(Gain range 1 to 10,000)
Wide power supply range (±2.3 V to ±18 V)
Higher performance than 3 op amp IA designs
Available in 8-lead DIP and SOIC packaging
Low power, 1.3 mA max supply current
Excellent dc performance (B grade)
50 µV max, input offset voltage
0.6 µV/°C max, input offset drift
1.0 nA max, input bias current
100 dB min common-mode rejection ratio (G = 10)
Low noise
9 nV/√Hz @ 1 kHz, input voltage noise
0.28 µV p-p noise (0.1 Hz to 10 Hz)
Excellent ac specifications
120 kHz bandwidth (G = 100)
15 µs settling time to 0.01%
APPLICATIONS
Weigh scales
ECG and medical instrumentation
Transducer interface
Data acquisition systems
Industrial process controls
Battery-powered and portable equipment
The AD620 is a low cost, high accuracy instrumentation
amplifier that requires only one external resistor to set gains of
1 to 10,000. Furthermore, the AD620 features 8-lead SOIC and
DIP packaging that is smaller than discrete designs and offers
lower power (only 1.3 mA max supply current), making it a
good fit for battery-powered, portable (or remote) applications.
The AD620, with its high accuracy of 40 ppm maximum
nonlinearity, low offset voltage of 50 µV max, and offset drift of
0.6 µV/°C max, is ideal for use in precision data acquisition
systems, such as weigh scales and transducer interfaces.
Furthermore, the low noise, low input bias current, and low power
of the AD620 make it well suited for medical applications, such
as ECG and noninvasive blood pressure monitors.
The low input bias current of 1.0 nA max is made possible with
the use of Superϐeta processing in the input stage. The AD620
works well as a preamplifier due to its low input voltage noise of
9 nV/√Hz at 1 kHz, 0.28 µV p-p in the 0.1 Hz to 10 Hz band,
and 0.1 pA/√Hz input current noise. Also, the AD620 is well
suited for multiplexed applications with its settling time of 15 µs
to 0.01%, and its cost is low enough to enable designs with one
in-amp per channel.
10,000
8
7
6
5
R
G
+V
S
OUTPUT
REF
00775-0-001
25,000
20,000
15,000
AD620A
10,000
R
G
5,000
TOTAL ERROR, PPM OF FULL SCALE
0
05101520
SUPPLY CURRENT (mA)
3 OP AMP
IN-AMP
(3 OP-07s)
00775-0-002
Figure 2. Three Op Amp IA Designs vs. AD620
Rev. G
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.
RTI VOLTAGE NOISE
1,000
100
V p-p)
µ
(0.1 – 10Hz) (
10
1
0.1
TYPICAL STANDARD
BIPOLAR INPUT
IN-AMP
G = 100
SOURCE RESISTANCE (Ω)
AD620 SUPERβETA
BIPOLAR INPUT
IN-AMP
Figure 3. Total Voltage Noise vs. Source Resistance
Ratio DC to 60 Hz with
1 kΩ Source Imbalance VCM = 0 V to ± 10 V
G = 1 73 90 80 90 73 90 dB
G = 10 93 110 100 110 93 110 dB
G = 100 110 130 120 130 110 130 dB
G = 1000 110 130 120 130 110 130 dB
OUTPUT
Output Swing RL = 10 kΩ
V
Overtemperature −VS + 1.4 +VS − 1.3
= ±2.3 V
S
to ± 5 V
VS = ±5 V
−VS +
+VS − 1.2
1.1
−VS + 1.2 +VS − 1.4
−VS + 1.1
−VS + 1.4
−VS + 1.2
+VS − 1.2 −VS + 1.1 +VS − 1.2 V
+VS − 1.3 −VS + 1.6 +VS − 1.3 V
+VS − 1.4 −VS + 1.2 +VS − 1.4 V
to ± 18 V
Overtemperature −VS + 1.6 +VS – 1.5
−VS + 1.6
+VS – 1.5 –VS + 2.3 +VS – 1.5 V
Short Circuit Current ±18 ±18 ±18 mA
DYNAMIC RESPONSE
Small Signal –3 dB Bandwidth
G = 1 1000 1000 1000 kHz
G = 10 800 800 800 kHz
G = 100 120 120 120 kHz
G = 1000 12 12 12 kHz
Slew Rate 0.75 1.2 0.75 1.2 0.75 1.2 V/µs
Settling Time to 0.01% 10 V Step
G = 1–100 15 15 15 µs
G = 1000 150 150 150 µs
NOISE
Voltage Noise, 1 kHz
Input, Voltage Noise, eni
Output, Voltage Noise, e
2
ni
9 13 9 13 9 13 nV/√Hz
72 100 72 100 72 100 nV/√Hz
no
2
)/()(GeeNoiseRTITotal
+=
no
RTI, 0.1 Hz to 10 Hz
G = 1 3.0 3.0 6.0 3.0 6.0 µV p-p
G = 10 0.55 0.55 0.8 0.55 0.8 µV p-p
G = 100–1000 0.28 0.28 0.4 0.28 0.4 µV p-p
Current Noise f = 1 kHz 100 100 100 fA/√Hz
0.1 Hz to 10 Hz 10 10 10 pA p-p
REFERENCE INPUT
RIN 20 20 20 kΩ
IIN V
, V
= 0 50 60 50 60 50 60 µA
IN+
REF
Voltage Range −VS + 1.6 +VS − 1.6 −VS + 1.6 +VS − 1.6 −VS + 1.6 +VS − 1.6 V
Gain to Output 1 ± 0.0001 1 ± 0.0001 1 ± 0.0001
POWER SUPPLY
Operating Range4
Quiescent Current VS = ±2.3 V
±2.3 ±18 ±2.3 ±18 ±2.3 ±18 V
0.9 1.3 0.9 1.3 0.9 1.3 mA
to ±18 V
Overtemperature 1.1 1.6 1.1 1.6 1.1 1.6 mA
TEMPERATURE RANGE
For Specified Performance
−40 to +85 −40 to +85 −55 to +125 °C
1
See Analog Devices military data sheet for 883B tested specifications.
2
Does not include effects of external resistor RG.
3
One input grounded. G = 1.
4
This is defined as the same supply range that is used to specify PSR.
Rev. G | Page 4 of 20
AD620
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Rating
Supply Voltage ±18 V
Internal Power Dissipation1 650 mW
Input Voltage (Common-Mode) ±VS
Differential Input Voltage 25 V
Output Short-Circuit Duration Indefinite
Storage Temperature Range (Q) −65°C to +150°C
Storage Temperature Range (N, R) −65°C to +125°C
Operating Temperature Range
AD620 (A, B) −40°C to +85°C
AD620 (S) −55°C to +125°C
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only; functional operation of the device at these or any
other condition s 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 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.
Figure 5. Typical Distribution of Input Offset Voltage
50
SAMPLE SIZE = 850
40
30
20
00775-0-005
2.0
1.5
1.0
0.5
0
–0.5
–1.0
INPUT BIAS CURRENT (nA)
–1.5
–2.0
2.0
1.5
1.0
+I
B
1257525–25
–75
–I
B
TEMPERATURE (°C)
Figure 8. Input Bias Current vs. Temperature
175
00775-0-008
PERCENTAGE OF UNITS
10
0
–12001200
–6000600
INPUT BIAS CURRENT (pA)
Figure 6. Typical Distribution of Input Bias Current
50
SAMPLE SIZE = 850
40
30
20
PERCENTAGE OF UNITS
10
0
–400
–2000200400
INPUT OFFSET CURRENT (pA)
Figure 7. Typical Distribution of Input Offset Current
00775-0-006
00775-0-007
0.5
CHANGE IN OFFSET VOLTAGE (µV)
0
01
WARM-UP TIME (Minutes)
432
5
Figure 9. Change in Input Offset Voltage vs. Warm-Up Time
1000
GAIN = 1
100
GAIN = 10
10
VOLTAGE NOISE (nV/ Hz)
GAIN = 100, 1,000
1
1100k
10
FREQUENCY (Hz)
GAIN = 1000
BW LIMIT
10k1k100
Figure 10. Voltage Noise Spectral Density vs. Frequency (G = 1−1000)
00775-0-009
00775-0-010
Rev. G | Page 7 of 20
AD620
1000
100
CURRENT NOISE (fA/ Hz)
10
1
10
FREQUENCY (Hz)
100
Figure 11. Current Noise Spectral Density vs. Frequency
V/DIV)
µ
RTI NOISE (2.0
TIME (1 SEC/DIV)
Figure 12. 0.1 Hz to 10 Hz RTI Voltage Noise (G = 1)
1000
00775-0-011
00775-0-012
Figure 14. 0.1 Hz to 10 Hz Current Noise, 5 pA/Div
100,000
V)
µ
10,000
C, RTI (
°
C TO 85
°
1000
100
TOTAL DRIFT FROM 25
10
1k10M
10k1M100k
SOURCE RESISTANCE (
FET INPUT
IN-AMP
Ω
)
Figure 15. Total Drift vs. Source Resistance
AD620A
00775-0-014
00775-0-015
V/DIV)
µ
RTI NOISE (0.1
TIME (1 SEC/DIV)
Figure 13. 0.1 Hz to 10 Hz RTI Voltage Noise (G = 1000)
00775-0-013
Rev. G | Page 8 of 20
160
140
120
100
CMR (dB)
G = 1000
G = 100
G = 10
G = 1
80
60
40
20
0
0.1
1
FREQUENCY (Hz)
100k10k1k10010
1M
Figure 16. Typical CMR vs. Frequency, RTI, Zero to 1 kΩ Source Imbalance
00775-0-016
AD620
180
160
140
120
100
PSR (dB)
80
60
40
20
0.1
1
FREQUENCY (Hz)
G = 1000
G = 100
G = 10
G = 1
100k10k1k10010
1M
00775-0-017
35
G = 10, 100, 1000
30
25
20
15
10
OUTPUT VOLTAGE (V p-p)
5
0
G = 1
G = 1000
1k
BW LIMIT
G = 100
10k
FREQUENCY (Hz)
100k
1M
00775-0-020
Figure 17. Positive PSR vs. Frequency, RTI (G = 1−1000)
180
160
140
120
100
PSR (dB)
80
60
40
20
0.1
1
FREQUENCY (Hz)
Figure 18. Negative PSR vs. Frequency, RTI (G = 1−1000)
1000
100
G = 1000
G = 100
G = 10
G = 1
100k10k1k10010
1M
00775-0-018
Figure 20. Large Signal Frequency Response
+VS–0.0
–0.5
–1.0
–1.5
+1.5
+1.0
INPUT VOLTAGE LIMIT (V)
(REFERRED TO SUPPLY VOLTAGES)
+0.5
+0.0
–V
S
50
SUPPLY VOLTAGE
± Volts
Figure 21. Input Voltage Range vs. Supply Voltage, G = 1
+V
–0.0
S
–0.5
–1.0
RL = 2k
–1.5
Ω
RL = 10k
1510
Ω
20
00775-0-021
10
GAIN (V/V)
1
0.1
10010M
1k
FREQUENCY (Hz)
100k1M10k
Figure 19. Gain vs. Frequency
00775-0-019
Rev. G | Page 9 of 20
OUTPUT VOLTAGE SWING (V)
(REFERRED TO SUPPLY VOLTAGES)
–V
+1.5
+1.0
+0.5
+0.0
S
0
5
SUPPLY VOLTAGE ± Volts
RL = 10k
RL = 2k
Ω
Ω
Figure 22. Output Voltage Swing vs. Supply Voltage, G = 10
1510
20
00775-0-022
AD620
30
VS = ±15V
G = 10
20
10
OUTPUT VOLTAGE SWING (V p-p)
0
0
1001k
LOAD RESISTANCE (
Ω)
Figure 23. Output Voltage Swing vs. Load Resistance
............................ ............
10k
00775-0-023
.................... ....................
.................... ....................
00775-0-026
Figure 26. Large Signal Response and Settling Time, G = 10 (0.5 mV = 0.01%)
........ ................................
............................ ............
Figure 24. Large Signal Pulse Response and Settling Time
G = 1 (0.5 mV = 0.01%)
.................... ....................
.................... ....................
Figure 25. Small Signal Response, G = 1, R
= 2 kΩ, CL = 100 pF
L
00775-0-024
00775-0-025
........ ................................
00775-0-027
Figure 27. Small Signal Response, G = 10, R
= 2 kΩ, CL = 100 pF
L
........................ ................
........................ ................
00775-0-030
Figure 28. Large Signal Response and Settling Time, G = 100 (0.5 mV = 0.01%)
Rev. G | Page 10 of 20
AD620
20
............................ ............
............................ ............
Figure 29. Small Signal Pulse Response, G = 100, R
........................ ................
........................ ................
00775-0-029
= 2 kΩ, CL = 100 pF
L
15
10
SETTLING TIME (µs)
5
0
02
5
OUTPUT STEP SIZE (V)
TO 0.01%
TO 0.1%
100
15
00775-0-032
Figure 32. Settling Time vs. Step Size (G = 1)
1000
s)
100
µ
(
10
SETTLING TIME
Figure 30. Large Signal Response and Settling Time,
G = 1000 (0.5 mV = 0.01% )
............................ ............
............................ ............
Figure 31. Small Signal Pulse Response, G = 1000, R
00775-0-030
00775-0-031
= 2 kΩ, CL = 100 pF
L
1
11000
10100
GAIN
Figure 33. Settling Time to 0.01% vs. Gain, for a 10 V Step
............................ ............
............................ ............
Figure 34. Gain Nonlinearity, G = 1, R
= 10 kΩ (10 µV = 1 ppm)
L
00775-0-033
00775-0-034
Rev. G | Page 11 of 20
AD620
Ω
.................... ............ ........
.................... ............ ........
Figure 35. Gain Nonlinearity, G = 100, R
= 10 kΩ
L
(100 µV = 10 ppm)
........ ................................
00775-0-035
INPUT
10V p-p
100k
Ω
11kΩ1kΩ100
G = 1000
49.9
*ALL RESISTORS 1% TOLERANCE
Figure 37. Settling Time Test Circuit
Ω
Ω
G=100
499
Ω
10kΩ*
G=1
G=10
5.49k
1k
2
1
AD620
Ω
8
3
10T
10k
Ω
V
OUT
+V
S
7
6
5
4
–V
S
00775-0-037
........ ................................
00775-0-036
Figure 36. Gain Nonlinearity, G = 1000, R
= 10 kΩ
L
(1 mV = 100 ppm)
Rev. G | Page 12 of 20
AD620
Ω
Ω
THEORY OF OPERATION
– IN
R3
400Ω
20µA
I1
Q1
Figure 38. Simplified Schematic of AD620
A1A2
C1
R1
GAIN
SENSE
R
–V
V
B
G
S
R2
GAIN
SENSE
20µA
C2
I2
10kΩ
10kΩ
A3
10kΩ
Q2
R4
400Ω
10kΩ
+IN
OUTPUT
REF
The AD620 is a monolithic instrumentation amplifier based on
a modification of the classic three op amp approach. Absolute
value trimming allows the user to program gain accurately
(to 0.15% at G = 100) with only one resistor. Monolithic
construction and laser wafer trimming allow the tight matching
and tracking of circuit components, thus ensuring the high level
of performance inherent in this circuit.
00775-0-038
The input transistors Q1 and Q2 provide a single differentialpair bipolar input for high precision (Figure 38), 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 external
gain setting resistor R
inputs to the A1/A2 outputs given by G = (R1 + R2)/R
. This creates a differential gain from the
G
+ 1. The
G
unity-gain subtractor, A3, removes any common-mode signal,
yielding a single-ended output referred to the REF pin potential.
The value of R
preamp stage. As R
also determines the transconductance of the
G
is reduced for larger gains, the
G
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
gain related errors. (b) The gain-bandwidth product
(determined by C1 and 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.
The internal gain resistors, R1 and R2, are trimmed to an
absolute value of 24.7 kΩ, allowing the gain to be programmed
accurately with a single external resistor.
The gain equation is then
4.49
k
1
=
G
=
R
G
+
R
G
G
k
4.49
1
−
Make vs. Buy: a Typical Bridge Application Error Budget
The AD620 offers improved performance over “homebrew”
three op amp IA designs, along with smaller size, fewer
components, and 10× lower supply current. In the typical
application, shown in Figure 39, 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. Table 3 shows how to
calculate the effect various error sources have on circuit
accuracy.
Rev. G | Page 13 of 20
AD620
R
Regardless of the system in which it is being used, the AD620
provides greater accuracy 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 homebrew 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.
R = 350
Ω
R = 350
Ω
PRECISION BRIDGE TRANSDUCE
10V
R = 350
R = 350
R
G
Ω
Ω
00775-0-039
499
SUPPLY CURRENT = 1.3mA MAX
AD620A
Ω
AD620A MONOLITHIC
INSTRUMENTATION
AMPLIFIER, G = 100
REFERENCE
00775-0-040
100
OP07D
Ω
**
OP07D
"HOMEBREW" IN-AMP, G = 100
*0.02% RESISTOR MATCH, 3ppm/
**DISCRETE 1% RESISTOR, 100ppm/
SUPPLY CURRENT = 15mA MAX
10k
10k
Ω
**
10k
Ω
**
10k
Ω
*
Ω
*
°
C TRACKING
10k
Ω
OP07D
Ω
10k
°
C TRACKING
*
*
00775-0-041
Figure 39. Make vs. Buy
Table 3. Make vs. Buy Error Budget
Error, ppm of Full Scale
Error Source AD620 Circuit Calculation “Homebrew” Circuit Calculation AD620 Homebrew
ABSOLUTE ACCURACY at TA = 25°C
Input Offset Voltage, µV 125 µV/20 mV (150 µV × √2)/20 mV 6,250 10,607
Output Offset Voltage, µV 1000 µV/100 mV/20 mV ((150 µV × 2)/100)/20 mV 500 150
Input Offset Current, nA 2 nA ×350 Ω/20 mV (6 nA ×350 Ω)/20 mV 18 53
CMR, dB 110 dB(3.16 ppm) ×5 V/20 mV (0.02% Match × 5 V)/20 mV/100 791 500
Total Drift Error 7,050 16,757
RESOLUTION
Gain Nonlinearity, ppm of Full Scale 40 ppm 40 ppm 40 40
Typ 0.1 Hz to 10 Hz Voltage Noise, µV p-p 0.28 µV p-p/20 mV (0.38 µV p-p × √2)/20 mV 14 27
Total Resolution Error 54 67
Grand Total Error 14,663 28,134
G = 100, VS = ±15 V.
(All errors are min/max and referred to input.)
Rev. G | Page 14 of 20
AD620
5V
7
3k
3k
Ω
3k
Ω
1.7mA0.10mA
Ω
G = 100
3k
499
Ω
3
8
1
2
1.3mA
AD620B
5
4
MAX
Ω
Figure 40. A Pressure Monitor Circuit that Operates on a 5 V Single Supply
Pressure Measurement
Although useful in many bridge applications, such as weigh
scales, the AD620 is especially suitable for higher resistance
pressure sensors powered at lower voltages where small size and
low power become more significant.
Figure 40 shows a 3 kΩ pressure transducer bridge powered
from 5 V. In such a circuit, the bridge consumes only 1.7 mA.
Adding the AD620 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 AD620 especially attractive for
voltage output pressure transducers. Since it delivers low noise
and drift, it will also serve applications such as diagnostic
noninvasive blood pressure measurement.
20k
Ω
REF
6
10k
Ω
20k
AD705
Ω
0.6mA
MAX
IN
AGND
ADC
DIGITAL
DATA
OUTPUT
00775-0-042
Medical ECG
The low current noise of the AD620 allows its use in ECG
monitors (Figure 41) where high source resistances of 1 MΩ or
higher are not uncommon. The AD620’s low power, low supply
voltage requirements, and space-saving 8-lead mini-DIP and
SOIC package offerings make it an excellent choice for batterypowered data recorders.
Furthermore, the low bias currents and low current noise,
coupled with the low voltage noise of the AD620, improve the
dynamic range for better performance.
The value of capacitor C1 is chosen to maintain stability of
the right leg drive loop. Proper safeguards, such as isolation,
must be added to this circuit to protect the patient from
possible harm.
PATIENT/CIRCUIT
PROTECTION/ISOLATION
R1
C1
Ω
10k
R4
1M
Ω
R3
24.9k
R2
24.9k
Ω
R
G
8.25k
Ω
Ω
+3V
AD620A
G = 7
0.03Hz
HIGH-
PASS
FILTER
G = 143
OUTPUT
AMPLIFIER
OUTPUT
1V/mV
AD705J
–3V
00775-0-043
Figure 41. A Medical ECG Monitor Circuit
Rev. G | Page 15 of 20
AD620
Precision V-I Converter
The AD620, along with another op amp and two resistors,
makes a precision current source (Figure 42). The op amp
buffers the reference terminal to maintain good CMR. The
output voltage, V
converts it to a current. This current, less only the input bias
current of the op amp, then flows out to the load.
The AD620’s gain is resistor-programmed by RG, or more
precisely, by whatever impedance appears between Pins 1 and 8.
The AD620 is designed to offer accurate gains using 0.1% to 1%
resistors. Table 4 shows required values of R
Note that for G = 1, the R
any arbitrary gain, R
, of the AD620 appears across R1, which
X
+V
S
7
3
8
G
AD620
1
I =
2
L
4
–V
S
[(V ) – (V )] G
V
x
IN+
=
R1
G
R1
pins are unconnected (RG = ∞). For
G
can be calculated by using the formula:
6
5
AD705
IN–
+ V –
X
R1
I
LOAD
for various gains.
G
L
00775-0-044
INPUT AND OUTPUT OFFSET VOLTAGE
The low errors of the AD620 are attributed to two sources,
input and output errors. The output error is divided by G when
referred to the input. In practice, the input errors dominate at
high gains, and the output errors dominate at low gains. The
total V
The reference terminal potential defines the zero output voltage
and is especially useful when the load does not share a precise
ground with the rest of the system. It provides a direct means of
injecting a precise offset to the output, with an allowable range
of 2 V within the supply voltages. Parasitic resistance should be
kept to a minimum for optimum CMR.
INPUT PROTECTION
The AD620 features 400 Ω of series thin film resistance at its
inputs and will safely withstand input overloads of up to ±15 V
or ±60 mA for several hours. This is true for all gains and power
on and off, which is particularly important since the signal
source and amplifier may be powered separately. For longer
time periods, the current should not exceed 6 mA
≤ VIN/400 Ω). For input overloads beyond the supplies,
(I
IN
clamping the inputs to the supplies (using a low leakage diode
such as an FD333) will reduce the required resistance, yielding
lower noise.
R
G
1
G
4.49−Ω
k
=
To minimize gain error, avoid high parasitic resistance in series
; to minimize gain drift, RG should have a low TC—less
with R
G
than 10 ppm/°C—for the best performance.
Table 4. Required Values of Gain Resistors
1% Std Table
Value of R
(Ω)
G
Calculated
Gain
0.1% Std Table
Value of RG(Ω )
Calculated
Gain
49.9 k 1.990 49.3 k 2.002
12.4 k 4.984 12.4 k 4.984
5.49 k 9.998 5.49 k 9.998
2.61 k 19.93 2.61 k 19.93
1.00 k 50.40 1.01 k 49.91
499 100.0 499 100.0
249 199.4 249 199.4
100 495.0 98.8 501.0
49.9 991.0 49.3 1,003.0
RF INTERFERENCE
All instrumentation amplifiers rectify small out of band signals.
The disturbance may appear as a small dc voltage offset. High
frequency signals can be filtered with a low pass R-C network
placed at the input of the instrumentation amplifier. Figure 43
demonstrates such a configuration. The filter limits the input
signal according to the following relationship:
FilterFreq
FilterFreq
where C
C
≥10CC.
D
affects the difference signal. CC affects the common-mode
D
DIFF
CM
=
=
2
1
D
1
RC
π
C
signal. Any mismatch in R × C
CMRR. To avoid inadvertently reducing CMRR-bandwidth
performance, make sure that C
smaller than C
larger C
. The effect of mismatched CCs is reduced with a
D
ratio.
D:CC
)2(2
CCR
+π
C
will degrade the AD620’s
C
is at least one magnitude
C
Rev. G | Page 16 of 20
AD620
+15V
0.1µ F1µ F0
C
C
R
C
R
C
+IN
+
AD620
499Ω
D
–
–IN
C
0.1µ F1µ F0
–15V
REF
V
OUT
00775-0-045
Figure 43. Circuit to Attenuate RF Interference
COMMON-MODE REJECTION
Instrumentation amplifiers, such as the AD620, offer high
CMR, which is a measure of the change in output voltage when
both inputs are 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; for best CMR over frequency, the shield
should be properly driven. Figure 44 and Figure 45 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
S
AD620
–V
S
REFERENCE
V
OUT
100
100
AD648
Ω
Ω
– INPUT
–V
+ INPUT
R
G
S
Figure 44. Differential Shield Driver
+V
100Ω
– INPUT
AD548
+ INPUT
R
G
2
R
G
2
AD620
–V
S
S
REFERENCE
V
OUT
Figure 45. Common-Mode Shield Driver
GROUNDING
Since the AD620 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.”
To isolate low level analog signals from a noisy digital
environment, many data-acquisition components have separate
analog and digital ground pins (Figure 46). 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 shown in Figure 46.
ANALOG P.S.
+15V C –15V
DIGITAL P.S.
+5VC
00775-0-046
00775-0-047
Rev. G | Page 17 of 20
0.1µF
AD620
0.1µF
AD585
S/H
1µF
µ
F
1
AD574A
ADC
Figure 46. Basic Grounding Practice
1µF
+
DIGITAL
DATA
OUTPUT
00775-0-048
AD620
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
Figure 47, Figure 48, and Figure 49. Refer to A Designer’s Guide to Instrumentation Amplifiers (free from Analog Devices) for
more information regarding in-amp applications.
+V
AD620
–V
S
S
REFERENCE
LOAD
TO POWER
SUPPLY
GROUND
V
OUT
– INPUT
R
G
+ INPUT
Figure 47. Ground Returns for Bias Currents with Transformer-Coupled Inputs
+V
AD620
–V
S
S
REFERENCE
V
LOAD
TO POWER
SUPPLY
GROUND
OUT
00775-0-050
– INPUT
+ INPUT
R
G
Figure 48. Ground Returns for Bias Currents with Thermocouple Inputs
+V
AD620
–V
S
S
REFERENCE
LOAD
TO POWER
SUPPLY
GROUND
V
OUT
00775-0-051
– INPUT
R
G
00775-0-049
+ INPUT
100k
Ω
100k
Ω
Figure 49. Ground Returns for Bias Currents with AC-Coupled Inputs
Rev. G | Page 18 of 20
AD620
OUTLINE DIMENSIONS
0.400 (10.16)
0.365 (9.27)
0.355 (9.02)
8
5
0.280 (7.11)
4
0.250 (6.35)
0.240 (6.10)
0.015
(0.38)
MIN
SEATING
PLANE
0.005 (0.13)
MIN
0.060 (1.52)
MAX
0.015 (0.38)
GAUGE
PLANE
1
PIN 1
0.100 (2.54)
0.210
(5.33)
MAX
0.150 (3.81)
0.130 (3.30)
0.115 (2.92)
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.
CORNER LEADS MAY BE CONFIGURED AS WHOLE OR HALF LEADS.
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
85
1.27 (0.0500)
BSC
0.51 (0.0201)
SEATING
COMPLIANT TO JEDEC STANDARDS MS-012AA
0.31 (0.0122)
PLANE
Figure 52. 8-Lead Standard Small Outline Package [SOIC]
Dimensions shown in millimeters and (inches)
6.20 (0.2440)
5.80 (0.2284)
41
1.75 (0.0688)
1.35 (0.0532)
0.25 (0.0098)
0.17 (0.0067)
Narrow Body (R-8)
0.50 (0.0196)
0.25 (0.0099)
8°
1.27 (0.0500)
0°
0.40 (0.0157)
× 45°
0.005 (0.13)
PIN 1
0.200 (5.08)
MAX
0.200 (5.08)
0.125 (3.18)
0.023 (0.58)
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
AD620AN −40°C to +85°C N-8
AD620ANZ2 −40°C to +85°C N-8
AD620BN −40°C to +85°C N-8
AD620BNZ2 −40°C to +85°C N-8
AD620AR −40°C to +85°C R-8
AD620ARZ2 −40°C to +85°C R-8
AD620AR-REEL −40°C to +85°C 13" REEL
AD620ARZ-REEL2 −40°C to +85°C 13" REEL
AD620AR-REEL7 −40°C to +85°C 7" REEL
AD620ARZ-REEL72 −40°C to +85°C 7" REEL
AD620BR −40°C to +85°C R-8
AD620BRZ2 −40°C to +85°C R-8
AD620BR-REEL −40°C to +85°C 13" REEL
AD620BRZ-RL2 −40°C to +85°C 13" REEL
AD620BR-REEL7 −40°C to +85°C 7" REEL
AD620BRZ-R72 −40°C to +85°C 7" REEL
AD620ACHIPS −40°C to +85°C Die Form
AD620SQ/883B −55°C to +125°C Q-8