Micropower, 85 μA maximum supply current
Wide power supply range (+2.2 V to ±18 V)
Easy to use
Gain set with one external resistor
Gain range 5 (no resistor) to 1000
Higher performance than discrete designs
Rail-to-rail output swing
High accuracy dc performance
0.03% typical gain accuracy (G = +5) (AD627A)
10 ppm/°C typical gain drift (G = +5)
125 μV maximum input offset voltage (AD627B dual supply)
200 μV maximum input offset voltage (AD627A dual supply)
1 μV/°C maximum input offset voltage drift (AD627B)
3 μV/°C maximum input offset voltage drift (AD627A)
10 nA maximum input bias current
Noise: 38 nV/√Hz RTI noise at 1 kHz (G = +100)
Excellent ac specifications
AD627A: 77 dB minimum CMRR (G = +5)
AD627B: 83 dB minimum CMRR (G = +5)
80 kHz bandwidth (G = +5)
135 μs settling time to 0.01% (G = +5, 5 V step)
APPLICATIONS
4 mA to 20 mA loop-powered applications
Low power medical instrumentation—ECG, EEG
Transducer interfacing
Thermocouple amplifiers
Industrial process controls
Low power data acquisition
Portable battery-powered instruments
GENERAL DESCRIPTION
The AD627 is an integrated, micropower instrumentation
amplifier that delivers rail-to-rail output swing on single and
dual (+2.2 V to ±18 V) supplies. The AD627 provides excellent
ac and dc specifications while operating at only 85 μA maximum.
The AD627 offers superior flexibility by allowing the user to set
the gain of the device with a single external resistor while conforming to the 8-lead industry-standard pinout configuration.
With no external resistor, the AD627 is configured for a gain of 5.
With an external resistor, it can be set to a gain of up to 1000.
A wide supply voltage range (+2.2 V to ±18 V) and micropower
current consumption make the AD627 a perfect fit for a wide
range of applications. Single-supply operation, low power
consumption, and rail-to-rail output swing make the AD627
Rev. E Document Feedback
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.
AD627
FUNCTIONAL BLOCK DIAGRAM
R
G
–IN
+IN
S
Figure 1. 8-Lead PDIP (N) and SOIC_N (R)
100
90
80
70
60
50
40
CMRR (dB)
30
20
10
0
110100
DISCRETE DESIGN
Figure 2. CMRR vs. Frequency, ±5 V
ideal for battery-powered applications. Its rail-to-rail output
stage maximizes dynamic range when operating from low
supply voltages. Dual-supply operation (±15 V) and low power
consumption make the AD627 ideal for industrial applications,
including 4 mA to 20 mA loop-powered systems.
The AD627 does not compromise performance, unlike other
micropower instrumentation amplifiers. Low voltage offset,
offset drift, gain error, and gain drift minimize errors in the
system. The AD627 also minimizes errors over frequency by
providing excellent CMRR over frequency. Because the CMRR
remains high up to 200 Hz, line noise and line harmonics are
rejected.
The AD627 provides superior performance, uses less circuit
board area, and costs less than micropower discrete designs.
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 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 CAUTION
Rev. E | Page 7 of 24
Page 8
AD627 Data Sheet
R
G
1
–IN
2
+IN
3
–V
S
4
R
G
8
+V
S
7
OUTPUT
6
REF
5
AD627
TOP VIEW
(Not to Scale)
00782-051
1
2
3
4
8
7
6
5
AD627
TOP VIEW
(Not to Scale)
R
G
–IN
+IN
–V
S
R
G
+V
S
OUTPUT
REF
00782-052
Pin No.
Mnemonic
Description
8
RG
External Gain Setting Resistor. Place gain setting resistor across RG pins to set the gain.
PIN CONFIGURATIONS AND FUNCTION DESCRIPTIONS
Figure 3. 8-Lead PDIP Pin Configuration
Table 5. Pin Function Descriptions
1 RG External Gain Setting Resistor. Place gain setting resistor across RG pins to set the gain.
2 −IN Negative Input.
3 +IN Positive Input.
4 −VS Negative Voltage Supply Pin.
5 REF Reference Pin. Drive with low impedance voltage source to level shift the output voltage.
6 OUTPUT Output Voltage.
7 +VS Positive Supply Voltage.
Figure 4. 8-Lead SOIC_N Pin Configuration
Rev. E | Page 8 of 24
Page 9
Data Sheet AD627
FREQUENCY ( Hz )
100
1
NOISE (nV/ Hz, RTI)
90
80
70
60
50
40
30
20
10
0
10
100
1k10k
100k
GAIN = +1000
GAIN = +5
GAIN = +100
00782-003
FREQUENCY ( Hz )
100
1
CURRENT NOIS E
(fA/ Hz)
90
80
70
60
50
40
30
20
10
0
101001k10k
00782-004
COMMON-MODE INPUT (V)
–3.2
–2.0
–1515
–10
INPUT BIAS CURRE NT (nA)
–5
0
510
–3.0
–2.8
–2.6
–2.4
–2.2
00782-005
TEMPERATURE (°C)
INPUT BIAS CURRE NT (nA)
–5.5
–3.5
–1.5
–60140–40 –20
0
20406080100 120
–5.0
–4.5
–2.5
–2.0
–4.0
–3.0
VS = ±15V
VS= ±5V
VS = +5V
00782-006
TOTAL POWER SUPPLY VOLTAGE (V)
POWER SUP P LY CURRENT (µA)
65.5
59.5
0
405
1015
2025
3035
64.5
63.5
62.5
61.5
60.5
00782-007
OUTPUT CURRE NT (mA)
OUTPUT VOLTAGE SWING (V)
0
(V+) –1
(V+) –2
(V+) –3
(V
–) +2
(V
–) +1
V–
510152025
SOURCING
VS = ±15V
SINKING
V
S
= ±1.5V
VS = ±1.5V
V
S
= ±2.5V
V
S
= ±2.5V
V
S
= ±5V
VS = ±5V
VS = ±15V
V+
00782-008
TYPICAL PERFORMANCE CHARACTERISTICS
At 25°C, VS = ±5 V, RL = 20 kΩ, unless otherwise noted.
Figure 5. Voltage Noise Spectral Density vs. Frequency
Figure 6. Current Noise Spectral Density vs. Frequency
Figure 8. Input Bias Current vs. Temperature
Figure 9. Supply Current vs. Supply Voltage
Figure 7. Input Bias Current vs. CMV, VS = ±15 V
Rev. E | Page 9 of 24
Figure 10. Output Voltage Swing vs. Output Current
Page 10
AD627 Data Sheet
500mV
100
10
1s
Figure 11. 0.1 Hz to 10 Hz Current Noise (0.71 pA/DIV)
20mV
100
10
1s
1s
Figure 12. 0.1 Hz to 10 Hz RTI Voltage Noise (400 nV/DIV), G = +5
2V
100
10
1s
Figure 13. 0.1 Hz to 10 Hz RTI Voltage Noise (200 nV/DIV), G = +1000
120
110
100
90
80
70
60
50
POSITIVE PSRR (dB)
40
30
00782-009
20
101001k10k100k
FREQUENCY (Hz)
G = +1000
G = +100
G = +5
00782-012
Figure 14. Positive PSRR vs. Frequency, ±5 V
100
90
80
70
60
50
40
30
NEGATIVE P S RR (dB)
20
00782-010
10
0
101001k10k100k
FREQUENCY (Hz)
G = +1000
G = +100
G = +5
00782-013
Figure 15. Negative PSRR vs. Frequency, ±5 V
120
110
100
90
80
70
60
POSITIVE PSRR (dB)
50
40
00782-011
30
20
101001k10k100k
FREQUENCY (Hz)
G = +1000
G = +100
G = +5
00782-014
Figure 16. Positive PSRR vs. Frequency (VS = 5 V, 0 V)
Rev. E | Page 10 of 24
Page 11
Data Sheet AD627
GAIN (V/V)
10
0.1
51k
SETTLING TIME (ms)
1
100
10
00782-015
1V1mV50µs
00782-016
1V1mV50µs
00782-017
OUTPUT PULSE (V)
400
200
0
0
±10
SETTLING TIME (µs)
±2±4
±6±8
300
100
00782-018
200µV
1V100µs
00782-019
200µV
1V500µs
00782-020
Figure 17. Settling Time to 0.01% vs. Gain for a 5 V Step at Output, RL = 20 kΩ,
= 100 pF, VS = ±5 V
C
L
Figure 18. Large Signal Pulse Response and Settling Time, G = –5, RL = 20 kΩ,
= 100 pF (1.5 mV = 0.01%)
C
L
Figure 20. Settling Time to 0.01% vs. Output Swing, G = +5, RL = 20 kΩ,
= 100 pF
C
L
Figure 21. Large Signal Pulse Response and Settling Time, G = –100,
= 20 kΩ, CL = 100 pF (100 µV = 0.01%)
R
L
Figure 19. Large Signal Pulse Response and Settling Time, G = −10,
R
= 20 kΩ, CL = 100 pF (1.0 mV = 0.01%)
L
Figure 22. Large Signal Pulse Response and Settling Time, G = –1000,
R
= 20 kΩ, CL = 100 pF (10 µV = 0.01%)
L
Rev. E | Page 11 of 24
Page 12
AD627 Data Sheet
G = +5
G = +100
G = +1000
FREQUENCY ( Hz )
100
CMRR (dB)
90
80
70
60
50
40
30
20
10
0
110
1k
10k100k
110
120
100
00782-021
FREQUENCY ( Hz )
GAIN (dB)
70
60
50
40
30
20
10
0
–10
–20
–30
1001k
10k
100k
G = +1000
G = +100
G = +5
G = +10
00782-022
A
CH2
20mV
20µs288mV
EXT1
00782-023
286mV
20mV
EXT1
20µs
A
CH2
00782-024
286mV
20mV
EXT1100µs
A
CH2
00782-025
286mV
50mV
EXT11msA
CH2
00782-026
Figure 23. CMRR vs. Frequency, ±5 VS (CMV = 200 mV p-p)
Figure 24. Gain vs. Frequency (VS = 5 V, 0 V), V
= 2.5 V
REF
Figure 26. Small Signal Pulse Response, G = +10, R
Figure 27. Small Signal Pulse Response, G = +100, R
= 20 kΩ, CL = 50 pF
L
= 20 kΩ, CL = 50 pF
L
Figure 25. Small Signal Pulse Response, G = +5, RL = 20 kΩ, CL = 50 pF
Figure 28. Small Signal Pulse Response, G = +1000, RL = 20 kΩ, CL = 50 pF
Rev. E | Page 12 of 24
Page 13
Data Sheet AD627
20µV/DIV
200µV/DIV
Figure 29. Gain Nonlinearity, Negative Input,
= ±2.5 V, G = +5 (4 ppm/DIV)
V
S
40µV/DIV
Figure 30. Gain Nonlinearity, Negative Input,
= ±2.5 V, G = +100 (8 ppm/DIV)
V
S
40µV/DIV
V
OUT
0.5V/DIV
V
OUT
0.5V/DIV
V
OUT
00782-027
3V/DIV
00782-030
Figure 32. Gain Nonlinearity, Negative Input,
= ±15 V, G = +100 (7 ppm/DIV)
V
S
200µV/DIV
V
OUT
00782-028
3V/DIV
00782-031
Figure 33. Gain Nonlinearity, Negative Input,
V
= ±15 V, G = +5 (7 ppm/DIV)
S
200µV/DIV
V
OUT
3V/DIV
Figure 31. Gain Nonlinearity, Negative Input,
= ±15 V, G = +5 (1.5 ppm/DIV)
V
S
00782-029
Figure 34. Gain Nonlinearity, Negative Input,
V
= ±15 V, G = +100 (7 ppm/DIV)
S
V
OUT
3V/DIV
00782-032
Rev. E | Page 13 of 24
Page 14
AD627 Data Sheet
R
G
EXTERNAL GAIN RESISTOR
REF
–IN
+IN
+V
S
–V
S
–V
S
–V
S
+V
S
R1
100kΩ
R2
25kΩ
R5
200kΩ
R6
200kΩ
R3
25kΩ
2kΩ2kΩ
0.1VV1
A2
A1
Q1Q2
OUTPUT
R4
100kΩ
00782-033
THEORY OF OPERATION
The AD627 is a true instrumentation amplifier, built using two
feedback loops. Its general properties are similar to those of the
classic two-op-amp instrumentation amplifier configuration but
internally the details are somewhat different. The AD627 uses a
modified current feedback scheme, which, coupled with interstage
feedforward frequency compensation, results in a much better
common-mode rejection ratio (CMRR) at frequencies above
dc (notably the line frequency of 50 Hz to 60 Hz) than might
otherwise be expected of a low power instrumentation amplifier.
In Figure 35, A1 completes a feedback loop that, in conjunction
with V1 and R5, forces a constant collector current in Q1. Assume
that the gain-setting resistor (R
) is not present. Resistors R2
G
and R1 complete the loop and force the output of A1 to be equal
to the voltage on the inverting terminal with a gain of nearly
1.25. A2 completes a nearly identical feedback loop that forces
a current in Q2 that is nearly identical to that in Q1; A2 also
provides the output voltage. When both loops are balanced, the
gain from the noninverting terminal to V
whereas the gain from the output of A1 to V
is equal to 5,
OUT
is equal to −4.
OUT
The inverting terminal gain of A1 (1.25) times the gain of A2
(−4) makes the gain from the inverting and noninverting
terminals equal.
The differential mode gain is equal to 1 + R4/R3, nominally 5,
and is factory trimmed to 0.01% final accuracy. Adding an
external gain setting resistor (R
amount equal to (R4 + R1)/R
) increases the gain by an
G
. The output voltage of the
G
AD627 is given by
V
= [VIN(+) – VIN(−)] × (5 + 200 kΩ/RG) + V
OUT
(1)
REF
Laser trims are performed on R1 through R4 to ensure that
their values are as close as possible to the absolute values in the
gain equation. This ensures low gain error and high commonmode rejection at all practical gains.
Figure 35. Simplified Schematic
Rev. E | Page 14 of 24
Page 15
Data Sheet AD627
+IN
V
OUT
V
IN
–IN
REF (INPUT)
–1.1V TO –18V
+1.1V TO + 18V
R
G
+V
S
–V
S
R
G
R
G
OUTPUT
REF
0.1µF
0.1µF
+IN
V
OUT
V
IN
–IN
REF (INPUT)
GAIN = 5 + (200kΩ/R
G
)
+2.2V TO + 36V
R
G
+V
S
R
G
R
G
OUTPUT
REF
0.1µF
00782-034
R
G
EXTERNAL GAIN RESISTOR
REF
–IN
+IN
–V
S
–V
S
+V
S
+V
S
100kΩ
25kΩ25kΩ
200kΩ
200kΩ
2kΩ
2kΩ
A1
0.1VV
A
A2
OUTPUT
–V
S
100kΩ
–IN
+IN
V+
V–
V
DIFF
2
V
DIFF
2
V
CM
Q1Q2
00782-035
USING THE AD627
BASIC CONNECTIONS
Figure 36 shows the basic connection circuit for the AD627.
The +V
supply can be either bipolar (V
supply (−V
the power supplies close to the power pins of the device. For
best results, use surface-mount 0.1 µF ceramic chip capacitors.
The input voltage can be single-ended (tie either −IN or +IN to
ground) or differential. The difference between the voltage on the
inverting and noninverting pins is amplified by the programmed
gain. The gain resistor programs the gain as described in the
Setting the Gain and Reference Terminal sections. Basic
connections are shown in Figure 36. The output signal appears
as the voltage difference between the output pin and the
externally applied voltage on the REF pin, as shown in Figure 37.
and −VS terminals connect to the power supply. The
S
= ±1.1 V to ±18 V) or single
S
= 0 V, +VS = 2.2 V to 36 V). Capacitively decouple
S
SETTING THE GAIN
The gain of the AD627 is resistor programmed by RG, or, more
precisely, by whatever impedance appears between Pin 1 and Pin 8.
The gain is set according to
Gain = 5 + (200 kΩ/R
Therefore, the minimum achievable gain is 5 (for 200 kΩ/
(Gain − 5)). With an internal gain accuracy of between 0.05%
and 0.7%, depending on gain and grade, a 0.1% external gain
resistor is appropriate to prevent significant degradation of the
overall gain error. However, 0.1% resistors are not available in a
wide range of values and are quite expensive. Table 6 shows
recommended gain resistor values using 1% resistors. For all
gains, the size of the gain resistor is conservatively chosen as the
closest value from the standard resistor table that is higher than
the ideal value. This results in a gain that is always slightly less
than the desired gain, thereby preventing clipping of the signal
at the output due to resistor tolerance.
The internal resistors on the AD627 have a negative temperature
coefficient of −75 ppm/°C maximum for gains > 5. Using a
gain resistor that also has a negative temperature coefficient
of −75 ppm/°C or less tends to reduce the overall gain drift of
the circuit.
) or RG = 200 kΩ/(Gain − 5) (2)
G
Figure 36. Basic Connections for Single and Dual Supplies
Figure 37. Amplifying Differential Signals with a Common-Mode Component
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. The reference terminal is
also useful when amplifying bipolar signals, because it provides
a virtual ground voltage.
The AD627 output voltage is developed with respect to the potential on the reference terminal; therefore, tying the REF pin to the
appropriate local ground solves many grounding problems. For
optimal CMR, tie the REF pin to a low impedance point.
The voltage on A1 can also be expressed as a function of the
actual voltages on the –IN and +IN pins (V− and V+) such that
= 1.25 ((V−) + 0.5 V) − 0.25 V
V
A1
− ((V+) − (V−)) 25 kΩ/RG (4)
REF
The output of A1 is capable of swinging to within 50 mV of the
negative rail and to within 200 mV of the positive rail. It is clear,
from either Equation 3 or Equation 4, that an increasing V
REF
(while it acts as a positive offset at the output of the AD627)
tends to decrease the voltage on A1. Figure 38 and Figure 39
show the maximum voltages that can be applied to the REF pin
for a gain of 5 for both the single-supply and dual-supply cases.
Figure 38. Reference Input Voltage vs. Negative Input Voltage,
V
= ±5 V, G = +5
S
INPUT RANGE LIMITATIONS IN SINGLE-SUPPLY
APPLICATIONS
In general, the maximum achievable gain is determined by the
available output signal range. However, in single-supply applications where the input common-mode voltage is nearly or equal
to 0, some limitations on the gain can be set. Although the
Specifications section nominally defines the input, output, and
reference pin ranges, the voltage ranges on these pins are
mutually interdependent. Figure 37 shows the simplified
schematic of the AD627, driven by a differential voltage (V
that has a common-mode component, V
A1 op amp output is a function of V
REF pin, and the programmed gain. This voltage is given by
V
A1
= 1.25 (VCM + 0.5 V) − 0.25 V
. The voltage on the
CM
, VCM, the voltage on the
DIFF
− V
REF
(25 kΩ/RG + 0.625) (3)
DIFF
Figure 39. Reference Input Voltage vs. Negative Input Voltage,
= 5 V, G = +5
V
S
Raising the input common-mode voltage increases the voltage
on the output of A1. However, in single-supply applications
where the common-mode voltage is low, a differential input
DIFF
)
voltage or a voltage on REF that is too high can drive the output
of A1 into the ground rail. Some low-side headroom is added
because both inputs are shifted upwards by about 0.5 V (that is,
by the V
of Q1 and Q2). Use Equation 3 and Equation 4 to
BE
check whether the voltage on Amplifier A1 is within its
operating range.
Rev. E | Page 16 of 24
Page 17
Data Sheet AD627
+100
270
155
3.1
1.1
38
V
IN
R
G
+V
S
–V
S
AD627
0.1µF
0.1µF
0.1µF
–V
S
V
OUT
REF
0.1µF
OP113
00782-038
Table 7. Maximum Gain for Low Common-Mode, Single-Supply Applications
VIN REF Pin Supply Voltage RG (1% Tolerance) Resulting Maximum Gain Output Swing WRT 0 V
±100 mV, VCM = 0 V 2 V 5 V to 15 V 28.7 kΩ 12.0 0.8 V to 3.2 V
±50 mV, VCM = 0 V 2 V 5 V to 15 V 10.7 kΩ 23.7 0.8 V to 3.2 V
±10 mV, VCM = 0 V 2 V 5 V to 15 V 1.74 kΩ 119.9 0.8 V to 3.2 V
V− = 0 V, V+ = 0 V to 1 V 1 V 10 V to 15 V 78.7 kΩ 7.5 1 V to 8.5 V
V− = 0 V, V+ = 0 mV to 100 mV 1 V 5 V to 15 V 7.87 kΩ 31 1 V to 4.1 V
V− = 0 V, V+ = 0 mV to 10 mV 1 V 5 V to 15 V 787 Ω 259.1 1 V to 3.6 V
Table 8. RTI Error Sources
Maximum Total RTI Offset Error (μV) Maximum Total RTI Offset Drift (μV/°C) Total RTI Noise (nV/√Hz)
Gain AD627A AD627B AD627A AD627B AD627A/AD627B
Tabl e 7 gives values for the maximum gain for various singlesupply input conditions. The resulting output swings refer to
0 V. To maximize the available gain and output swing, set the
voltages on the REF pins to either 2 V or 1 V. In most cases,
there is no advantage to increasing the single supply to greater
than 5 V (the exception is an input range of 0 V to 1 V).
OUTPUT BUFFERING
The AD627 is designed to drive loads of 20 kΩ or greater but
can deliver up to 20 mA to heavier loads at lower output voltage
swings (see Figure 10). If more than 20 mA of output current is
required at the output, buffer the AD627 output with a precision
op amp, such as the OP113. Figure 40 shows this for a single
supply. This op amp can swing from 0 V to 4 V on its output
while driving a load as small as 600 Ω.
INPUT AND OUTPUT OFFSET ERRORS
The low errors of the AD627 are attributed to two sources,
input and output errors. The output error is divided by G when
referred to the input. In practice, input errors dominate at high
gains and output errors dominate at low gains. The total offset
error for a given gain is calculated as
RTI offset errors and noise voltages for different gains are listed
in Tab l e 8.
Figure 40. Output Buffering
Rev. E | Page 17 of 24
Page 18
AD627 Data Sheet
V
OUT
V
OUT
+2.5V
+2.5V
+5V+5V
AD627A GAIN = 9.98 (5+(200kΩ/R
G
))HOMEBREW IN- AM P , G = +10
*1% RESISTOR MATCH, 50ppm/°C TRACKING
R
G
40.2kΩ
1%
+10ppm/°C
AD627A
+5V
350Ω
350Ω
350Ω
350Ω
3.15kΩ*350Ω*
350Ω*3.15kΩ*
±100mV
1/2
LT10781SB
LT10781SB
1/2
00782-039
Total RTI Offset Voltage, mV/°C
(2 × 3.5 μV/°C × 60°C)/100 mV
2,600
4,200
MAKE vs. BUY: A TYPICAL APPLICATION ERROR
BUDGET
The example in Figure 41 serves as a good comparison between
the errors associated with an integrated and a discrete in-amp
implementation. A ±100 mV signal from a resistive bridge
(common-mode voltage = 2.5 V) is amplified. This example
compares the resulting errors from a discrete two-op-amp
instrumentation amplifier and the AD627. The discrete
implementation uses a four-resistor precision network
(1% match, 50 ppm/°C tracking).
The errors associated with each implementation (see Tabl e 9)
show the integrated in-amp to be more precise at both ambient
and overtemperature. Note that the discrete implementation is
more expensive, primarily due to the relatively high cost of the
low drift precision resistor network.
The input offset current of the discrete instrumentation amplifier
implementation is the difference in the bias currents of the twoop amplifiers, not the offset currents of the individual op amps.
In addition, although the values of the resistor network are chosen
so that the inverting and noninverting inputs of each op amp
see the same impedance (about 350 Ω), the offset current of
each op amp adds another error that must be characterized.
Total Drift Error 6,504 7,207
Grand Total Error 27,039 45,879
Rev. E | Page 18 of 24
Page 19
Data Sheet AD627
V
OUT
+5V
VIN–
VIN+
–5V
R1
9999.5ΩR2999.76ΩR31000.2ΩR49997.7Ω
1/2
OP296
A1
A2
1/2
OP296
00782-040
FREQUENCY ( Hz )
CMRR (dB)
120
1
110
100
90
80
70
60
50
40
30
20
101001k10k100k
00782-041
V
OUT
TO POWER
SUPPLY
GROUND
R
G
–V
S
+V
S
AD627
7
4
5
8
3
6
1
2
REFERENCE
+INPUT
–INPUT
LOAD
00782-042
V
OUT
TO POWER
SUPPLY
GROUND
R
G
–V
S
+V
S
AD627
7
4
5
8
3
6
1
2
REFERENCE
+INPUT
–INPUT
LOAD
00782-043
V
OUT
TO POWER
SUPPLY
GROUND
R
G
–V
S
+V
S
AD627
7
4
5
8
3
6
1
2
REFERENCE
+INPUT
–INPUT
100kΩ
LOAD
00782-044
ERRORS DUE TO AC CMRR
In Tab l e 9, the error due to common-mode rejection results
from the common-mode voltage from the bridge 2.5 V. Th e
ac error due to less than ideal common-mode rejection cannot
be calculated without knowing the size of the ac common-mode
voltage (usually interference from 50 Hz/60 Hz mains frequencies).
A mismatch of 0.1% between the four gain setting resistors
determines the low frequency CMRR of a two-op-amp
instrumentation amplifier. The plot in Figure 43 shows the
practical results of resistor mismatch at ambient temperature.
The CMRR of the circuit in Figure 42 (Gain = +11) was
measured using four resistors with a mismatch of nearly 0.1%
(R1 = 9999.5 Ω, R2 = 999.76 Ω, R3 = 1000.2 Ω, R4 = 9997.7 Ω).
As expected, the CMRR at dc was measured at about 84 dB
(calculated value is 85 dB). However, as frequency increases,
CMRR quickly degrades. For example, a 200 mV p-p harmonic
of the mains frequency at 180 Hz would result in an output
voltage of about 800 µV. To put this in context, a 12-bit data
acquisition system, with an input range of 0 V to 2.5 V, has an
LSB weighting of 610 µV.
By contrast, the AD627 uses precision laser trimming of internal
resistors, along with patented CMR trimming, to yield a higher
dc CMRR and a wider bandwidth over which the CMRR is flat
(see Figure 23).
GROUND RETURNS FOR INPUT BIAS CURRENTS
Input bias currents are dc currents that must flow to bias the
input transistors of an amplifier. They are usually transistor base
currents. When amplifying floating input sources, such as
transformers or ac-coupled sources, there must be a direct dc
path into each input so that the bias current can flow. Figure 44,
Figure 45, and Figure 46 show how to provide a bias current
path for the cases of, respectively, transformer coupling, a
thermocouple application, and capacitive ac-coupling.
In dc-coupled resistive bridge applications, providing this path
is generally not necessary because the bias current simply flows
from the bridge supply through the bridge and into the amplifier.
However, if the impedance that the two inputs see are large, and
differ by a large amount (>10 kΩ), the offset current of the input
stage causes dc errors compatible with the input offset voltage of
the amplifier.
Figure 44. Ground Returns for Bias Currents with Transformer Coupled Inputs
Figure 43. CMRR over Frequency of Discrete In-Amp in Figure 42
Figure 42. 0.1% Resistor Mismatch Example
Rev. E | Page 19 of 24
Figure 45. Ground Returns for Bias Currents with Thermocouple Inputs
Figure 46. Ground Returns for Bias Currents with AC-Coupled Inputs
Page 20
AD627 Data Sheet
LAYOUT AND GROUNDING
The use of ground planes is recommended to minimize the
impedance of ground returns (and hence, the size of dc errors).
To isolate low level analog signals from a noisy digital environment,
many data acquisition components have separate analog and
digital ground returns (see Figure 47). Return all ground pins
from mixed-signal components, such as analog-to-digital
converters, through the high quality analog ground plane.
Digital ground lines of mixed-signal components should also
be returned through the analog ground plane. This may seem
to break the rule of separating analog and digital grounds;
however, in general, there is also a requirement to keep the
voltage difference between digital and analog grounds on a
converter as small as possible (typically, <0.3 V). The increased
noise, caused by the digital return currents of the converter
flowing through the analog ground plane, is generally negligible.
To maximize isolation between analog and digital, connect the
ground planes back at the supplies.
If there is only one power supply available, it must be shared by
both digital and analog circuitry. Figure 48 shows how to minimize
interference between the digital and analog circuitry. As in the
previous case, use separate analog and digital ground planes or
use reasonably thick traces as an alternative to a digital ground
plane. Connect the ground planes at the ground pin of the power
supply. Run separate traces (or power planes) from the power
supply to the supply pins of the digital and analog circuits. Ideally,
each device should have its own power supply trace, but they
can be shared by multiple devices if a single trace is not used to
route current to both digital and analog circuitry.
2
3
ANALOG POW E R SUPP L Y
+5V–5VGND
0.1µF
0
.
1
µ
7
4
AD627
AD627
6
5
0
F
4
3
.
1614
V
IN1VDD
ADC
V
IN2
1
µ
F
AGND
AD7892-2
DGND
DIGITAL PO W E R SUPP L Y
12
+5VGND
0
.
F
1
µ
V
AGND
MICRO-
PROCESSOR
DD
00782-045
Figure 47. Optimal Grounding Practice for a Bipolar Supply Environment with Separate Analog and Digital Supplies
POWER SUPPLY
5VGND
.
F
1
µ
0
0
.
F
1
µ
1
V
DD
V
IN
ADC
AGND
AD7892-2
DGND
12
V
DGND
DD
MICRO-
PROCESSOR
00782-046
2
AD627
3
7
0.1µF
4
6
5
4
Figure 48. Optimal Ground Practice in a Single-Supply Environment
Rev. E | Page 20 of 24
Page 21
Data Sheet AD627
V
–
INPUT PROTECTION
As shown in the simplified schematic (see Figure 35), both the
inverting and noninverting inputs are clamped to the positive
and negative supplies by ESD diodes. In addition, a 2 k series
resistor on each input provides current limiting in the event of
an overvoltage. These ESD diodes can tolerate a maximum
continuous current of 10 mA. So an overvoltage (that is, the
amount by which the input voltage exceeds the supply voltage)
of ±20 V can be tolerated. This is true for all gains, and for
power on and off. This last case is particularly important
because the signal source and amplifier can be powered
separately.
If the overvoltage is expected to exceed 20 V, use additional
external series current-limiting resistors to keep the diode
current below 10 mA.
RF INTERFERENCE
All instrumentation amplifiers can rectify high frequency outof-band signals. Once rectified, these signals appear as dc offset
errors at the output. The circuit in Figure 49 provides good RFI
suppression without reducing performance within the pass
band of the instrumentation amplifier. Resistor R1 and
Capacitor C1 (and likewise, R2 and C2) form a low-pass RC
filter that has a –3 dB BW equal to
f = 1/(2π(R1 × C1)) (7)
Using the component values shown in Figure 49, this filter has
a –3 dB bandwidth of approximately 8 kHz. Resistor R1 and
Resistor R2 were selected to be large enough to isolate the circuit
input from the capacitors but not large enough to significantly
increase circuit noise. To preserve common-mode rejection in
the amplifier pass band, Capacitor C1 and Capacitor C2 must
be 5% mica units, or low cost 20% units can be tested and binned
to provide closely matched devices.
Capacitor C3 is needed to maintain common-mode rejection at
low frequencies. R1/R2 and C1/C2 form a bridge circuit whose
output appears across the input pins of the in-amp. Any mismatch
between C1 and C2 unbalances the bridge and reduces commonmode rejection. C3 ensures that any RF signals are common
mode (the same on both in-amp inputs) and are not applied
differentially. This second low-pass network, R1 + R2 and C3,
has a −3 dB frequency equal to
1/(2π((R1 + R2) × C3)) (8)
+
S
0.01µF
AD627
0.01µF
–V
S
REFERE NCE
V
OUT
00782-047
+IN
R
G
0.33µF
0.33µF
1000pF
5%
0.022µF
1000pF
5%
C1
C3
C2
R1
20kΩ
1%
R2
20kΩ
IN
1%
Figure 49. Circuit to Attenuate RF Interference
Using a C3 value of 0.022 µF, as shown in Figure 49, the −3 dB
signal bandwidth of this circuit is approximately 200 Hz. The
typical dc offset shift over frequency is less than 1 mV and the
RF signal rejection of the circuit is better than 57 dB. To increase
the 3 dB signal bandwidth of this circuit, reduce the value of
Resistor R1 and Resistor R2. The performance is similar to that
when using 20 kΩ resistors, except that the circuitry preceding
the in-amp must drive a lower impedance load.
When building a circuit like that shown in Figure 49, use a PC
board with a ground plane on both sides. Make all component
leads as short as possible. Resistor R1 and Resistor R2 can be
common 1% metal film units, but Capacitor C1 and Capacitor C2
must be ±5% tolerance devices to avoid degrading the commonmode rejection of the circuit. Either the traditional 5% silver mica
units or Panasonic ±2% PPS film capacitors are recommended.
Rev. E | Page 21 of 24
Page 22
AD627 Data Sheet
V
OUT
V
DIFF
+V
S
–V
S
V
REF
0.1µF
0.1µF
AD627
R
G =
200kΩ
GAIN–5
00782-048
V
OUT
5V
V
REF
0.1µF
AD627
R
G
2.1kΩ
J-TYPE
THERMOCOUPLE
REF
00782-050
APPLICATIONS CIRCUITS
CLASSIC BRIDGE CIRCUIT
Figure 50 shows the AD627 configured to amplify the signal
from a classic resistive bridge. This circuit works in dual-supply
mode or single-supply mode. Typically, the same voltage that
powers the instrumentation amplifiers excites the bridge.
Connecting the bottom of the bridge to the negative supply of
the instrumentation amplifiers (usually 0 V, −5 V, −12 V, or
−15 V), sets up an input common-mode voltage that is
optimally located midway between the supply voltages. It is
also appropriate to set the voltage on the REF pin to midway
between the supplies, especially if the input signal is bipolar.
However, the voltage on the REF pin can be varied to suit the
application. For example, the REF pin is tied to the V
an analog-to-digital converter (ADC) whose input range is
(V
± VIN). With an available output swing on the AD627 of
REF
(−V
+ 100 mV) to (+VS − 150 mV), the maximum programmable
S
gain is simply this output range divided by the input range.
Figure 50. Classic Bridge Circuit
REF
pin of
4 mA TO 20 mA SINGLE-SUPPLY RECEIVER
Figure 51 shows how a signal from a 4 mA to 20 mA transducer
can be interfaced to the ADuC812, a 12-bit ADC with an
embedded microcontroller. The signal from a 4 mA to 20 mA
transducer is single-ended, which initially suggests the need for
a simple shunt resistor to convert the current to a voltage at the
high impedance analog input of the converter. However, any
line resistance in the return path (to the transducer) adds a
current dependent offset error; therefore, the current must be
sensed differentially.
In this example, a 24.9 Ω shunt resistor generates a maximum
differential input voltage to the AD627 of between 100 mV
(for 4 mA in) and 500 mV (for 20 mA in). With no gain resistor
present, the AD627 amplifies the 500 mV input voltage by a
factor of 5, to 2.5 V, the full-scale input voltage of the ADC. The
zero current of 4 mA corresponds to a code of 819 and the LSB
size is 4.88 μA.
THERMOCOUPLE AMPLIFIER
Because the common-mode input range of the AD627 extends
0.1 V below ground, it is possible to measure small differential
signals that have a low, or no, common-mode component.
Figure 51 shows a thermocouple application where one side of
the J-type thermocouple is grounded.
Over a temperature range from −200°C to +200°C, the J-type
thermocouple delivers a voltage ranging from −7.890 mV to
+10.777 mV. A programmed gain on the AD627 of 100 (R
2.1 kΩ) and a voltage on the AD627 REF pin of 2 V result in the
output voltage of the AD627 ranging from 1.110 V to 3.077 V
relative to ground. For a different input range or different
voltage on the REF pin, it is important to verify that the voltage
on Internal Node A1 (see Figure 37) is not driven below
ground. This can be checked using the equations in the Input
Range Limitations in Single-Supply Applications section.
=
G
Figure 51. Amplifying Bipolar Signals with Low Common-Mode Voltage
Rev. E | Page 22 of 24
Page 23
Data Sheet AD627
0.1µF
5V
0.1µF
5V
0.1µF
5V
V
REF
AD627
AD627
ADuC812
MICROCONVERTER
®
AGNDDGND
AV
DD
AIN 0
to AIN 7
REF
LINE
IMPEDANCE
DV
DD
4–20mA24. 9ΩG = +5
4–20mA
TRANSDUCER
00782-049
Figure 52. 4 mA to 20 mA Receiver Circuit
Rev. E | Page 23 of 24
Page 24
AD627 Data Sheet
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 DI M ENS I ONS ARE IN INCHES ; M I L LIMETER DIME NS I O NS
(IN PARENTHESES) ARE ROUNDED-OFF I NCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPRO P RIATE 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.
Figure 54. 8-Lead Small Standard Outline Package [SOIC_N]
5.00(0.1968)
4.80(0.1890)
85
1
1.27 (0.0500)
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDSMS-012-AA
BSC
6.20 (0.2441)
5.80 (0.2284)
4
1.75 (0.0688)
1.35 (0.0532)
0.51 (0.0201)
0.31 (0.0122)
8°
0°
0.25 (0.0098)
0.17 (0.0067)
Narrow Body (R-8)
Dimensions shown in millimeters (and inches)
0.50 (0.0196)
0.25 (0.0099)
1.27 (0.0500)
0.40 (0.0157)
45°
012407-A
ORDERING GUIDE
Model1 Temperature Range Package Description Package Option
AD627ANZ −40°C to +85°C 8-Lead Plastic Dual In-Line Package [PDIP] N-8
AD627AR −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627AR-REEL −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627AR-REEL7 −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627ARZ −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627ARZ-R7 −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627ARZ-RL −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627BNZ −40°C to +85°C 8-Lead Plastic Dual In-Line Package [PDIP] N-8
AD627BR −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627BR-REEL −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627BR-REEL7 −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627BRZ −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627BRZ-RL −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8
AD627BRZ-R7 −40°C to +85°C 8-Lead Small Standard Outline [SOIC_N] R-8