−8 V to +28 V at a 5 V supply voltage
Operating temperature range: −40°C to +125°C
Supply voltage range: 3.5 V to 12 V
Low-pass filter (1-pole or 2-pole)
EXCELLENT AC AND DC PERFORMANCE
±1 mV voltage offset
±1 ppm/°C typ gain drift
80 dB CMRR min dc to 10 kHz
PLATFORMS
Transmission control
Diesel injection control
Engine management
Adaptive suspension control
Vehicle dynamics control
GENERAL DESCRIPTION
The AD8202 is a single-supply difference amplifier for amplifying
and low-pass filtering small differential voltages in the presence of a
large common-mode voltage. The input CMV range extends from
−8 V to +28 V at a typical supply voltage of 5 V.
Single-Supply Difference Amplifier
AD8202
FUNCTIONAL BLOCK DIAGRAM
+V
A2
3
INDUCTIVE
LOAD
+IN
–IN
647
G = ×2
+IN
A2
–IN
5V
NC
+V
AD8202
GND
A1
S
AD8202
5
OUT
10kΩ
10kΩ
2
GND
OUT
S
A2
04981-001
OUTPUT
8
+IN
1
–IN
BATTERY
NCA1
200kΩ200kΩ
NC = NO CONNECT
Figure 1. SOIC (R) Package Die Form
CLAMP
DIODE
14V
G = ×10
+IN
A1
–IN
4-TERM
SHUNT
POWER
DEVICE
100kΩ
The AD8202 is offered in die and packaged form. Both package
options are specified over a wide temperature range of −40°C to
+125°C, making the AD8202 well-suited for use in many automotive platforms.
Automotive platforms demand precision components for better
system control. The AD8202 provides excellent ac and dc
performance, which keeps errors to a minimum in the user’s
system. Typical offset and gain drift in the SOIC package are
0.3 µV/°C and 1 ppm/°C, respectively. Typical offset and gain
drift in the MSOP package are 2 µV/°C and 1 ppm/°C, respectively. The device also delivers a minimum CMRR of 80 dB
from dc to 10 kHz.
The AD8202 features an externally accessible 100 kΩ resistor at
the output of the preamp A1, which can be used for low-pass
filter applications and for establishing gains other than 20.
Rev. C
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 that may result from its use.
Specifications subject to change without notice. No license is granted by implication
or otherwise under any patent or patent rights of Analog Devices. Trademarks and
registered trademarks are the property of their respective owners.
For Specified Performance −40 +125 −40 +125 −40 +150 °C
See notes on next page.
−0.3 +0.3 −0.3 +0.3 %
80 80 80 dB
30 50 30 50 30 50 kHz
0.28 0.28 0.28 V/µs
Rev. C | Page 3 of 16
AD8202
1
Source imbalance < 2 Ω.
2
The AD8202 preamplifier exceeds 80 dB CMRR at 10 kHz. However, because the signal is available only by way of a 100 kΩ resistor, even the small amount of pin-to-
pin capacitance between Pins 1, 8 and 3, 4 might couple an input common-mode signal larger than the greatly attenuated preamplifier output. The effect of pin-topin coupling can be neglected in all applications by using filter capacitors at Node 3.
Rev. C | Page 4 of 16
AD8202
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Rating
Supply Voltage 12.5 V
Transient Input Voltage (400 ms) 44 V
Continuous Input Voltage (Common Mode) 35 V
Reversed Supply Voltage Protection 0.3 V
Operating Temperature Range
Die −40°C to +150°C
SOIC −40°C to +125°C
MSOP −40°C to +125°C
Storage Temperature −65°C to +150°C
Output Short-Circuit Duration Indefinite
Lead Temperature Range (Soldering, 10 sec) 300°C
ESD 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 this product 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.
Stresses above those listed under Absolute Maximum Ratings
may cause permanent 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 affect
device reliability.
TA = 25°C, VS = 5 V, VCM = 0 V, RL = 10 kΩ, unless otherwise noted.
90
80
70
60
50
40
PSRR (dB)
30
20
10
0
101001k10k100k
FREQUENCY (Hz)
Figure 6. Power Supply Rejection Ratio vs.
Frequency Valid for CM Range −8 V to +28 V
30
04981-006
0
–5
–10
–15
–20
–25
COMMON-MODE VOLTAGE (V)
–30
–35
345678910111213
POWER SUPPLY (V)
–55°C
–40°C
+25°C
+125°C
+150°C
Figure 9. Negative Common-Mode Voltage vs. Voltage Supply
40
04981-009
25
20
15
OUTPUT (dB)
10
5
0
1001k10k100k1M
FREQUENCY (Hz)
Figure 7. AD8202 Bandwidth
100
95
90
85
CMRR (dB)
80
75
70
101001k10k100k
FREQUENCY (Hz)
Figure 8. Common -Mode Rejection Ratio vs. Frequency
Valid for CM Range −8 V to +28 V
04981-007
04981-008
35
30
–55°C
25
20
15
10
COMMON-MODE VOLTAGE (V)
5
0
3654871091112
+150°C
+125°C
–40°C
+25°C
POWER SUPPLY (V)
Figure 10. Positive Common-Mode Voltage vs. Voltage Supply
5.0
4.5
4.0
3.5
3.0
2.5
2.0
OUTPUT SWING (V)
1.5
1.0
0.5
0
101001k10k
LOAD RESISTANCE (Ω)
Figure 11. Output Swing vs. Load Resistance
04981-010
13
04981-011
Rev. C | Page 7 of 16
AD8202
0
–10
–20
–30
–40
–50
OUTPUT MINUS SUPPLY (mV)
–60
NO LOAD
10k LOAD
HITS
30
25
20
15
10
5
V
= 5V
SUPPLY
TEMPERATURE RANGE =
°
C TO 125°C
25
–70
3654871091112
SUPPLY VOLTAGE (V)
Figure 12. Output Minus Supply vs. Supply Voltage
OUTPUT
1
2
CH1 500mVΩ50mVΩ M 20µs 2.5MS/s 400NS/PT
CH2
INPUT
A CH1 1.73V
Figure 13. Pulse Response
25
20
15
HITS
10
V
= 5V
SUPPLY
TEMPERATURE RANGE =
°
C TO+25°C
–40
04981-012
13
04981-013
HITS
HITS
0
–9.0
–8.0
–7.0
–6.0
–5.0
–4.0
–3.0
–2.0
–10.0
–1.0
V
DRIFT (µV/°C)
OS
Figure 15. Offset Drift Distribution, SOIC
40
35
30
25
20
15
10
5
0
–900
–800
–700
–600
–500
–400
–300
–1500
–1400
–1300
–1100
–1200
–1000
Figure 16. V
35
30
25
20
15
–200
V
Distribution, SOIC
OS
2.0
1.003.0
TEMPERATURE = 25°C
200
1000300
400
–100
(µV)
OS
TEMPERATURE = –40°C
500
4.0
600
5.0
700
800
6.0
900
7.0
1000
8.0
1100
1200
9.0
1300
10.0
1400
04981-027
04981-028
1500
5
0
–9.0
–8.0
–7.0
–6.0
–5.0
–4.0
–3.0
–2.0
–10.0
–1.0
V
DRIFT (µV/°C)
OS
Figure 14. Offset Drift Distribution, SOIC
2.0
1.003.0
4.0
5.0
6.0
7.0
8.0
9.0
04981-025
10.0
Rev. C | Page 8 of 16
10
5
1200
1300
1400
04981-029
1500
0
–1500
–1400
–1300
–1200
–900
–800
–1100
–1000
Figure 17. V
–700
–600
–500
–400
–300
Distribution, SOIC
OS
–200
V
OS
–100
1000300
(µV)
200
400
500
600
700
800
900
1000
1100
AD8202
HITS
30
25
20
15
10
5
0
–900
–800
–700
–600
–500
–400
–1500
–1400
–1300
–1100
–1200
–1000
Figure 18. V
40
35
30
–300
Distribution, SOIC
OS
TEMPERATURE = 125°C
200
1000300
–200
–100
V
(µV)
OS
TEMPERATURE = 25°C
400
500
600
700
800
900
1000
1100
1200
1300
1400
04981-030
1500
HITS
50
45
40
35
30
25
20
15
10
5
0
0
0.01
0.02
0.04
0.03
0.05
0.06
0.07
0.08
0.09
0.10
0.11
0.12
0.13
ERROR (%)
TEMPERATURE = –40°C
0.17
0.14
0.16
0.15
0.18
0.19
0.20
0.21
0.22
0.23
0.24
0.25
0.26
0.27
0.28
0.29
04981-033
0.30
Figure 21. SOIC Gain Accuracy
8
7
6
V
= 5V
SUPPLY
TEMPERATURE RANGE =
–40°C TO
+
25°C
HITS
HITS
HITS
HITS
5
4
3
2
1
0
–28
–26
–24
–22
–20
–18
–16
–14
–12
–10
–6–8–4
–2
DRIFT (µV/°C)
V
OS
Figure 22. Offset Drift Distribution, MSOP
12
10
8
6
4
2
0
–28
–26
–24
–22
–20
–18
–16
–14
–12
–10
–6–8–4
–2
V
DRIFT (µV/°C)
OS
Figure 23. Offset Drift Distribution, MSOP
02468
02468
101214181620222428
V
= 5V
SUPPLY
TEMPERATURE RANGE =
25°C TO 125°C
101214181620222428
04981-034
26
04981-036
26
25
20
15
10
5
0.27
0.28
0.29
04981-031
0.30
0
0
0.01
0.02
0.04
0.03
0.05
0.06
0.07
0.08
0.09
0.10
0.11
0.12
0.13
0.14
0.15
ERROR (%)
0.16
0.17
0.18
0.19
0.20
0.21
0.22
0.23
0.24
0.25
0.26
Figure 19. SOIC Gain Accuracy
45
40
35
30
25
20
15
10
5
0
0
0.01
0.02
0.04
0.03
0.05
0.06
0.07
0.08
0.09
0.10
0.11
0.12
ERROR (%)
TEMPERATURE = 125°C
0.17
0.13
0.14
0.16
0.15
0.18
0.19
0.20
0.21
0.22
0.23
0.24
0.25
0.26
0.27
0.28
0.29
04981-032
0.30
Figure 20. SOIC Gain Accuracy
Rev. C | Page 9 of 16
AD8202
14
12
TEMPERATURE = 25°C
14
12
TEMPERATURE = 25°C
HITS
HITS
HITS
HITS
HITS
HITS
10
8
6
4
2
0.25
0.27
04981-040
0.29
0
0.01
0.05
0.03
0.07
0.09
0.11
0.13
0.17
0.15
0.19
0.21
–0.15
–0.13
–0.11
–0.07
–0.09
–0.05
–0.03
–0.01
ERROR (%)
0.23
Figure 27. MSOP Gain Accuracy
14
12
10
8
6
4
2
0
0.01
–0.15
–0.13
–0.11
–0.07
–0.09
–0.05
0.03
–0.03
–0.01
ERROR (%)
TEMPERATURE = 125°C
0.05
0.07
0.09
0.11
0.13
0.15
0.17
0.19
0.21
0.23
0.25
0.27
04981-041
0.29
Figure 28. MSOP Gain Accuracy
14
12
10
8
6
4
2
0
0.01
–0.15
–0.13
–0.11
–0.07
–0.09
–0.05
0.03
–0.03
–0.01
ERROR (%)
TEMPERATURE = –40°C
0.05
0.07
0.09
0.11
0.13
0.15
0.17
0.19
0.21
0.23
0.25
0.27
04981-042
0.29
Figure 29. MSOP Gain Accuracy
10
8
6
4
2
1800
1800
1800
2000
2000
2000
04981-037
2200
04981-038
2200
04981-039
2200
0
–2200
–2000
–1800
–1600
–1400
–1200
–1000
–800
Figure 24. V
10
9
8
7
6
5
4
3
2
1
0
–2200
–2000
–1800
–1600
–1400
–1200
–1000
–800
Figure 25. V
9
8
7
6
5
4
3
2
1
0
–2200
–2000
–1800
–1600
–1400
–1200
–1000
–800
Figure 26. V
0
200
400
–600
–400
–200
V
OS
Distribution, MSOP
OS
–600
–400
–200
V
OS
Distribution, MSOP
OS
–600
–400
–200
V
OS
Distribution, MSOP
OS
600
(µV)
TEMPERATURE = 125°C
0
200
400
600
(µV)
TEMPERATURE = –40°C
0
200
400
600
(µV)
800
800
800
1000
1000
1000
1200
1200
1200
1400
1400
1400
1600
1600
1600
Rev. C | Page 10 of 16
AD8202
HITS
18
16
14
12
10
8
6
4
2
0
–70
–65
–60
–45
–55
–50
–40
–35
–30
–25
–20
–15
CMRR (µV/V)
TEMPERATURE = 25°C
0
5
–5
10152030253540455055656070
–10
Figure 30. CMRR Distribution, −8 V to +28 V Common Mode
04981-043
1000
800
600
400
200
V)
µ
(
0
OS
V
–200
–400
–600
–800
–1000
–10–51050201530
+125°C
Figure 31. V
+25°C
COMMON-MODE VOLTAGE (V)
OS
+85°C
vs. Common-Mode Voltage
–40°C
25
04981-044
Rev. C | Page 11 of 16
AD8202
THEORY OF OPERATION
The AD8202 consists of a preamp and buffer arranged as shown
in Figure 32. Like-named resistors have equal values.
The preamp uses a dynamic bridge (subtractor) circuit. Identical networks (within the shaded areas), consisting of R
, attenuate input signals applied to Pins 1 and 8. When
and R
G
equal amplitude signals are asserted at inputs 1 and 8, and the
output of A1 is equal to the common potential (that is, 0), the
two attenuators form a balanced-bridge network. When the
bridge is balanced, the differential input voltage at A1, and
thus its output, is 0.
Any common-mode voltage applied to both inputs keeps the
bridge balanced and the A1 output at zero. Because the resistor
networks are carefully matched, the common-mode signal
rejection approaches this ideal state.
However, if the signals applied to the inputs differ, the result is a
difference at the input to A1. A1 responds by adjusting its output
to drive R
, by way of RG, to adjust the voltage at its inverting
B
input until it matches the voltage at its noninverting input.
By attenuating voltages at Pins 1 and 8, the amplifier inputs are
held within the power supply range, even if Pin 1 and Pin 8
input levels exceed the supply or fall below common (ground).
The input network also attenuates normal (differential) mode
voltages. R
and RG form an attenuator that scales A1 feedback,
C
forcing large output signals to balance relatively small differential inputs. The resistor ratios establish the preamp gain at 10.
Because the differential input signal is attenuated and then
amplified to yield an overall gain of 10, Amplifier A1 operates at
a higher noise gain, multiplying deficiencies such as input offset
voltage and noise with respect to Pins 1 and 8.
+IN
8
R
R
R
R
G
–IN
1
R
A
A
A1
R
R
CM
R
B
B
R
R
G
C
C
CM
A3
100kΩ
(TRIMMED)
AD8202
3
, RB, RC,
A
4
A2
5
R
F
R
F
To minimize these errors while extending the common-mode
range, a dedicated feedback loop is employed to reduce the
range of common-mode voltage applied to A1 for a given overall range at the inputs. By offsetting the voltage range applied to
the compensator, the input common-mode range is also offset
to include voltages more negative than the power supply.
Amplifier A3 detects the common-mode signal applied to A1
and adjusts the voltage on the matched R
resistors to reduce
CM
the common-mode voltage range at the A1 inputs. By adjusting
the common voltage of these resistors, the common-mode input
range is extended while, at the same time, the normal mode
signal attenuation is reduced, leading to better performance
referred to input.
The output of the dynamic bridge taken from A1 is connected
to Pin 3 by way of a 100 kΩ series resistor, provided for lowpass filtering and gain adjustment. The resistors in the input
networks of the preamp and the buffer feedback resistors are
ratio trimmed for high accuracy.
The output of the preamp drives a gain-of-2 buffer amplifier,
A2, implemented with carefully matched feedback resistors, R
F
The 2-stage system architecture of the AD8202 enables the
user to incorporate a low-pass filter prior to the output buffer.
By separating the gain into two stages, a full-scale, rail-to-rail
signal from the preamp can be filtered at Pin 3, and a half-scale
signal, resulting from filtering, can be restored to full scale by
the output buffer amp. The source resistance seen by the inverting input of A2 is approximately 100 kΩ to minimize the effects
of A2’s input bias current. However, this current is quite small
and errors resulting from applications that mismatch the resistance are correspondingly small.
.
2
COM
Figure 32. Simplified Schematic
04981-014
Rev. C | Page 12 of 16
AD8202
+
APPLICATIONS
+V
The AD8202 difference amplifier is intended for applications
where it is required to extract a small differential signal in the
presence of large common-mode voltages. The differential input
resistance is nominally 325 kΩ, and the device can tolerate
common-mode voltages higher than the supply voltage and
lower than ground.
The open-collector output stage sources current to within
20 mV of ground and to within 200 mV of V
.
S
V
DIFF
2
V
V
CM
DIFF
2
AD8202
100kΩ
S
NC+IN
OUT+V
S
10kΩ10kΩ
OUT
20R
R
EXT
= 100kΩ
EXT
+ 100kΩ
GAIN
20 – GAIN
GAIN =
R
EXT
A2A1GND–IN
CURRENT SENSING
High-Line, High Current Sensing
Basic automotive applications using the large common-mode
range are shown in Figure 2 and Figure 3. The capability of the
device to operate as an amplifier in primary battery-supply
circuits is shown in Figure 2; Figure 3 illustrates the ability of
the device to withstand voltages below system ground.
Low Current Sensing
The AD8202 can also be used in low current sensing applications,
such as the 4 to 20 mA current loop shown in Figure 33. In such
applications, the relatively large shunt resistor can degrade the
common-mode rejection. Adding a resistor of equal value on the
low impedance side of the input corrects for this error.
10Ω
1%
+IN
10Ω
1%
–IN
Figure 33. 4 to 20 mA Current Loop Receiver
5V
NC
+V
S
AD8202
GND
A1
NC = NO CONNECT
OUT
A2
OUTPUT
04981-015
GAIN ADJUSTMENT
The default gain of the preamplifier and buffer are ×10 and ×2,
respectively, resulting in a composite gain of ×20. With the
addition of external resistor(s) or trimmer(s), the gain may be
lowered, raised, or finely calibrated.
Gains Less than 20
Because the preamplifier has an output resistance of 100 kΩ, an
external resistor connected from Pins 3 and 4 to GND decreases
the gain by a factor R
/(100 kΩ + R
EXT
) as shown in Figure 34.
EXT
R
EXT
NC = NO CONNECT
04981-016
Figure 34. Adjusting for Gains Less than 20
The overall bandwidth is unaffected by changes in gain by using
this method, although there may be a small offset voltage due to
the imbalance in source resistances at the input to the buffer. In
many cases this can be ignored, but if desired, it can be nulled
by inserting a resistor equal to 100 kΩ minus the parallel sum of
and 100 kΩ, in series with Pin 4. For example, with R
R
EXT
EXT
=
100 kΩ (yielding a composite gain of ×10), the optional offset
nulling resistor is 50 kΩ.
Gains Greater than 20
Connecting a resistor from the output of the buffer amplifier to
its noninverting input, as shown in Figure 35, increases the
/(R
gain. The gain is multiplied by the factor R
for example, it is doubled for R
= 200 kΩ. Overall gains as
EXT
EXT
− 100 kΩ);
EXT
high as 50 are achievable in this way. The accuracy of the gain
becomes critically dependent on the resistor value at high gains.
Also, the effective input offset voltage at Pin 1 and Pin 8 (about
six times the actual offset of A1) limits the part’s use in high
gain, dc-coupled applications.
+V
S
NC+IN
V
DIFF
2
V
V
CM
DIFF
2
NC = NO CONNECT
AD8202
100kΩ
OUT+V
S
10kΩ10kΩ
R
A2A1GND–IN
Figure 35. Adjusting for Gains Greater than 20
EXT
OUT
GAIN =
R
EXT
R
EXT
= 100kΩ
20R
– 100kΩ
GAIN – 20
EXT
GAIN
04981-017
Rev. C | Page 13 of 16
AD8202
GAIN TRIM
Figure 36 shows a method for incremental gain trimming by
using a trim potentiometer and external resistor, R
The following approximation is useful for small gain ranges:
ΔG ≈ (10 MΩ ÷ R
Thus, the adjustment range is ±2% for R
= 1 MΩ, and so on.
R
EXT
V
DIFF
2
V
V
CM
DIFF
2
EXT
)%
+IN
–IN
5V
+V
NC
AD8202
GND
A1
= 5 MΩ; ±10% for
EXT
OUT
S
A2
R
EXT
.
EXT
OUT
GAIN TRIM
20kΩ MIN
Low-pass filters can be implemented in several ways by
using the AD8202. In the simplest case, a single-pole filter
(20 dB/decade) is formed when the output of A1 is connected
to the input of A2 via the internal 100 kΩ resistor by tying Pin 3
and Pin 4 and adding a capacitor from this node to ground, as
shown in Figure 37. If a resistor is added across the capacitor to
lower the gain, the corner frequency increases; it should be
calculated using the parallel sum of the resistor and 100 kΩ.
5V
+IN
+V
NC
AD8202
GND
A1
S
V
DIFF
2
V
V
CM
DIFF
2
–IN
OUT
A2
fC=
C IN FARADS
C
OUTPUT
2πC10
1
5
NC = NO CONNECT
04981-018
Figure 36. Incremental Gain Trim
Internal Signal Overload Considerations
When configuring gain for values other than 20, the maximum input voltage with respect to the supply voltage and
ground must be considered, because either the preamplifier
or the output buffer reaches its full-scale output (approximately
– 0.2 V) with large differential input voltages. The input of
V
S
the AD8202 is limited to (V
– 0.2) ÷ 10 for overall gains ≤ 10,
S
because the preamplifier, with its fixed gain of ×10, reaches
its full-scale output before the output buffer. For gains greater
than 10, the swing at the buffer output reaches its full scale first
and limits the AD8202 input to (V
– 0.2) ÷ G, where G is the
S
overall gain.
LOW-PASS FILTERING
In many transducer applications, it is necessary to filter the
signal to remove spurious high frequency components including noise, or to extract the mean value of a fluctuating signal
with a peak-to-average ratio (PAR) greater than unity. For
example, a full-wave rectified sinusoid has a PAR of 1.57, a
raised cosine has a PAR of 2, and a half-wave sinusoid has a
PAR of 3.14. Signals having large spikes may have PARs of 10
or more.
When implementing a filter, the PAR should be considered so
that the output of the AD8202 preamplifier (A1) does not clip
before A2, because this nonlinearity would be averaged and
appear as an error at the output. To avoid this error, both amplifiers should clip at the same time. This condition is achieved
when the PAR is no greater than the gain of the second amplifier (2 for the default configuration). For example, if a PAR of 5
is expected, the gain of A2 should be increased to 5.
NC = NO CONNECT
04981-019
Figure 37. Single-Pole, Low-Pass Filter Using the Internal 100 kΩ Resistor
If the gain is raised using a resistor, as shown in Figure 35, the
corner frequency is lowered by the same factor as the gain is
raised. Thus, using a resistor of 200 kΩ (for which the gain
would be doubled), the corner frequency is now 0.796 Hz/µF
(0.039 µF for a 20 Hz corner frequency.)
5V
+IN
+V
OUT
NC
AD8202
GND
A1
S
A2
255kΩ
C
V
DIFF
2
V
V
DIFF
CM
2
–IN
NC = NO CONNECT
Figure 38. 2-Pole, Low-Pass Filter
C
f
(Hz) = 1/C(µF)
C
OUT
04981-020
A 2-pole filter (with a roll-off of 40 dB/decade) can be implemented using the connections shown in Figure 38. This is a
Sallen-Key form based on a ×2 amplifier. It is useful to remember
that a 2-pole filter with a corner frequency f
with a corner at f
2
/f1). The attenuation at that frequency is 40 log (f2/f1), which is
(f
2
have the same attenuation at the frequency
1
and a 1-pole filter
2
illustrated in Figure 39. Using the standard resistor value shown
and equal capacitors (Figure 38), the corner frequency is conveniently scaled at 1 Hz/µF (0.05 µF for a 20 Hz corner). A maximally flat response occurs when the resistor is lowered to 196 kΩ
and the scaling is then 1.145 Hz/µF. The output offset is raised by
approximately 5 mV (equivalent to 250 µV at the input pins).
Rev. C | Page 14 of 16
AD8202
Y
FREQUENCY
40dB/DECADE
20dB/DECADE
ATTENUATION
40LOG (f2/f1)
A 1-POLE FILTER, CORNER f1, AND
A 2-POLE FILTER, CORNER f
THE SAME ATTENUATION –40LOG (f
AT FREQUENCY f
2
f
1
, HAVE
2
2
/f
1
f
2
2/f1
)
2
f
/f
2
1
04981-021
Figure 39. Comparative Responses of 1-Pole and 2-Pole Low-Pass Filters
HIGH-LINE CURRENT SENSING WITH LPF AND
GAIN ADJUSTMENT
Figure 40 is another refinement of Figure 2, including gain
adjustment and low-pass filtering.
INDUCTIVE
LOAD
BATTER
CLAMP
DIODE
14V
NC = NO CONNECTCOMMON
4-TERM
SHUNT
POWER
DEVICE
Figure 40. High-Line Current Sensor Interface;
Gain = ×40, Single-Pole, Low-Pass Filter
A power device that is either on or off controls the current in
the load. The average current is proportional to the duty cycle
of the input pulse and is sensed by a small value resistor. The
average differential voltage across the shunt is typically 100 mV,
although its peak value is higher by an amount that depends on
the inductance of the load and the control frequency. The
common-mode voltage, conversely, extends from roughly 1 V
above ground for the on condition to about 1.5 V above the
battery voltage in the off condition. The conduction of the
clamping diode regulates the common-mode potential applied
to the device. For example, a battery spike of 20 V may result in
an applied common-mode potential of 21.5 V to the input of
the devices.
To produce a full-scale output of 4 V, a gain ×40 is used, adjustable by ±5% to absorb the tolerance in the shunt. Sufficient
headroom allows 10% overrange (to 4.4 V). The roughly triangular voltage across the sense resistor is averaged by a 1-pole,
NC
+INA1+V
AD8202
GND
–IN
5V
OUT
S
191kΩ
20kΩ
A2
V
OS/IB
NULL
C
5% CALIBRATION RANGE
f
(Hz) = 0.796Hz/C(µF)
C
(0.22µF FOR f
= 3.6Hz)
C
OUT
4V/AMP
low-pass filter, set here with a corner frequency of 3.6 Hz,
which provides about 30 dB of attenuation at 100 Hz. A higher
rate of attenuation can be obtained using a 2-pole filter with
= 20 Hz, as shown in Figure 41. Although this circuit uses
f
C
two separate capacitors, the total capacitance is less than half
that needed for the 1-pole filter.
INDUCTIVE
CLAMP
DIODE
BATTERY
14V
NC = NO CONNECTCOMMON
4-TERM
SHUNT
POWER
DEVICE
LOAD
Figure 41. 2-Pole Low-Pass Filter
+IN
–IN
5V
+V
NC
AD8202
GND
A1
OUT
S
A2
127kΩ
C
fC(Hz) = 1/C(µF)
(0.05µF FOR f
C
432kΩ
50kΩ
= 20Hz)
C
OUTPUT
04981-023
DRIVING CHARGE REDISTRIBUTION ADCS
When driving CMOS ADCs such as those embedded in popular microcontrollers, the charge injection (∆Q) can cause a
significant deflection in the output voltage of the AD8202.
Though generally of short duration, this deflection may persist
until after the sample period of the ADC expires due to the
relatively high open-loop output impedance (typ 21 kΩ) of the
AD8202. Including an R-C network in the output can significantly reduce the effect. The capacitor helps to absorb the transient charge, effectively lowering the high frequency output
impedance of the AD8202. For these applications, the output
− C
04981-022
signal should be taken from the midpoint of the R
combination, as shown in Figure 42.
LAG
Because the perturbations from the analog-to-digital converter are
small, the output impedance of the AD8202 appears to be low. The
transient response, therefore, has a time constant governed by the
× R
product of the two LAG components, C
LAG
. For the values
LAG
shown in Figure 42, this time constant is programmed at approximately 10 µs. Therefore, if samples are taken at several tenths of
microseconds or more, there is negligible charge stack-up.
5V
46
+IN
–IN
Figure 42. Recommended Circuit for Driving CMOS A/D
AD8202
A2
10kΩ
10kΩ
R
LAG
1kΩ
5
2
C
0.01µF
LAG
MICROPROCESSOR
A/D
LAG
04981-024
Rev. C | Page 15 of 16
AD8202
OUTLINE DIMENSIONS
4.00 (0.1574)
3.80 (0.1497)
5.00 (0.1968)
4.80 (0.1890)
85
6.20 (0.2440)
5.80 (0.2284)
41
1.27 (0.0500)
BSC
0.25 (0.0098)
0.10 (0.0040)
COPLANARITY
0.10
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDS MS-012AA
1.75 (0.0688)
1.35 (0.0532)
0.51 (0.0201)
0.31 (0.0122)
0.25 (0.0098)
0.17 (0.0067)
0.50 (0.0196)
0.25 (0.0099)
8°
1.27 (0.0500)
0°
0.40 (0.0157)
× 45°
Figure 43. 8-Lead Standard Small Outline Package [SOIC_N], Narrow Body (R-8),
Dimensions shown in millimeters and (inches)
3.00
BSC
8
5
3.00
BSC
1
PIN 1
0.65 BSC
0.15
0.00
0.38
0.22
COPLANARITY
0.10
COMPLIANT TO JEDEC STANDARDS MO-187AA
BSC
4
SEATING
PLANE
4.90
1.10 MAX
0.23
0.08
8°
0°
0.80
0.60
0.40
Figure 44. 8-Lead Mini Small Outline Package [MSOP], (RM-8),
Dimensions shown in millimeters
ORDERING GUIDE
Model Temperature Package Package Description Package Outline Branding
AD8202YR −40°C to +125°C 8 Lead Standard Small Outline Package (SOIC_N) R-8
AD8202YR-REEL −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8202YR-REEL7 −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8202YRZ
AD8202YRZ-RL1 −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8202YRZ-R71 −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8202YRMZ1 −40°C to +125°C 8-Lead Mini Small Outline Package (MSOP) RM-8 JWY
AD8202YRMZ-RL1 −40°C to +125°C 8-Lead Mini Small Outline Package (MSOP) RM-8 JWY
AD8202YRMZ-R71 −40°C to +125°C 8-Lead Mini Small Outline Package (MSOP) RM-8 JWY
AD8202YCSURF Die