INA117P and INA117KU
ⴞ270 V Common-Mode Voltage Range
Input Protection to:
ⴞ500 V Common Mode
ⴞ500 V DifferentialWide Power Supply Range (ⴞ2.5 V to ⴞ18 V)
ⴞ10 V Output Swing on ⴞ12 V Supply
1 mA Max Power Supply Current
HIGH ACCURACY DC PERFORMANCE
3 ppm Max Gain Nonlinearity
20 V/ⴗC Max Offset Drift (AD629A)
10 V/ⴗC Max Offset Drift (AD629B)
10 ppm/ⴗC Max Gain Drift
EXCELLENT AC SPECIFICATIONS
77 dB Min CMRR @ 500 Hz (AD629A)
86 dB Min CMRR @ 500 Hz (AD629B)
500 kHz Bandwidth
APPLICATIONS
High Voltage Current Sensing
Battery Cell Voltage Monitor
Power Supply Current Monitor
Motor Control
Isolation
Difference Amplifier
AD629
FUNCTIONAL BLOCK DIAGRAM
8-Lead Plastic Mini-DIP (N) and SOIC (R) Packages
REF(–)
–V
–IN
+IN
380k⍀
2
380k⍀
3
4
S
21.1k⍀
1
GENERAL DESCRIPTION
The AD629 is a difference amplifier with a very high input
common-mode voltage range. It is a precision device that
allows the user to accurately measure differential signals in the
presence of high common-mode voltages up to ±270 V.
The AD629 can replace costly isolation amplifiers in applications
that do not require galvanic isolation. The device will operate
over a ±270 V common-mode voltage range and has inputs
that are protected from common-mode or differential mode
transients up to ±500 V.
The AD629 has low offset, low offset drift, low gain error drift,
as well as low common-mode rejection drift, and excellent CMRR
over a wide frequency range.
The AD629 is available in low-cost, plastic 8-lead DIP and
SOIC packages. For all packages and grades, performance is
guaranteed over the entire industrial temperature range from
–40°C to +85°C.
380k⍀
20k⍀
AD629
NC = NO CONNECT
NC
8
7
+V
6
OUTPUT
5
REF(+)
S
100
95
90
85
80
75
70
65
60
COMMON-MODE REJECTION RATIO – dB
55
50
20100
FREQUENCY – Hz
1k10k 20k
Figure 1. Common-Mode Rejection Ratio vs. Frequency
REV. A
Information furnished by Analog Devices is believed to be accurate and
reliable. However, no responsibility is assumed by Analog Devices for its
use, nor for any infringements of patents or other rights of third parties
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
2mV/DIV
OUTPUT ERROR – 2mV/DIV
60V/DIV
–240–120
COMMON-MODE VOLTAGE – Volts
0120240
Figure 2. Common-Mode Operating Range. Error Voltage
vs. Input Common-Mode Voltage
Operating Temperature Range . . . . . . . . . . –55°C to +125°C
Storage Temperature Range . . . . . . . . . . . . –65°C to +150°C
Lead Temperature Range (Soldering 60 sec) . . . . . . . . . 300°C
NOTES
1
Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent damage to the device. This is a stress rating only; functional operation of the
device at these or any other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute maximum rating
conditions for extended periods may effect device reliability.
2
Specification is for device in free air: 8-Lead Plastic DIP, θJA = 100°C/W; 8-Lead
SOIC Package, θJA = 155°C/W.
2.0
TJ = 150ⴗC
8-LEAD MINI-DIP PACKAGE
1.5
1.0
8-LEAD SOIC PACKAGE
0.5
MAXIMUM POWER DISSIPATION – Watts
0
–40 –30 –20 –100 102030405060708090
–50
AMBIENT TEMPERATURE – ⴗC
Figure 3. Derating Curve of Maximum Power Dissipation
vs. Temperature for SOIC and PDIP Packages
ORDERING GUIDE
THEORY OF OPERATION
The AD629 is a unity gain differential-to-single-ended amplifier
(Diff Amp) that can reject extremely high common-mode
signals (in excess of 270 V with 15 V supplies). It consists of an
operational amplifier (Op Amp) and a resistor network.
In order to achieve high common-mode voltage range, an internal
resistor divider (Pin 3, Pin 5) attenuates the noninverting signal
by a factor of 20. Other internal resistors (Pin 1, Pin 2, and the
feedback resistor) restores the gain to provide a differential gain
of unity. The complete transfer function equals:
V
= V (+IN ) – V (–IN )
OUT
Laser wafer trimming provides resistor matching so that commonmode signals are rejected while differential input signals are
amplified.
The op amp itself, in order to reduce output drift, uses super
beta transistors in its input stage The input offset current and
its associated temperature coefficient contribute no appreciable
output voltage offset or drift. This has the added benefit of
reducing voltage noise because the corner where 1/f noise becomes
dominant is below 5 Hz. In order to reduce the dependence of
gain accuracy on the op amp, the open-loop voltage gain of the
op amp exceeds 20 million, and the PSRR exceeds 140 dB.
REF(–)
–IN
+IN
–V
21.1k⍀
1
380k⍀
2
380k⍀
3
4
S
380k⍀
20k⍀
AD629
NC = NO CONNECT
NC
8
7
+V
6
OUTPUT
5
REF(+)
S
Figure 4. Functional Block Diagram
TemperaturePackagePackage
ModelRangeDescriptionOption
AD629AR–40°C to +85°C8-Lead Plastic SOICSO-8
AD629AR-REEL
AD629AR-REEL7
AD629BR–40°C to +85°C8-Lead Plastic SOICSO-8
AD629BR-REEL
AD629BR-REEL7
1
2
1
2
–40°C to +85°C8-Lead Plastic SOICSO-8
–40°C to +85°C8-Lead Plastic SOICSO-8
–40°C to +85°C8-Lead Plastic SOICSO-8
–40°C to +85°C8-Lead Plastic SOICSO-8
AD629AN–40°C to +85°C8-Lead Plastic DIPN-8
AD629BN–40°C to +85°C8-Lead Plastic DIPN-8
NOTES
1
13" Tape and Reel of 2500 each
2
7" Tape and Reel of 1000 each
CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily
accumulate on the human body and test equipment and can discharge without detection.
Although the AD629 features proprietary ESD protection circuitry, permanent damage may
occur on devices subjected to high energy electrostatic discharges. Therefore, proper ESD
precautions are recommended to avoid performance degradation or loss of functionality.
REV. A
–3–
Page 4
AD629
–Typical Performance Characteristics
(@25ⴗC, VS = ⴞ15 V unless otherwise noted)
100
90
80
70
60
50
40
30
20
COMMON-MODE REJECTION RATIO – dB
10
0
100
1k10k100k
FREQUENCY – Hz
1M10M
Figure 5. Common-Mode Rejection Ratio vs. Frequency
2mV/DIV
VS = ⴞ18V
VS = ⴞ15V
RL = 10k⍀
400
360
320
280
240
200
160
120
80
COMMON-MODE VOLTAGE – ⴞVolts
40
0
020
POWER SUPPLY VOLTAGE – ⴞVolts
TA = +85ⴗC
TA = +25ⴗC
TA = –40ⴗC
18161412108642
Figure 8. Common-Mode Operating Range vs. Power
Supply Voltage
RL = 2k⍀
VS = ⴞ18V
VS = ⴞ15V
VS = ⴞ12V
OUTPUT ERROR – 2mV/DIV
VS = ⴞ10V
–20–40 420
–8–12–1681216
V
– Volts
OUT
Figure 6. Typical Gain Error Normalized @ V
4V/DIV
= 0 V and
OUT
Output Voltage Operating Range vs. Supply Voltage,
RL = 10 kΩ (Curves Offset for Clarity)
RL = 1k⍀
VS = ⴞ18V
VS = ⴞ15V
VS = ⴞ12V
OUTPUT ERROR – 2mV/DIV
VS = ⴞ10V
–20–40 420
–8–12–1681216
V
– Volts
OUT
Figure 7. Typical Gain Error Normalized @ V
4V/DIV
OUT
= 0 V
and Output Voltage Operating Range vs. Supply Voltage,
= 1 kΩ (Curves Offset for Clarity)
R
L
VS = ⴞ12V
OUTPUT ERROR – 2mV/DIV
VS = ⴞ10V
–20–40 420
–8–12–1681216
V
– Volts
OUT
Figure 9. Typical Gain Error Normalized @ V
4V/DIV
= 0 V and
OUT
Output Voltage Operating Range vs. Supply Voltage,
= 2 kΩ (Curves Offset for Clarity)
R
L
VS = ⴞ5V, RL = 10k⍀
VS = ⴞ5V, RL = 2k⍀
= ⴞ5V, RL = 1k⍀
V
S
OUTPUT ERROR – 2mV/DIV
V
= ⴞ2.5V, RL = 1k⍀
S
–5–10 15
–2–3–4234
– Volts
V
OUT
Figure 10. Typical Gain Error Normalized @ V
1V/DIV
OUT
= 0 V
and Output Voltage Operating Range vs. Supply Voltage
(Curves Offset for Clarity)
–4–
REV. A
Page 5
AD629
OUTPUT CURRENT – mA
OUTPUT VOLTAGE – Volts
020
14.0
18161412108642
13.0
12.0
11.0
10.0
9.0
–12.0
–12.5
–13.0
–13.5
–11.5
–40ⴗC
–40ⴗC
+85ⴗC
+25ⴗC
VS = ⴞ15V
–40ⴗC
+85ⴗC
+25ⴗC
ERROR – 0.8ppm/DIV
–10–5
0510
V
– Volts
OUT
Figure 11. Gain Nonlinearity; VS = ±15 V, RL =10 k
ERROR – 1ppm/DIV
–10–20 210
–4–6–8468
V
– Volts
OUT
Figure 12. Gain Nonlinearity; VS = ±12 V, RL =10 k
ERROR – 2ppm/DIV
–10–20 210
Ω
Ω
Figure 14. Gain Nonlinearity; VS = ±15 V, RL = 2 k
Figure 15. Output Voltage Operating Range vs. Output
Current; V
= ±15 V
S
–4–6–8468
V
– Volts
OUT
Ω
ERROR – 6.67ppm/DIV
REV. A
–3.0–0.600.63.0
Figure 13. Gain Nonlinearity; VS = ±5 V, RL =1 k
–1.2–1.8–2.41.2 1.8 2.4
V
– Volts
OUT
Ω
Figure 16. Output Voltage Operating Range vs. Output
Current; V
–5–
11.5
10.5
–40ⴗC
9.5
8.5
7.5
6.5
–9.0
–9.5
OUTPUT VOLTAGE – Volts
–10.0
–10.5
–11.0
020
= ±12 V
S
+85ⴗC
VS = ⴞ12V
–40ⴗC
OUTPUT CURRENT – mA
–40ⴗC
+25ⴗC
+85ⴗC
+25ⴗC
+85ⴗC
18161412108642
Page 6
AD629
+85ⴗC
–40ⴗC
+85ⴗC
VS = ⴞ5V
+85ⴗC
–40ⴗC
+25ⴗC
020
+85ⴗC
OUTPUT CURRENT – mA
–40ⴗC
+25ⴗC
+25ⴗC
18161412108642
–2.0
–2.5
OUTPUT VOLTAGE – Volts
–3.0
–3.5
–4.0
4.5
3.5
2.5
1.5
0.5
Figure 17. Output Voltage Operating Range vs. Output
120
110
100
= ±5 V
S
+V
S
–V
S
90
80
70
60
50
40
30
Current; V
POWER SUPPLY REJECTION RATIO – dB
RL = 2k⍀
= 0pF
C
L
25mV/DIV
4s/DIV
Figure 20. Small Signal Pulse Response; G = 1, RL = 2 k
RL = 2k⍀
= 1000pF
C
L
25mV/DIV
4s/DIV
Ω
0.11
FREQUENCY – Hz
1001k1010k
Figure 18. Power Supply Rejection Ratio vs. Frequency
5.0
4.5
4.0
3.5
3.0
2.5
V/ Hz
2.0
1.5
1.0
0.5
0.11
0.01
FREQUENCY – Hz
1001k1010k100k
Figure 19. Voltage Noise Spectral Density vs. Frequency
Figure 21. Small Signal Pulse Response; G = 1, RL = 2 kΩ,
= 1000 pF
C
L
G = +1
= 2k⍀
R
L
= 1000pF
C
L
5V/DIV
5s/DIV
Figure 22. Large Signal Pulse Response; G = 1,
= 2 kΩ, CL = 1000 pF
R
L
–6–
REV. A
Page 7
AD629
+1 GAIN ERROR – ppm
350
0
–600
NUMBER OF UNITS
–400–2000
50
200
600
400
300
250
200
150
100
N = 2180
n ⬇ 200 PCS. FROM
10 ASSEMBLY LOTS
400
5V/DIV
+10V
V
OUT
0V
OUTPUT
ERROR
1mV/DIV
1mV = 0.01%
10s/DIV
Figure 23. Settling Time to 0.01%, For 0 V to 10 V Output
= 2 k
Step; G = –1, R
350
N = 2180
n ⬇ 200 PCS. FROM
300
10 ASSEMBLY LOTS
250
200
150
NUMBER OF UNITS
100
50
Ω
L
5V/DIV
0V
V
OUT
–10V
OUTPUT
ERROR
1mV/DIV
1mV = 0.01%
10s/DIV
Figure 26. Settling Time to 0.01% for 0 V to –10 V Output
Step; G = –1, R
300
250
200
150
100
NUMBER OF UNITS
50
= 2 k
Ω
L
N = 2180
⬇
200 PCS. FROM
n
10 ASSEMBLY LOTS
0
–150
–100–500
COMMON-MODE REJECTION RATIO – ppm
50
100
150
Figure 24. Typical Distribution of Common-Mode
Rejection; Package Option N-8
400
N = 2180
350
n ⬇ 200 PCS. FROM
10 ASSEMBLY LOTS
300
250
200
150
NUMBER OF UNITS
100
50
0
–600
–400–2000
–1 GAIN ERROR – ppm
200
400
600
Figure 25. Typical Distribution of –1 Gain Error;
Package Option N-8
0
–900
–600–3000
OFFSET VOLTAGE – V
300
600
900
Figure 27. Typical Distribution of Offset Voltage;
Package Option N-8
Figure 28. Typical Distribution of +1 Gain Error;
Package Option N-8
REV. A
–7–
Page 8
AD629
APPLICATIONS
Basic Connections
Figure 29 shows the basic connections for operating the AD629
with a dual supply. A supply voltage of between ±3 V and
±18 V is applied between Pins 7 and 4. Both supplies should be
decoupled close to the pins using 0.1 µF capacitors. 10 µF elec-
trolytic capacitors, also located close to the supply pins, may
also be required if low frequency noise is present on the power
supply. While multiple amplifiers can be decoupled by a single
set of 10 µF capacitors, each in amp should have its own set of
0.1 µF capacitors so that the decoupling point can be located
physically close to the power pins.
+V
S
8
7
6
5
NC
+V
REF(+)
3V TO 18V
0.1F
S
V
OUT
= I
(SEE
TEXT)
SHUNT
ⴛ R
SHUNT
I
SHUNT
TEXT)
(SEE
R
SHUNT
REF(–)
–IN
+IN
–V
S
0.1F
–V
S
–3V TO –18V
AD629
21.1k⍀
1
380k⍀
2
3
4
380k⍀
380k⍀
20k⍀
NC = NO CONNECT
Figure 29. Basic Connections
The differential input signal, which will typically result from a
load current flowing through a small shunt resistor, is applied to
Pins 2 and 3 with the polarity shown in order to obtain a positive gain. The common-mode range on the differential input
signal can range from –270 V to +270 V and the maximum differential range is ±13 V. When configured as shown, the device
operates as a simple gain-of-one differential-to-single-ended
amplifier, the output voltage being the shunt resistance times the
shunt current. The output is measured with respect to Pins 1 and 5.
Pins 1 and 5 (REF(–) and REF(+)) should be grounded for a
gain of unity and should be connected to the same low impedance ground plane. Failure to do this will result in degraded
common-mode rejection. Pin 8 is a no connect pin and should
be left open.
Single Supply Operation
Figure 30 shows the connections for operating the AD629 with
a single supply. Because the output can swing to within only
about 2 V of either rail, it is necessary to apply an offset to the
output. This can be conveniently done by connecting REF(+) and
REF(–) to a low impedance reference voltage (some analogto-digital converters provide this voltage as an output), which is
capable of sinking current. Thus, for a single supply of 10 V,
might be set to 5 V for a bipolar input signal. This would
V
REF
allow the output to swing ±3 V around the central 5 V reference
voltage. Alternatively, for unipolar input signals, V
could be
REF
set to about 2 V, allowing the output to swing from +2 V (for a 0 V
input) to within 2 V of the positive rail.
+V
NC
+V
S
REF(+)
S
0.1F
OUTPUT = V
OUT
–V
REF
I
SHUNT
R
SHUNT
AD629
REF(–)
V
REF
21.1k⍀
1
380k⍀
–IN
2
380k⍀
+IN
3
–V
S
4
NC = NO CONNECT
8
380k⍀
7
V
X
20k⍀
6
5
V
Y
Figure 30. Operation with a Single Supply
Applying a reference voltage to REF(+) and REF(–) and operating
on a single supply will reduce the input common-mode range of
the AD629. The new input common-mode range depends upon
the voltage at the inverting and noninverting inputs of the internal
operational amplifier, labeled V
and VY in Figure 30. These
X
nodes can swing to within 1 V of either rail. So for a (single)
supply voltage of 10 V, V
9 V. If V
is set to 5 V, the permissible common-mode range
REF
and VY can range between 1 V and
X
is +85 V to –75 V. The common-mode voltage ranges can be
calculated using the following equation.
VVV
±
=±
(
)
CMX YREF
−2019
(
)
/
System-Level Decoupling and Grounding
The use of ground planes is recommended to minimize the
impedance of ground returns (and hence the size of dc errors).
Figure 31 shows how to work with grounding in a mixed-signal
environment, that is, with digital and analog signals present. In
order to isolate low-level analog signals from a noisy digital
environment, many data-acquisition components have separate
analog and digital ground returns. All ground pins from mixedsignal components such as analog-to-digital converters should
be returned through the “high quality” analog ground plane.
This includes the digital ground lines of mixed-signal converters
that should also be connected to the analog ground plane. This
may seem to break the rule of keeping analog and digital grounds
separate, but in general, there is also a requirement to keep the
voltage difference between digital and analog grounds on a converter as small as possible (typically <0.3 V). The increased
noise, caused by the converter’s digital return currents flowing
through the analog ground plane, will typically be negligible.
Maximum isolation between analog and digital is achieved by
connecting the ground planes back at the supplies. Note that
Figure 31, as drawn, suggests a “star” ground system for the
analog circuitry, with all ground lines being connected, in this
case, to the ADC’s analog ground. However, when ground planes
are used, it is sufficient to connect ground pins to the nearest
point on the low impedance ground plane.
–8–
REV. A
Page 9
AD629
V
OUT
REF(–)
–IN
+IN
–V
S
NC
+V
S
REF(+)
AD629
380k⍀
380k⍀
380k⍀
20k⍀
NC = NO CONNECT
0.1F
+V
S
R
SHUNT
8
7
6
5
1
2
3
4
R
COMP
–V
S
0.1F
I
SHUNT
21.1k⍀
DIGITAL
POWER SUPPLY
GND
GND
12
PROCESSOR
0.1F
+5V
V
DD
+IN
–IN
0.1F 0.1F
–V
S
AD629
REF(–)
ANALOG POWER
+V
S
V
OUT
REF(+)
SUPPLY
+5VGND–5V
0.1F
V
DD
V
IN1
V
IN2
AGND
AD7892-2
DGND
Figure 31. Optimal Grounding Practice for a Bipolar Supply
Environment with Separate Analog and Digital Supplies
+IN
–IN
+V
AD629
REF(–)
0.1F
S
–V
S
V
OUT
REF(+)
POWER SUPPLY
+5V
V
V
V
DD
IN
REF
GND
0.1F
AGND DGND
ADC
0.1F
VDDGND
PROCESSOR
shows some sample error voltages generated by a common-mode
voltage of 200 V dc with shunt resistors from 20 Ω to 2000 Ω.
Assuming that the shunt resistor has been selected to utilize the
full ±10 V output swing of the AD629, the error voltage becomes
quite significant as R
Table I. Error Resulting from Large Values of R
SHUNT
increases.
SHUNT
(Uncompensated Circuit)
RS (⍀)Error V
(V)Error Indicated (mA)
OUT
200.010.5
10000.4980.498
200010.5
If it is desired to measure low current or current near zero in a
high common-mode environment, an external resistor equal to
the shunt resistor value may be added to the low impedance side
of the shunt resistor as shown in Figure 33.
Figure 32. Optimal Ground Practice in a Single Supply
Environment
If there is only a single power supply available, it must be shared
by both digital and analog circuitry. Figure 32 shows how to
minimize interference between the digital and analog circuitry.
In this example, the ADC’s reference is used to drive the
AD629’s REF(+) and REF(–) pins. This means that the reference
must be capable of sourcing and sinking a current equal to V
CM
/
200 kΩ. As in the previous case, separate analog and digital
Figure 33. Compensating for Large Sense Resistors
Output Filtering
A simple 2-pole low-pass Butterworth filter can be implemented
using the OP177 at the output of the AD629 to limit noise at
the output, as shown in Figure 34. Table II gives recommended
component values for various corner frequencies, along with the
peak-to-peak output noise for each case.
ground planes should be used (reasonably thick traces can be
used as an alternative to a digital ground plane). These ground
planes should be connected at the power supply’s ground pin.
Separate traces (or power planes) should be run from the power
supply to the supply pins of the digital and analog circuits. Ideally,
each device should have its own power supply trace, but these
can be shared by a number of devices as long as a single trace is
not used to route current to both digital and analog circuitry.
Using a Large Sense Resistor
Insertion of a large shunt resistance across the input Pins 2 and 3
will imbalance the input resistor network, introducing a commonmode error. The magnitude of the error will depend on the
common-mode voltage and the magnitude of R
SHUNT
. Table I
AD629
21.1k⍀
1
380k⍀
2
380k⍀
3
–V
S
4
NC = NO CONNECT
380k⍀
20k⍀
–IN
+IN
–V
0.1F
REF(–)
S
Figure 34. Filtering of Output Noise Using a 2-Pole
Butterworth Filter
8
7
6
5
+V
NC
+V
S
REF(+)
S
0.1F
+V
S
OP177
–V
0.1F
0.1F
S
C1
R2
R1
C2
Table II. Recommended Values for 2-Pole Butterworth Filter
The AD629 is designed to drive loads of 2 kΩ to within 2 V of
the rails, but can deliver higher output currents at lower output
voltages (see Figure 15). If higher output current is required,
the AD629’s output should be buffered with a precision op
amp such as the OP113 as shown in Figure 35. This op amp
can swing to within 1 V of either rail while driving a load as
small as 600 Ω.
+V
S
OP113
–V
S
0.1F
0.1F
V
OUT
–IN
+IN
–V
0.1F
REF(–)
S
AD629
21.1k⍀
1
380k⍀
2
3
4
380k⍀
380k⍀
20k⍀
NC = NO CONNECT
8
7
6
5
NC
0.1F
REF(+)
Figure 35. Output Buffering Application
A Gain of 19 Differential Amplifier
While low level signals can be connected directly to the –IN and
+IN inputs of the AD629, differential input signals can also be
connected as shown in Figure 36 to give a precise gain of 19.
However, large common-mode voltages are no longer permissible.
Cold junction compensation can be implemented using a temperature sensor such as the AD590.
+V
8
7
6
5
NC
0.1F
REF(+)
S
V
OUT
THERMOCOUPLE
REF(–)
1
–IN
2
+IN
3
V
REF
4
AD629
21.1k⍀
380k⍀
380k⍀
380k⍀
20k⍀
NC = NO CONNECT
Figure 36. A Gain of 19 Thermocouple Amplifier
Error Budget Analysis Example 1
In the dc application below, the 10 A output current from a
device with a high common-mode voltage (such as a power supply or current-mode amplifier) is sensed across a 1 Ω shunt
resistor (Figure 37). The common-mode voltage is 200 V, and
the resistor terminals are connected through a long pair of lead
wires located in a high-noise environment, for example, 50 Hz/
60 Hz 440 V ac power lines. The calculations in Table III
assume an induced noise level of 1 V at 60 Hz on the leads, in
addition to a full-scale dc differential voltage of 10 V. The error
budget table quantifies the contribution of each error source.
Note that the dominant error source in this example is due to
the dc common-mode voltage.
Table III. AD629 vs. INA117 Error Budget Analysis Example 1 (VCM = 200 V dc)
Error, ppm of FS
Error SourceAD629INA117AD629INA117
ACCURACY, T
Initial Gain Error(0.0005 × 10) ÷ 10 V × 10
Offset Voltage(0.001 V ÷ 10 V) × 10
= 25°C
A
6
6
(0.0005 × 10) ÷ 10 V × 10
(0.002 V ÷ 10 V) × 10
6
6
500500
100200
DC CMR (Over Temperature)(224 × 10-6 × 200 V) ÷ 10 V × 106(500 × 10-6 × 200 V) ÷ 10 V × 1064,48010,000
Figure 37. Error Budget Analysis Example 1. VIN = 10 V
Full-Scale, V
= 200 V DC. R
CM
= 1 Ω, 1 V p-p 60 Hz
SHUNT
Power-Line Interference
Error Budget Analysis Example 2
This application is similar to the previous example except that
the sensed load current is from an amplifier with an ac commonmode component of ±100 V (frequency = 500 Hz) present on
the shunt (Figure 38). All other conditions are the same as
before. Note that the same kind of power line interference can
happen as detailed in Example 1. However, the ac commonmode component of 200 V p-p coming from the shunt is much
larger than the interference of 1 V p-p, so that this interference
component can be neglected.
OUTPUT
CURRENT
1⍀
SHUNT
10 AMPS
AC CM
ⴞ100V
TO GROUND
60Hz
POWER LINE
REF(–)
–V
S
21.1k⍀
1
380k⍀
–IN
2
380k⍀
+IN
3
4
AD629
0.1F
NC = NO CONNECT
380k⍀
20k⍀
8
7
6
5
NC
0.1F
REF(+)
+V
S
V
OUT
Figure 38. Error Budget Analysis Example 2. VIN = 10 V
Full-Scale, V
= ±100 V at 500 Hz, R
CM
SHUNT
= 1
Ω
Table IV. AD629 vs. INA117 AC Error Budget Example 2 (VCM = ⴞ100 V @ 500 Hz)
Error, ppm of FS
Error SourceAD629INA117AD629INA117
ACCURACY, T
Initial Gain Error(0.0005 × 10) ÷ 10 V × 10
Offset Voltage(0.001 V ÷ 10 V) × 10