AD AD8200_03

High Common-Mode Voltage, Single-Supply
Difference Amplifier
AD8200
FEATURES
High Common-Mode Voltage Range –2 V to +24 V at a
5 V Supply Voltage
Operating Temperature Range
Die: –40C to +150C
Supply Voltage Range: 4.7 V to 12 V
Low-Pass Filter (One Pole or Two Pole)
FUNCTIONAL BLOCK DIAGRAM
SOIC (R) Package
Die Form
NC
+VS
A2
A1
AD8200
100k
EXCELLENT AC AND DC PERFORMANCE
1 mV Voltage Offset
10 ppm/C Typ Gain Drift
80 dB CMRR Min DC to 10 kHz
–IN
200k
OUT
200k
10k
NC = NO CONNECT
GENERAL DESCRIPTION
The AD8200 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 –2 V to +24 V at a typical supply voltage of 5 V.
The AD8200 is offered in die and packaged form. Both package
options are specified over wide temperature ranges, making the
AD8200 well suited for use in many automotive platforms. The
SOIC package is specified over a temperature range of –40°C to
+125°C. The die is specified from –40°C to +150°C.
INDUCTIVE
LOAD
GND
Automotive platforms demand precision components for better
system control. The AD8200 provides excellent ac and dc performance that keeps errors to a minimum in the user’s system.
Typical offset and gain drift in the SOIC package are 6 µV/°C
and 10 ppm/°C, respectively. The device also delivers a minimum CMRR of 80 dB from dc to 10 kHz.
The AD8200 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.
POWER
DEVICE
5V
5V
OUTPUT
+IN
BATTERY
+IN
A2
–IN
10k
PLATFORMS
Transmission Control
Diesel Injection Control
Engine Management
Adaptive Suspension Control
Vehicle Dynamics Control
CLAMP
DIODE
G =2
G =10
+IN
A1
–IN
+IN
NC
+VS OUT
OUTPUT
NC
+IN
BATTERY
14V
+VS OUT
14V
4 TERM
SHUNT
4 TERM
SHUNT
AD8200
–IN
GND
A1
A2
AD8200
–IN
GND
A1
A2
POWER
DEVICE
CLAMP
DIODE
COMMON
NC = NO CONNECT
Figure 1. High Line Current Sensor
COMMON
INDUCTIVE
LOAD
NC = NO CONNECT
Figure 2. Low Line Current Sensor
REV. B
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. 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.
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.
Tel: 781/329-4700
www.analog.com
Fax: 781/326-8703
© 2003 Analog Devices, Inc. All rights reserved.
AD8200–SPECIFICATIONS
SINGLE SUPPLY
(TA = 25C, VS = 5 V, VCM = 0 V, RL = 10 k.)
Parameter
SYSTEM GAIN
Initial
Error
vs. Temperature
VOLTAGE OFFSET
Input Offset (RTI)
INPUT
Input Impedance
Differential
Common-Mode
CMV
Common-Mode Rejection1
Condition
Min
VO ≥ 0.1 V dc
20
–1
AD8200 SOIC
Typ
Max
10
VCM = 0.15 V; 25°C
VCM = 0.15 V; 125°C (SOIC)
+150°C (DIE)
VCM = 0.15 V; –40°C
Continuous
VCM = 10 V
f = 1 kHz
f = 10 kHz2
PREAMPLIFIER
Gain
Gain Error
Output Voltage Range
Output Resistance
TEMPERATURE RANGE
For Specified Performance
25
V/V
%
ppm/°C
+1
mV
–2.5
–2
+2.5
+2
–3.5
–3
+3.5
+3
mV
mV
480
240
+24
320
160
–2
480
240
+24
kΩ
kΩ
V
320
160
–2
400
200
80
80
100
+1
4.8
103
10
–1
0.02
97
+1
4.8
–1
0.02
50
0.22
30
10
300
4.7
VO = 0.1 V dc
0.25
75
–40
dB
dB
100
+1
4.8
103
2
2
30
400
200
80
80
2
VS = 4.7 V to 12 V
+1
30
–1
NOISE
0.1 Hz to 10 Hz
Spectral Density, 1 kHz, RTI
POWER SUPPLY
Operating Range
Quiescent Current vs.
Temperature
PSRR
20
–1
Unit
+1
–1
0.02
DYNAMIC RESPONSE
3 dB Bandwidth
Slew Rate
AD8200 DIE
Typ
Max
–1
10
–1
0.02
97
OUTPUT BUFFER
Gain
Gain Error
Output Voltage Range
Output Resistance
+1
20
Min
12
1
80
+125
2
V/V
%
V
Ω
50
0.22
kHz
V/µs
10
300
µV p-p
nV/√Hz
+1
4.8
4.7
0.25
75
–40
V/V
%
V
kΩ
12
1
80
V
mA
dB
+150
°C
NOTES
1
Source imbalance < 2 Ω.
2
The AD8200 preamplifier exceeds 80 dB CMRR at 10 kHz. However, since the signal is available only by way of a 100 k Ω resistor, even the small amounts of pinto-pin capacitance between Pins 1, 8 and 3, 4 may couple an input common-mode signal larger than the greatly attenuated preamplifier output. The effect of pin-topin coupling may be neglected in all applications using filter capacitors at Node 3.
Specifications subject to change without notice.
–2–
REV. B
AD8200
PIN CONFIGURATION
ABSOLUTE MAXIMUM RATINGS*
Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12.5 V
Transient Input Voltage (300 ms) . . . . . . . . . . . . . . . . . . 44 V
Continuous Input Voltage . . . . . . . . . . . . . . . . . . . . . . . . 35 V
Reversed Supply Voltage Protection . . . . . . . . . . . . . . . . 0.3 V
Operating Temperature
DIE . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . –40°C to +150°C
SOIC . . . . . . . . . . . . . . . . . . . . . . . . . . . . . –40°C to +125°C
Storage Temperature . . . . . . . . . . . . . . . . . . –65°C to +150°C
Output Short-Circuit Duration . . . . . . . . . . . . . . . . Indefinite
Lead Temperature Range (Soldering 60 sec) . . . . . . . . . 300°C
–IN 1
GND 2
8
AD8200
+IN
NC
TOP VIEW
A1 3 (Not to Scale) 6 +VS
A2 4
7
5
OUT
NC = NO CONNECT
*Stresses beyond those listed under Absolute Maximum Ratings may cause permanent damage to the device. This is a stress rating only; the functional operation of
the device at these or any other conditions above those indicated in the operational
sections of this specification is not implied. Exposure to absolute maximum rating
conditions for extended periods may affect device reliability.
ORDERING GUIDE
Model
Temperature Range Package Description Package Option
AD8200YR
AD8200YR-Reel
AD8200YR-Reel-7
AD8200YCHIPS
AD8200YCSURF
–40°C to +125°C
–40°C to +125°C
–40°C to +125°C
–40°C to +150°C
–40°C to +150°C
SOIC
SOIC
SOIC
R-8
R-8
R-8
DIE Form
DIE Form
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
AD8200 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.
METALLIZATION PHOTOGRAPH
+VS
6
REV. B
+IN
8
–IN
1
2
3
GND
A1
–3–
5
OUT
4
A2
AD8200–Typical Performance Characteristics
(TA = 25C, VS = 5 V, VCM = 0 V, RL = 10 k, unless otherwise noted.)
0
–2
+VCM
20
–4
15
–6
–VCM
10
–8
5
–10
0
–12
2
3
4
SUPPLY VOLTAGE – V
5
25
20
15
GAIN – dB
25
30
NEGATIVE COMMON-MODE RANGE – V
POSITIVE COMMON-MODE RANGE – V
30
10
5
0
–5
–10
–15
–20
1k
TPC 1. Input Common-Mode Range vs. Supply
1M
TPC 4. Gain vs. Frequency
0
100
95
–5
RL =
90
–10
85
CMRR – dB
OUTPUT VOLTAGE – mV
10k
100k
FREQUENCY – Hz
–15
–20
80
75
70
65
–25
60
RL = 10k TO GND
–30
55
–35
2
4
3
SUPPLY VOLTAGE – V
50
10
5
TPC 2. Output Voltage – VS vs. Supply
100
1k
10k
FREQUENCY – Hz
100k
1M
TPC 5. Common-Mode Rejection Ratio vs. Frequency
5
100
90
80
70
3
PSRR – dB
OUTPUT VOLTAGE – V
4
2
60
50
40
30
1
20
10
0
10
100
1k
LOAD RESISTANCE – 0
10
10k
TPC 3. Output Voltage Swing vs. Load Resistance
100
1k
FREQUENCY – Hz
10k
100k
TPC 6. Power Supply Rejection Ratio vs. Frequency
–4–
REV. B
AD8200
TEK RUN: 2.5MS/s
TEK RUN: 2.5MS/s AVERAGE
HI RES
VOUT, RL = 10k
1
VOUT, RL = 10k
1
T
MAGNIFIED VOUT
VIN
VIN
3
2
2
CH1 500mV CH2 50mV M 20s CH1
CH1 1V
CH 2 10mV M 20s CH1
CH3 100mV
1.5V
TPC 7. Pulse Response
TPC 8. Settling Time
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 range of voltage 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 RCM resistors to reduce 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.
THEORY OF OPERATION
The AD8200 consists of a preamp and buffer arranged as shown
in Figure 3. Like-named resistors have equal values.
The preamp incorporates a dynamic bridge (subtractor) circuit.
Identical networks (within the shaded areas), consisting of RA,
RB, RC, and RG, attenuate input signals applied to Pins 1 and 8.
Note that when equal amplitude signals are asserted at inputs 1
and 8, and the output of A1 is equal to the common potential
(i.e., zero), the two attenuators form a balanced-bridge network.
When the bridge is balanced, the differential input voltage at
A1, and thus its output, will be zero.
Any common-mode voltage applied to both inputs will keep 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.
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.
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 RB, by way of RG, to adjust the voltage at its inverting
input until it matches the voltage at its noninverting input.
The output of the preamp drives a gain-of-two buffer-amplifier
A2, implemented with carefully matched feedback resistors RF.
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. RC and RG form an attenuator that scales A1 feedback,
forcing large output signals to balance relatively small differential inputs. The resistor ratios establish the preamp gain at 10.
The two-stage system architecture of the AD8200 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.
Because the differential input signal is attenuated, and then
amplified to yield an overall gain of 10, the 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
APPLICATIONS
–IN
RA
The AD8200 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 input resistance
is nominally 200 kΩ, and the device can tolerate common-mode
voltages higher than the supply voltage and lower than ground.
RA
100k
A1
(TRIMMED)
RCM
RB
RB
A2
RF
RCM
The open collector output stage will source current to within
20 mV of ground.
A3
RF
RG
RC
RC
RG
AD8200
COM
Figure 3. Simplified Schematic
REV. B
1.36V
–5–
AD8200
CURRENT SENSING
High Line, High Current Sensing
Gains Greater than 20
Basic automotive applications making use of the large commonmode range are shown in Figures 1 and 2. The capability of the
device to operate as an amplifier in primary battery supply circuits
is shown in Figure 1; Figure 2 illustrates the ability of the device
to withstand voltages below system ground.
Low Current Sensing
The AD8200 can also be used in low current sensing applications, such as the 4–20 mA current loop shown in Figure 4. In
such applications, the relatively large shunt resistor can degrade
the common-mode rejection. Adding a resistor of equal value in
the low impedance side of the input corrects for this error.
Connecting a resistor from the output of the buffer amplifier to
its noninverting input, as shown in Figure 6, will increase the
gain. The gain is now multiplied by the factor REXT/(REXT –
100 kΩ); for example, it is doubled for REXT = 200 kΩ. Overall
gains as high as 50 are achievable in this way. Note that the
accuracy of the gain becomes critically dependent on resistor
value at high gains. Also, the effective input offset voltage at
Pins 1 and 8 (about six times the actual offset of A1) limits the
part’s use in very high gain, dc-coupled applications.
+VS
OUT
+IN
5V
10
+IN
+
VDIFF
2
OUTPUT
1%
NC
+VS
10k
VDIFF
2
A1
REXT
GND
20REXT
REXT – 100k
REXT = 100k
100k
–IN
GND
10k
AD8200
AD8200
–IN
OUT
+VS
GAIN =
OUT
VCM
10
1%
NC
A1
GAIN
GAIN – 20
A2
A2
NC = NO CONNECT
Figure 6. Adjusting for Gains Greater than 20
NC = NO CONNECT
Figure 4. 4–20 mA Current Loop Receiver
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.
GAIN TRIM
Figure 7 shows a method for incremental gain trimming using a
trimpot and external resistor REXT.
The following approximation is useful for small gain ranges
∆G ≈ (10MΩ ÷ REXT )%
Thus, the adjustment range would be ± 2% for REXT = 5 MΩ;
± 10% for REXT = 1 MΩ, and so on.
Gains Less than 20
Since the preamplifier has an output resistance of 100 kΩ, an external resistor connected from Pins 3 and 4 to GND will decrease the
gain by a factor REXT/(100 kΩ + REXT) (see Figure 5).
5V
OUT
+IN
AD8200
OUT
VCM
NC
+VS
OUT
VDIFF
2
–IN
VDIFF
2
10k
10k
GAIN =
AD8200
VCM
VDIFF
2
20REXT
GND
A1
A2
REXT
REXT + 100k
REXT = 100k
100k
+VS OUT
VDIFF
2
+VS
+IN
NC
GAIN TRIM
20k MIN
GAIN
20 – GAIN
NC = NO CONNECT
–IN
GND
A1
A2
Figure 7. Incremental Gain Trim
REXT
NC = NO CONNECT
Figure 5. Adjusting for Gains Less than 20
The overall bandwidth is unaffected by changes in gain 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, can be nulled by
inserting a resistor equal to 100 kΩ minus the parallel sum of
REXT and 100 kΩ, in series with Pin 4. For example, with REXT
= 100 kΩ (yielding a composite gain of ⫻10), the optional offset
nulling resistor is 50 kΩ (see Figure 11.)
–6–
REV. B
AD8200
Internal Signal Overload Considerations
5V
OUT
When configuring gain for values other than 20, the maximum
input voltage with respect to the supply voltage and ground
must be considered, since either the preamplifier or the output
buffer will reach its full-scale output (approximately VS – 0.2 V)
with large differential input voltages. The input of the AD8200
is limited to (VS – 0.2) ÷ 10, for overall gains ≤10, since 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 AD8200 input to (VS – 0.2) ÷ G, where G is the overall gain.
+IN
AD8200
VCM
C
VDIFF
2
–IN
GND
A1
A2
255k
C
FC = 1Hz – F
NC = NO CONNECT
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
the output of the AD8200 preamplifier (A1) does not clip before
A2, since this nonlinearity would be averaged and appear as an
error at the output. To avoid this error, both amplifiers should
be made to 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
+VS
OUT
FC =
AD8200
VDIFF
2
1
2C105
GND
A1
40dB/DECADE
20dB/DECADE
f1
C IN FARADS
–IN
FREQUENCY
A 1-POLE FILTER, CORNER f1, AND
A 2-POLE FILTER, CORNER f2, HAVE
THE SAME ATTENUATION –40LOG (f2/f1)
AT FREQUENCY f22/f1
OUT
+IN
A 2-pole filter (with a roll-off of 40 dB/decade) can be implemented
using the connections shown in Figure 9. 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 f2 and a 1-pole filter with a corner
at f1 have the same attenuation at the frequency (f22/f1). The
attenuation at that frequency is 40 log (f2/f1). This is illustrated
in Figure 10. Using the standard resistor value shown and equal
capacitors (Figure 9), 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 ␮V at the input pins).
40LOG (f2/f1)
5V
VDIFF
2
Figure 9. 2-Pole Low-Pass Filter
ATTENUATION
Low-pass filters can be implemented in several ways using the
features provided by the AD8200. In the simplest case, a singlepole 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
strapping Pins 3 and 4 and a capacitor added from this node to
ground, as shown in Figure 8. If a resistor is added across the
capacitor to lower the gain, the corner frequency will increase; it
should be calculated using the parallel sum of the resistor and
100 kΩ.
f2
f22/f1
Figure 10. Comparative Responses of 1-Pole and
2-Pole Low-Pass Filters
A2
C
NC = NO CONNECT
Figure 8. A Single-Pole, Low-Pass Filter Using the
Internal 100 kΩ Resistor
If the gain is raised using a resistor, as shown in Figure 8, 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.)
REV. B
+VS OUT
VDIFF
2
LOW-PASS FILTERING
VCM
NC
–7–
AD8200
HIGH-LINE CURRENT SENSING WITH LPF AND GAIN
ADJUSTMENT
DRIVING CHARGE REDISTRIBUTION A/D
CONVERTERS
Figure 11 is another refinement of Figure 1, including gain
adjustment and low-pass filtering.
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 AD8200.
Though generally of short duration, this deflection may persist
until after the sample period of the ADC has expired, due to the
relatively high open-loop output impedance of the AD8200.
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
AD8200. For these applications, the output signal should be
taken from the midpoint of the RLAG – CLAG combination as
shown in Figure 13.
INDUCTIVE
LOAD
CLAMP
DIODE
+IN
BATTERY
5V
OUTPUT
4V/AMP
+VS OUT
NC
14V
191k
4 TERM
SHUNT
AD8200
20k
–IN
GND
A1
A2
POWER
DEVICE
VOS/IB
NULL
C
NC = NO CONNECT
5% CALIBRATION RANGE
FC = 0.796Hz–F
(0.22F FOR f = 3.6 Hz)
COMMON
Figure 11. 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 will be higher by an amount that depends
on the inductance of the load and the control frequency. The
common-mode voltage, on the other hand, extends from roughly
1 V above ground, when the switch is ON, to about 1.5 V
above the battery voltage, when the device is OFF, and the
clamp diode conducts. If the maximum battery voltage spikes
up to 20 V, the common-mode voltage at the input can be as
high as 21.5 V.
5V
AD8200
+IN
A2
–IN
INDUCTIVE
LOAD
CLAG
0.01F
MICROPROCESSOR
A/D
Figure 13. Recommended Circuit for Driving CMOS A /D
5V
OUTPUT
+IN
BATTERY
10k
RLAG
1k
10k
To produce a full-scale output of 4 V, a gain ×40 is used, adjustable by ± 5% to absorb the tolerance in the shunt. There is
sufficient headroom to allow 10% overrange (to 4.4 V). The
roughly triangular voltage across the sense resistor is averaged
by a 1-pole, low-pass filter, here set with a corner frequency =
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
having fC = 20 Hz, as shown in Figure 12. Although this circuit
uses two separate capacitors, the total capacitance is less than
half that needed for the 1-pole filter.
CLAMP
DIODE
Since the perturbations from the analog-to-digital converter are
small, the output impedance of the AD8200 will appear to be
low. The transient response will, therefore, have a time constant
governed by the product of the two LAG components, CLAG ×
RLAG. For the values shown in Figure 13, this time constant is
programmed at approximately 10 µs. Therefore, if samples are
taken at several tens of microseconds or more, there will be
negligible charge “stack-up.”
NC
+VS OUT
14V
432k
4 TERM
SHUNT
AD8200
C
50k
–IN
GND
A1
A2
POWER
DEVICE
127k
C
NC = NO CONNECT
COMMON
FC = 1Hz–F
(0.05F FOR fC = 20Hz)
Figure 12. Illustration of 2-Pole Low-Pass Filtering
–8–
REV. B
AD8200
OUTLINE DIMENSIONS
8-Lead Standard Small Outline Package [SOIC]
Narrow Body
(R-8)
Dimensions shown in millimeters and (inches)
5.00 (0.1968)
4.80 (0.1890)
4.00 (0.1574)
3.80 (0.1497)
8
5
1
4
1.27 (0.0500)
BSC
0.25 (0.0098)
0.10 (0.0040)
COPLANARITY
SEATING
0.10
PLANE
6.20 (0.2440)
5.80 (0.2284)
1.75 (0.0688)
1.35 (0.0532)
0.51 (0.0201)
0.31 (0.0122)
0.50 (0.0196)
ⴛ 45ⴗ
0.25 (0.0099)
8ⴗ
0.25 (0.0098) 0ⴗ 1.27 (0.0500)
0.40 (0.0157)
0.17 (0.0067)
COMPLIANT TO JEDEC STANDARDS MS-012AA
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
REV. B
–9–
AD8200
Revision History
Location
Page
11/03—Data Sheet Changed from REV. A to REV. B.
Change to FEATURES . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
Change to SPECIFICATIONS . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
Change to ORDERING GUIDE . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
Change to OUTLINE DIMENSIONS . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9
6/02—Data Sheet Changed from REV. 0 to REV. A.
Change to ORDERING GUIDE . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
–10–
REV. B
–11–
–12–
C02054–0–11/03(B)