REV. C
AD624
–9–
NOISE
The AD624 is designed to provide noise performance near the
theoretical noise floor. This is an extremely important design
criteria as the front end noise of an instrumentation amplifier is
the ultimate limitation on the resolution of the data acquisition
system it is being used in. There are two sources of noise in an
instrument amplifier, the input noise, predominantly generated
by the differential input stage, and the output noise, generated
by the output amplifier. Both of these components are present
at the input (and output) of the instrumentation amplifier. At
the input, the input noise will appear unaltered; the output
noise will be attenuated by the closed loop gain (at the output,
the output noise will be unaltered; the input noise will be ampli-
fied by the closed loop gain). Those two noise sources must be
root sum squared to determine the total noise level expected at
the input (or output).
The low frequency (0.1 Hz to 10 Hz) voltage noise due to the
output stage is 10 µV p-p, the contribution of the input stage is
0.2 µV p-p. At a gain of 10, the RTI voltage noise would be
1 µV p-p,
10
G
2
+ 0. 2
()
2
. The RTO voltage noise would be
10.2 µV p-p,
10
2
+ 0. 2 G
()
()
2
. These calculations hold for
applications using either internal or external gain resistors.
INPUT BIAS CURRENTS
Input bias currents are those currents necessary to bias the input
transistors of a dc amplifier. Bias currents are an additional
source of input error and must be considered in a total error
budget. The bias currents when multiplied by the source resis-
tance imbalance appear as an additional offset voltage. (What is
of concern in calculating bias current errors is the change in bias
current with respect to signal voltage and temperature.) Input
offset current is the difference between the two input bias cur-
rents. The effect of offset current is an input offset voltage whose
magnitude is the offset current times the source resistance.
AD624
V
S
+V
S
LOAD
TO
POWER
SUPPLY
GROUND
a. Transformer Coupled
AD624
V
S
+V
S
LOAD
TO
POWER
SUPPLY
GROUND
b. Thermocouple
AD624
V
S
+V
S
LOAD
TO
POWER
SUPPLY
GROUND
c. AC-Coupled
Figure 31. Indirect Ground Returns for Bias Currents
Although instrumentation amplifiers have differential inputs,
there must be a return path for the bias currents. If this is not
provided, those currents will charge stray capacitances, causing
the output to drift uncontrollably or to saturate. Therefore,
when amplifying floating input sources such as transformers
and thermocouples, as well as ac-coupled sources, there must
still be a dc path from each input to ground, (see Figure 31).
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. Common-Mode
Rejection Ratio (CMRR) is a ratio expression while Common-
Mode Rejection (CMR) is the logarithm of that ratio. For
example, a CMRR of 10,000 corresponds to a CMR of 80 dB.
In an instrumentation amplifier, ac common-mode rejection is
only as good as the differential phase shift. Degradation of ac
common-mode rejection is caused by unequal drops across
differing track resistances and a differential phase shift due to
varied stray capacitances or cable capacitances. In many appli-
cations shielded cables are used to minimize noise. This tech-
nique can create common-mode rejection errors unless the
shield is properly driven. Figures 32 and 33 shows active data
guards which are configured to improve ac common-mode
rejection by bootstrapping the capacitances of the input
cabling, thus minimizing differential phase shift.
AD624
RG
2
V
S
REFERENCE
V
OUT
INPUT
+INPUT
+V
S
G = 200
AD711
100
Figure 32. Shield Driver, G
100
AD624
RG
1
V
S
REFERENCE
V
OUT
INPUT
+INPUT
+V
S
V
S
AD712
100
100
RG
2
Figure 33. Differential Shield Driver
REV. C
AD624
–10–
GROUNDING
Many data-acquisition components have two or more ground
pins which are not connected together within the device. These
grounds must be tied together at one point, usually at the sys-
tem power supply ground. Ideally, a single solid ground would
be desirable. However, since current flows through the ground
wires and etch stripes of the circuit cards, and since these paths
have resistance and inductance, hundreds of millivolts can be
generated between the system ground point and the data acqui-
sition components. Separate ground returns should be provided
to minimize the current flow in the path from the most sensitive
points to the system ground point. In this way supply currents
and logic-gate return currents are not summed into the same
return path as analog signals where they would cause measure-
ment errors (see Figure 34).
OUTPUT
REFERENCE
ANALOG
GROUND*
*IF INDEPENDENT, OTHERWISE RETURN AMPLIFIER REFERENCE
TO MECCA AT ANALOG P.S. COMMON
SIGNAL
GROUND
AD574A
DIGITAL
DATA
OUTPUT
+
1
F
0.1
F
1
F1
F
DIG
COM
0.1
F
0.1
F
0.1
F
AD624
SAMPLE
AND HOLD
AD583
ANALOG P.S.
+15V C 15V
+5V
DIGITAL P.S.
C
Figure 34. Basic Grounding Practice
Since the output voltage is developed with respect to the poten-
tial on the reference terminal an instrumentation amplifier can
solve many grounding problems.
SENSE TERMINAL
The sense terminal is the feedback point for the instrument
amplifiers output amplifier. Normally it is connected to the
instrument amplifier output. If heavy load currents are to be
drawn through long leads, voltage drops due to current flowing
through lead resistance can cause errors. The sense terminal can
be wired to the instrument amplifier at the load thus putting the
IxR drops inside the loop and virtually eliminating this error
source.
AD624
V+
OUTPUT
CURRENT
BOOSTER
V
V
IN
+
V
IN
X1
R
L
(REF)
(SENSE)
Figure 35. AD624 Instrumentation Amplifier with Output
Current Booster
Typically, IC instrumentation amplifiers are rated for a full
±10 volt output swing into 2 k. In some applications, how-
ever, the need exists to drive more current into heavier loads.
Figure 35 shows how a current booster may be connected
inside the loop of an instrumentation amplifier to provide the
required current without significantly degrading overall perfor-
mance. The effects of nonlinearities, offset and gain inaccuracies
of the buffer are reduced by the loop gain of the IA output
amplifier. Offset drift of the buffer is similarly reduced.
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. It must be remem-
bered that the total output swing is ±10 volts, from ground, to
be shared between signal and reference offset.
AD624
V
IN
+
V
IN
REF
SENSE
LOAD
AD711
V
S
+V
S
V
OFFSET
Figure 36. Use of Reference Terminal to Provide Output
Offset
When the IA is of the three-amplifier configuration it is neces-
sary that nearly zero impedance be presented to the reference
terminal. Any significant resistance, including those caused by
PC layouts or other connection techniques, which appears
between the reference pin and ground will increase the gain of
the noninverting signal path, thereby upsetting the common-
mode rejection of the IA. Inadvertent thermocouple connections
created in the sense and reference lines should also be avoided
as they will directly affect the output offset voltage and output
offset voltage drift.
In the AD624 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 that low impedance reference point as shown in Figure
36. The input offset voltage characteristics of that amplifier will
add directly to the output offset voltage performance of the
instrumentation amplifier.
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 37.
AD624
+INPUT
REF
R
1
+V
X
SENSE
LOAD
AD711
A2
I
L
INPUT
40.000
R
G
1 +
I
L
= =
V
X
R
1
V
IN
R
1
Figure 37. Voltage-to-Current Converter
REV. C
AD624
–11–
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 A2, 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 IA.
PROGRAMMABLE GAIN
Figure 38 shows the AD624 being used as a software program-
mable gain amplifier. Gain switching can be accomplished with
mechanical switches such as DIP switches or reed relays. It
should be noted that the on resistance of the switch in series
with the internal gain resistor becomes part of the gain equation
and will have an effect on gain accuracy.
A significant advantage in using the internal gain resistors in a
programmable gain configuration is the minimization of thermo-
couple signals which are often present in multiplexed data
acquisition systems.
If the full performance of the AD624 is to be achieved, the user
must be extremely careful in designing and laying out his circuit
to minimize the remaining thermocouple signals.
The AD624 can also be connected for gain in the output stage.
Figure 39 shows an AD547 used as an active attenuator in the
output amplifiers feedback loop. The active attenuation pre-
sents a very low impedance to the feedback resistors therefore
minimizing the common-mode rejection ratio degradation.
Another method for developing the switching scheme is to use a
DAC. The AD7528 dual DAC which acts essentially as a pair of
switched resistive attenuators having high analog linearity and
symmetrical bipolar transmission is ideal in this application. The
multiplying DACs advantage is that it can handle inputs of
either polarity or zero without affecting the programmed gain.
The circuit shown uses an AD7528 to set the gain (DAC A) and
to perform a fine adjustment (DAC B).
V
DD
GND
225.3
124
4445.7
80.2
50
16
15
14
13
12
11
10
9
1
2
3
4
5
6
7
8
10k
20k
V
B
20k
10k
10k
50
V
S
+V
S
1F
35V
IN
+IN
10k
10k
INPUT
OFFSET
NULL
OUTPUT
OFFSET
NULL
10k
TO V
(+INPUT)
(INPUT)
V
OUT
39.2k
WRA4A3A2A1
V
SS
1k
10pF
+V
S
28.7k
316k
1k
1k
V
S
AD624
AD7590
AD711
Figure 39. Programmable Output Gain
225.3
124
4445.7
80.2
50
G = 100
K1
16
15
14
13
12
11
10
9
1
2
3
4
5
6
7
8
10k
20k
V
B
20k
10k
10k
50
V
S
+V
S
1F
35V
IN
+IN
R2
10k
R1
10k
INPUT
OFFSET
TRIM
OUTPUT
OFFSET
TRIM
RELAY
SHIELDS
G = 200
K2
G = 500
K3
D1 D2
D3
Y0
K2 K3
74LS138
DECODER
7407N
BUFFER
DRIVER
A
B
Y1
Y2
INPUTS
GAIN
RANGE
+5V
10F
C1 C2
K1 K3 =
THERMOSEN DM2C
4.5V COIL
D1 D3 = IN4148
ANALOG
COMMON
GAIN TABLE
A B GAIN
0 0 100
0 1 500
1 0 200
11 1
LOGIC
COMMON
K1
OUT
10k
+5V
AD624
NC
Figure 38. Gain Programmable Amplifier

AD624SD/883B

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