(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
Table 1. Next Generation Upgrades for AD620
Part Comment
AD8221 Better specs at lower price
AD8222 Dual channel or differential out
AD8226 Low power, wide input range
AD8220 JFET input
AD8228Best gain accuracy
AD8295+2 precision op amps or differential out
AD8429Ultra low noise
Rev. H
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.
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.
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
ni
9 13 9 13 9 13 nV/√Hz
72 100 72 100 72 100 nV/√Hz
no
22
)/()(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. H | Page 4 of 20
Page 5
AD620
ABSOLUTE MAXIMUM RATINGS
Table 3.
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
Lead Temperature Range
(Soldering 10 seconds) 300°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.
Figure 3. 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 6. Input Bias Current vs. Temperature
175
00775-0-008
PERCENTAGE OF UNITS
10
0
–12001200
–6000600
INPUT BIAS CURRENT (pA)
Figure 4. 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 5. 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 7. 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 8. Voltage Noise Spectral Density vs. Frequency (G = 1−1000)
00775-0-009
00775-0-010
Rev. H | Page 6 of 20
Page 7
AD620
1000
100
CURRENT NOISE (fA/ Hz)
10
1
10
FREQUENCY (Hz)
100
Figure 9. Current Noise Spectral Density vs. Frequency
V/DIV)
μ
RTI NOISE (2.0
TIME (1 SEC/DIV)
Figure 10. 0.1 Hz to 10 Hz RTI Voltage Noise (G = 1)
1000
00775-0-011
00775-0-012
Figure 12. 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 13. Total Drift vs. Source Resistance
AD620A
00775-0-014
00775-0-015
V/DIV)
μ
RTI NOISE (0.1
TIME (1 SEC/DIV)
Figure 11. 0.1 Hz to 10 Hz RTI Voltage Noise (G = 1000)
00775-0-013
Rev. H | Page 7 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)
1M
100k10k1k10010
Figure 14. Typical CMR vs. Frequency, RTI, Zero to 1 kΩ Source Imbalance
00775-0-016
Page 8
AD620
180
160
140
120
100
PSR (dB)
80
60
40
20
0.1
35
G = 10, 100, 1000
30
G = 1000
G = 100
G = 10
G = 1
100k10k1k10010
1
FREQUENCY (Hz)
1M
00775-0-017
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 15. 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 16. Negative PSR vs. Frequency, RTI (G = 1−1000)
1000
100
G = 1000
G = 100
G = 10
G = 1
100k10k1k10010
1M
00775-0-018
Figure 18. 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
10
±
Figure 19. Input Voltage Range vs. Supply Voltage, G = 1
+V
–0.0
S
–0.5
–1.0
RL = 2k
–1.5
Ω
Volts
RL = 10k
15
Ω
20
00775-0-021
10
GAIN (V/V)
1
0.1
10010M
1k
FREQUENCY (Hz)
100k1M10k
Figure 17. Gain vs. Frequency
00775-0-019
Rev. H | Page 8 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 20. Output Voltage Swing vs. Supply Voltage, G = 10
1510
20
00775-0-022
Page 9
AD620
30
VS = ±15V
G = 10
20
10
OUTPUT VOLTAGE SWING (V p-p)
0
0
1001k
LOAD RESISTANCE (
Ω)
Figure 21. Output Voltage Swing vs. Load Resistance
........ .... ................ ............
10k
00775-0-023
.... ........ ................ ............
.... ........ ................ ............
00775-0-026
Figure 24. Large Signal Response and Settling Time, G = 10 (0.5 mV = 0.01%)
............................ ............
........ .... ................ ............
Figure 22. Large Signal Pulse Response and S ettling Time
G = 1 (0.5 mV = 0.01%)
.... ........ ................ ............
.... ........ ................ ............
Figure 23. Small Signal Response, G = 1, R
= 2 kΩ, CL = 100 pF
L
00775-0-024
00775-0-025
............................ ............
00775-0-027
Figure 25. Small Signal Response, G = 10, R
= 2 kΩ, CL = 100 pF
L
........ ........ .... .... .... .... ........
........ ........ .... .... .... .... ........
00775-0-030
Figure 26. Large Signal Response and Settling Time, G = 100 (0.5 mV = 0.01%)
Rev. H | Page 9 of 20
Page 10
AD620
20
.................... .... .... .... ........
.................... .... .... .... ........
Figure 27. 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 30. Settling Time vs. Step Size (G = 1)
1000
100
(μs)
10
SETTLING TIME
Figure 28. Large Signal Response and Settling Time,
G = 1000 (0.5 mV = 0.01% )
.................... .... .... .... ........
.................... .... .... .... ........
Figure 29. Small Signal Pulse Response, G = 1000, R
00775-0-030
00775-0-031
= 2 kΩ, CL = 100 pF
L
1
11000
10100
GAIN
Figure 31. Settling Time to 0.01% vs. Gain, for a 10 V Step
........ ................ .... ............
........ ................ .... ............
Figure 32. Gain Nonlinearity, G = 1, R
= 10 kΩ (10 μV = 1 ppm)
L
00775-0-033
00775-0-034
Rev. H | Page 10 of 20
Page 11
AD620
Ω
.... .... .... .................... ........
.... .... .... .................... ........
Figure 33. 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 35. 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 34. Gain Nonlinearity, G = 1000, R
= 10 kΩ
L
(1 mV = 100 ppm)
Rev. H | Page 11 of 20
Page 12
AD620
V
Ω
Ω
THEORY OF OPERATION
+
S
A1A2
C1
R1R2
GAIN
SENSE
R
–V
V
B
G
GAIN
SENSE
S
– IN
I1
+V
S
R3
400Ω
Q1
Figure 36. Simplified Schematic of AD620
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.
I2
20µA20µA
C2
Q2
10kΩ
10kΩ
R4
400Ω
+V
10kΩ
A3
S
OUTPUT
10kΩ
REF
+IN
The input transistors Q1 and Q2 provide a single differentialpair bipolar input for high precision (Figure 36), 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
00775-0-038
(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 37, 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 4 shows how to
calculate the effect various error sources have on circuit
accuracy.
Rev. H | Page 12 of 20
Page 13
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
removes 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.
10V
R = 350
Ω
R = 350
Ω
PRECISION BRIDGE TRANSDUCE
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
Ω
**
10k
10k
Ω
**
10k
Ω
*
Ω
*
°
C TRACKING
10k
Ω
OP07D
Ω
10k
°
C TRACKING
*
*
00775-0-041
Figure 37. Make vs. Buy
Table 4. 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. H | Page 13 of 20
Page 14
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 38. 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 38 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 also serves 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 39) 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
10k
Ω
R4
Ω
1M
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 39. A Medical ECG Monitor Circuit
Rev. H | Page 14 of 20
Page 15
AD620
Y
Precision V-I Converter
The AD620, along with another op amp and two resistors,
makes a precision current source (Figure 40). The op amp
buffers the reference terminal to maintain good CMR. The
output voltage, V
, of the AD620 appears across R1, which
X
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 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 5 shows required values of R
Note that for G = 1, the R
any arbitrary gain, R
4.49−Ω
k
=
R
G
1
G
pins are unconnected (RG = ∞). For
G
can be calculated by using the formula:
G
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 5. Required Values of Gain Resistors
1% Std Table
Value of RG(Ω)
Calculated
Gain
0.1% Std Table
Value of RG(Ω )
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
for various gains.
G
Calculated
Gain
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 safely withstands an input current of ±60 mA for
several hours at room temperature. This is true for all gains and
power on and off, which is useful if the signal source and
amplifier are powered separately. For longer time periods, the
input current should not exceed 6 mA.
For input voltages beyond the supplies, a protection resistor
should be placed in series with each input to limit the current to
6 mA. These can be the same resistors as those used in the RFI
filter. High values of resistance can impact the noise and AC
CMRR performance of the system. Low leakage diodes (such as
the BAV199) can be placed at the inputs to reduce the required
protection resistance.
+SUPPL
R
R
Figure 41. Diode Protection for Voltages Beyond Supply
+IN
–IN
AD620
–SUPPLY
REF
V
OUT
00775-0-052
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 42
demonstrates such a configuration. The filter limits the input
Rev. H | Page 15 of 20
Page 16
AD620
signal according to the following relationship:
FilterFreq+π=
DIFF
1
D
)2(2
CCR
C
100
AD648
Ω
– INPUT
+V
S
1
FilterFreqπ=
where C
C
affects the difference signal. CC affects the common-mode
D
≥10CC.
D
CM
2
signal. Any mismatch in R × C
RC
C
degrades the AD620 CMRR. To
C
avoid inadvertently reducing CMRR-bandwidth performance,
make sure that C
The effect of mismatched C
is at least one magnitude smaller than CD.
C
s is reduced with a larger CD:CC
C
ratio.
+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 42. 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 43 and Figure 44 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.
100
R
G
Ω
–V
+ INPUT
S
AD620
–V
S
REFERENCE
V
OUT
Figure 43. Differential Shield Driver
+V
100Ω
– INPUT
AD548
+ INPUT
R
G
2
R
G
2
AD620
–V
S
S
REFERENCE
V
OUT
Figure 44. 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 45). 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 45.
0.1μF
ANALOG P.S.
+15V C –15V
0.1μF
1μF
μ
F
1
DIGITAL P.S.
+5VC
1μF
00775-0-046
00775-0-047
Rev. H | Page 16 of 20
AD620
AD585
S/H
AD574A
ADC
Figure 45. Basic Grounding Practice
+
DIGITAL
DATA
OUTPUT
00775-0-048
Page 17
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 46, Figure 47, and Figure 48. 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 46. Ground Returns for Bias Currents with Transformer-Coupled Inputs
+V
AD620
–V
S
S
REFERENCE
LOAD
TO POWER
SUPPLY
GROUND
V
OUT
00775-0-050
– INPUT
+ INPUT
R
G
Figure 47. 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 48. Ground Returns for Bias Currents with AC-Coupled Inputs
Rev. H | Page 17 of 20
Page 18
AD620
AD620ACHIPS INFORMATION
Die size: 1803 μm × 3175 μm
Die thickness: 483 μm
Bond Pad Metal: 1% Copper Doped Aluminum
To minimize gain errors introduced by the bond wires, use Kelvin connections between the chip and the gain resistor, R
Pad 1A and Pad 1B in parallel to one end of R
where R
is not required, Pad 1A and Pad 1B must be bonded together as well as the Pad 8A and Pad 8B.
G
and Pad 8A and Pad 8B in parallel to the other end of RG. For unity gain applications
The pad coordinates indicate the center of each pad, referenced to the center of the die. The die orientation is indicated by the logo, as shown in Figure 49.
Rev. H | Page 18 of 20
Page 19
AD620
OUTLINE DIMENSIONS
0.400 (10.16)
0.365 (9.27)
0.355 (9.02)
8
5
0.280 (7.11)
1
0.100 (2.54)
0.210 (5.33)
0.150 (3.81)
0.130 (3.30)
0.115 (2.92)
0.022 (0.56)
0.018 (0.46)
0.014 (0.36)
MAX
BSC
0.070 (1.78)
0.060 (1.52)
0.045 (1.14)
CONTROLLI NG DIMENSIONS ARE IN INCHES; MILL IMETER DIMENSI ONS
(IN PARENTHESES) ARE ROUNDED-OFF I NCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE I N DESIGN.
CORNER LEADS MAY BE CONFIGURED AS WHOLE O R HALF LEADS.
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLYAND ARE NOT APPROPRIATE FOR USE IN DESIGN.
070606-A
Figure 52. 8-Lead Standard Small Outline Package [SOIC_N]
85
1
4
1.27 (0.0500)
BSC
0.51 (0.0201)
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDS MS-012-AA
0.31 (0.0122)
Dimensions shown in millimeters and (inches)
6.20 (0.2441)
5.80 (0.2284)
1.75 (0.0688)
1.35 (0.0532)
Narrow Body (R-8)
8°
0°
0.25 (0.0098)
0.17 (0.0067)
0.50 (0.0196)
0.25 (0.0099)
1.27 (0.0500)
0.40 (0.0157)
45°
012407-A
0.005 (0.13)
MIN
0.055 (1.40)
MAX
58
0.310 (7.87)
0.220 (5.59)
14
0.100 (2.54) BSC
0.405 (10.29) MAX
0.320 (8.13)
0.290 (7.37)
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.