AD8293G80/AD8293G160
Rev. 0 | Page 10 of 16
THEORY OF OPERATION
The AD8293G80/AD8293G160 are precision current-mode
correction instrumentation amplifiers capable of single-supply
operation. The current-mode correction topology results in
excellent accuracy. Figure 18 shows a simplified diagram
illustrating the basic operation of the AD8293G80/AD8293G160
(without correction). The circuit consists of a voltage-to-current
amplifier (M1 to M6), followed by a current-to-voltage amplifier
(R2 and A1). Application of a differential input voltage forces a
current through External Resistor R1, resulting in conversion of
the input voltage to a signal current. Transistor M3 to Transistor
M6 transfer twice this signal current to the inverting input of
the op amp A1. Amplifier A1 and External Resistor R2 form
a current-to-voltage converter to produce a rail-to-rail output
voltage at V
OUT
.
Op amp A1 is a high precision auto-zero amplifier. This amplifier
preserves the performance of the autocorrecting, current-mode
amplifier topology while offering the user a true voltage-in,
voltage-out instrumentation amplifier. Offset errors are corrected
internally.
An external reference voltage is applied to the noninverting
input of A1 to set the output reference level. External Capacitor
C2 is used to filter out correction noise.
HIGH PSR AND CMR
Common-mode rejection and power supply rejection indicate
the amount that the offset voltage of an amplifier changes when
its common-mode input voltage or power supply voltage changes.
The autocorrection architecture of the AD8293G80/AD8293G160
continuously corrects for offset errors, including those induced
by changes in input or supply voltage, resulting in exceptional
rejection performance. The continuous autocorrection provides
great CMR and PSR performances over the entire operating
temperature range (−40°C to +85°C).
The parasitic resistance in series with R2 does not degrade CMR,
but causes a small gain error and a very small offset error.
Therefore, an external buffer amplifier is not required to drive
V
REF
to maintain excellent CMR performance. This helps reduce
system costs over conventional instrumentation amplifiers.
1/f NOISE CORRECTION
Flicker noise, also known as 1/f noise, is noise inherent in the
physics of semiconductor devices and decreases 10 dB per decade.
The 1/f corner frequency of an amplifier is the frequency at which
the flicker noise is equal to the broadband noise of the amplifier. At
lower frequencies, flicker noise dominates, causing large errors
in low frequency or dc applications.
Flicker noise is seen effectively as a slowly varying offset
error, which is reduced by the autocorrection topology of the
AD8293G80/AD8293G160. This allows the AD8293G80/
AD8293G160 to have lower noise near dc than standard low
noise instrumentation amplifiers.
II
I – I
R1
M2
V
INP
M3 M4
M1
R1
(V
INP
– V
INN
)
I
R1
=
R1
2I
2I
V
INN
V
BIAS
M5
M6
I – I
R1
I + I
R1
2I
R1
C2
R2
R3
A1
V
INP
– V
INN
R1
2R2
V
OUT
= V
REF
V
REF
EXTERNAL
+
07451-020
V
CC
C3
Figure 18. Simplified Schematic
AD8293G80/AD8293G160
Rev. 0 | Page 11 of 16
APPLICATIONS INFORMATION
OVERVIEW
The AD8293G80/AD8293G160 reduce board area by integrating
filter components, such as Resistors R1, R2, and R3, as shown in
Figure 19. Two outputs are available to the user: OUT (Pin 6) and
ADC OUT (Pin 4). The difference between the two is the inclusion
of a series 5 k resistor at ADC OUT. With the addition of an
external capacitor, C3, ADC OUT forms a second filter, comprising
of the 5 k resistor and C3, which can be used as an ADC anti-
aliasing filter. In contrast, OUT is the direct output of the instru-
mentation amplifier. When using the antialiasing filter, there is
slightly less switching ripple at ADC OUT than when obtaining
the signal directly from OUT.
+5
V
0.1µF
0.1µF
+5V
1
8
7 5 6
4
ADC OUT
OUTPUT TO ADC
WITH ANTIALIASING
FILTER
FILT+V
S
–IN
+IN
R1
4k
R2
320k
R3
5k
100k
100k
C3
39nF
OUT
C2
680pF
07451-021
AD8293G160
REFGND
32
IN-AMP
Figure 19. AD8293G160 with Antialiasing Filter and Level-Shifted Output
(Using the Resistor Divider at the REF Pin, the Output Is Biased at 2.5 V)
REFERENCE CONNECTION
Unlike traditional 3-op-amp instrumentation amplifiers, parasitic
resistance in series with REF (Pin 3) does not degrade CMR
performance. The AD8293G80/AD8293G160 can attain extremely
high CMR performance without the use of an external buffer
amplifier to drive the REF pin, which is required by industry-
standard instrumentation amplifiers. Reducing the need for
buffer amplifiers to drive the REF pin helps to save valuable
printed circuit board (PCB) space and minimizes system costs.
For optimal performance in single-supply applications, REF
should be set with a low noise precision voltage reference, such
as the ADR44x (see Figure 20). However, for a lower system cost,
the reference voltage can be set with a simple resistor voltage
divider between the supply and GND (see Figure 19). This
configuration results in degraded output offset performance if
the resistors deviate from their ideal values. In dual-supply
applications, V
REF
can simply be connected to GND.
The REF pin current is approximately 10 pA, and as a result, an
external buffer is not required.
1µF0.1µF
0.1µF
VOLTAGE
REFERENCE
+5
V
0.1µF
1
8
7
5 6
4
ADC OUT
OUTPUT
FILT+V
S
–IN
+IN
R1
4k
R2
R3
5k
OUT
C2
07451-022
AD8293Gxx
REFGND
32
IN-AMP
Figure 20. Operating on a Single Supply Using an External Voltage Reference
(The Output Can Be Used Without an Antialiasing Filter if the Signal
Bandwidth Is <10 Hz)
OUTPUT FILTERING
The output of the AD8293G80/AD8293G160 can be filtered to
reduce switching ripple. Two filters can be used in conjunction
to set the filter frequency. In the example that follows, two 700 Hz
filters are used in conjunction to form a 500 Hz (recommended)
bandwidth. Because the filter resistors are integrated in the
AD8293G80/AD8293G160, only external capacitors are needed
to set the filter frequencies.
The primary filter is needed to limit the amount of switching
noise at the output. Regardless of the output that is being used,
OUT or ADC OUT, the primary filter comprising R2 and C2
must be implemented. The R2 value depends on the model; Table 7
shows the R2 value for each model.
Table 7. Internal R2 Values
Model R2 (kΩ)
AD8293G80 160
AD8293G160 320
The following equation results in the C2 value needed to set a
700 Hz primary filter. For a gain of 160, substitute R2 with
320 k; for a gain of 80, substitute R2 with 160 k.
C2 = 1/(700 × 2 × π × R2)
Adding an external capacitor, C3, and measuring the output from
ADC OUT further reduces the correction ripple. The internal
5 kΩ resistor, labeled R3 in Figure 18, forms a low-pass filter
with C3. This low-pass filter is the secondary filter. Set to
700 Hz, the secondary filter equation for C3 is as follows:
C3 = 1/(700 × 2 × π × 5 k)
AD8293G80/AD8293G160
Rev. 0 | Page 12 of 16
he addition of another single pole of 700 Hz on the output
hs
C3 (nF)
T
(from the secondary filter in Figure 18) is required for bandwidt
greater than 10 Hz. These two filters, together, produce an overall
bandwidth of 500 Hz. The internal resistors, R2 and R3, have an
absolute tolerance of 20%. Tabl e 8 lists the standard capacitors
needed to create a filter with an overall bandwidth of 500 Hz.
Table 8. Standard Capacitors Used to Form a Filter with an
Overall Bandwidth of 500 Hz
Model C2 (pF)
AD8293G80 1300 39
AD8293G160 680 39
For applications with low bandwi ths (<10 Hz), only the primary
H
use two synchronized clocks
ncies can be observed at
d
filter is required. In such an event, the high frequency noise
from the auto-zero amplifier (output amplifier) is not filtered
before the following stage.
CLOCK FEEDTHROUG
The AD8293G80/AD8293G160
to perform the autocorrection. The input voltage-to-current
amplifiers are corrected at 60 kHz.
Trace amounts of these clock freque
the OUT pin. The amount of visible correction feedthrough
is dependent on the values of the filters set by R2/C2. Use
ADC OUT to create a filter using R3/C3 to further reduce
correction feedthrough as described in the Output Filtering
section.
POWER SUPPLY BYPASSING
The AD8293G80/AD8293G160 use internally generated clock
signals to perform autocorrection. As a result, proper bypassing
is necessary to achieve optimum performance. Inadequate or
improper bypassing of the supply lines can lead to excessive
noise and offset voltage.
A 0.1 µF surface-mount capacitor should be connected between
the supply lines. This capacitor is necessary to minimize ripple
from the correction clocks inside the IC. For dual-supply operation,
a 0.1 µF (ceramic) surface-mount capacitor should be connected
from each supply pin to GND.
For single-supply operation, a 0.1 µF surface-mount capacitor
should be connected from the supply line to GND.
All bypass capacitors should be positioned as close to the DUT
supply pins as possible, especially the bypass capacitor between
the supplies. Placement of the bypass capacitor on the back of
the board directly under the DUT is preferred.
INPUT OVERVOLTAGE PROTECTION
All terminals of the AD8293G80/AD8293G160 are protected
against ESD. In the case of a dc overload voltage beyond either
supply, a large current would flow directly through the ESD
protection diodes. If such a condition can occur, an external resistor
should be used in series with the inputs to limit current for voltages
beyond the supply rails. The AD8293G80/AD8293G160 can safely
handle 5 mA of continuous current, resulting in an external
resistor selection of
R
EXT
= (V
IN
V
S
)/5 mA
1
8
7 5 6
4
ADC OUT
FILT+V
S
I
1.8V
–IN
+IN
R1
4k
R2
160k
R
SHUNT
R3
5k
+3.3V
10µF
0.1µF
C3
39nF
OUT
C2
1.3nF
07451-023
AD8293G80
REFGND
32
IN-AMP
ADC
REF
LOAD
DC-DC
+5
V
0.1µF
Figure 21. Measuring Current Through a Shunt Resistor (Filter Is Set to 500 Hz)

AD8293G160ARJZ-R2

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Instrumentation Amplifiers Zero-Drift w/ Filter & Fixed Gain
Lifecycle:
New from this manufacturer.
Delivery:
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