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Электронный компонент: OP295GBC

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PIN CONNECTIONS
8-Lead Narrow-Body SO
8-Lead Epoxy DIP
(S Suffix)
(P Suffix)
OUT A
IN A
+IN A
V
V+
OUT B
IN B
+IN B
1
2
3
4
5
6
7
8
OP295
OUT A
IN A
+IN A
V
V+
OUT B
IN B
+IN B
1
2
3
4
5
6
7
8
OP295
14-Lead Epoxy DIP
16-Lead SO (300 Mil)
(P Suffix)
(S Suffix)
OUT A
IN A
+IN A
V
OUT B
IN D
+IN D
OUT D
IN B
+IN B
V+
OUT C
IN C
+IN C
1
2
3
4
11
12
13
14
OP495
5
6
7
8
9
10
OUT A
IN A
+IN A
V
OUT D
IN D
+IN D
OUT B
IN B
+IN B
NC
V+
OUT C
IN C
+IN C
1
2
3
4
13
14
15
16
5
6
7
8
9
10
11
12
OP495
NC
NC = NO CONNECT
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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
a
Dual/Quad Rail-to-Rail
Operational Amplifiers
OP295/OP495
Analog Devices, Inc., 1995
One Technology Way, P.O. Box 9106, Norwood. MA 02062-9106, U.S.A.
Tel: 617/329-4700
Fax: 617/326-8703
FEATURES
Rail-to-Rail Output Swing
Single-Supply Operation: +3 V to +36 V
Low Offset Voltage: 300 V
Gain Bandwidth Product: 75 kHz
High Open-Loop Gain: 1000 V/mV
Unity-Gain Stable
Low Supply Current/Per Amplifier: 150 A max
APPLICATIONS
Battery Operated Instrumentation
Servo Amplifiers
Actuator Drives
Sensor Conditioners
Power Supply Control
GENERAL DESCRIPTION
Rail-to-rail output swing combined with dc accuracy are the key
features of the OP495 quad and OP295 dual CBCMOS opera-
tional amplifiers. By using a bipolar front end, lower noise and
higher accuracy than that of CMOS designs has been achieved.
Both input and output ranges include the negative supply, pro-
viding the user "zero-in/zero-out" capability. For users of 3.3
volt systems such as lithium batteries, the OP295/OP495 is
specified for three volt operation.
Maximum offset voltage is specified at 300
V for +5 volt opera-
tion, and the open-loop gain is a minimum of 1000 V/mV. This
yields performance that can be used to implement high accuracy
systems, even in single supply designs.
The ability to swing rail-to-rail and supply +15 mA to the load
makes the OP295/OP495 an ideal driver for power transistors
and "H" bridges. This allows designs to achieve higher efficien-
cies and to transfer more power to the load than previously pos-
sible without the use of discrete components. For applications
that require driving inductive loads, such as transformers, in-
creases in efficiency are also possible. Stability while driving
capacitive loads is another benefit of this design over CMOS
rail-to-rail amplifiers. This is useful for driving coax cable or
large FET transistors. The OP295/OP495 is stable with loads in
excess of 300 pF.
The OP295 and OP495 are specified over the extended indus-
trial (40
C to +125
C) temperature range. OP295s are avail-
able in 8-pin plastic and ceramic DIP plus SO-8 surface mount
packages. OP495s are available in 14-pin plastic and SO-16
surface mount packages. Contact your local sales office for
MIL-STD-883 data sheet.
REV. B
2
OP295/OP495SPECIFICATIONS
ELECTRICAL CHARACTERISTICS
Parameter
Symbol
Conditions
Min
Typ
Max
Units
INPUT CHARACTERISTICS
Offset Voltage
V
OS
30
300
V
40
C
T
A
+125
C
800
V
Input Bias Current
I
B
8
20
nA
40
C
T
A
+125
C
30
nA
Input Offset Current
I
OS
1
3
nA
40
C
T
A
+125
C
5
nA
Input Voltage Range
V
CM
0
+4.0
V
Common-Mode Rejection Ratio
CMRR
0 V
V
CM
4.0 V, 40
C
T
A
+125
C
90
110
dB
Large Signal Voltage Gain
A
VO
R
L
= 10 k
, 0.005
V
OUT
4.0 V
1000
10,000
V/mV
R
L
= 10 k
, 40
C
T
A
+125
C
500
V/mV
Offset Voltage Drift
V
OS
/
T
1
5
V/
C
OUTPUT CHARACTERISTICS
Output Voltage Swing High
V
OH
R
L
= 100 k
to GND
4.98
5.0
V
R
L
= 10 k
to GND
4.90
4.94
V
I
OUT
= 1 mA, 40
C
T
A
+125
C
4.7
V
Output Voltage Swing Low
V
OL
R
L
= 100 k
to GND
0.7
2
mV
R
L
= 10 k
to GND
0.7
2
mV
I
OUT
= 1 mA, 40
C
T
A
+125
C
90
mV
Output Current
I
OUT
11
18
mA
POWER SUPPLY
Power Supply Rejection Ratio
PSRR
1.5 V
V
S
15 V
90
110
dB
1.5 V
V
S
15 V,
40
C
T
A
+125
C
85
dB
Supply Current Per Amplifier
I
SY
V
OUT
= 2.5 V, R
L
=
, 40
C
T
A
+125
C
150
A
DYNAMIC PERFORMANCE
Skew Rate
SR
R
L
= 10 k
0.03
V/
s
Gain Bandwidth Product
GBP
75
kHz
Phase Margin
O
86
Degrees
NOISE PERFORMANCE
Voltage Noise
e
n
p-p
0.1 Hz to 10 Hz
1.5
V p-p
Voltage Noise Density
e
n
f = 1 kHz
51
nV/
Hz
Current Noise Density
i
n
f = 1 kHz
<0.1
pA/
Hz
Specifications subject to change without notice.
ELECTRICAL CHARACTERISTICS
Parameter
Symbol
Conditions
Min
Typ
Max
Units
INPUT CHARACTERISTICS
Offset Voltage
V
OS
30
500
V
Input Bias Current
I
B
8
20
nA
Input Offset Current
I
OS
1
3
nA
Input Voltage Range
V
CM
0
+2.0
V
Common-Mode Rejection Ratio
CMRR
0 V
V
CM
2.0 V, 40
C
T
A
+125
C
90
110
dB
Large Voltage Gain
A
VO
R
L
= 10 k
750
V/mV
Offset Voltage Drift
V
OS
/
T
1
V/
C
OUTPUT CHARACTERISTICS
Output Voltage Swing High
V
OH
R
L
= 10 k
to GND
2.9
V
Output Voltage Swing Low
V
OL
R
L
= 10 k
to GND
0.7
2
mV
POWER SUPPLY
Power Supply Rejection Ratio
PSRR
1.5 V
V
S
15 V
90
110
dB
1.5 V
V
S
15 V,
40
C
T
A
+125
C
85
dB
Supply Current Per Amplifier
I
SY
V
OUT
= 1.5 V, R
L
=
, 40
C
T
A
+125
C
150
A
DYNAMIC PERFORMANCE
Slew Rate
SR
R
L
= 10 k
0.03
V/
s
Gain Bandwidth Product
GBP
75
kHz
Phase Margin
O
85
Degrees
NOISE PERFORMANCE
Voltage Noise
e
n
p-p
0.1 Hz to 10 Hz
1.6
V p-p
Voltage Noise Density
e
n
f = 1 kHz
53
nV/
Hz
Current Noise Density
i
n
f = 1 kHz
<0.1
pA/
Hz
Specifications subject to change without notice.
(@ V
S
= +5.0 V, V
CM
= +2.5 V, T
A
= +25 C unless otherwise noted)
(@ V
S
= +3.0 V, V
CM
= +1.5 V, T
A
= +25 C unless otherwise noted)
ELECTRICAL CHARACTERISTICS
Parameter
Symbol
Conditions
Min
Typ
Max
Units
INPUT CHARACTERISTICS
Offset Voltage
V
OS
30
300
V
40
C
T
A
+125
C
800
V
Input Bias Current
I
B
V
CM
= 0 V
7
20
nA
V
CM
= 0 V, 40
C
T
A
+125
C
30
nA
Input Offset Current
I
OS
V
CM
= 0 V
1
3
nA
V
CM
= 0 V, 40
C
T
A
+125
C
5
nA
Input Voltage Range
V
CM
15
+13.5
V
Common-Mode Rejection Ratio
CMRR
15.0 V
V
CM
+13.5 V, 40
C
T
A
+125
C
90
110
dB
Large Signal Voltage Gain
A
VO
R
L
= 10 k
1000
4000
V/mV
Offset Voltage Drift
V
OS
/
T
1
V/
C
OUTPUT CHARACTERISTICS
Output Voltage Swing High
V
OH
R
L
= 100 k
to GND
14.95
V
R
L
= 10 k
to GND
14.80
V
Output Voltage Swing Low
V
OL
R
L
= 100 k
to GND
14.95
V
R
L
= 10 k
to GND
14.85
V
Output Current
I
OUT
15
25
mA
POWER SUPPLY
Power Supply Rejection Ratio
PSRR
V
S
=
1.5 V to
15 V
90
110
dB
V
S
=
1.5 V to
15 V, 40
C
T
A
+125
C
85
dB
Supply Current
I
SY
V
O
= 0 V, R
L
=
, V
S
=
18 V,
40
C
T
A
+125
C
175
A
Supply Voltage Range
V
S
+3 (
1.5)
+36 (
18)
V
DYNAMIC PERFORMANCE
Slew Rate
SR
R
L
= 10 k
0.03
V/
s
Gain Bandwidth Product
GBP
85
kHz
Phase Margin
O
83
Degrees
NOISE PERFORMANCE
Voltage Noise
e
n p-p
0.1 Hz to 10 Hz
1.25
V p-p
Voltage Noise Density
e
n
f =1 kHz
45
nV/
Hz
Current Noise Density
i
n
f = 1 kHz
<0.1
pA/
Hz
Specifications subject to change without notice.
WAFER TEST LIMITS
Parameter
Symbol
Conditions
Limit
Units
Offset Voltage
Vos
300
V max
Input Bias Current
I
B
20
nA max
Input Offset Current
I
OS
2
nA max
Input Voltage Range
1
V
CM
0 to +4
V min
Common-Mode Rejection Ratio
CMRR
0 V
V
CM
4 V
90
dB min
Power Supply Rejection Ratio
PSRR
1.5 V
V
S
15 V
90
V/V
Large Signal Voltage Gain
A
VO
R
L
= 10 k
1000
V/mV min
Output Voltage Swing High
V
OH
R
L
= 10 k
4.9
V min
Supply Current Per Amplifier
I
SY
V
OUT
= 2.5 V, R
L
=
150
A max
NOTES
Electrical tests and wafer probe to the limits shown. Due to variations in assembly methods and normal yield loss, yield after packaging is not guaranteed for standard
product dice. Consult factory to negotiate specifications based on dice lot qualifications through sample lot assembly and testing.
1
Guaranteed by CMRR test.
ORDERING GUIDE
OP295/OP495
REV. B
3
(@ V
S
=
15.0 V, T
A
= +25 C unless otherwise noted)
Temperature
Package
Package
Model
Range
Description
Option
OP295GP
40
C to +125
C
8-Pin Plastic DIP
N-8
OP295GS
40
C to +125
C
8-Pin SOIC
SO-8
OP295GBC +25
C
DICE
Temperature
Package
Package
Model
Range
Description
Option
OP495GP
40
C to +125
C
14-Pin Plastic DIP
N-14
OP495GS
40
C to +125
C
16-Pin SOL
R-16
OP495GBC +25
C
DICE
(@ V
S
= +5.0 V, V
CM
= 2.5 V, T
A
= +25 C unless otherwise noted)
REV. B
4
OP295/OP495
ABSOLUTE MAXIMUM RATINGS
1
Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
18 V
Input Voltage
2
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
18 V
Differential Input Voltage
2
. . . . . . . . . . . . . . . . . . . . . . . +36 V
Output Short-Circuit Duration . . . . . . . . . . . . . . . . . Indefinite
Storage Temperature Range
P, S Package . . . . . . . . . . . . . . . . . . . . . . . . 65
C to +150
C
Operating Temperature Range
OP295G, OP495G . . . . . . . . . . . . . . . . . . . 40
C to +125
C
Junction Temperature Range
P, S Package . . . . . . . . . . . . . . . . . . . . . . . . 65
C to +150
C
Lead Temperature Range (Soldering, 60 Sec) . . . . . . . +300
C
Package Type
JA
3
JC
Unit
8-Pin Plastic DIP (P)
103
43
C/W
8-Pin SOIC (S)
158
43
C/W
14-Pin Plastic DIP (P)
83
39
C/W
16-Pin SO (S)
98
30
C/W
NOTES
1
Absolute maximum ratings apply to both DICE and packaged parts, unless
otherwise noted.
2
For supply voltages less than
18 V, the absolute maximum input voltage is equal
to the supply voltage.
3
JA
is specified for the worst case conditions, i.e.,
JA
is specified for device in socket
for cerdip, P-DIP, and LCC packages;
JA
is specified for device soldered in circuit
board for SOIC package.
DICE CHARACTERISTICS
OP295 Die Size 0.066
0.080 inch, 5,280 sq. mils.
Substrate (Die Backside) Is Connected to V+.
Transistor Count, 74.
OP495 Die Size 0.113
0.083 inch, 9,380 sq. mils.
Substrate (Die Backside) Is Connected to V+.
Transistor Count, 196.
Typical Characteristics
140
20
100
80
40
25
60
50
120
100
75
50
25
0
TEMPERATURE
C
SUPPLY CURRENT PER AMPLIFIER
A
V
S
= +5V
V
S
= +3V
V
S
= +36V
15.2
15.2
100
14.6
15.0
25
14.8
50
14.2
14.4
14.4
14.6
14.8
15.0
75
50
25
0
TEMPERATURE
C
OUTPUT SWING Volts
+ OUTPUT SWING Volts
V
S
=
15V
R
L
= 100k
R
L
= 2k
R
L
= 2k
R
L
= 100k
R
L
= 10k
R
L
= 10k
Supply Current Per Amplifier vs. Temperature
Output Voltage Swing vs. Temperature
REV. B
5
Typical CharacteristicsOP295/OP495
3.10
2.50
100
2.80
2.60
25
2.70
50
3.00
2.90
75
50
25
0
TEMPERATURE
C
OUTPUT VOLTAGE SWING Volts
R
L
= 2k
V
S
= +3V
R
L
= 100k
R
L
= 10k
Output Voltage Swing vs. Temperature
200
0
250
50
25
200
250
100
75
125
150
175
200
150
100
50
0
50
100
150
V
S
= +5V
T
A
= +25
C
INPUT OFFSET VOLTAGE
V
UNITS
BASED ON 600 OP AMPS
OP295 Input Offset (V
OS
) Distribution
UNITS
250
0
3.2
75
25
0.4
50
0
150
100
125
175
200
225
2.8
2.4
2.0
1.6
1.2
0.8
BASED ON 600 OP AMPS
V
S
= +5V
40
T
A
+85
C
T
C
V
OS
V/
C
OP295 TCV
OS
Distribution
5.10
4.50
100
4.80
4.60
25
4.70
50
5.00
4.90
75
50
25
0
TEMPERATURE
C
OUTPUT VOLTAGE SWING Volts
V
S
= +5V
R
L
= 100k
R
L
= 2k
R
L
= 10k
Output Voltage Swing vs. Temperature
500
0
300
150
50
50
100
100
300
200
250
350
400
450
250
200
150
100
50
0
INPUT OFFSET VOLTAGE
V
UNITS
V
S
= +5V
T
A
= +25
C
BASED ON 1200 OP AMPS
OP495 Input Offset (V
OS
) Distribution
500
0
3.2
150
50
0.4
100
0
300
200
250
350
400
450
2.8
2.4
2.0
1.6
1.2
0.8
T
C
V
OS
V/
C
UNITS
V
S
= +5V
40
T
A
+85
C
BASED ON 1200 OP AMPS
OP495 TCV
OS
Distribution
REV. B
6
OP295/OP495Typical Characteristics
V
S
= +5V
20
0
100
12
4
25
8
50
16
75
50
25
0
TEMPERATURE
C
INPUT BIAS CURRENT nA
Input Bias Current vs. Temperature
V
S
= +5V
TEMPERATURE
C
40
0
100
10
5
25
50
20
15
25
30
35
75
50
25
0
V
S
=
15V
SOURCE
SINK
SOURCE
SINK
OUTPUT CURRENT mA
Output Current vs. Temperature
TEMPERATURE
C
OPEN-LOOP GAIN V/
V
R
L
= 2k
100
10
1
50
25
100
0
25
50
75
V
S
=
15V
V
O
=
10V
R
L
= 10k
R
L
= 100k
Open-Loop Gain vs. Temperature
12
0
100
6
2
25
4
50
10
8
75
50
25
0
TEMPERATURE
C
OPEN-LOOP GAIN V/
V
V
S
= +5V
V
O
= +4V
R
L
= 100k
R
L
= 10k
R
L
= 2k
Open-Loop Gain vs. Temperature
1V
100
V
1
A
10
A
10mA
1mA
100
A
100mV
10mV
1mV
LOAD CURRENT
OUTPUT VOLTAGE
TO RAIL
SOURCE
SINK
V
S
= +5V
T
A
= +25
C
Output Voltage to Supply Rail vs. Load Current
OP295/OP495
REV. B
7
APPLICATIONS
Rail-to-Rail Applications Information
The OP295/OP495 has a wide common-mode input range ex-
tending from ground to within about 800 mV of the positive
supply. There is a tendency to use the OP295/OP495 in buffer
applications where the input voltage could exceed the common-
mode input range. This may initially appear to work because of
the high input range and rail-to-rail output range. But above the
common-mode input range the amplifier is, of course, highly
nonlinear. For this reason it is always required that there be
some minimal amount of gain when rail-to-rail output swing is
desired. Based on the input common-mode range this gain
should be at least 1.2.
Low Drop-Out Reference
The OP295/OP495 can be used to gain up a 2.5 V or other low
voltage reference to 4.5 volts for use with high resolution A/D
converters that operate from +5 volt only supplies. The circuit
in Figure 1 will supply up to 10 mA. Its no-load drop-out volt-
age is only 20 mV. This circuit will supply over 3.5 mA with a
+5 volt supply.
16k
V
OUT
= 4.5V
1 TO 10
F
10
0.001
F
20k
REF43
2
6
4
+5V
+5V
1/2
OP295/
OP495
Figure 1. 4.5 Volt, Low Drop-Out Reference
Low Noise, Single Supply Preamplifier
Most single supply op amps are designed to draw low supply
current, at the expense of having higher voltage noise. This
tradeoff may be necessary because the system must be powered
by a battery. However, this condition is worsened because all
circuit resistances tend to be higher; as a result, in addition to
the op amp's voltage noise, Johnson noise (resistor thermal
noise) is also a significant contributor to the total noise of the
system.
The choice of monolithic op amps that combine the characteris-
tics of low noise and single supply operation is rather limited.
Most single supply op amps have noise on the order of 30 nV/
Hz
to 60 nV/
Hz
and single supply amplifiers with noise below
5 nV/
Hz
do not exist.
In order to achieve both low noise and low supply voltage opera-
tion, discrete designs may provide the best solution. The circuit
on Figure 2 uses the OP295/OP495 rail-to-rail amplifier and a
matched PNP transistor pair--the MAT03--to achieve zero-in/
zero-out single supply operation with an input voltage noise of
3.1 nV/
Hz
at 100 Hz. R5 and R6 set the gain of 1000, making
this circuit ideal for maximizing dynamic range when amplifying
low level signals in single supply applications. The OP295/OP495
provides rail-to-rail output swings, allowing this circuit to oper-
ate with 0 to 5 volt outputs. Only half of the OP295/OP495 is
used, leaving the other uncommitted op amp for use elsewhere.
MAT- 03
5
6
3
2
1
7
R3
R4
Q1
Q2
R1
R6
10
V
OUT
LED
1
8
4
3
2
R5
10k
C2
10
F
R7
510
C1
1500pF
R8
100
R2
27k
V
IN
0.1
F
10
F
Q2
2N3906
OP295/
OP495
Figure 2. Low Noise Single Supply Preamplifier
The input noise is controlled by the MAT03 transistor pair and
the collector current level. Increasing the collector current re-
duces the voltage noise. This particular circuit was tested with
1.85 mA and 0.5 mA of current. Under these two cases, the in-
put voltage noise was 3.1 nV/
Hz
and 10 nV/
Hz
, respectively.
The high collector currents do lead to a tradeoff in supply cur-
rent, bias current, and current noise. All of these parameters will
increase with increasing collector current. For example, typically
the MAT03 has an h
FE
= 165. This leads to bias currents of
11
A and 3
A, respectively. Based on the high bias currents,
this circuit is best suited for applications with low source imped-
ance such as magnetic pickups or low impedance strain gages.
Furthermore, a high source impedance will degrade the noise
performance. For example, a 1 k
resistor generates 4 nV/
Hz
of broadband noise, which is already greater than the noise of
the preamp.
The collector current is set by R1 in combination with the LED
and Q2. The LED is a 1.6 V "Zener" that has a temperature co-
efficient close to that of Q2's base-emitter junction, which pro-
vides a constant 1.0 V drop across R1. With R1 equal to 270
,
the tail current is 3.7 mA and the collector current is half that,
or 1.85 mA. The value of R1 can be altered to adjust the collec-
tor current. Whenever R1 is changed, R3 and R4 should also be
adjusted. To maintain a common-mode input range that in-
cludes ground, the collectors of the Q1 and Q2 should not go
above 0.5 V--otherwise they could saturate. Thus, R3 and R4
have to be small enough to prevent this condition. Their values
and the overall performance for two different values of R1 are
summarized in Table I. Lastly, the potentiometer, R8, is needed
to adjust the offset voltage to null it to zero. Similar perfor-
mance can be obtained using an OP90 as the output amplifier
with a savings of about 185
A of supply current. However, the
output swing will not include the positive rail, and the band-
width will reduce to approximately 250 Hz.
REV. B
8
OP295/OP495
Table I. Single Supply Low Noise Preamp Performance
I
C
= 1.85 mA
I
C
= 0.5 mA
R1
270
1.0 k
R3, R4
200
910
e
n
@ 100 Hz
3.15 nV/
Hz
8.6 nV/
Hz
e
n
@ 10 Hz
4.2 nV/
Hz
10.2 nV/
Hz
I
SY
4.0 mA
1.3 mA
I
B
11
A
3
A
Bandwidth
1 kHz
1 kHz
Closed-Loop Gain
1000
1000
Driving Heavy Loads
The OP295/OP495 is well suited to drive loads by using a
power transistor, Darlington or FET to increase the current to
the load. The ability to swing to either rail can assure that the
device is turned on hard. This results in more power to the load
and an increase in efficiency over using standard op amps with
their limited output swing. Driving power FETs is also possible
with the OP295/OP495 because of its ability to drive capacitive
loads of several hundred picofarads without oscillating.
Without the addition of external transistors the OP295/OP495
can drive loads in excess of
15 mA with
15 or +30 volt
supplies. This drive capability is somewhat decreased at lower
supply voltages. At
5 volt supplies the drive current is
11 mA.
Driving motors or actuators in two directions in a single supply
application is often accomplished using an "H" bridge. The
principle is demonstrated in Figure 3a. From a single +5 volt
supply this driver is capable of driving loads from 0.8 V to 4.2 V
in both directions. Figure 3b shows the voltages at the inverting
and noninverting outputs of the driver. There is a small crossover
glitch that is frequency dependent and would not cause problems
5k
10k
1.67V
10k
10k
2N2222
2N2222
OUTPUTS
2N2907
2N2907
+5V
0
V
IN
2.5V
Figure 3a. "H" Bridge
10
90
100
0%
2V
2V
1ms
Figure 3b. "H" Bridge Outputs
unless this was a low distortion application such as audio. If this
is used to drive inductive loads, be sure to add diode clamps to
protect the bridge from inductive kickback.
Direct Access Arrangement
OP295/OP495 can be used in a single supply Direct Access Ar-
rangement (DAA) as is shown an in Figure 4. This figure shows
a portion of a typical DM capable of operating from a single
+5 volt supply and it may also work on +3 volt supplies with
minor modifications. Amplifiers A2 and A3 are configured so
that the transmit signal TXA is inverted by A2 and is not in-
verted by A3. This arrangement drives the transformer differen-
tially so that the drive to the transformer is effectively doubled
over a single amplifier arrangement. This application takes ad-
vantage of the OP295/OP495's ability to drive capacitive loads,
and to save power in single supply applications.
2.5V REF
A3
20k
20k
750pF
20k
22.1k
0.1
F
475
3.3k
0.0047
F
0.1
F
0.033
F
A2
A1
20k
20k
37.4k
390pF
RXA
TXA
OP295/
OP495
OP295/
OP495
OP295/
OP495
1:1
Figure 4. Direct Access Arrangement
A Single Supply Instrumentation Amplifier
The OP295/OP495 can be configured as a single supply instru-
mentation amplifier as in Figure 5. For our example, V
REF
is set
equal to
V
+
2
and V
O
is measured with respect to V
REF
. The in-
put common-mode voltage range includes ground and the out-
put swings to both rails.
V+
V
IN
V
REF
1
R1
100k
R2
20k
R3
20k
R4
100k
V
O
V
IN
+ V
REF
V
O
= 5 +
200k
R
G
(
)
R
G
3
2
8
7
4
5
6
1/2
OP295/
OP495
1/2
OP295/
OP495
Figure 5. Single Supply Instrumentation Amplifier
Resistor R
G
sets the gain of the instrumentation amplifier. Mini-
mum gain is 6 (with no R
G
). All resistors should be matched in
absolute value as well as temperature coefficient to maximize
OP295/OP495
REV. B
9
common-mode rejection performance and minimize drift. This
instrumentation amplifier can operate from a supply voltage as
low as 3 volts.
A Single Supply RTD Thermometer Amplifier
This RTD amplifier takes advantage of the rail-to-rail swing of
the OP295/OP495 to achieve a high bridge voltage in spite of a
low 5 V supply. The OP295/OP495 amplifier servos a constant
200
A current to the bridge. The return current drops across
the parallel resistors 6.19 k
and the 2.55 M
, developing a
voltage that is servoed to 1.235 V, which is established by the
AD589 bandgap reference. The 3-wire RTD provides an equal
line resistance drop in both 100
legs of the bridge, thus im-
proving the accuracy.
The AMP04 amplifies the differential bridge signal and converts
it to a single-ended output. The gain is set by the series resis-
tance of the 332
resistor plus the 50
potentiometer. The
gain scales the output to produce a 4.5 V full scale. The
0.22
F capacitor to the output provides a 7 Hz low-pass filter
to keep noise at a minimum.
3
7
1
8
6
5
4
2
AMP04
0.22
F
332
50
26.7k
0.5%
100
0.5%
100
RTD
2.55M
1%
6.19k
1%
AD589
1.235
37.4k
+5V
200
10-TURNS
ZERO ADJ
26.7k
0.5%
V
O
4.5V = 450
C
0V = 0
C
+5V
1
2
3
1/2
OP295/
OP495
Figure 6. Low Power RTD Amplifier
A Cold Junction Compensated, Battery Powered
Thermocouple Amplifier
The OP295/OP495's 150
A quiescent current per amplifier
consumption makes it useful for battery powered temperature
measuring instruments. The K-type thermocouple terminates
into an isothermal block where the terminated junctions' ambi-
ent temperatures can be continuously monitored and corrected
by summing an equal but opposite thermal EMF to the ampli-
fier, thereby canceling the error introduced by the cold junctions.
V
O
0V = 0
C
5V = 500
C
4.99k
1%
1.33M
20k
SCALE
ADJUST
9V
24.3k
1%
24.9k
7.15k
1%
1.235V
AD589
24.9k
1%
500
10-TURN
2.1k
1%
475
1%
1.5M
1%
1N914
ISOTHERMAL
BLOCK
COLD
JUNCTIONS
CR
AL
CHROMEL
K-TYPE
THERMOCOUPLE
40.7
V/
C
ZERO
ADJUST
8
1
4
2
3
ALUMEL
OP295/
OP495
Figure 7. Battery Powered, Cold-Junction Compensated
Thermocouple Amplifier
To calibrate, immerse the thermocouple measuring junction in a
0
C ice bath, adjust the 500
Zero Adjust pot to zero volts out.
Then immerse the thermocouple in a 250
C temperature bath
or oven and adjust the Scale Adjust pot for an output voltage of
2.50 V, which is equivalent to 250
C. Within this temperature
range, the K-type thermocouple is quite accurate and produces
a fairly linear transfer characteristic. Accuracy of
3
C is achiev-
able without linearization.
Even if the battery voltage is allowed to decay to as low as 7 volts,
the rail-to-rail swing allows temperature measurements to
700
C. However, linearization may be necessary for tempera-
tures above 250
C where the thermocouple becomes rather
nonlinear. The circuit draws just under 500
A supply current
from a 9 V battery.
A 5 V Only, 12-Bit DAC That Swings 0 V to 4.095 V
Figure 8 shows a complete voltage output DAC with wide out-
put voltage swing operating off a single +5 V supply. The serial
input 12-bit D/A converter is configured as a voltage output
device with the 1.235 V reference feeding the current output pin
(I
OUT
) of the DAC. The V
REF
which is normally the input now
becomes the output.
The output voltage from the DAC is the binary weighted volt-
age of the reference, which is gained up by the output amplifier
such that the DAC has a 1 mV per bit transfer function.
+5V
R2
41.2k
R3
5k
R4
100k
V
DD
R
FB
V
REF
SRI
CLK
GND
I
OUT
DAC8043
3
4
7
6
5
1
2
8
+5V
DIGITAL
CONTROL
+5V
AD589
R1
17.8k
+1.23V
LD
V
O
=
(4.096V)
D
4096
TOTAL POWER DISSIPATION = 1.6mW
8
1
4
2
3
OP295/
OP495
Figure 8. A 5 Volt 12-Bit DAC with 0 V to +4.095 Output
Swing
420 mA Current Loop Transmitter
Figure 9 shows a self powered 420 mA current loop transmit-
ter. The entire circuit floats up from the single supply (12 V to
36 V) return. The supply current carries the signal within the 4
to 20 mA range. Thus the 4 mA establishes the baseline
8
1
2
3
220pF
220
REF02
GND
6
2
4
100
2N1711
100k
1%
HP
5082-2800
100
1%
V
IN
0 + 3V
100k
10-TURN
1.21M
1%
NULL ADJ
SPAN ADJ
182k
1%
10k
10-TURN
5V
+12V
TO
+36V
R
L
100
420mA
4
1/2
OP295/
OP495
Figure 9. 420 mA Current Loop Transmitter
REV. B
10
OP295/OP495
current budget with which the circuit must operate. This circuit
consumes only 1.4 mA maximum quiescent current, making 2.6
mA of current available to power additional signal conditioning
circuitry or to power a bridge circuit.
A 3 Volt Low-Dropout Linear Voltage Regulator
Figure 10 shows a simple 3 V voltage regulator design. The
regulator can deliver 50 mA load current while allowing a 0.2 V
dropout voltage. The OP295/OP495's rail-to-rail output swing
handily drives the MJE350 pass transistor without requiring spe-
cial drive circuitry. At no load, its output can swing less than the
pass transistor's base-emitter voltage, turning the device nearly
off. At full load, and at low emitter-collector voltages, the tran-
sistor beta tends to decrease. The additional base current is eas-
ily handled by the OP295/OP495 output.
The amplifier servos the output to a constant voltage, which
feeds a portion of the signal to the error amplifier.
Higher output current, to 100 mA, is achievable at a higher
dropout voltage of 3.8 V.
1000pF
43k
44.2k
1%
30.9k
1%
AD589
1.235V
V
O
100
F
I
L
< 50mA
MJE 350
V
IN
5V TO 3.2V
1/2
OP295/
OP495
8
1
4
2
3
Figure 10. 3 V Low Dropout Voltage Regulator
Figure 11 shows the regulator's recovery characteristic when its
output underwent a 20 mA to 50 mA step current change.
10
100
0%
90
1ms
20mV
2V
50mA
20mA
OUTPUT
STEP
CURRENT
CONTROL
WAVEFORM
Figure 11. Output Step Load Current Recovery
Low-Dropout, 500 mA Voltage Regulator with Fold-Back
Current Limiting
Adding a second amplifier in the regulation loop as shown in
Figure 12 provides an output current monitor as well as fold-
back current limiting protection.
Amplifier A1 provides error amplification for the normal voltage
regulation loop. As long as the output current is less than 1 am-
pere, amplifier A2's output swings to ground, reverse biasing the
diode and effectively taking itself out of the circuit. However, as
the output current exceeds 1 amp, the voltage that develops
across the 0.1
sense resistor forces the amplifier A2's output
to go high, forward-biasing the diode, which in turn closes the
current limit loop. At this point A2's lower output resistance
dominates the drive to the power MOSFET transistor, thereby
effectively removing the A1 voltage regulation loop from the
circuit.
If the output current greater than 1 amp persists, the current
limit loop forces a reduction of current to the load, which causes
a corresponding drop in output voltage. As the output voltage
drops, the current limit threshold also drops fractionally, result-
ing in a decreasing output current as the output voltage de-
creases, to the limit of less than 0.2 A at 1 V output. This
"fold-back" effect reduces the power dissipation considerably
during a short circuit condition, thus making the power supply
far more forgiving in terms of the thermal design requirements.
Small heat sinking on the power MOSFET can be tolerated.
The OP295's rail-to-rail swing exacts higher gate drive to
the power MOSFET, providing a fuller enhancement to the
transistor. The regulator exhibits 0.2 V dropout at 500 mA of
load current. At 1 amp output, the dropout voltage is typically
5.6 volts.
124k
1%
124k
1%
REF43
4
6
2
0.01
F
100k
5%
210k
1%
205k
1%
45.3k
1%
45.3k
1%
R
SENSE
0.1
1/4W
+5V V
O
I
O
(NORM) = 0.5A
I
O
(MAX) = 1A
S
D
G
IRF9531
1N4148
2.500V
A1
A2
1
3
2
8
7
4
5
6
6V
1/2
OP295/
OP495
1/2
OP295/
OP495
Figure 12. Low Dropout, 500 mA Voltage Regulator with
Fold-Back Current Limiting
Square Wave Oscillator
The circuit in Figure 13 is a square wave oscillator (note the
positive feedback). The rail-to-rail swing of the OP295/OP495
helps maintain a constant oscillation frequency even if the sup-
ply voltage varies considerably. Consider a battery powered sys-
tem where the voltages are not regulated and drop over time.
The rail-to-rail swing ensures that the noninverting input sees
the full V+/2, rather than only a fraction of it.
The constant frequency comes from the fact that the 58.7 k
feedback sets up Schmitt Trigger threshold levels that are di-
rectly proportional to the supply voltage, as are the RC charge
voltage levels. As a result, the RC charge time, and therefore the
frequency, remains constant independent of supply voltage. The
slew rate of the amplifier limits the oscillation frequency to a
maximum of about 800 Hz at a +5 V supply.
Single Supply Differential Speaker Driver
Connected as a differential speaker driver, the OP295/OP495
can deliver a minimum of 10 mA to the load. With a 600
load, the OP295/OP495 can swing close to 5 volts peak-to-peak
across the load.
OP295/OP495
REV. B
11
8
1
4
2
3
58.7k
100k
C
R
V+
FREQ OUT
f
OSC
=
< 350Hz @ V+ = +5V
1
RC
100k
1/2
OP295/
OP495
Figure 13. Square Wave Oscillator Has Stable Frequency
Regardless of Supply Changes
V
IN
10k
V+
10k
100k
90.9k
20k
20k
V+
SPEAKER
2.2
F
1/4
OP295/
OP495
1/4
OP295/
OP495
1/4
OP295/
OP495
Figure 14. Single Supply Differential Speaker Driver
High Accuracy, Single-Supply, Low Power Comparator
The OP295/OP495 makes an accurate open-loop comparator.
With a single +5 V supply, the offset error is less than 300
V. Fig-
ure 15 shows the OP295/OP495's response time when operating
open-loop with 4 mV overdrive. It exhibits a 4 ms response time at
the rising edge and a 1.5 ms response time at the falling edge.
10
100
0%
90
5ms
2V
1V
OUTPUT
(5mV OVERDRIVE
@ OP295 INPUT)
INPUT
Figure 15. Open-Loop Comparator Response Time with
5 mV Overdrive
OP295/OP495 SPICE MODEL Macro-Model
* Node Assignments
*
Noninverting Input
*
Inverting Input
*
Positive Supply
*
Negative Supply
*
Output
*
*
.SUBCKT OP295
1
2
99
50
20
*
* INPUT STAGE
*
I1
99
4
2E-6
R1
1
6
5E3
R2
2
5
5E3
CIN
1
2
2E-12
IOS
1
2
0.5E-9
D1
5
3
DZ
D2
6
3
DZ
EOS
7
6
POLY (1) (31,39) 30E-6 0.024
Q1
8
5
4
QP
Q2
9
7
4
QP
R3
8
50
25.8E3
R4
9
50
25.8E3
*
* GAIN STAGE
*
R7
10
98
270E6
G1
98
10
POLY (1) (9,8) 4.26712E-9 27.8E-6
EREF 98
0
(39, 0) 1
R5
99
39
100E3
R6
39
50
100E3
*
* COMMON MODE STAGE
*
ECM
30
98
POLY(2) (1,39) (2,39) 0 0.5 0.5
R12
30
31
1E6
R13
31
98
100
*
* OUTPUT STAGE
*
I2
18
50
1.59E-6
V2
99
12
DC 2.2763
Q4
10
14
50
QNA
1.0
R11
14
50
33
M3
15
10
13
13
MN L=9E-6 W=102E-6 AD=15E-10 AD=15E-10
M4
13
10
50
50
MN L=9E-6 W=50E-6 AD=75E-11 AS=75E-11
D8
10
22
DX
V3
22
50
DC 6
M2
20
10
14
14
MN L=9E-6 W=2000E-6 AD=30E-9 AS=30E-9
Q5
17
17
99
QPA
1.0
Q6
18
17
99
QPA
4.0
R8
18
99
2.2E6
Q7
18
19
99
QPA
1.0
R9
99
19
8
C2
18
99
20E-12
M6
15
12
17
99
MP L=9E-6 W=27E-6 AD=405E-12 AS=405E-12
M1
20
18
19
99
MP L=9E-6 W=2000E-6 AD=30E-9 AS=30E-9
D4
21
18
DX
V4
99
21
DC 6
R10
10
11
6E3
C3
11
20
50E-12
.MODEL QNA NPN (IS=1.19E-16 BF=253 NF=0.99 VAF=193 IKF=2.76E-3
+ ISE=2.57E-13 NE=5 BR=0.4 NR=0.988 VAR=15 IKR=1.465E-4
+ ISC=6.9E-16 NC=0.99 RB=2.0E3 IRB=7.73E-6 RBM=132.8 RE=4
RC=209
+ CJE=2.1E-13 VJE=0.573 MJE=0.364 FC=0.5 CJC=1.64E-13 VJC=0.534
MJC=0.5
+ CJS=1.37E-12 VJS=0.59 MJS=0.5 TF=0.43E-9 PTF=30)
.MODEL QPA PNP (IS=5.21E-17 BF=131 NF=0.99 VAF=62 IKF=8.35E-4
+ ISE=1.09E-14 NE=2.61 BR=0.5 NR=0.984 VAR=15 IKR=3.96E-5
+ ISC=7.58E-16 NC=0.985 RB=1.52E3 IRB=1.67E-5 RBM=368.5 RE=6.31
RC=354.4
+ CJE=1.1E-13 VJE=0.745 MJE=0.33 FC=0.5 CJC=2.37E-13 VJC=0.762
MJC=0.4
+ CJS =7.11E-13 VJS=0.45 MJS=0.412 TF=1.0E-9 PTF=30)
.MODEL MN NMOS (LEVEL=3 VTO=1.3 RS=0.3 RD=0.3
+ TOX=8.5E-8 LD=1.48E-6 NSUB=1.53E16 UO=650 DELTA=10 VMAX=2E5
+ XJ=1.75E-6 KAPPA=0.8 ETA=0.066 THETA=0.01 TPG=1 CJ=2.9E-4
PB=0.837
+ MJ=0.407 CJSW=0.5E-9 MJSW=0.33)
.MODEL MP PMOS (LEVEL=3 VTO=1.1 RS=0.7 RD=0.7
+ TOX=9.5E-8 LD=1.4E-6 NSUB=2.4E15 UO=650 DELTA=5.6 VMAX=1E5
+ XJ=1.75E-6 KAPPA=1.7 ETA=0.71 THETA=5.9E-3 TPG=1 CJ=1.55E-4
PB=0.56
+ MJ=0.442 CJSW=0.4E-9 MJSW=0.33)
.MODEL DX D(IS=1E-15)
.MODEL DZ D (IS=1E-15, BV=7)
.MODEL QP PNP (BF=125)
.ENDS
REV. B
12
OP295/OP495
C1806a107/95
PRINTED IN U.S.A.
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm)
8 Lead Plastic DIP (P Suffix)
0.160 (4.06)
0.115 (2.93)
0.130
(3.30)
MIN
0.210
(5.33)
MAX
0.015
(0.381) TYP
0.430 (10.92)
0.348 (8.84)
0.280 (7.11)
0.240 (6.10)
4
5
8
1
0.070 (1.77)
0.045 (1.15)
0.022 (0.558)
0.014 (0.356)
0.325 (8.25)
0.300 (7.62)
0
- 15
0.100
(2.54)
BSC
0.015 (0.381)
0.008 (0.204)
SEATING
PLANE
0.195 (4.95)
0.115 (2.93)
14-Lead Plastic DIP (P Suffix)
PIN 1
0.280 (7.11)
0.240 (6.10)
7
8
14
1
0.210
(5.33)
MAX
0.160 (4.06)
0.115 (2.92)
0.795 (20.19)
0.725 (18.42)
0.022 (0.558)
0.014 (0.36)
0.100
(2.54)
BSC
0.070 (1.77)
0.045 (1.15)
SEATING
PLANE
0.130
(3.30)
MIN
0.015
(0.381)
MIN
0.325 (8.25)
0.300 (7.62)
0.015 (0.38)
0.008 (0.20)
15
0
8-Lead Narrow-Body SO (S Suffix)
0.0098 (0.25)
0.0075 (0.19)
0.0500 (1.27)
0.0160 (0.41)
8
0
0.0196 (0.50)
0.0099 (0.25)
x 45
PIN 1
0.1574 (4.00)
0.1497 (3.80)
0.2440 (6.20)
0.2284 (5.80)
4
5
1
8
0.0192 (0.49)
0.0138 (0.35)
0.0500
(1.27)
BSC
0.0688 (1.75)
0.0532 (1.35)
0.0098 (0.25)
0.0040 (0.10)
0.1968 (5.00)
0.1890 (4.80)
16-Lead Wide-Body SO (S Suffix)
PIN 1
0.2992 (7.60)
0.2914 (7.40)
0.4193 (10.65)
0.3937 (10.00)
1
16
9
8
0.0192 (0.49)
0.0138 (0.35)
0.0500 (1.27)
BSC
0.1043 (2.65)
0.0926 (2.35)
0.4133 (10.50)
0.3977 (10.10)
0.0118 (0.30)
0.0040 (0.10)
0.0125 (0.32)
0.0091 (0.23)
0.0500 (1.27)
0.0157 (0.40)
8
0
0.0291 (0.74)
0.0098 (0.25)
x 45