters are smart
rectifiers; they provide an accurate rms reading regardless of the
type of waveform being measured. However, average
responding converters can exhibit very high errors when their
input signals deviate from their precalibrated waveform; the
magnitude of the error depends on the type of waveform being
measured. For example, if an average responding converter is
calibrated to measure the rms value of sine wave voltages and is
then used to measure either symmetrical square waves or dc
voltages, the converter will have a computational error 11% (of
reading) higher than the true rms value (see Table 3).
Table 3. Error Introduced by an Average Responding Circuit when Measuring Common Waveforms
Average Responding Circuit
Waveform Type 1 V Peak
Amplitude
% of Reading Error Using
Average Responding Circuit
Rev. F | Page 9 of 16
AD736
THEORY OF OPERATION
V
IN
OPTIONAL RETURN PATH
FWR
CURRENT
MODE
ABSOLUTE
C
IN
1
2
AMPLIFIER
I
VALUE
8kΩ
INPUT
<10pA
B
C
V
C
DC
C =
+
AC
10µF
AD736
OUTPUT
AMPLIFIER
8kΩ
COM
8
7
0.1µF
+V
S
BIAS
3
SECTION
RMS
TRANSLINEAR
CORE
–V
S
4
0.1µF
TO
COM
PIN
Figure 18. AD736 True RMS Circuit
As shown by Figure 18, the AD736 has five functional subsections: the input amplifier, full-wave rectifier (FWR), rms core,
output amplifier, and bias section. The FET input amplifier
allows both a high impedance, buffered input (Pin 2) and a low
impedance, wide dynamic range input (Pin 1). The high
impedance input, with its low input bias current, is well suited
for use with high impedance input attenuators.
The output of the input amplifier drives a full-wave precision
rectifier, which in turn drives the rms core. The essential rms
operations of squaring, averaging, and square rooting are
performed in the core, using an external averaging capacitor,
. Without CAV, the rectified input signal travels through the
C
AV
core unprocessed, as is done with the average responding
connection (Figure 19).
A final subsection, an output amplifier, buffers the output from
the core and allows optional low-pass filtering to be performed
via the external capacitor, C
, which is connected across the
F
feedback path of the amplifier. In the average responding connection, this is where all of the averaging is carried out. In the
rms circuit, this additional filtering stage helps reduce any output ripple that was not removed by the averaging capacitor, C
AV
C
33µF
C
10µF
.
A
+
F
+
6
C
5
(OPTIONAL)
RMS
OUTPUT
AV
00834-F-017
RMS MEASUREMENT—CHOOSING THE OPTIMUM
VALUE FOR C
Since the external averaging capacitor, CAV, holds the rectified
input signal during rms computation, its value directly affects
the accuracy of the rms measurement, especially at low
frequencies. Furthermore, because the averaging capacitor
appears across a diode in the rms core, the averaging time
constant increases exponentially as the input signal is reduced.
This means that as the input level decreases, errors due to
nonideal averaging decrease while the time required for the
circuit to settle to the new rms level increases. Therefore, lower
input levels allow the circuit to perform better (due to increased
averaging) but increase the waiting time between measurements. Obviously, when selecting C
computational accuracy and settling time is required.
AV
, a trade-off between
AV
Rev. F | Page 10 of 16
AD736
RAPID SETTLING TIMES VIA THE AVERAGE
RESPONDING CONNECTION
Because the average responding connection shown in Figure 19
does not use the C
averaging capacitor, its settling time does
AV
not vary with input signal level. It is determined solely by the
RC time constant of C
and the internal 8 kΩ resistor in the
F
output amplifier’s feedback path.
C
C
10µF
+
(OPTIONAL)
8kΩ
C
1
C
V
IN
2
V
IN
C
F
3
–V
S
–V
S
4
INPUT
AMPLIFIER
BIAS
SECTION
POSITIVE SUPPLY
COMMON
NEGATIVE SUPPLY
FULL
WAVE
RECTIFIER
rms
CORE
C
33µF
AD736
8kΩ
OUTPUT
AMPLIFIER
+
F
0.1µF
0.1µF
Figure 19. AD736 Average Responding Circuit
8
COM
+V
S
7
+V
S
OUTPUT
6
5
+V
S
–V
S
V
OUT
C
AV
00834-F-018
DC ERROR, OUTPUT RIPPLE, AND AVERAGING
ERROR
Figure 20 shows the typical output waveform of the AD736 with
a sine wave input applied. As with all real-world devices, the
ideal output of V
output contains both a dc and an ac error component.
As shown, the dc error is the difference between the average of
the output signal (when all the ripple in the output has been
removed by external filtering) and the ideal dc output. The dc
error component is therefore set solely by the value of the averaging capacitor used—no amount of post filtering (i.e., using a
very large C
value. The ac error component, an output ripple, may be easily
removed by using a large enough post-filtering capacitor, C
In most cases, the combined magnitudes of both the dc and ac
error components need to be considered when selecting appropriate values for capacitors C
representing the maximum uncertainty of the measurement, is
termed the averaging error and is equal to the peak value of the
output ripple plus the dc error.
= VIN is never achieved exactly. Instead, the
OUT
) will allow the output voltage to equal its ideal
F
and CF. This combined error,
AV
.
F
E
O
IDEAL
E
O
DC ERROR = EO– EO (IDEAL)
DOUBLE-FREQUENCY
RIPPLE
AVERAGE E
= E
O
O
00834-F-019
TIME
Figure 20. Output Waveform for Sine Wave Input Voltage
As the input frequency increases, both error components
decrease rapidly; if the input frequency doubles, the dc error
and ripple reduce to one quarter and one half of their original
values, respectively, and rapidly become insignificant.
AC MEASUREMENT ACCURACY AND CREST
FAC TO R
The crest factor of the input waveform is often overlooked
when determining the accuracy of an ac measurement. Crest
factor is defined as the ratio of the peak signal amplitude to the
rms amplitude (crest factor = V
/V rms). Many common
PEAK
waveforms, such as sine and triangle waves, have relatively low
crest factors (≤2). Other waveforms, such as low duty cycle
pulse trains and SCR waveforms, have high crest factors. These
types of waveforms require a long averaging time constant (to
average out the long time periods between pulses). Figure 8
shows the additional error versus the crest factor of the AD736
for various values of C
.
AV
SELECTING PRACTICAL VALUES FOR INPUT
COUPLING (C
(C
) CAPACITORS
F
Table 4 provides practical values of CAV and CF for several
common applications.
The input coupling capacitor, C
internal input scaling resistor, determines the −3 dB low
frequency roll-off. This frequency, F
Note that at F
(–3 dB) of reading. To reduce this error to 0.5% of reading,
choose a value of C
frequency to be measured.
In addition, if the input voltage has more than 100 mV of dc
offset, then the ac-coupling network shown in Figure 23 should
be used in addition to capacitor C
), AVERAGING (CAV), AND FILTERING
C
, in conjunction with the 8 kΩ
C
, is equal to
L
=
F
L
π
, the amplitude error is approximately −30%
L
that sets FL at one-tenth of the lowest
C
1
FaradsinCofValueThe
C
.
C
))(000,8(2
Rev. F | Page 11 of 16
AD736
Table 4. Capacitor Selection Chart
Low Frequency
Application RMS Input Level
Cutoff (−3 dB)
General-Purpose rms Computation 0 V to 1 V 20 Hz 5 150 10 360 ms
200 Hz 5 15 1 36 ms
0 mV to 200 mV 20 Hz 5 33 10 360 ms
200 Hz 5 3.3 1 36 ms
General-Purpose 0 V to 1 V 20 Hz None 33 1.2 sec
Average 200 Hz None 3.3 120 ms
Responding 0 mV to 200 mV 20 Hz None 33 1.2 sec
200 Hz None 3.3 120 ms
SCR Waveform Measurement 0 mV to 200 mV 50 Hz 5 100 33 1.2 sec
60 Hz 5 82 27 1.0 sec
0 mV to 100 mV 50 Hz 5 50 33 1.2 sec
60 Hz 5 47 µF 27 µF 1.0 sec
Audio Applications
Speech 0 mV to 200 mV 300 Hz 3 1.5 µF 0.5 µF 18 ms
Music 0 mV to 100 mV 20 Hz 10 100 µF 68 µF 2.4 sec
6
Settling time is specified over the stated rms input level with the input signal increasing from zero. Settling times are greater for decreasing amplitude input signals.
Max Crest
Factor
C
AV
(µF)
CF
(µF)
Settling Time
6
to 1%
Rev. F | Page 12 of 16
AD736
APPLICATION CIRCUITS
OPTIONAL
AC COUPLING
CAPACITOR
V
IN
0.01µF
1kV
200mV
9M
Ω
2V
900k
Ω
20V
90k
Ω
200V
10k
Ω
3
–IN
2
+IN
INPUT IMPEDANCE: 10
INPUT IMPEDANCE: 10pF
8kΩ
C
1
C
V
IN
2
C
F
3
–V
S
–V
S
4
INPUT
AMPLIFIER
BIAS
SECTION
47kΩ
1W
+V
–V
S
1N4148
1N4148
S
1µF
Figure 21. AD736 with a High Impedance Input Attenuator
C
AD711
6
10µF
C
C
C
8kΩ
+
1
V
IN
2
12
Ω
C
F
3
–V
S
–V
S
4
INPUT
AMPLIFIER
BIAS
SECTION
WAVE
RECTIFIER
rms
CORE
FULL
WAVE
RECTIFIER
rms
CORE
C
10µF
+
FULL
C
AV
33µF
C
10µF
C
+
+
F
(OPTIONAL)
AD736
AMPLIFIER
(OPTIONAL)
AD736
8kΩ
OUTPUT
AMPLIFIER
8kΩ
OUTPUT
8
+V
S
7
OUTPUT
6
C
AV
5
8
+V
S
7
OUTPUT
6
C
AV
5
COM
1µF
COM
1µF
+V
S
OUTPUT
+V
S
OUTPUT
00834-F-020
+
C
1µF
AV
33µF
C
10µF
+
F
(OPTIONAL)
00834-F-021
Figure 22. Differential Input Connection
Rev. F | Page 13 of 16
AD736
V
DC-COUPLED
V
IN
AC-COUPLED
1MΩ
0.1µF
IN
0.1µF
+V
–V
1MΩ
S
S
1MΩ
39MΩ
OUTPUT
V
OS
ADJUST
C
V
–V
V
IN
V
C
C
10µF
+
8kΩ
C
1
C
V
IN
2
C
F
3
–V
S
–V
S
4
INPUT
AMPLIFIER
BIAS
SECTION
FULL
WAVE
RECTIFIER
rms
CORE
+
C
1µF
Figure 23. External Output V
33µF
C
10µF
AV
+
F
OS
C
C
10µF
+
C
8kΩ
1
IN
2
C
F
3
S
4
INPUT
AMPLIFIER
BIAS
SECTION
FULL
WAVE
RECTIFIER
rms
CORE
AD736
8kΩ
OUTPUT
AMPLIFIER
+
C
F
10µF
(OPTIONAL)
Figure 24. Battery-Powered Option
CCC
C
8kΩ
+
1
2
IN
3
INPUT
AMPLIFIER
FULL
WAVE
RECTIFIER
AD736
Figure 25. Low Z, AC-Coupled Input Connection
(OPTIONAL)
AD736
8kΩ
OUTPUT
AMPLIFIER
(OPTIONAL)
Adjustment
8
7
6
C
5
8
7
6
COM
V
2
+V
S
OUTPUT
AV
+
33µF
COM
+V
S
OUTPUT
S
8
COM
+V
S
7
OUTPUT
6
C
AV
5
100kΩ
100kΩ
+V
S
1µF
OUTPUT
00834-F-022
4.7µF
9V
4.7µF
00834-F-023
00834-F-024
Rev. F | Page 14 of 16
AD736
C
R
N
OUTLINE DIMENSIONS
0.375 (9.53)
0.365 (9.27)
0.355 (9.02)
8
1
0.100 (2.54)
0.180
(4.57)
MAX
0.150 (3.81)
0.130 (3.30)
0.110 (2.79)
0.022 (0.56)
0.018 (0.46)
0.014 (0.36)
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
ONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETERS DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FO
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIG
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
5.00 (0.1968)
4.80 (0.1890)
85
1.27 (0.0500)
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDS MS-012AA
BSC
6.20 (0.2440)
5.80 (0.2284)
41
1.75 (0.0688)
1.35 (0.0532)
0.51 (0.0201)
0.31 (0.0122)
0.25 (0.0098)
0.17 (0.0067)
8°
0°
0.50 (0.0196)
0.25 (0.0099)
1.27 (0.0500)
0.40 (0.0157)
× 45°
Figure 28. 8-Lead Standard Small Outline Package [SOIC] Narrow Body
(R-8)
Dimensions shown in millimeters and (inches)
ORDERING GUIDE
Model Temperature Range Package Description Package Option
AD736JN 0°C to +70°C PDIP N-8
AD736KN 0°C to +70°C PDIP N-8
AD736AQ –40°C to +85°C CERDIP Q-8
AD736BQ –40°C to +85°C CERDIP Q-8
AD736AR –40°C to +85°C SOIC R-8
AD736AR-Reel –40°C to +85°C SOIC R-8
AD736AR-Reel-7 –40°C to +85°C SOIC R-8
AD736BR –40°C to +85°C SOIC R-8
AD736BR-Reel –40°C to +85°C SOIC R-8
AD736BR-Reel-7 –40°C to +85°C SOIC R-8
AD736JR 0°C to +70°C SOIC R-8
AD736JR-Reel 0°C to +70°C SOIC R-8
AD736JR-Reel-7 0°C to +70°C SOIC R-8
AD736JRZ1 0°C to +70°C SOIC R-8
AD736JRZ-RL1 0°C to +70°C SOIC R-8
AD736JRZ-R71 0°C to +70°C SOIC R-8
AD736KR 0°C to +70°C SOIC R-8
AD736KR-Reel 0°C to +70°C SOIC R-8
AD736KR-Reel-7 0°C to +70°C SOIC R-8
AD736KRZ1 0°C to +70°C SOIC R-8
AD736KRZ-RL1 0°C to +70°C SOIC R-8
AD736KRZ-R71 0°C to +70°C SOIC R-8