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AD524AR

Part # AD524AR
Description
Category IC
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Technical Document


DISCLAIMER: The information provided herein is solely for informational purposes. Customers must be aware of the suitability of this product for their application, and consider that variable factors such as Manufacturer, Product Category, Date Codes, Pictures and Descriptions may differ from available inventory.

AD524
REV. E–10–
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, appear as an offset voltage. What is of concern in calculat-
ing bias current errors is the change in bias current with respect to
signal voltage and temperature. Input offset current is the differ-
ence between the two input bias currents. The effect of offset
current is an input offset voltage whose magnitude is the offset
current times the source impedance imbalance.
–V
S
+V
S
AD524
LOAD
TO POWER
SUPPLY
GROUND
a. Transformer Coupled
AD524
LOAD
TO POWER
SUPPLY
GROUND
–V
S
+V
S
b. Thermocouple
AD524
LOAD
TO POWER
SUPPLY
GROUND
–V
S
+V
S
c. AC Coupled
Figure 34. Indirect Ground Returns for Bias Currents
Table I. Output Gain Resistor Values
Output Nominal
Gain R2 R1, R3 Gain
25 k 2.26 k 2.02
5 1.05 k 2.05 k 5.01
10 1 k 4.42 k 10.1
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.
COMMON-MODE REJECTION
Common-mode rejection is a measure of the change in output
voltage when both inputs are changed 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 35 and 36 shows active data
guards that are configured to improve ac common mode rejec-
tion by “bootstrapping” the capacitances of the input cabling,
thus minimizing differential phase shift.
V
OUT
REFERENCE
AD524
–V
S
+V
S
100V
AD711
G = 100
RG
2
+INPUT
–INPUT
Figure 35. Shield Driver, G
100
V
OUT
REFERENCE
AD524
–V
S
+V
S
100V
AD712
RG
2
+INPUT
–INPUT
–V
S
RG
1
100V
Figure 36. Differential Shield Driver
GROUNDING
Many data acquisition components have two or more ground
pins that 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
AD524
REV. E –11–
acquisition components. Separate ground returns should be
provided to minimize the current flow in the path from the sensi-
tive 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.
Since the output voltage is developed with respect to the poten-
tial on the reference terminal, an instrumentation amplifier can
solve many grounding problems.
0.1
mF
0.1
mF
DIGITAL P.S.
+5V
C–15V
ANALOG P.S.
1mF
DIG
COM
AD574A
C+15V
6
OUTPUT
REFERENCE
*ANALOG
GROUND
AD524
DIGITAL
DATA
OUTPUT
SIGNAL
GROUND
*IF INDEPENDENT; OTHERWISE RETURN AMPLIFIER REFERENCE
TO MECCA AT ANALOG P.S. COMMON
1mF1mF
0.1
mF
0.1
mF
AD583
SAMPLE
AND HOLD
Figure 37. Basic Grounding Practice
SENSE TERMINAL
The sense terminal is the feedback point for the instrument
amplifier’s 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.
V–
V+
X1
AD524
OUTPUT
CURRENT
BOOSTER
(REF)
(SENSE)
R
L
V
IN
+
V
IN
Figure 38. AD524 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, however, the
need exists to drive more current into heavier loads. Figure 38
shows how a high-current booster may be connected “inside the
loop” of an instrumentation amplifier to provide the required
current boost without significantly degrading overall perfor-
mance. Nonlinearities, offset and gain inaccuracies of the buffer
are minimized by the loop gain of the IA output amplifier. Off-
set 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 to be shared be-
tween signal and reference 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 from the reference terminal to ground
increases the gain of the noninverting signal path, thereby upset-
ting the common-mode rejection of the IA.
In the AD524 a reference source resistance will unbalance the
CMR trim by the ratio of 20 k/R
REF
. For example, if the refer-
ence source impedance is 1 , CMR will be reduced to 86 dB
(20 k/1 = 86 dB). An operational amplifier may be used to
provide that low impedance reference point as shown in Figure
39. The input offset voltage characteristics of that amplifier will
add directly to the output offset voltage performance of the
instrumentation amplifier.
–V
S
+V
S
AD524
REF
SENSE
LOAD
V
IN
+
V
IN
V
OFFSET
AD711
Figure 39. Use of Reference Terminal to Provide Output
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 40.
AD524
REF
SENSE
LOAD
AD711
+INPUT
–INPUT
R1
V
X
I
L
V
X
R1
I
L
= =
= (1 +
V
IN
R1
)
40,000
R
G
A2
Figure 40. 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 A
2
, the
forced current I
L
will largely flow through the load. Offset and
drift specifications of A
2
must be added to the output offset and
drift specifications of the IA.
AD524
REV. E–12–
PROGRAMMABLE GAIN
Figure 41 shows the AD524 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.
The AD524 can also be connected for gain in the output stage.
Figure 42 shows an AD711 used as an active attenuator in the
output amplifier’s feedback loop. The active attenuation pre-
sents a very low impedance to the feedback resistors, therefore
minimizing the common-mode rejection ratio degradation.
R2
10kV
1mF
35V
–V
S
OUTPUT
OFFSET
NULL
+V
S
TO –V
AD524
1
2
3
4
5
6
7
8
16
15
14
13
12
11
10
9
20kV
20kV
20kV
404V
4.44kV
20kV
+V
S
20kV
20kV
40V
PROTECTION
PROTECTION
–IN
+IN
(+INPUT)
(–INPUT)
10kV
INPUT
OFFSET
NULL
10pF
20kV
AD711
–V
S
+V
S
AD7590
V
SS
V
DD
GND
39.2kV
28.7kV
316kV
1kV
1kV
1kV
V
DD
A2 A3
A4
WR
V
OUT
Figure 42. Programmable Output Gain
Y0
Y2
Y1
+5V
INPUT
OFFSET
TRIM
C1
C2
ANALOG
COMMON
A
B
INPUTS
GAIN
RANGE
LOGIC
COMMON
+5V
G = 10
K1
G = 100
K2
G = 1000
K3
RELAY
SHIELDS
–IN
+IN
–V
S
K1 – K3 =
THERMOSEN DM2C
4.5V COIL
D1 – D3 = IN4148
OUT
K1
K2
K3D1
D2
D3
10mF
NC
GAIN TABLE
A
B
GAIN
0
0
1
1
0
1
0
1
10
1000
100
1
OUTPUT
OFFSET
TRIM
R2
10kV
+V
S
74LS138
DECODER
7407N
BUFFER
DRIVER
1mF
35V
NC = NO CONNECT
R1
10kV
A1
AD524
1
2
3
4
5
6
7
8
20kV
20kV
20kV
404V
4.44kV
20kV
+V
S
20kV
20kV
40V
PROTECTION
PROTECTION
16
15
14
13
12
11
10
9
Figure 41. Three Decade Gain Programmable Amplifier
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