Data Sheet AD622
Rev. E | Page 9 of 16
THEORY OF OPERATION
The AD622 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
0.5% at G = 1000) with only one resistor. Monolithic construction
and laser wafer trimming allow the tight matching and tracking
of circuit components, thus insuring AD622 performance.
Input Transistor Q1 and Input Transistor Q2 provide a single
differential-pair bipolar input for high precision (see Figure 16).
Feedback through the Q1-A1-R1 loop and the Q2-A2-R2 loop
maintains constant collector current of the Q1 and Q2 input
devices, thereby impressing the input voltage across External
Gain-Setting Resistor R
G
. This creates a differential gain from the
inputs to the A1 and A2 outputs given by G = (R1 + R2)/R
G
+ 1.
Unity-Gain Subtractor A3 removes any common-mode signal,
yielding a single-ended output referred to the REF pin potential.
00777-022
V
B
–V
S
A1 A2
A
3
C2
R
G
R1 R2
GAIN
SENSE
GAIN
SENSE
10k
10k
I2
I1
10k
REF
10k
+
IN
IN
R4
400
OUTPUT
C1
Q2
Q1
R3
400
+V
S
+V
S
+V
S
20µA20µA
Figure 16. Simplified Schematic of the AD622
The value of R
G
also determines the transconductance of the
preamp stage. As R
G
is reduced for larger gains, the trans-
conductance increases asymptotically to that of the input
transistors. This has the following three important advantages:
Open-loop gain is boosted for increasing programmed
gain, thus reducing gain-related errors.
The gain-bandwidth product (determined by C1, C2, and
the preamp transconductance) increases with programmed
gain, thus optimizing frequency response.
The input voltage noise is reduced to a value of 12 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 25.25 kΩ, allowing the gain to be programmed
accurately with a single external resistor.
MAKE vs. BUY: A TYPICAL APPLICATION ERROR
BUDGET
The AD622 offers cost and performance advantages over
discrete two op amp instrumentation amplifier designs along
with smaller size and fewer components. In a typical application
shown in Figure 17, a gain of 10 is required to receive and
amplify a 0 to 20 mA signal from the AD694 current transmitter.
The current is converted to a voltage in a 50 shunt. In
applications where transmission is over long distances, line
impedance can be significant so that differential voltage
measurement is essential. Where there is no connection
between the ground returns of transmitter and receiver, there
must be a dc path from each input to ground, implemented in
this case using two 1 kresistors. The error budget detailed in
Table 5 shows how to calculate the effect of various error
sources on circuit accuracy.
AD694
0 TO 20mA
TRANSMITTER
R
L2
10Ω
R
L2
10Ω
0 TO 20mA
50Ω
0 TO 20mA CURRENT LOOP
WITH 50Ω SHUNT IMPEDANCE
R
G
5.62kΩ
1kΩ
1kΩ
REF
AD622
AD622 MONOLITHIC INSTRUMENTATION
AMPLIFIER, G = 9.986
HOMEBREW IN-AMP, G = 10
1kΩ
1kΩ
1/2
LT1013
1/2
LT1013
9kΩ*
1kΩ* 1kΩ* 9kΩ*
+
V
IN
*0.1% RESISTOR MATCH, 50ppm/°C TRACKING
00777-016
Figure 17. Make vs. Buy
AD622 Data Sheet
Rev. E | Page 10 of 16
The AD622 provides greater accuracy at lower cost. The higher
cost of the homebrew circuit is dominated in this case by the
matched resistor network. One could also realize a homebrew
design using cheaper discrete resistors that are either trimmed
or hand selected to give high common-mode rejection. This
level of common-mode rejection, however, degrades significantly
over temperature due to the drift mismatch of the discrete
resistors.
Note that for the homebrew circuit, the LT1013 specification for
noise has been multiplied by √2. This is because a two op amp
type instrumentation amplifier has two op amps at its inputs,
both contributing to the overall noise.
Table 5. Make vs. Buy Error Budget
Error Source AD622 Circuit Calculation Homebrew Circuit Calculation
Total Error in ppm
Relative to 1 V FS
AD622 Homebrew
ABSOLUTE ACCURACY at T
A
= 25°C
Total RTI Offset Voltage, µV 125 µV + 1500 µV/10 800 µV × 2 275 1600
Input Offset Current, nA 2.5 nA × 1 kΩ 15 nA × 1 kΩ 2.5 15
CMR, dB
86 dB
50 ppm × 0.5 V
(0.1% Match × 0.5 V)/10 V 25 50
Total Absolute Error 302.5 1665
DRIFT TO 85°C
Gain Drift, ppm/°C (50 ppm + 5 ppm) × 60°C (50 ppm)/°C × 60°C 3300 3000
Total RTI Offset Voltage, µV/°C (1 µV/°C + 15 µV/°C /10) × 60°C 9 µV/°C × 2 × 60°C 150 1080
Input Offset Current, pA/°C 2 pA/°C × 1 kΩ × 60°C 155 pA/°C × 1 kΩ × 60°C 0.12 9.3
Total Drift Error 3450.12 4089.3
RESOLUTION
Gain Nonlinearity, ppm of Full Scale 10 ppm 20 ppm 10 20
Typ 0.1 Hz to 10 Hz Voltage Noise, µV p-p
0.6 µV p-p
0.55 µV p-p × √2
0.6
0.778
Total Resolution Error 10.6 20.778
Grand Total Error 3763 5775
Data Sheet AD622
Rev. E | Page 11 of 16
GAIN SELECTION
The AD622 gain is resistor programmed by R
G
or, more
precisely, by whatever impedance appears between Pin 1 and
Pin 8. The AD622 is designed to offer gains as close as possible
to popular integer values using standard 1% resistors. Table 6
shows required values of R
G
for various gains. Note that for
G = 1, the R
G
pins are unconnected (R
G
= ∞). For any arbitrary
gain, R
G
can be calculated by using the formula
1
k5.50
=
G
R
G
To minimize gain error, avoid high parasitic resistance in series
with R
G
. To minimize gain drift, R
G
should have a low temperature
coefficient less than 10 ppmC for the best performance.
Table 6. Required Values of Gain Resistors
Desired
Gain 1% Std Table Value of R
G
, Ω
Calculated
Gain
2 51.1 k 1.988
5 12.7 k 4.976
10 5.62 k 9.986
20
2.67 k
19.91
33 1.58 k 32.96
40 1.3 k 39.85
50 1.02 k 50.50
65 787 65.17
100 511 99.83
200
255
199.0
500 102 496.1
1000 51.1 989.3
INPUT AND OUTPUT OFFSET VOLTAGE
The low errors of the AD622 are attributable 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
OS
for a given gain is calculated as follows:
Total Error RTI = input error + (output error/G)
Total Error RTO = (input error × G) + output error
REFERENCE TERMINAL
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. The reference terminal 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 AD622 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.
00777-023
AD622
R
REF
R
+SUPPLY
–SUPPLY
V
OUT
+IN
–IN
Figure 18. Diode Protection for Voltages Beyond Supply

AD622ARZ-R7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Instrumentation Amplifiers LOW COST
Lifecycle:
New from this manufacturer.
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