Datasheet
Table Of Contents
- Features
- Applications
- Functional Block Diagram
- General Description
- Table of Contents
- Specifications
- Absolute Maximum Ratings
- Pin Configurations and Function Descriptions
- Typical Performance Characteristics
- Theory of Operation
- Using the AD627
- Basic Connections
- Setting the Gain
- Reference Terminal
- Input Range Limitations in Single-Supply Applications
- Output Buffering
- Input and Output Offset Errors
- Make vs. Buy: A Typical Application Error Budget
- Errors Due to AC CMRR
- Ground Returns for Input Bias Currents
- Layout and Grounding
- Input Protection
- RF Interference
- Applications Circuits
- Outline Dimensions

Data Sheet AD627
Rev. E | Page 19 of 24
ERRORS DUE TO AC CMRR
In Table 9, the error due to common-mode rejection results
from the common-mode voltage from the bridge 2.5 V. T h 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 µ V.
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).
V
OUT
+5V
VIN–
VIN+
–5V
R1
9999.5Ω
R2
999.76Ω
R3
1000.2Ω
R4
9997.7Ω
1/2
OP296
A1
A2
1/2
OP296
00782-040
Figure 42. 0.1% Resistor Mismatch Example
FREQUENCY (Hz)
CMRR (dB)
120
1
110
100
90
80
70
60
50
40
30
20
10 100 1k 10k 100k
00782-041
Figure 43. CMRR over Frequency of Discrete In-Amp in Figure 42
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.
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
Figure 44. Ground Returns for Bias Currents with Transformer Coupled Inputs
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
Figure 45. Ground Returns for Bias Currents with Thermocouple Inputs
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
Figure 46. Ground Returns for Bias Currents with AC-Coupled Inputs