Wide Bandwidth: 3.4 MHz
Low Offset Voltage: 100 V
Very Low Drift: 0.2 V/C
Unity Gain Stable
No Phase Reversal
APPLICATIONS
Digital Scales
Multimedia
Strain Gages
Battery-Powered Instrumentation
Temperature Transducer Amplifier
GENERAL DESCRIPTION
The OP113 family of single supply operational amplifiers
features both low noise and drift. It has been designed for
systems with internal calibration. Often these processor-based
systems are capable of calibrating corrections for offset and gain,
but they cannot correct for temperature drifts and noise. Optimized for these parameters, the OP113 family can be used to
take advantage of superior analog performance combined with
digital correction. Many systems using internal calibration operate from unipolar supplies, usually either 5 V or 12 V. The
OP113 family is designed to operate from single supplies from 4 V
to 36 V, and to maintain its low noise and precision performance.
The OP113 family is unity gain stable and has a typical gain
bandwidth product of 3.4 MHz. Slew rate is in excess of 1 V/µs.
Noise density is a very low 4.7 nV/√Hz, and noise in the 0.1 Hz to
10 Hz band is 120 nV p-p. Input offset voltage is guaranteed
and offset drift is guaranteed to be less than 0.8 µV/°C. Input
common-mode range includes the negative supply and to within
1 V of the positive supply over the full supply range. Phase reversal
protection is designed into the OP113 family for cases where
input voltage range is exceeded. Output voltage swings also include
the negative supply and go to within 1 V of the positive rail. The
output is capable of sinking and sourcing current throughout
its range and is specified with 600 Ω loads.
Digital scales and other strain gage applications benefit from the
very low noise and low drift of the OP113 family. Other applications include use as a buffer or amplifier for both A/D and D/A
sigma-delta converters. Often these converters have high resolutions requiring the lowest noise amplifier to utilize their full
potential. Many of these converters operate in either single supply
or low supply voltage systems, and attaining the greater signal
swing possible increases system performance.
OP113/OP213/OP413
PIN CONNECTIONS
8-Lead Narrow-Body SO8-Lead Plastic DIP
NULL
NULL
–IN A
+IN A
1
OP113
V–
4
NC = NO CONNECT
NC
8
V+
OUT A
NULL
5
8-Lead Narrow-Body SO
OUT A
–IN A
+IN A
1
8
V+
OP213
V–
4
OUT B
–IN B
5
+IN B
14-Lead Plastic DIP
1
OUT A
2
–IN A
+IN A
3
V+V–
+IN B
–IN B
OUT B
OP413
4
5
6
7
14
13
12
11
10
9
8
OUT D
–IN D
+IN D
+IN C
–IN C
OUT C
1
–IN A
2
+IN A
3
V–
4
OP113
NC = NO CONNECT
8-Lead Plastic DIP
OUT A
1
–IN A
2
+IN A
3
V–
4
OP213
16-Lead Wide-Body SO
OUT A
–IN A
+IN A
+IN B
–IN B
OUT B
116
V+
NC
OP413
89
NC = NO CONNECT
The OP113 family is specified for single 5 V and dual ±15 V
operation over the XIND—extended industrial (–40°C to +85°C)
temperature range. They are available in plastic and SOIC
surface mount packages.
8
7
6
5
5
8
7
6
NC
V+
OUT A
NULL
V+
OUT B
–IN B
+IN B
OUT D
–IN D
+IN D
V–
+IN C
–IN C
OUT C
NC
REV. D
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.
OP113ES–40°C to +85°C8-Lead SOICSO-8
OP113FP* –40°C to +85°C8-Lead Plastic DIPN-8
OP113FS–40°C to +85°C8-Lead SOICSO-8
OP213EP* –40°C to +85°C8-Lead Plastic DIPN-8
OP213ES–40°C to +85°C8-Lead SOICSO-8
OP213FP–40°C to +85°C8-Lead Plastic DIPN-8
OP213FS–40°C to +85°C8-Lead SOICSO-8
OP413ES–40°C to +85°C16-Lead Wide SOIC R-16
OP413FP* –40°C to +85°C14-Lead Plastic DIP N-14
OP413FS–40°C to +85°C16-Lead Wide SOIC R-16
Absolute maximum ratings apply to both DICE and packaged parts, unless
otherwise noted.
2
θJA is specified for the worst-case conditions, i.e., θJA is specified for device in
socket for cerdip, P-DIP, and LCC packages; θJA is specified for device soldered in circuit board for SOIC package.
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 OP113/OP213/OP413 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.
–4–
REV. D
Typical Performance Characteristics–
TCVOS – V
UNITS
600
0
1.0
300
100
0.1
200
0
500
400
0.90.70.60.50.80.40.30.2
VS = 15V
–40
C T
A
+85C
1220 OP AMPS
PLASTIC PKG
OP113/OP213/OP413
100
VS = 15V
= 25C
T
A
80
400 OP AMPS
PLASTIC PKG
60
UNITS
40
20
0
–40
–50
INPUT OFFSET VOLTAGE, V
– V
OS
403020100–10–20–30
TPC 1a. OP113 Input Offset (VOS) Distribution
±
15 V
@
500
VS = 15V
= 25C
T
400
300
A
896 (PLASTIC) OP AMPS
150
VS = 15V
–40
120
90
UNITS
60
C TA +85C
400 OP AMPS
PLASTIC PKG
30
50
0
0.1
0
TCVOS – V
1.0
0.90.80.70.60.50.40.30.2
TPC 2a. OP113 Temperature Drift (TCVOS)
Distribution @
500
400
300
±
15 V
VS = 15V
–40
C TA +85C
896 (PLASTIC) OP AMPS
UNITS
200
100
0
–80
–100
INPUT OFFSET VOLTAGE, VOS – V
806040200–20–40–60
TPC 1b. OP213 Input Offset (VOS) Distribution
@
±
15 V
500
VS = 15V
= 25C
T
A
400
1220 OP AMPS
PLASTIC PKG
300
UNITS
200
100
0
–60
–40
INPUT OFFSET VOLTAGE, VOS – V
120100806040200–20
100
140
UNITS
200
100
0
0.1
0
TCVOS – V
TPC 2b. OP213 Temperature Drift (TCVOS)
±
Distribution @
15 V
1.0
0.90.80.70.60.50.40.30.2
TPC 1c. OP413 Input Offset (VOS) Distribution
@
±
15 V
REV. D
–5–
TPC 2c. OP413 Temperature Drift (TCVOS)
±
Distribution @
15 V
OP113/OP213/OP413
1000
800
VCM = 0V
1007550250–25
INPUT BIAS CURRENT – nA
600
400
200
0
–75
–50
VS = 5.0V
V
CM
VS = 15V
V
= 0V
CM
TEMPERATURE – C
= 2.5V
TPC 3. OP113 Input Bias Current vs. Temperature
5.0
4.5
4.0
3.5
POSITIVE OUTPUT SWING – Volts
3.0
–75
+SWING
R
= 2k
L
+SWING
R
= 600
L
–50
TEMPERATURE – C
–SWING
R
= 2k
L
–SWING
R
L
VS = 5.0V
= 600
7510050250–25
125
125
1.5
1.0
2.0
0.5
0
NEGATIVE OUTPUT SWING – mV
500
400
300
VS = 15V
200
INPUT BIAS CURRENT – nA
100
0
–50
–75
0–25
TEMPERATURE – C
VS = 5.0V
125
100755025
TPC 6. OP213 Input Bias Current vs. Temperature
15.0
14.5
14.0
13.5
13.0
12.5
–13.5
–14.0
POSITIVE OUTPUT SWING – Volts
–14.5
–15.0
–75
VS = 15V
–50
–SWING
R
= 600
L
+SWING
R
= 2k
L
+SWING
= 600
R
L
TEMPERATURE – C
–SWING
R
= 2k
L
1007550250–25
125
TPC 4. Output Swing vs. Temperature and RL @ 5 V
60
VS = 15V
40
= 25C
T
A
20
0
–20
–40
–60
–80
CHANNEL SEPARATION – dB
–100
–120
1010010M1M100k10k1k
105
FREQUENCY – Hz
TPC 5. Channel Separation
TPC 7. Output Swing vs. Temperature and RL @ ±15 V
20
18
16
14
12
10
8
6
OPEN-LOOP GAIN – V/V
4
2
0
–50
–75
RL = 2k
RL = 600
0–25
TEMPERATURE – C
VS = 5.0V
= 3.9V
V
O
100755025
125
TPC 8. Open-Loop Gain vs. Temperature @ 5 V
–6–
REV. D
OP113/OP213/OP413
100
40
–20
10k10M1M100k1k
20
0
60
80
FREQUENCY – Hz
OPEN-LOOP GAIN – dB
90
225
135
180
45
0
PHASE – Degrees
TA= 25C
V
S
= 15V
GAIN
PHASE
m = 72
12.5
VS = 15V
V
= 10V
D
1007550250–25
10.0
OPEN-LOOP GAIN – V/V
7.5
5.0
2.5
RL = 2k
RL = 1k
RL = 600
0
–75
TEMPERATURE – C
TPC 9. OP413 Open-Loop Gain vs. Temperature
100
OPEN-LOOP GAIN – dB
V+ = 5V
V– = 0V
T
= 25C
80
60
40
20
A
GAIN
PHASE
m = 57
0
10
9
8
–50
RL = 2k
RL = 600
0–25
TEMPERATURE – C
7
6
5
4
3
OPEN LOOP GAIN – V/V
2
1
0
125–50
–75
VS = 15V
V
= 10V
O
100755025
125
TPC 12. OP213 Open-Loop Gain vs. Temperature
0
45
90
135
PHASE – Degrees
180
–20
10k10M1M100k1k
FREQUENCY – Hz
TPC 10. Open-Loop Gain, Phase vs. Frequency @ 5 V
50
V+ = 5V
40
AV = 100
30
20
AV = 10
10
0
CLOSED-LOOP GAIN – dB
AV = 1
–10
–20
10k10M1M100k1k
FREQUENCY – Hz
V– = 0V
T
= 25C
A
TPC 11. Closed-Loop Gain vs. Frequency @ 5 V
225
TPC 13. Open-Loop Gain, Phase vs. Frequency @ ±15 V
50
TA= 25C
= 15V
V
S
CLOSED-LOOP GAIN – dB
–10
–20
40
AV = 100
30
20
AV = 10
10
0
AV = 1
10k10M1M100k1k
FREQUENCY – Hz
TPC 14. Closed-Loop Gain vs. Frequency @ ±15 V
REV. D
–7–
OP113/OP213/OP413
70
65
60
55
PHASE MARGIN – Degrees
50
–75
V+ = 5V
V– = 0V
–50
GBW
m
7510050250–25
TEMPERATURE – C
125
5
4
3
2
GAIN-BANDWIDTH PRODUCT – MHz
1
TPC 15. Gain Bandwidth Product and Phase Margin vs.
Temperature @ 5 V
30
25
20
TA = 25C
= 15V
V
S
70
65
60
55
PHASE MARGIN – Degrees
50
–75
VS = 15V
–50
GBW
m
TEMPERATURE – C
7510050250–25
125
5
4
3
2
1
TPC 18. Gain Bandwidth Product and Phase Margin vs.
Temperature @
3.0
2.5
2.0
±
15 V
TA = 25C
= 15V
V
S
GAIN-BANDWIDTH PRODUCT – MHz
15
10
5
VOLTAGE NOISE DENSITY – nV/ Hz
0
1101k100
FREQUENCY – Hz
TPC 16. Voltage Noise Density vs. Frequency
COMMON-MODE REJECTION – dB
140
120
100
80
60
40
20
0
1k1M100k10k100
FREQUENCY – Hz
V+ = 5V
V– = 0V
T
= 25C
A
TPC 17. Common-Mode Rejection vs. Frequency @ 5 V
1.5
1.0
0.5
CURRENT NOISE DENSITY – pA/ Hz
0
1101k100
FREQUENCY – Hz
TPC 19. Current Noise Density vs. Frequency
140
120
100
80
60
40
COMMON-MODE REJECTION – dB
20
0
1k1M100k10k100
FREQUENCY – Hz
TA= 25C
= 15V
V
S
TPC 20. Common-Mode Rejection vs. Frequency @ ±15 V
–8–
REV. D
OP113/OP213/OP413
20
0
500
6
2
100
4
0
12
8
10
14
16
18
400300200
LOAD CAPACITANCE – pF
OVERSHOOT – %
VS = 15V
R
L
= 2k
V
IN
= 100mV p-p
T
A
= 25C
A
VCL
= 1
POSITIVE
EDGE
NEGATIVE
EDGE
140
120
100
80
60
40
POWER SUPPLY REJECTION – dB
20
0
–PSRR
1k1M100k10k100
FREQUENCY – Hz
+PSRR
TA = 25C
= 15V
V
S
TPC 21. Power Supply Rejection vs. Frequency @ ±15 V
6
VS = 5V
= 2k
R
5
4
L
T
A
A
VCL
= 25C
= 1
40
30
20
IMPEDANCE –
10
0
1k1M100k10k100
AV = 100
AV = 10
FREQUENCY – Hz
TA = 25C
= 15V
V
S
AV = 1
TPC 24. Closed-Loop Output Impedance vs. Frequency
@
±
15 V
30
25
20
VS = 15V
R
= 2k
L
= 25C
T
A
= 1
A
VOL
3
2
MAXIMUM OUTPUT SWING – Volts
1
0
TPC 22. Maximum Output Swing vs. Frequency @ 5 V
50
45
40
35
30
25
20
OVERSHOOT – %
15
10
REV. D
5
0
0
TPC 23. Small Signal Overshoot vs. Load
Capacitance @ 5 V
VS = 5V
= 2k
R
L
V
= 100mV p-p
IN
= 25C
T
A
= 1
A
VCL
100
10k10M1M100k1k
FREQUENCY – Hz
NEGATIVE
EDGE
LOAD CAPACITANCE – pF
POSITIVE
EDGE
TPC 25. Maximum Output Swing vs. Frequency @ ±15 V
400300200
500
–9–
15
10
MAXIMUM OUTPUT SWING – Volts
5
0
10k10M1M100k1k
FREQUENCY – Hz
TPC 26. Small Signal Overshoot vs. Load
±
Capacitance @
15 V
OP113/OP213/OP413
2.0
VS = 5, 0
V
4.0V
OUT
TEMPERATURE – C
+SLEW RATE
0.5V
1.5
1.0
SLEW RATE – V/s
0.5
0
–75
–50
TPC 27. Slew Rate vs. Temperature @ 5 V
V
(0.5 V
100
90
OUT
4.0 V)
–SLEW RATE
7510050250–25
1s
125
2.0
VS = 15V
V
1.5
1.0
SLEW RATE – V/s
0.5
0
–75
–50
TPC 30. Slew Rate vs. Temperature @ ±15 V
(–10 V
100
90
OUT
= 10V
≤
V
TEMPERATURE – C
≤ +10.0 V)
OUT
+SLEW RATE
–SLEW RATE
7510050250–25
1s
125
10
0%
20mV
TPC 28. Input Voltage Noise @ ±15 V (20 nV/div)
909
100
0.1Hz–10Hz
= 1000
A
V
AV = 100
t
OUT
TPC 29. Noise Test Diagram
10
0%
20mV
TPC 31. Input Voltage Noise @ 5 V (20 nV/div)
5
4
VS = 18V
3
2
SUPPLY CURRENT – mA
1
0
–75
–50
0–25
TEMPERATURE – C
VS = 15V
VS = 5.0V
100755025
125
TPC 32. Supply Current vs. Temperature
–10–
REV. D
OP113/OP213/OP413
16
2
136711 12
4
14
15
9
1
3
AD588BD
8
10
3
2
8
1
R5
1k
A2
2N2219A
+10.000V
+15V
–15V
10F
1/2
OP213
+10.000V
6
5
4
7
A1
R3
17.2k
0.1%
R4
500
CMRR TRIM
10-TURN
T.C. LESS THAN 50ppm/C
OUTPUT
0 10V
FS
–15V
350
LOAD
CELL
100mV
F.S.
R1
17.2k
0.1%
R2
301
0.1%
1/2
OP213
APPLICATIONS
The OP113, OP213, and OP413 form a new family of high
performance amplifiers that feature precision performance in
standard dual supply configurations and, more importantly,
maintain precision performance when a single power supply is
used. In addition to accurate dc specifications, it is the lowest
noise single supply amplifier available with only 4.7 nV/√Hz
typical noise density.
Single supply applications have special requirements due to the
generally reduced dynamic range of the output signal. Single
supply applications are often operated at voltages of 5 V or 12 V,
compared to dual supply applications with supplies of ±12 V or
± 15 V. This results in reduced output swings. Where a dual
supply application may often have 20 V of signal output swing,
single supply applications are limited to, at most, the supply range
and, more commonly, several volts below the supply. In order to
attain the greatest swing, the single supply output stage must
swing closer to the supply rails than in dual supply applications.
The OP113 family has a new patented output stage that allows
the output to swing closer to ground, or the negative supply,
than previous bipolar output stages. Previous op amps had
outputs that could swing to within about ten millivolts of the
negative supply in single supply applications. However, the
OP113 family combines both a bipolar and a CMOS device in
the output stage, enabling it to swing to within a few hundred
microvolts of ground.
When operating with reduced supply voltages, the input range is
also reduced. This reduction in signal range results in reduced
signal-to-noise ratio, for any given amplifier. There are only two
ways to improve this: increase the signal range or reduce the
noise. The OP113 family addresses both of these parameters.
Input signal range is from the negative supply to within one
volt of the positive supply over the full supply range. Competitive parts have input ranges that are a half a volt to five
volts less than this. Noise has also been optimized in the OP113
family. At 4.7 nV/√Hz, it is less than one fourth that of competitive devices.
Phase Reversal
The OP113 family is protected against phase reversal as long
as both of the inputs are within the supply ranges. However, if
there is a possibility of either input going below the negative
supply (or ground in the single supply case), the inputs should
be protected with a series resistor to limit input current to 2 mA.
OP113 Offset Adjust
The OP113 has the facility for external offset adjustment,
using the industry standard arrangement. Pins 1 and 5 are used
in conjunction with a potentiometer of 10 kΩ total resistance,
of approximately 3.3 µV/°C
OS
connected with the wiper to V– (or ground in single supply
applications). The total adjustment range is about ±2 mV using
this configuration.
Adjusting the offset to zero has minimal effect on offset drift
(assuming the potentiometer has a tempco of less than 1000 ppm/
°C). Adjustment away from zero, however, (like all bipolar
amplifiers) will result in a TCV
for every millivolt of induced offset.
It is therefore not generally recommended that this trim be
used to compensate for system errors originating outside of the
OP113. The initial offset of the OP113 is low enough that external
trimming is almost never required but, if necessary, the 2 mV trim
REV. D
range may be somewhat excessive. Reducing the trimming
potentiometer to a 2 kΩ value will give a more reasonable range
of ±400 µV.
Figure 1. Precision Load Cell Scale Amplifier
APPLICATION CIRCUITS
A High Precision Industrial Load-Cell Scale Amplifier
The OP113 family makes an excellent amplifier for conditioning
a load-cell bridge. Its low noise greatly improves the signal resolution, allowing the load cell to operate with a smaller output
range, thus reducing its nonlinearity. Figure 1 shows one half of
the OP113 family used to generate a very stable 10.000 V bridge
excitation voltage while the second amplifier provides a differential
gain. R4 should be trimmed for maximum common-mode rejection.
A Low Voltage Single Supply, Strain-Gage Amplifier
The true zero swing capability of the OP113 family allows the
amplifier in Figure 2 to amplify the strain-gage bridge accurately
even with no signal input while being powered by a single 5 V
supply. A stable 4.000 V bridge voltage is made possible by the
rail-to-rail OP295 amplifier, whose output can swing to within a
millivolt of either rail. This high voltage swing greatly increases
the bridge output signal without a corresponding increase in
bridge input.
5V
2
IN
6
OUT
GND
5
6
4
REF43
5V
8
1/2
OP295
4
100k
OUTPUT
0V 3.5V
7
R4
350
35mV
FS
2N2222A
4.000V
3
2
R1
100k
1
12.0k
1/2
OP213
R8
8
1/2
OP295
4
1
R2
20k
R5
2.10k
R
= 2,127.4
G
3
2
27.4
2.500V
R7
20.0k
R3
20k
R6
Figure 2. Single Supply Strain-Gage Amplifier
–11–
OP113/OP213/OP413
A High Accuracy Linearized RTD Thermometer Amplifier
Zero suppressing the bridge facilitates simple linearization of the
RTD by feeding back a small amount of the output signal to the
RTD (Resistor Temperature Device). In Figure 3, the left leg of
the bridge is servoed to a virtual ground voltage by amplifier
A1, while the right leg of the bridge is also servoed to zero volt
by amplifier A2. This eliminates any error resulting from commonmode voltage change in the amplifier. A 3-wire RTD is used to
balance the wire resistance on both legs of the bridge, thereby
reducing temperature mismatch errors. The 5.000 V bridge
excitation is derived from the extremely stable AD588 reference
device with 1.5 ppm/°C drift performance.
Linearization of the RTD is done by feeding a fraction of the
output voltage back to the RTD in the form of a current. With
just the right amount of positive feedback, the amplifier output
will be linearly proportional to the temperature of the RTD.
+15V–15V
2
16
10F
100
RTD
11
12
13
4
6
AD588BD
7
14
15
1
R3
3
50
10
8
9
R
R
R
R1
8.25k
W1
W2
W3
RG FULL SCALE ADJUST
R2
8.25k
R4
100
2
3
1
A1
1/2
R5
4.02k
6
A2
5
+15V
8
4
–15V
R7
100
7
1/2
OP213
R8
49.9k
V
(10mV/C)
OUT
–1.50V = –150C
+5.00V = +500C
R9
5k
LINEARITY
ADJUST
@1/2 FS
OP213
Figure 3. Ultraprecision RTD Amplifier
To calibrate the circuit, first immerse the RTD in a zero-degree
ice bath or substitute an exact 100 Ω resistor in place of the
RTD. Adjust the ZERO ADJUST potentiometer for a 0.000 V
output, then set R9 LINEARITY ADJUST potentiometer to
the middle of its adjustment range. Substitute a 280.9 Ω resistor
(equivalent to 500°C) in place of the RTD, and adjust the
FULL-SCALE ADJUST potentiometer for a full-scale voltage
of 5.000 V.
To calibrate out the nonlinearity, substitute a 194.07 Ω resistor
(equivalent to 250°C) in place of the RTD, then adjust the
LINEARITY ADJUST potentiometer for a 2.500 V output.
Check and readjust the full-scale and half-scale as needed.
Once calibrated, the amplifier outputs a 10 mV/°C temperature
coefficient with an accuracy better than ±0.5°C over an RTD
measurement range of –150°C to +500°C. Indeed the amplifier
can be calibrated to a higher temperature range, up to 850°C.
A High Accuracy Thermocouple Amplifier
Figure 4 shows a popular K-type thermocouple amplifier with
cold-junction compensation. Operating from a single 12 V supply,
the OP113 family’s low noise allows temperature measurement
to better than 0.02°C resolution from 0°C to 1000°C range.
The cold-junction error is corrected by using an inexpensive silicon
diode as a temperature measuring device. It should be placed as
close to the two terminating junctions as physically possible. An
aluminum block might serve well as an isothermal system.
1N4148
D1
R4
5.000V
R1
10.7k
R2
2.74k
200
R3
53.6
R9
124k
R5
40.2k
R8
453
R6
2
OP213
3
12V
1/2
10F
0.1F
8
4
+
1
0V TO 10.00V
(0C TO 1000C)
12V
0.1F
K-TYPE
THERMOCOUPLE
40.7V/C
26
REF02EZ
4
––
++
5.62k
Figure 4. Accurate K-Type Thermocouple Amplifier
R6 should be adjusted for a zero-volt output with the thermocouple measuring tip immersed in a zero-degree ice bath. When
calibrating, be sure to adjust R6 initially to cause the output to
swing in the positive direction first. Then back off in the negative direction until the output just stops changing.
An Ultralow Noise, Single Supply Instrumentation Amplifier
Extremely low noise instrumentation amplifiers can be built
using the OP113 family. Such an amplifier that operates off a
single supply is shown in Figure 5. Resistors R1–R5 should be
of high precision and low drift type to maximize CMRR performance. Although the two inputs are capable of operating to zero
volt, the gain of –100 configuration will limit the amplifier input
common mode to not less than 0.33 V.
5V TO 36V
+
V
IN
–
*R1
10k
*ALL RESISTORS 0.1%, 25ppm/C
1/2
OP213
10k
*R2
(200 + 12.7)
*R3
10k
*R
G
1/2
OP213
*R4
10k
GAIN = + 6
20k
R
V
OUT
G
Figure 5. Ultralow Noise, Single Supply Instrumentation
Amplifier
–12–
REV. D
OP113/OP213/OP413
Supply Splitter Circuit
The OP113 family has excellent frequency response characteristic that makes it an ideal pseudo-ground reference generator as
shown in Figure 6. The OP113 family serves as a voltage follower
buffer. In addition, it drives a large capacitor that serves as a charge
reservoir to minimize transient load changes, as well as a low
impedance output device at high frequencies. The circuit easily
supplies 25 mA load current with good settling characteristics.
+ = 5V 12V
V
S
R3
2.5k
C1
8
1/2
OP113
4
0.1F
R4
100
1
+
C2
1F
VS+
2
OUTPUT
5k
5k
R1
2
3
R2
Figure 6. False Ground Generator
Low Noise Voltage Reference
Few reference devices combine low noise and high output drive
capabilities. Figure 7 shows the OP113 family used as a two-pole
active filter that band limits the noise of the 2.500 V reference.
Total noise measures 3 µV p-p.
5V
5V
2
IN
OUT
REF43
GND
4
–
10F
+
10k
10k
6
+
C2
10F
2
3
8
1/2
OP113
4
1
3V p-p NOISE
OUTPUT
2.500V
Figure 7. Low Noise Voltage Reference
5 V Only Stereo DAC for Multimedia
The OP113 family’s low noise and single supply capability are
ideally suited for stereo DAC audio reproduction or sound
synthesis applications such as multimedia systems. Figure 8
shows an 18-bit stereo DAC output setup that is powered from a
single 5 V supply. The low noise preserves the 18-bit dynamic
range of the AD1868. For DACs that operate on dual supplies,
the OP113 family can also be powered from the same supplies.
5V SUPPLY
L
DL
18-BIT
DAC
18-BIT
SERIAL
REG.
18-BIT
SERIAL
REG.
18-BIT
DAC
AD1868
1
V
LL
2
3
4
CK
DR
5
LR
6
DGND
7
8
VBR
VBL
16
15
7.68k
7.68k
9.76k
9.76k
14
VOL
V
REF
AGND
V
REF
VOR
330pF
13
12
11
10
9
V
S
330pF
OP213
7.68k
7.68k
6
OP213
5
1/2
1/2
8
100pF
100pF
220F
1
+
220F
7
+
LEFT
CHANNEL
–
OUTPUT
47k
RIGHT
CHANNEL
–
OUTPUT
47k
Figure 8. 5 V Only 18-Bit Stereo DAC
SoundPort is a registered trademark of Analog Devices, Inc.
REV. D
–13–
OP113/OP213/OP413
Low Voltage Headphone Amplifiers
Figure 9 shows a stereo headphone output amplifier for the
AD1849 16-bit SoundPort
®
Stereo Codec device. The pseudoreference voltage is derived from the common-mode voltage
generated internally by the AD1849, thus providing a convenient bias for the headphone output amplifiers.
OPTIONAL
GAIN
LOUT1L
AD1849
CMOUT
LOUT1R
1k
V
REF
10F
31
V
19
29
REF
10k
10k
10F
L VOLUME
CONTROL
R VOLUME
CONTROL
1k
OPTIONAL
GAIN
V
REF
5k
5V
1/2
OP213
5V
1/2
OP213
1/2
OP213
5k
16
16
220F
+
47k
220F
+
47k
HEADPHONE
LEFT
HEADPHONE
RIGHT
Figure 9. Headphone Output Amplifier for Multimedia
Sound Codec
Low Noise Microphone Amplifier for Multimedia
The OP113 family is ideally suited as a low noise microphone
preamp for low voltage audio applications. Figure 10 shows a
gain of 100 stereo preamp for the AD1849 16-bit SoundPort
Stereo Codec chip. The common-mode output buffer serves as
a “phantom power” driver for the microphones.
10k
5V
LEFT
ELECTRET
CONDENSER
MIC
INPUT
RIGHT
ELECTRET
CONDENSER
MIC
INPUT
20
20
10F
OP213
10F
1/2
50
5V
1/2
10k
50
OP213
10010k
100
1/2
OP213
10k
17
MINL
AD1849
19
CMOUT
15
MINR
Precision Voltage Comparator
With its PNP inputs and zero volt common-mode capability, the
OP113 family can make useful voltage comparators. There is
only a slight penalty in speed in comparison to IC comparators.
However, the significant advantage is its voltage accuracy. For
example, V
can be a few hundred microvolts or less, combined
OS
with CMRR and PSRR exceeding 100 dB, while operating on 5 V
supply. Standard comparators like the 111/311 family operate
on 5 V, but not with common-mode at ground, nor with offset
below 3 mV. Indeed, no commercially available single supply
comparator has a V
less than 200 µV.
OS
Figure 11 shows the OP113 family response to a 10 mV overdrive signal when operating in open loop. The top trace shows
the output rising edge has a 15 µs propagation delay, while the
bottom trace shows a 7 µs delay on the output falling edge. This
ac response is quite acceptable in many applications.
10mV OVERDRIVE
+2.5V
0V
–2.5V
t
=
t
= 5ms
r
f
100
90
10
0%
25k
100
2V
2V
5V
1/2
OP113
5s
Figure 11. Precision Comparator
The low noise and 250 µV (maximum) offset voltage enhance the
overall dc accuracy of this type of comparator. Note that zero
crossing detectors and similar ground referred comparisons can be
implemented even if the input swings to –0.3 V below ground.