AD625
REV. D
–9–
Any resistors in series with the inputs of the AD625 will degrade
the noise performance. For this reason the circuit in Figure 26b
should be used if the gains are all greater than 5. For gains less
than 5, either the circuit in Figure 26a or in Figure 26c can be
used. The two 1.4 k resistors in Figure 26a will degrade the
noise performance to:
4 kTR
ext
+(4 nV/ Hz )
2
= 7.9 nV / Hz
RESISTOR PROGRAMMABLE GAIN AMPLIFIER
In the resistor-programmed mode (Figure 27), only three exter-
nal resistors are needed to select any gain from 1 to 10,000.
Depending on the application, discrete components or a
pretrimmed network can be used. The gain accuracy and gain
TC are primarily determined by the external resistors since the
AD625C contributes less than 0.02% to gain error and under
5 ppm/°C gain TC. The gain sense current is insensitive to
common-mode voltage, making the CMRR of the resistor pro-
grammed AD625 independent of the match of the two feedback
resistors, R
F
.
Selecting Resistor Values
As previously stated each R
F
provides feedback to the input
stage and sets the unity gain transconductance. These feedback
resistors are provided by the user. The AD625 is tested and
specified with a value of 20 k for R
F
. Since the magnitude of
RTO errors increases with increasing feedback resistance, values
much above 20 k are not recommended (values below 10 k
for R
F
may lead to instability). Refer to the graph of RTO noise,
offset, drift, and bandwidth (Figure 28) when selecting the
feedback resistors. The gain resistor (R
G
) is determined by the
formula R
G
= 2 R
F
/(G l).
+GAIN
SENSE
GAIN
SENSE
+INPUT INPUT
RTI NULL
RTI NULL
RTO
NULL
RTO
NULL
+V
S
+GAIN DRIVE GAIN DRIVE
R
F
R
G
R
F
NC
REF
V
S
V
OUT
+V
S
G = +1
2R
F
R
G
A1 A2
AD625
10k
10k 10k
10k
A3
1
2
3
4
5
6
7
8
16
15
14
13
12
11
10
9
Figure 27. AD625 in Fixed Gain Configuration
A list of standard resistors which can be used to set some com-
mon gains is shown in Table I.
For single gain applications, only one offset null adjust is neces-
sary; in these cases the RTI null should be used.
RTO OFFSET VOLTAGE DRIFT
6
5
4
3
2
1
60k50k40k30k20k10k
MULTIPLYING FACTOR
BANDWIDTH
1M
100k
10k
1 10 100 1k
FREQUENCY Hz
10k
20k
50k
FEEDBACK RESISTANCE FEEDBACK RESISTANCE
RTO NOISE RTO OFFSET VOLTAGE
300
200
100
3
2
10k 20k 30k 40k 50k 60k 10k 20k 30k 40k 50k 60k
VOLTAGE NOISE nV Hz
MULTIPLYING FACTOR
FEEDBACK RESISTANCE FEEDBACK RESISTANCE
Figure 28. RTO Noise, Offset, Drift and Bandwidth vs.
Feedback Resistance Normalized to 20 k
Table I. Common Gains Nominally Within 0.5% Error
Using Standard 1% Resistors
GAIN R
F
R
G
1 20 kΩ∞
2 19.6 k 39.2 k
5 20 k 10 k
10 20 k 4.42 k
20 20 k 2.1 k
50 19.6 k 806
100 20 k 402
200 20.5 k 205
500 19.6 k 78.7
1000 19.6 k 39.2
4 20 k 13.3 k
8 19.6 k 5.62 k
16 20 k 2.67 k
32 19.6 k 1.27 k
64 20 k 634
128 20 k 316
256 19.6 k 154
512 19.6 k 76.8
1024 19.6 k 38.3
SENSE TERMINAL
The sense terminal is the feedback point for the AD625 output
amplifier. Normally it is connected directly to the output. If
heavy load currents are to be drawn through long leads, voltage
drops through lead resistance can cause errors. In these in-
stances the sense terminal can be wired to the load thus putting
AD625
REV. D–10–
the I × R drops inside the loop and virtually eliminating this
error source.
Typically, IC instrumentation amplifiers are rated for a full ±10
volt output swing into 2 k. In some applications, however, the
need exists to drive more current into heavier loads. Figure 29
shows how a high-current booster may be connected inside the
loop of an instrumentation amplifier. By using an external
power boosting circuit, the power dissipated by the AD625 will
remain low, thereby, minimizing the errors induced by self-
heating. The effects of nonlinearities, offset and gain inaccura-
cies of the buffer are reduced by the loop gain of the AD625s
output amplifier.
AD625
+V
S
V
S
R
F
R
G
R
F
V
IN
+
V
IN
R
I
SENSE
REFERENCE
X1
Figure 29. AD625 /Instrumentation Amplifier with Output
Current Booster
REFERENCE TERMINAL
The reference terminal may be used to offset the output by up
to ±10 V. This is useful when the load is floating or does not
share a ground with the rest of the system. It also provides a
direct means of injecting a precise offset. However, it must be
remembered that the total output swing is ±10 volts, from
ground, to be shared between signal and reference offset.
The AD625 reference terminal must be presented with nearly
zero impedance. Any significant resistance, including those
caused by PC layouts or other connection techniques, will in-
crease the gain of the noninverting signal path, thereby, upset-
ting the common-mode rejection of the in-amp. Inadvertent
thermocouple connections created in the sense and reference
lines should also be avoided as they will directly affect the out-
put offset voltage and output offset voltage drift.
In the AD625 a reference source resistance will unbalance the
CMR trim by the ratio of 10 k/R
REF
. For example, if the refer-
ence source impedance is 1 , CMR will be reduced to 80 dB
(10 k/1 = 80 dB). An operational amplifier may be used to
provide the low impedance reference point as shown in Figure
30. The input offset voltage characteristics of that amplifier will
add directly to the output offset voltage performance of the
instrumentation amplifier.
The circuit of Figure 30 also shows a CMOS DAC operating in
the bipolar mode and connected to the reference terminal to
provide software controllable offset adjustments. The total offset
range is equal to ±(V
REF
/2 × R5/R4), however, to be symmetri-
cal about 0 V R3 = 2 × R4.
The offset per bit is equal to the total offset range divided by 2
N
,
where N = number of bits of the DAC. The range of offset for
Figure 30 is ±120 mV, and the offset is incremented in steps of
0.9375 mV/LSB.
AD625
+V
S
V
S
V
OUT
SENSE
AD7502
A
0
A
1
E
N
GND V
DD
V
SS
+IN
IN
1/2
AD712
1/2
AD712
REFERENCE
V
REF
AD589 1.2V
V
S
39k
MSB
LSB
DATA
INPUTS
CS
WR
+V
S
AD7524
8-BIT DAC
R
FB
C
1
OUT 1
OUT 2
+V
S
R4
10k
R3
20k
5k
V
S
R5
2k
0.01F
Figure 30. Software Controllable Offset
An instrumentation amplifier can be turned into a voltage-to-
current converter by taking advantage of the sense and reference
terminals as shown in Figure 31.
AD625
R
F
R
G
R
F
V
IN
+
V
IN
SENSE
I
L
AD711
LOAD
+V
X
R1
Figure 31. Voltage-to-Current Converter
By establishing a reference at the low side of a current setting
resistor, an output current may be defined as a function of input
voltage, gain and the value of that resistor. Since only a small
current is demanded at the input of the buffer amplifier A1, the
forced current I
L
will largely flow through the load. Offset and
drift specifications of A2 must be added to the output offset and
drift specifications of the In-Amp.
INPUT AND OUTPUT OFFSET VOLTAGE
Offset voltage specifications are often considered a figure of
merit for instrumentation amplifiers. While initial offset may be
adjusted to zero, shifts in offset voltage due to temperature
variations will cause errors. Intelligent systems can often correct
for this factor with an autozero cycle, but this requires extra
circuitry.
AD625
REV. D
–11–
Offset voltage and offset voltage drift each have two compo-
nents: input and output. Input offset is that component of offset
that is generated at the input stage. Measured at the output it is
directly proportional to gain, i.e., input offset as measured at the
output at G = 100 is 100 times greater than that measured at
G = 1. Output offset is generated at the output and is constant
for all gains.
The input offset and drift are multiplied by the gain, while the
output terms are independent of gain, therefore, input errors
dominate at high gains and output errors dominate at low gains.
The output offset voltage (and drift) is normally specified at
G = 1 (where input effects are insignificant), while input offset
(and drift) is given at a high gain (where output effects are negli-
gible). All input-related parameters are specified referred to the
input (RTI) which is to say that the effect on the output is G
times larger. Offset voltage vs. power supply is also specified as
an RTI error.
By separating these errors, one can evaluate the total error inde-
pendent of the gain. For a given gain, both errors can be com-
bined to give a total error referred to the input (RTI) or output
(RTO) by the following formula:
Total Error RTI = input error + (output error/gain)
Total Error RTO = (Gain × input error) + output error
The AD625 provides for both input and output offset voltage
adjustment. This simplifies nulling in very high precision appli-
cations and minimizes offset voltage effects in switched gain
applications. In such applications the input offset is adjusted
first at the highest programmed gain, then the output offset is
adjusted at G = 1. If only a single null is desired, the input offset
null should be used. The most additional drift when using only
the input offset null is 0.9 µV/°C, RTO.
COMMON-MODE REJECTION
Common-mode rejection 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.
In an instrumentation amplifier, degradation of common-mode
rejection is caused by a differential phase shift due to differences
in distributed stray capacitances. In many applications shielded
cables are used to minimize noise. This technique can create
AD625
+V
S
V
S
R
F
R
G
R
F
SENSE
REFERENCE
AD711
V
OUT
+INPUT
INPUT
100
Figure 32. Common-Mode Shield Driver
common-mode rejection errors unless the shield is properly
driven. Figures 32 and 33 show active data guards which are
configured to improve ac common-mode rejection by boot-
strapping the capacitances of the input cabling, thus minimiz-
ing differential phase shift.
AD625
+V
S
V
S
R
F
R
G
R
F
AD712
100
100
V
OUT
SENSE
REFERENCE
INPUT
+INPUT
V
S
Figure 33. Differential Shield Driver
GROUNDING
In order to isolate low level analog signals from a noisy digital
environment, many data-acquisition components have two or
more ground pins. These grounds must eventually be tied to-
gether at one point. 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 mini-
mize the current flow from the sensitive points to the system
ground (see Figure 34). Since the AD625 output voltage is
developed with respect to the potential on the reference termi-
nal, it can solve many grounding problems.
AD625
AD7502
V
S
+V
S
V
S
+V
S
AD583
SAMPLE
AND
HOLD
HOLD
CAP
V
S
+V
S
INPUT
SIGNAL
STATUS
ANALOG
OUT
V
S
+V
S
DIGITAL
COMMON
V
LOGIC
ANALOG POWER
GROUND
AD574A
A/D
CONVERTER
Figure 34. Basic Grounding Practice for a Data Acquisition System

5962-8771901EA

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Instrumentation Amplifiers PROGRAMMABLE GAIN IN-AMP
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union