FEATURES
EASY TO USE
Pin-Strappable Gains of 10 and 100
All Errors Specified for Total System Performance
Higher Performance than Discrete In Amp Designs
Available in 8-Lead DIP and SOIC
Low Power, 1.3 mA Max Supply Current
Wide Power Supply Range (ⴞ2.3 V to ⴞ18 V)
EXCELLENT DC PERFORMANCE
0.15% Max, Total Gain Error
ⴞ5 ppm/ⴗC, Total Gain Drift
125 V Max, Total Offset Voltage
1.0 V/ⴗC Max, Offset Voltage Drift
LOW NOISE
9 nV/√Hz, @ 1 kHz, Input Voltage Noise
0.28 V p-p Noise (0.1 Hz to 10 Hz)
EXCELLENT AC SPECIFICATIONS
800 kHz Bandwidth (G = 10), 200 kHz (G = 100)
12 s Settling Time to 0.01%
APPLICATIONS
Weigh Scales
Transducer Interface and Data Acquisition Systems
Industrial Process Controls
Battery-Powered and Portable Equipment
PRODUCT DESCRIPTION
The AD621 is an easy to use, low cost, low power, high accuracy instrumentation amplifier that is ideally suited for a wide
range of applications. Its unique combination of high performance, small size and low power, outperforms discrete in amp
implementations. High functionality, low gain errors, and low
30,000
25,000
3OPAMP
20,000
INAMP
OP07S)
(3
Instrumentation Amplifier
AD621
CONNECTION DIAGRAM
8-Lead Plastic Mini-DIP (N), Cerdip (Q)
and SOIC (R) Packages
–IN
+IN
S
1
2
AD621
TOP VIEW
3
(Not to Scale)
4
G = 10/100
gain drift errors are achieved by the use of internal gain setting
resistors. Fixed gains of 10 and 100 can easily be set via external
pin strapping. The AD621 is fully specified as a total system,
therefore, simplifying the design process.
For portable or remote applications, where power dissipation,
size, and weight are critical, the AD621 features a very low
supply current of 1.3 mA max and is packaged in a compact
8-lead SOIC, 8-lead plastic DIP or 8-lead cerdip. The AD621
also excels in applications requiring high total accuracy, such
as precision data acquisition systems used in weigh scales and
transducer interface circuits. Low maximum error specifications
including nonlinearity of 10 ppm, gain drift of 5 ppm/°C, 50 µV
offset voltage, and 0.6 µV/°C offset drift (“B” grade), make
possible total system performance at a lower cost than has been
previously achieved with discrete designs or with other monolithic instrumentation amplifiers.
When operating from high source impedances, as in ECG and
blood pressure monitors, the AD621 features the ideal combination of low noise and low input bias currents. Voltage noise is
specified as 9 nV/√Hz at 1 kHz and 0.28 µV p-p from 0.1 Hz to
10 Hz. Input current noise is also extremely low at 0.1 pA/√Hz.
The AD621 outperforms FET input devices with an input bias
current specification of 1.5 nA max over the full industrial temperature range.
10,000
8
G = 10/100
7
+V
6
OUTPUT
5
REF–V
S
15,000
10,000
5,000
TOTAL ERROR, ppm OF FULL SCALE
0
0205
AD621A
1015
SUPPLY CURRENT – mA
Figure 1. Three Op Amp IA Designs vs. AD621
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.
1,000
TYPICAL STANDARD
BIPOLAR INPUT
IN AMP
10
1
1k100M10k
AD621 SUPERETA
BIPOLAR INPUT
IN AMP
100k10M
SOURCE RESISTANCE – ⍀
1M
TOTAL INPUT VOLTAGE NOISE, G = 100 – Vp-p
100
(0.1 – 10Hz)
0.1
Figure 2. Total Voltage Noise vs. Source Resistance
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.
ESD (electrostatic discharge) sensitive device. Electrostatic
charges as high as 4000 volts, which readily accumulate on the
human body and on test equipment, can discharge without
detection. Although the AD621 features proprietary ESD protection circuitry, permanent damage may still occur on these
devices if they are subjected to high energy electrostatic discharges. Therefore, proper ESD precautions are recommended
to avoid any performance degradation or loss of functionality.
ORDERING GUIDE
TemperaturePackagePackage
ModelRangeDescriptionOption
1
AD621AN–40°C to +85°C 8-Lead Plastic DIPN-8
AD621BN–40°C to +85°C 8-Lead Plastic DIPN-8
AD621AR–40°C to +85°C 8-Lead Plastic SOIC R-8
AD621BR– 40°C to +85°C 8-Lead Plastic SOIC R-8
AD621SQ/883B
2
–55°C to +125°C 8-Lead CerdipQ-8
AD621ACHIPS –40°C to +85°C Die
NOTES
1
N = Plastic DIP; Q = Cerdip; R = SOIC.
2
See Analog Devices’ military data sheet for 883B specifications.
RG 8
RG 1
METALIZATION PHOTOGRAPH
Dimensions shown in inches and (mm).
Contact factory for latest dimensions.
1.125 (3.57)
–IN
+V
S
7
2
+IN
3
OUTPUT
6
5
REFERENCE
0.0708
(2.545)
4 –V
S
–4–
REV. B
Page 5
Typical Performance Characteristics–AD621
WARM-UP TIME – Minutes
2.0
0
051
CHANGE IN OFFSET VOLTAGE – V
23
1.5
1.0
0.5
4
FREQUENCY – Hz
1000
100
1
1100k10
VOLTAGE NOISE – nV/ Hz
1001k10k
10
GAIN = 10
GAIN = 100
50
SAMPLE SIZE = 90
40
30
20
PERCENTAGE OF UNITS
10
0
–200–100
INPUT OFFSET VOLTAGE – V
0+100+200
TPC 1. Typical Distribution of V
50
SAMPLE SIZE = 90
40
30
Gain = 10
OS,
50
SAMPLE SIZE = 90
40
30
20
PERCENTAGE OF UNITS
10
0
–800–400
INPUT BIAS CURRENT – pA
0+400+800
TPC 4. Typical Distribution of Input Bias Current
20
PERCENTAGE OF UNITS
10
0
–80–40
INPUT OFFSET VOLTAGE – V
0+40+80
TPC 2. Typical Distribution of VOS, Gain = 100
50
SAMPLE SIZE = 90
40
30
20
PERCENTAGE OF UNITS
10
0
–400–200
INPUT OFFSET CURRENT – pA
0+200+400
TPC 3. Typical Distribution of Input Offset Current
TPC 5. Change in Input Offset Voltage vs. Warm-Up Time
TPC 6. Voltage Noise Spectral Density
REV. B
–5–
Page 6
AD621
1000
100
CURRENT NOISE – nV/ Hz
10
1
10
FREQUENCY – Hz
100
1000
TPC 7. Current Noise Spectral Density vs. Frequency
100
100mV
90
10
0%
1s
TPC 9. 0.1 Hz to 10 Hz Current Noise, 5 pA per Vertical
Div, 1 Second per Horizontal Div
100,000
10,000
1000
FET INPUT
IN AMP
RTI NOISE – 0.2V/div
TIME – 1 sec/div
TPC 8a. 0.1 Hz to 10 Hz RTI Voltage Noise, Gain = 10
RTI NOISE – 0.1V/div
TIME – 1 sec/div
100
TOTAL DRIFT FROM 25ⴗC TO 85ⴗC, RTI – V
10
1k10M
10k1M100k
SOURCE RESISTANCE – ⍀
TPC 10. Total Drift vs. Source Resistance
160
GAIN = 100
140
120
GAIN = 10
100
80
CMR – dB
60
40
20
0
0.11M1101001k10k100k
FREQUENCY – Hz
AD621A
TPC 8b. 0.1 Hz to 10 Hz RTI Voltage Noise, G = 100
TPC 11. CMR vs. Frequency, RTI, for a Zero to 1 k
Source Imbalance
–6–
Ω
REV. B
Page 7
PSR – dB
OUTPUT VOLTAGE – Volts p-p
FREQUENCY – Hz
35
0
1M
15
5
10k
10
1k
30
20
25
100k
G = 10 & 100
INPUT VOLTAGE LIMIT – Volts
(REFERRED TO SUPPLY VOLTAGES)
20
+1.0
+0.5
50
+1.5
–1.5
–1.0
–0.5
1510
SUPPLY VOLTAGE ⴞ Volts
–0.0
+0.0
+V
S
–V
S
INPUT VOLTAGE LIMIT – Volts
(REFERRED TO SUPPLY VOLTAGES)
20
+1.0
+0.5
50
+1.5
–1.5
–1.0
–0.5
1510
SUPPLY VOLTAGE ⴞ Volts
–0.0
+0.0
+V
S
–V
S
RL = 10k⍀
RL = 2k⍀
RL = 10k⍀
RL = 2k⍀
180
160
140
120
100
AD621
G = 100
G = 10
80
60
40
20
0.1
1
FREQUENCY – Hz
100k10k1k10010
1M
TPC 12. Positive PSR vs. Frequency
180
160
G = 100
G = 10
1
FREQUENCY – Hz
PSR – dB
140
120
100
80
60
40
20
0.1
TPC 13. Negative PSR vs. Frequency
1000
100
TPC 15. Large Signal Frequency Response
1M
100k10k1k10010
TPC 16. Input Voltage Range vs. Supply Voltage
10
1
CLOSED-LOOP GAIN – V/V
REV. B
0.1
10010M
TPC 14. Closed-Loop Gain vs. Frequency
1k
FREQUENCY – Hz
100k1M10k
TPC 17. Output Voltage Swing vs. Supply Voltage,
G = 10
–7–
Page 8
AD621
30
VS = ⴞ 15V
G = 10
20
10
OUTPUT VOLTAGE SWING – Volts p-p
0
0
1001k
LOAD RESISTANCE – ⍀
10k
TPC 18. Output Voltage Swing vs. Resistive Load
5V1mV
100
90
10s
5V1mV
100
90
10
0%
10s
TPC 21. Large Signal Pulse Response and Settling
Time, G = 100 (0.5 mV = 0.1%), R
20mV
100
90
= 2 kΩ, CL = 100 pF
L
10s
10
0%
TPC 19. Large Signal Pulse Response and Settling
10s
= 1 kΩ,
L
Time Gain, G = 10 (0.5 mV = 0.01%), R
C
= 100 pF
L
20mV
100
90
10
0%
10
0%
TPC 22. Small Signal Pulse Response, G = 100,
R
= 2 kΩ, CL = 100 pF
L
20
15
10
SETTLING TIME – s
5
0
020
5
TO 0.01%
OUTPUT STEP SIZE – Volts
1015
TO 0.1%
TPC 20. Small Signal Pulse Response, G = 10,
= 1 kΩ, CL = 100 pF
R
L
–8–
TPC 23. Settling Time vs. Step Size, G = 10
REV. B
Page 9
AD621
20
TO 0.01%
15
10
SETTLING TIME – s
5
0
020
5
OUTPUT STEP SIZE – Volts
10
TPC 24. Settling Time vs. Step Size, Gain = 100
TO 0.1%
15
TPC 27. Gain Nonlinearity, G = 10, RL = 10 kΩ, Vertical
100
90
10
0%
Scale: 100
100V
µ
V/Div = 100 ppm/Div, Horizontal Scale:
2 Volts/Div
2.0
INPUT CURRENT – nA
1.5
1.0
0.5
–0.5
–1.0
–I
0
B
+I
B
100k⍀
INPUT
20V p-p
1%
G = 10 G = 100
11k⍀
0.1%
1k⍀
0.1%
G = 10
G = 100
10k⍀
1%
–
AD621
+
2V
1k⍀
+V
S
10T
10k⍀
1%
V
OUT
–1.5
–2.0
–125
–75
TEMPERATURE – ⴗC
1257525–25
TPC 25. Input Bias Current vs. Temperature
0PW 0
100
90
10
0%
0 WFM
VZR 0
100V
2V
20 WFM AQR WARNING
TPC 26. Gain Nonlinearity, G = 100, RL = 10 kΩ,
= 0 pF. Vertical Scale: 100 µV/Div = 100 ppm/Div
C
L
Horizontal Scale: 2 Volts/Div
175
–V
S
TPC 28. Settling Time Test Circuit
REV. B
–9–
Page 10
AD621
+V
S
7
I120A
R3
–IN
400⍀
2
Q1
Figure 3. Simplified Schematic of AD621
THEORY OF OPERATION
The AD621 is a monolithic instrumentation amplifier based on
a modification of the classic three op amp circuit. Careful layout
of the chip, with particular attention to thermal symmetry builds
in tight matching and tracking of critical components, thus
preserving the high level of performance inherent in this circuit,
at a low price.
On chip gain resistors are pretrimmed for gains of 10 and 100.
The AD621 is preset to a gain of 10. A single external jumper
(between Pins 1 and 8) is all that is needed to select a gain of
100. Special design techniques assure a low gain TC of 5 ppm/°C
max, even at a gain of 100.
Figure 3 is a simplified schematic of the AD621. The input
transistors Q1 and Q2 provide a single differential-pair bipolar
input for high precision, yet offer 10× lower Input Bias Current,
thanks to Superβeta processing. Feedback through the Q1-A1-R1
loop and the Q2-A2-R2 loop maintains constant collector current of the input devices Q1 and Q2, thereby impressing the
input voltage across the gain-setting resistor, RG, which equals
V
B
+–+
–
A1
C1C2
R1 25k⍀
R6
555.6⍀
G = 100
R5
5555.6⍀
8
1
4
–V
S
A2
R2 25k⍀
G = 100
Q2
I220A
10k⍀
10k⍀
10k⍀
R4
400⍀
3
–
A3
+
10k⍀
+IN
OUTPUT
6
REF
5
R5 at a gain of 10 or the parallel combination of R5 and R6 at a
gain of 100.
This creates a differential gain from the inputs to the A1/A2
outputs given by G = (R1 + R2) / RG + 1. The unity-gain
subtracter A3 removes any common-mode signal, yielding a
single-ended output referred to the REF pin potential.
The value of RG also determines the transconductance of the
preamp stage. As RG is reduced for larger gains, the transconductance increases asymptotically to that of the input transistors.
This has three important advantages: (a) Open-loop gain is
boosted for increasing programmed gain, thus reducing gainrelated errors. (b) The gain-bandwidth product (determined by
C1, C2 and the preamp transconductance) increases with programmed gain, thus optimizing frequency response. (c) The
input voltage noise is reduced to a value of 9 nV/√Hz, determined mainly by the collector current and base resistance of the
input devices.
Make vs. Buy: A Typical Bridge Application Error Budget
The AD621 offers improved performance over discrete three op
amp IA designs, along with smaller size, fewer components and
10 times lower supply current. In the typical application, shown
in Figure 4, a gain of 100 is required to amplify a bridge output of
20 mV full scale over the industrial temperature range of –40°C to
+85°C. The error budget table below shows how to calculate
the effect various error sources have on circuit accuracy.
Regardless of the system it is being used in, the AD621 provides
greater accuracy, and at low power and price. In simple systems,
absolute accuracy and drift errors are by far the most significant
contributors to error. In more complex systems with an intelligent
processor, an autogain/autozero cycle will remove all absolute
accuracy and drift errors leaving only the resolution errors of
gain nonlinearity and noise, thus allowing full 14-bit accuracy.
Note that for the discrete circuit, the OP07 specifications for
input voltage offset and noise have been multiplied by 2. This is
because a three op amp type in amp has two op amps at its inputs,
both contributing to the overall input error.
10V
R = 350⍀
R = 350⍀
PRECISION BRIDGE TRANSDUCER
R = 350⍀
R = 350⍀
+
AD621A
–
REFERENCE
AD621A MONOLITHIC
INSTRUMENTATION
AMPLIFIER, G = 100
Figure 5. A Pressure Monitor Circuit which Operates on a 5 V Power Supply
Pressure Measurement
Although useful in many bridge applications such as weigh-scales,
the AD621 is especially suited for higher resistance pressure
sensors powered at lower voltages where small size and low
power become more even significant.
Figure 5 shows a 3 kΩ pressure transducer bridge powered from
5 V. In such a circuit, the bridge consumes only 1.7 mA. Adding
the AD621 and a buffered voltage divider allows the signal to be
conditioned for only 3.8 mA of total supply current.
Small size and low cost make the AD621 especially attractive for
voltage output pressure transducers. Since it delivers low noise
and drift, it will also serve applications such as diagnostic noninvasion blood pressure measurement.
Wide Dynamic Range Gain Block Suppresses Large CommonMode and Offset Signals
The AD621 is especially useful in wide dynamic range applications such as those requiring the amplification of signals in the
20k⍀
REF
IN
DIGITAL
DATA
AGND
ADC
OUTPUT
10k⍀
20k⍀
+
AD705
–
0.6mA
MAX
presence of large, unwanted common-mode signals or offsets.
Many monolithic in amps achieve low total input drift and noise
errors only at relatively high gains (~100). In contrast the AD621’s
low output errors allow such performance at a gain of 10, thus
allowing larger input signals and therefore greater dynamic
range. The circuit of Figure 6 (±15 V supply, G = 10) has
only 2.5 µV/°C max. V
drift and 0.55 µ/V p-p typical 0.1 Hz
OS
to 10 Hz noise, yet will amplify a ±0.5 V differential signal while
suppressing a ±10 V common-mode signal, or it will amplify a
±1.25 V differential signal while suppressing a 1 V offset by use
of the DAC driving the reference pin of the AD621. An added
benefit, the offsetting DAC connected to the reference pin allows
removal of a dc signal without the associated time-constant
of ac coupling. Note the representations of a differential and
common-mode signal shown in Figure 6 such that a single-ended
(or normal mode) signal of 1 V would be composed of a 0.5 V
common-mode component and a 1 V differential component.
Table I. Make vs. Buy Error Budget
AD621 CircuitDiscrete CircuitError, ppm of Full Scale
Gain Nonlinearity, ppm of Full Scale40 ppm40 ppm12,14012,140
Typ 0.1 Hz–10 Hz Voltage Noise, µV p-p 0.28 µV p-p/20 mV(0.38 µV p-p × √2)120 mV121,1412,127
Total Resolution Error121,54121,67
Grand Total Error11,47236,008
G = 100, VS = ±15 V.
(All errors are min/max and referred to input.)
REV. B
–11–
Page 12
AD621
INPUT A:
ⴞ10V CM
V
COM
ⴞ10V–
INPUT B:
OFFSET
+
ⴞ1V
+
V
DIFF
ⴞ0.5V
–
+
+ V
V
DIFF
ⴞ(1.25V + 1V)
–
–
+
OPTIONAL
10k⍀
10k⍀
R
–
ⴛ10
AD621
+
TO
V
OUT1
–
ⴛ10
AD621
+
0 TO ⴞ10V
OFFSET
USE THIS IN PLACE OF THE DAC FOR ZERO SUPPRESSION FUNCTION.
TO
REF
V
G = 10
DAC
AD548
OUT1
C
V
OUT2
TOTAL GAIN = 100
Figure 6. Suppressing a Large Common-Mode or Offset Voltage in Order to Measure a Small Differential Signal
= ±15 V)
(V
S
The AD621, as well as many other monolithic instrumentation
amplifiers, is based on the “three op amp” in amp circuit (Figure 7) amplifier. Since the input amplifiers (A1 and A2) have a
common-mode gain of unity and a differential gain equal to the
set gain of the overall in amp, the voltages V1 and V2 are defined
by the equations
V
= VCM + G × V
1
V
= VCM – G × V
2
DIFF
DIFF
/2
/2
The common-mode voltage will drive the outputs of amplifiers
A1 and A2 to the differential-signal voltage, multiplied by the
gain, spreads them apart. For a 10 V common-mode 0.1 V
differential input, V1 would be at 10.5 V and V2 at 9.5 V.
INPUT AMPLIFIER
DIFFERENTIAL GAIN = 10
COMMON MODE GAIN = 1
+
A1
–
20k⍀
4.44k⍀
20k⍀
–
A2
+
V1
V2
OUTPUT AMPLIFIER
DIFFERENTIAL GAIN = 1
COMMON MODE GAIN = 1/1000
10k⍀
10k⍀
–
A3
+
10k⍀
10k⍀
Figure 7. Typical Three Op Amp Instrumentation
Amplifier, Differential Gain = 10
The AD621’s input amplifiers can provide output voltage within
2.5 V of the supplies. To avoid saturation of the input amplifier
the input voltage must therefore obey the equations:
V
CM
V
CM
+ G × V
– G × V
/2 ≤ (Upper Supply – 2.5 V)
DIFF
/2 ≥ (Lower Supply + 2.5 V)
DIFF
Figure 8 shows the trade-off between common-mode and
differential-mode input for ±15 V supplies and G = 10.
By cascading with use of the optional AD621, the circuit of
Figure 6 will provide ±1 V of zero suppression at gains of 10
and 100 (at V
OUT1
and V
respectively) with maximum TCs
OUT2
of ±4 ppm/°C and ± 8 ppm/°C, respectively. Therefore, depending on the magnitude of the differential input signal, either
V
OUT1
or V
– ⴞVolts
DIFF
V
may be used as the output.
OUT2
1.2
1.0
0.8
0.6
0.4
0.2
0
0102
48
6
VCM – ⴞVolts
12
Figure 8. Trade-Off Between VCM and V
±
15 V, G = 10), for Reference Pin at Ground
–12–
Range (VS =
DIFF
REV. B
Page 13
AD621
Precision V-I Converter
The AD621 along with another op amp and two resistors make
a precision current source (Figure 9). The op amp buffers the
reference terminal to maintain good CMR. The output voltage
of the AD621 appears across R1 which converts it to a cur-
V
X
rent. This current less only the input bias current of the op amp
then flows out to the load.
+V
S
AD705
R1
+V
X–
I
L
LOAD
V
IN+
AD621
V
IN–
–V
S
) – (V
IL =
(V
V
X
IN+
=
R1
) G
IN–
R1
Figure 9. Precision Voltage to Current Converter
±
(Operates on 1.8 mA,
3 V)
INPUT AND OUTPUT OFFSET VOLTAGE
The AD621 is fully specified for total input errors at gains of 10
and 100. That is, effects of all error sources within the AD621
are properly included in the guaranteed input error specs, eliminating the need for separate error calculation.
Although usually grounded, the reference terminal may be used
to offset the output of the AD621. This is useful when the load
is “floating” or does not share a ground with the rest of the system.
It also provides a direct means of injecting a precise offset.
Another benefit of having a reference terminal is that it can be
quite effective in eliminating ground loops and noise in a circuit
or system.
+V
S
INPUT OVERLOAD CONSIDERATIONS
Failure of a transducer, faults on input lines, or power supply
sequencing can subject the inputs of an instrumentation amplifier to voltages well beyond their linear range, or even the supply
voltage, so it is essential that the amplifier handle these overloads without being damaged.
The AD621 will safely withstand continuous input overloads of
±3.0 volts (±6.0 mA). This is true for gains of 10 and 100, with
power on or off.
The inputs of the AD621 are protected by high current capacity
dielectrically isolated 400 Ω thin-film resistors R3 and R4 (Figure 3) and by diodes which protect the input transistors Q1 and
Q2 from reverse breakdown. If reverse breakdown occurred, there
would be a permanent increase in the amplifier’s input current.
The input overload capability of the AD621 can be easily increased
while only slightly degrading the noise, common-mode rejection
and offset drift of the device by adding external resistors in series
with the amplifier’s inputs as shown in Figure 10.
Table II summarizes the overload voltages and total input
noise for a range of range of r values. Note that a 2 kΩ resistor in series with each input will protect the AD621 from a
±15 volt continuous overload, while only increasing input noise
to 13 nV√Hz—about the same level as would be expected from
a typical unprotected 3 op amp in amp.
Table II. Input Overload Protection vs. Value of Resistor R
P
Total Input NoiseMaximum Continuous
Value ofin nV√Hz @ 1 kHzOverload Voltage, V
OL
Resistor RPG = 10G = 100In Volts
01493
499 Ω14106
1.00 kΩ14119
2.00 kΩ151315
3.01 kΩ*161421
4.99 kΩ*171633
*1/4 watt, 1% metal-film resistor. All others are 1/8 watt, 1% RN55
or equivalent.
REV. B
R
P
V
OL
R
V
P
OL
GAIN = 10 OR 100
AD621
–V
S
V
OUT
Figure 10. Input Overload Protection
–13–
Page 14
AD621
Gain Selection
The AD621 has accurate, low temperature coefficient (TC),
gains of 10 and 100 available. The gain of the AD621 is nominally set at 10; this is easily changed to a gain of 100 by simply
connecting a jumper between Pins 1 and 8.
555.5
⍀
R
EXT
5,555.5
⍀
AD621
Figure 11. Programming the AD621 for Gains Between
10 and 100
As shown in Figure 11, the device can be programmed for any
gain between 10 and 100 by connecting a single external resistor
between Pins 1 and 8. Note that adding the external resistor will
degrade both the gain accuracy and gain TC. Since the gain
equation of the AD621 yields:
+ 6,111.111)
9(R
G = 1 +
(R
X
X
+ 555. 555)
This can be solved for the nominal value of external resistor for
gains between 10 and 100:
(G – 1) 555.555 – 55,000
RX=
(10 – G )
Table III gives practical 1% resistor values for several common gains.
Table III. Practical 1% External Resistor
Values for Gains Between 10 and 100
The excellent performance of the AD621 at a gain of 10 makes
it a good choice to team up with the AD526 programmable gain
amplifier (PGA) to yield a differential input PGA with gains of
10, 20, 40, 80, 160. As shown in Figure 12, the low offset of the
AD621 allows total circuit offset to be trimmed using the offset
null of the AD526, with only a negligible increase in total drift
error. The total gain TC will be 9 ppm/°C max, with 2 µV/°C
typical input offset drift. Bandwidth is 600 kHz to gains of 10 to
80, and 350 kHz at G = 160. Settling time is 13 µs to 0.01%
for a 10 V output step for all gains.
+V
–
INPUTS
+
0.1F
–
AD621
+
–V
S
S
0.1F
G = 10
0.1F
+V
–
AD526
+
S
0.1F
OUTPUT
2
20k⍀
–V
S
Figure 12. A High Performance Programmable Gain
Amplifier
COMMON-MODE REJECTION
Instrumentation amplifiers like the AD621 offer high CMR
which is a measure of the change in output voltage when both
inputs arc changed by equal amounts. These specifications are
usually given for a full-range input voltage change and a specified source imbalance.
For optimal CMR, the reference terminal should be tied to a
low impedance point, and differences in capacitance and resistance should be kept to a minimum between the two inputs. In
many applications shielded cables are used to minimize noise,
and for best CMR over frequency the shield should he properly
driven. Figures 13 and 14 show active data guards that are configured to improve ac common-mode rejections by “bootstrapping”
the capacitances of input cable shields, thus minimizing the
capacitance mismatch between the inputs.
+V
100⍀
100⍀
AD648
–INPUT
100k⍀
100k⍀
+INPUT
–V
S
–
+
S
AD621
–V
S
V
REFERENCE
OUT
Figure 13. Differential Shield Driver, G = 10
+V
7
AD621
4
–V
S
S
6
5
REFERENCE
V
OUT
100⍀
– INPUT
AD548
+ INPUT
2
1
8
3
Figure 14. Common-Mode Shield Driver, G = 100
–14–
REV. B
Page 15
GROUNDING
Since the AD621 output voltage is developed with respect to the
potential on the reference terminal, it can solve many grounding problems by simply tying the REF pin to the appropriate
“local ground.”
In order to isolate low level analog signals from a noisy digital
environment, many data-acquisition components have separate
analog and digital ground pins (Figure 15). It would be convenient to use a single ground line; however, current through
ground wires and PC runs of the circuit card can cause hundreds
of millivolts of error. Therefore, separate ground returns should
be provided to minimize the current flow from the sensitive
points to the system ground. These ground returns must be tied
together at some point, usually best at the ADC package as shown.
ANALOG P.S.
+15VC–15V
DIGITAL P.S.
C
+5V
AD621
+V
S
–INPUT
LOAD
V
OUT
AD621
+INPUT
–V
S
REFERENCE
TO POWER SUPPLY GROUND
Figure 16a. Ground Returns for Bias Currents when Using
Transformer Input Coupling
+V
S
–INPUT
0.1F
7
2
AD621
3
4
5
0.1F
4
11
6
AD585
S/H
6
1F
7
1F1F
9
15
11
AD574A
ADC
+
1
DIGITAL
DATA
OUTPUT
Figure 15. Basic Grounding Practice
GROUND RETURNS FOR INPUT BIAS CURRENTS
Input bias currents are those currents necessary to bias the input
transistors of an amplifier. There must be a direct return path
for these currents; therefore when amplifying “floating” input
sources such as transformers, or ac-coupled sources, there must
be a dc path from each input to ground as shown in Figures 16a
through 16c. Refer to the Instrumentation Amplifier ApplicationGuide (free from Analog Devices) for more information regarding in amp applications.
+INPUT
AD621
–V
S
REFERENCE
TO POWER SUPPLY GROUND
LOAD
V
OUT
Figure 16b. Ground Returns for Bias Currents when Using
a Thermocouple Input
+V
S
–INPUT
+INPUT
100k⍀100k⍀
AD621
REFERENCE
–V
S
TO POWER SUPPLY GROUND
LOAD
V
OUT
Figure 16c. Ground Returns for Bias Currents when Using
AC Input Coupling
REV. B
–15–
Page 16
AD621
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
Plastic DIP (N-8) Package
0.165 0.01
(4.19
SEATING PLANE
0.125 (3.18)
0.005 (0.13) MIN0.055 (1.4) MAX
0.200
(5.08)
MAX
0.200 (5.08)
0.125 (3.18)
8
1
0.39 (9.91)
MAX
0.25)
MIN
0.018
0.003
(0.46
0.08)
0.033
(0.84)
NOM
Cerdip (Q-8) Package
58
41
0.405 (10.29) MAX
5
4
0.10
(2.54)
TYP
0.310 (7.87)
0.220 (5.59)
0.070 (1.78)
0.030 (0.76)
0.060 (1.52)
0.015 (0.38)
0.25
(6.35)
0.035 0.01
(0.89
0.18
(4.57
0.150
(3.81)
MIN
0.03
0.76)
0.31
(7.87)
0.25)
0 - 15
0.320 (8.13)
0.290 (7.37)
0.015 (0.38)
0.008 (0.20)
0.30 (7.62)
REF
0.011 0.003
0.76)
(4.57
C00776–0–1/01 (rev. B)
0.050 (1.27)
0.010 (0.25)
0.004 (0.10)
0.023 (0.58)
0.014 (0.36)
0.198 (5.03)
0.188 (4.77)
8
1
TYP
0.100 (2.54)
BSC
0 - 15
SEATING PLANE
SOIC (R-8) Package
5
0.158 (4.00)
0.150 (3.80)
0.244 (6.200)
4
0.228 (5.80)
0.018 (0.46)
0.014 (0.36)
0.094(2.39)
0.100 (2.59)
0.015 (0.38)
0.007 (0.18)
–16–
PRINTED IN U.S.A.
0.205 (5.20)
0.181 (4.60)
0.045 (1.15)
0.020 (0.50)
REV. B
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