FEATURES
Excellent Speed: 8 V/s Typ
Low Noise: 11 nV/÷
Unity-Gain Stable
High Gain Bandwidth: 6.5 MHz Typ
Low Input Offset Voltage: 0.8 mV Max
Low Offset Voltage Drift: 4 V/C Max
High Gain: 500 V/mV Min
Outstanding CMR: 105 dB Min
Industry Standard Quad Pinouts
GENERAL DESCRIPTION
The OP471 is a monolithic quad op amp featuring low noise,
11 nV/÷Hz Max @ 1 kHz, excellent speed, 8 V/ms typical, a
gain bandwidth of 6.5 MHz, and unity-gain stability.
The OP471 has an input offset voltage under 0.8 mV and an
input offset voltage drift below 4 mV/∞C, guaranteed over the full
military temperature range. Open-loop gain of the OP471 is over
500,000 into a 10 kW load ensuring outstanding gain accuracy
and linearity. The input bias current is under 25 nA limiting
errors due to signal source resistance. The OP471’s CMR of
over 105 dB and PSRR of under 5.6 mV/V significantly reduce
errors caused by ground noise and power supply fluctuations.
The OP471 offers excellent amplifier matching which is important
for applications such as multiple gain blocks, low-noise instrumentation amplifiers, quad buffers and low-noise active filters.
The OP471 conforms to the industry standard 14-lead DIP
pinout. It is pin-compatible with the LM148/LM149, HA4741,
RM4156, MC33074, TL084 and TL074 quad op amps and can
be used to upgrade systems using these devices.
For applications requiring even lower voltage noise the OP470
with a voltage density of 5 nV/÷HzMax @ 1 kHz is recommended.
Hz @ 1 kHz Max
Operational Amplifier
PIN CONFIGURATIONS
14-Lead
Hermetic Dip
(Y-Suffix)
OUT AOUT D
–IN A–IN D
+IN A+IN D
+IN B+IN C
–IN B–IN C
OUT BOUT C
NCNC
OUT A
–IN A
+IN A
V+
+IN B
–IN B
OUT B
16-Lead SOIC
(S-Suffix)
1
2
3
4
V+V–
OP471
5
6
7
8
NC = NO CONNECT
16
15
14
13
12
11
10
9
V+
OP471
14-Lead
Plastic Dip
(P-Suffix)
1
2
3
4
OP471
5
6
7
14
13
12
11
10
9
8
OUT D
–IN D
+IN D
V–
+IN C
–IN C
OUT C
BIAS
IN
+IN
OUT
V–
Figure 1. Simplified Schematic
REV. A
Information furnished by Analog Devices is believed to be accurate and
reliable. However, no responsibility is assumed by Analog Devices for its
use, nor for any infringements of patents or other rights of third parties that
may result from its use. No license is granted by implication or otherwise
under any patent or patent rights of Analog Devices.
Absolute Maximum Ratings apply to packaged parts, unless otherwise noted.
2
The OP471’s inputs are protected by back-to-back diodes. Current limiting
resistors are not used in order to achieve low noise performance. If differential
voltage exceeds ± 1.0 V, the input current should be limited to ± 25 mA.
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 OP471 features proprietary ESD protection circuitry, permanent damage may occur on
devices subjected to high-energy electrostatic discharges. Therefore, proper ESD precautions
are recommended to avoid performance degradation or loss of functionality.
REV. A
–3–
Page 4
OP471
k
k
100
40
30
20
10
–Typical Performance Characteristics
10
T
TA = 25C
= 15V
V
S
= 25C
A
8
6
AT 10Hz
AT 1kHz
5mV
100
90
1s
5
4
3
I/F CORNER = 5Hz
VOLTA G E NOISE – nV/ Hz
2
1
1
101001
FREQUENCY – Hz
TPC 1. Voltage Noise Density
vs. Frequency
100
TA = 25C
= 15V
V
S
40
30
20
10
5
4
3
I/F CORNER = 5Hz
VOLTA G E NOISE – nV/ Hz
2
1
1
101001
FREQUENCY – Hz
TPC 4. Current Noise Density
vs. Frequency
4
VOLTA G E NOISE – nV/ Hz
2
0520
1015
SUPPLY VOLTAGE – V
TPC 2. Voltage Noise Density
vs. Supply Voltage
400
VS = 15V
300
200
100
INPUT OFFSET VOLTAGE – V
0
–75
–50 –25 025 50 75 100 125
TEMPERATURE – C
TPC 5. Input Offset Voltage vs.
Temperature
10
0%
NOISE VOLTAGE – 100nV/DIV
024 6810
TIME – Seconds
TA = 25C
= 15V
V
S
TPC 3. 0.1 Hz to 10 Hz Noise
20
TA = 25C
18
= 15V
V
S
16
14
12
10
8
6
4
CHANGE IN OFFSET VOLTAGE – V
2
0
12345
0
TIME – Minutes
TPC 6. Warm-Up Offset
Voltage Drift
20
15
10
5
INPUT BIAS CURRENT – nA
0
–75
–50 –25 025 50 75 100 125
TEMPERATURE – C
TPC 7. Input Bias Current vs.
Temperature
VS = 15V
= 0V
V
CM
10
VS = 15V
9
= 0V
V
CM
8
7
6
5
4
3
2
INPUT OFFSET CURRENT – nA
1
0
–50 –25 025 50 75 100 125
–75
TEMPERATURE – C
TPC 8. Input Offset Current vs.
Temperature
10
TA = 25C
= 15V
V
S
9
8
7
6
INPUT BIAS CURRENT – nA
5
–7.5–2.52.57.512.5
–12.5
COMMON-MODE VOLTAGE – V
TPC 9. Input Bias Current vs.
Common-Mode Voltage
–4–
REV. A
Page 5
OP471
0
130
120
110
100
90
80
70
60
CMR – dB
50
40
30
20
10
101001k10k 100k1M
1
FREQUENCY – Hz
TPC 10. CMR vs. Frequency
140
130
120
110
100
90
80
70
60
PSR – dB
50
40
30
20
10
0
10 100 1k 10k 100k 1M 10M 100M
1
+PSR
FREQUENCY – Hz
TPC 13. PSR vs. Frequency
–PSR
TA = 25C
= 15V
V
S
TA = 25C
= 15V
V
S
10
TA = +25C
8
6
4
TOTA L SUPPLY CURRENT – mA
2
052
TA = +125C
TA = –55C
1015
SUPPLY VOLTAGE – V
TPC 11. Total Supply Current
vs. Supply Voltage
140
130
120
110
100
90
80
70
60
50
40
OPEN-LOOP GAIN – dB
30
20
10
0
10 100 1k 10k 100k 1M 10M 100M
1
FREQUENCY – Hz
TA = 25C
= 15V
V
S
TPC 14. Open-Loop Gain vs. Frequency
10
VS = 15V
9
8
7
6
5
4
TOTA L SUPPLY CURRENT – mA
3
2
–50 –25 025 50 75 100 125
–75
TEMPERATURE – C
TPC 12. Total Supply Current
vs. Temperature
80
60
40
20
CLOSED-LOOP GAIN – dB
0
–20
1k
10k100k1M10M
FREQUENCY – Hz
TA = 25C
V
TPC 15. Closed-Loop Gain
vs. Frequency
= 15V
S
25
20
PHASE
15
10
GAIN
5
0
OPEN-LOOP GAIN – dB
–5
–10
1
2345
FREQUENCY – MHz
PHASE MARGIN
TPC 16. Open-Loop Gain,
Phase Shift vs. Frequency
TA = 25C
= 15V
V
S
= 57
67 89
80
100
120
140
160
180
200
220
10
2000
PHASE SHIFT – Degrees
1500
1000
OPEN-LOOP GAIN – V/mV
TA = 25C
= 10k
R
L
500
0
5101520
0
SUPPLY VOLTAGE – V
TPC 17. Open-Loop Gain vs.
Supply Voltage
80
GBW
70
60
VS = 15V
50
PHASE MARGIN – Degrees
40
–50 –25 0 25 50 75 100 125 150
–75
TEMPERATURE – C
TPC 18. Gain-Bandwidth Product,
Phase Margin vs. Temperature
8
6
4
2
GAIN-BANDWIDTH PRODUCT – MHz
0
REV. A
–5–
Page 6
OP471
28
24
20
16
12
8
PEAK-TO-PEAK AMPLITUDE – V
4
0
1k
10k100k1M10M
FREQUENCY – Hz
TA = 25C
= 15V
V
S
THD = 1%
TPC 19. Maximum Output Swing
vs. Frequency
9.0
8.5
8.0
7.5
7.0
SLEW RATE – V/s
6.5
6.0
–50 –25025 5075100125
–75
–SR
+SR
TEMPERATURE – C
TPC 22. Slew Rate vs. Temperature
20
TA = 25C
18
= 15V
V
S
16
14
12
10
8
6
MAXIMUM OUTPUT – V
4
2
0
100
POSITIVE
SWING
NEGATIVE
SWING
LOAD RESISTANCE –
1k10k
TPC 20. Maximum Output Voltage
vs. Load Resistance
170
160
150
140
130
120
110
100
90
80
CHANNEL SEPARATION – dB
70
60
50
10
1001k10k 100k1M10M
TA = 25C
= 15V
V
S
= 20V p-p TO 100kHz
V
O
FREQUENCY – Hz
TPC 23. Channel Separation vs.
Frequency
360
TA = 25C
= 15V
V
S
300
240
180
120
OUTPUT IMPEDANCE –
60
0
100
AV = 100
AV = 1
1k10k 100k 1M10M 100M
FREQUENCY – Hz
TPC 21. Closed-Loop Output
Impedance vs. Frequency
1
TA = 25C
= 15V
V
S
= 10V p-p
V
O
= 2k
R
L
0.1
0.01
AV = 10
TOTA L HARMONIC DISTORTION – %
0.001
10
1001k10k
FREQUENCY – Hz
AV = 1
TPC 24. Total Harmonic Distortion
vs. Frequency
TA = 25C
= 15V
V
100
90
10
0%
5V
A
5µs
S
= 1
V
TPC 25. Large-Signal Transient
Response
TA = 25C
= 15V
V
100
90
10
0%
50mV
S
A
V
0.2µs
= 1
TPC 26. Small-Signal Transient
Response
–6–
REV. A
Page 7
OP471
5k
500
1/4
OP471
50k
50
1/4
OP471
CHANNEL SEPARATION = 20 LOG
V
20V p-p
1
V
2
V
1
V2 / 1000
Figure 2. Channel Separation Test Circuit
+18V
+1V
–1V
2
4
1
A
3
11
–18V
9
C
10
+1V
8
–1V
6
5
13
12
7
B
14
D
Figure 3. Burn-In Circuit
APPLICATIONS INFORMATION
Voltage and Current Noise
The OP471 is a very low-noise quad op amp, exhibiting a typical
voltage noise of only 6.5
Hz @ 1 kHz. The low noise character-
istic of the OP471 is, in part, achieved by operating the input
transistors at high collector currents since the voltage noise is
inversely proportional to the square root of the collector current.
Current noise, however, is directly proportional to the square
root of the collector current. As a result, the outstanding voltage
noise performance of the OP471 is gained at the expense of current
noise performance which is typical for low noise amplifiers.
To obtain the best noise performance in a circuit, it is vital to
understand the relationship between voltage noise (e
noise (i
), and resistor noise (et).
n
), current
n
Total Noise and Source Resistance
The total noise of an op amp can be calculated by:
EeiRe
nnnSt
222
=
()+()
+
()
where:
E
= total input referred noise
n
e
= op amp voltage noise
n
= op amp current noise
i
n
e
= source resistance thermal noise
t
R
= source resistance
S
The total noise is referred to the input and at the output would
be amplified by the circuit gain.
100
OP11
OP400
10
OP471
TOTAL NOISE – nV/ Hz
OP470
RESISTOR
NOISE ONLY
1
100100k
RS – SOURCE RESISTANCE –
10k1k
Figure 4. Total Noise vs. Source Resistance (Including
Resistor Noise) at 1 kHz
100
OP11
OP400
10
OP471
TOTAL NOISE – nV/ Hz
OP470
RESISTOR
NOISE ONLY
1
100100k
RS – SOURCE RESISTANCE –
10k1k
Figure 5. Total Noise vs. Source Resistance (Including
Resistor Noise) at 10 Hz
Figure 4 shows the relationship between total noise at 1 kHz
and source resistance. For R
nated by the voltage noise of the OP471. As R
< 1 kW the total noise is domi-
S
rises above 1 kW,
S
total noise increases and is dominated by resistor noise rather
than by voltage or current noise of the OP471. When R
exceeds
S
20 kW, current noise of the OP471 becomes the major contributor
to total noise.
Figure 5 also shows the relationship between total noise and source
resistance, but at 10 Hz. Total noise increases more quickly
than shown in Figure 4 because current noise is inversely proportional to the square root of frequency. In Figure 5, current
noise of the OP471 dominates the total noise when R
> 5 kW.
S
From Figures 4 and 5, it can be seen that to reduce total noise,
source resistance must be kept to a minimum. In applications
with a high source resistance, the OP400, with lower current
noise than the OP471, will provide lower total noise.
REV. A
–7–
Page 8
OP471
1000
OP11
OP400
OP471
100
OP470
RESISTOR
PEAK-TO-PEAK NOISE – nV
10
100100k
NOISE ONLY
RS – SOURCE RESISTANCE –
10k1k
Figure 6. Peak-to-Peak Noise (0.1 Hz to 10 Hz) vs. Source
Resistance (Includes Resistor Noise)
Figure 6 shows peak-to-peak noise versus source resistance over
the 0.1 Hz to 10 Hz range. Once again, at low values of R
, the
S
voltage noise of the OP471 is the major contributor to peak-to-peak
noise. Current noise becomes the major contributor as R
increases.
S
The crossover point between the OP471 and the OP400 for
peak-to-peak noise is at R
= 17 W.
S
The OP470 is a lower noise version of the OP471, with a typical
noise voltage density of 3.2 nV/÷Hz@ 1 kHz. The OP470 offers
lower offset voltage and higher gain than the OP471, but is a slower
speed device, with a slew rate of 2 V/ms compared to a slew rate
of 8 V/ms for the OP471.
For reference, typical source resistances of some signal sources
are listed in Table I.
TABLE I.
Source
DeviceImpedanceComments
Strain gauge< 500 WTypically used in
low-frequency applications.
Magnetic< 1,500 WLow I
very important to reduce
B
tapeheadself-magnetization problems
when direct coupling is used.
OP471 IB can be neglected.
Magnetic< 1,500 WSimilar need for low I
in direct
B
phonographcoupled applications. OP471
cartridgeswill not introduce any
self -magnetization problem.
Linear variable < 1,500 WUsed in rugged servo-feedback
differentialapplications. Bandwidth of
transformerinterest is 400 Hz to 5 kHz.
*For further information regarding noise calculations, see “Minimization of
Noise in Op Amp Applications,” Application Note AN-15.
5
R2
5
R3
1.24k
R1
OP471
DUT
200
OP27E
909
R4
C1
2F
R11
C4
0.22F
C3
0.22F
R12
10k
OP15E
R13
5.9k
GAIN = 50,000
V
S
= 15V
R14
4.99k
C5
1F
e
OUT
R5
R6
600k
D1
1N4148D21N4148
R8
10k
OP15E
306k
0.032F
R10
65.4k
R9
C2
65.4k
Figure 7. Peak-to-Peak Voltage Noise Test Circuit (0.1 Hz to 10 Hz)
–8–
REV. A
Page 9
Noise Measurements - Peak-to-Peak Voltage Noise
FREQUENCY – Hz
100
0.01
GAIN – dB
80
60
40
20
0
0.1110100
The circuit of Figure 7 is a test setup for measuring peak-to-peak
voltage noise. To measure the 500 nV peak-to-peak noise specification of the OP471 in the 0.1 Hz to 10 Hz range, the following
precautions must be observed:
1. The device must be warmed up for at least five minutes. As
shown in the warm-up drift curve, the offset voltage typically
changes 13 mV due to increasing chip temperature after
power-up. In the 10-second measurement interval, these
temperature-induced effects can exceed tens-of-nanovolts.
2. For similar reasons, the device must be well-shielded from
air currents. Shielding also minimizes thermocouple effects.
3.
Sudden motion in the vicinity of the device can also “feedthrough”
to increase the observed noise.
4. The test time to measure 0.1 Hz to 10 Hz noise should not exceed
10 seconds. As shown in the noise-tester frequency-response curve
of Figure 8, the 0.1 Hz corner is defined by only one pole. The
test time of 10 seconds acts as an additional pole to eliminate
noise contribution from the frequency band below 0.1 Hz.
5. A noise voltage density test is recommended when measuring
noise on a large number of units. A 10 Hz noise voltage density
measurement will correlate well with a 0.1 Hz to 10 Hz
peak-to-peak noise reading, since both results are determined
by the white noise and the location of the 1/f corner frequency.
6. Power should be supplied to the test circuit by well bypassed,
low noise supplies, e.g, batteries. These will minimize output
noise introduced through the amplifier supply pins.
OP471
Figure 8. 0.1 Hz to 10 Hz Peak-to-Peak Voltage Noise
Test Circuit Frequency Response
Noise Measurement - Noise Voltage Density
The circuit of Figure 9 shows a quick and reliable method of
measuring the noise voltage density of quad op amps. Each
individual amplifier is series connected and is in unity-gain, save
the final amplifier which is in a noninverting gain of 101. Since
the ac noise voltages of each amplifier are uncorrelated, they
add in rms fashion to yield:
Ê
e=101 e+ eee
OUTnAnBnCnD
222 2
Ë
++
The OP471 is a monolithic device with four identical amplifiers.
The noise voltage density of each individual amplifier will
match, giving:
ˆ
¯
1/4
OP471
e101 4e = 101 2e
OUTnn
R2
10k
1/4
OP471
(nV Hz) = 101(2en)
= 15V
TO SPECTRUM ANALYZER
1/4
OP471
1/4
OP471
R1
100
e
V
OUT
S
Figure 9. Noise Voltage Density Test Circuit
Ê
=
Ë
e
OUT
ˆ
2
¯
()
REV. A
–9–
Page 10
OP471
Noise Measurement - Current Noise Density
The test circuit shown in Figure 10 can be used to measure current
noise density. The formula relating the voltage output to current
noise density is:
nOUT
G
2
ˆ
40nV / Hz
-
˜
()
¯
R
S
e
Ê
Á
Ë
i
=
n
2
where:
G = gain of 10,000
R
= 100 kW source resistance
S
Capacative Load Driving and Power Supply Considerations
The OP471 is unity-gain stable and is capable of driving large
capacitive loads without oscillating. Nonetheless, good supply
bypassing is highly recommended. Proper supply bypassing
reduces problems caused by supply line noise and improves the
capacitive load driving capability of the OP471.
R3
1.24k
R2
R1
100k
5
OP471
DUT
200
OP27E
R5
8.06k
R4
en OUT TO
SPECTRUM ANALYZER
GAIN = 10,000
V
= 15V
S
Figure 10. Current Noise Density Test Circuit
V
IN
R1
100*
*SEE TEXT
V+
OP471
*
V–
C2
10F
+
C3
0.1F
R2
C1
200pF
0.1F
R3
50
C4
10F
+
C5
PLACE SUPPLY DECOUPLING
CAPACITORS AT OP471
V
OUT
C
L
1000pF
Figure 11. Driving Large Capacitive Loads
In the standard feedback amplifier, the op amp’s output resistance
combines with the load capacitance to form a lowpass filter that
adds phase shift in the feedback network and reduces stability. A
simple circuit to eliminate this effect is shown in Figure 11. The
added components, C1 and R3, decouple the amplifier from the
load capacitance and provide additional stability. The values of
C1 and R3 shown in Figure 11 are for load capacitances of up
to 1,000 pF when used with the OP471.
In applications where the OP471’s inverting or noninverting inputs
are driven by a low source impedance (under 100 W) or connected
to ground, if V+ is applied before V–, or when V– is disconnected,
excessive parasitic currents will flow.
Most applications use dual tracking supplies and with the device
supply pins properly bypassed, power-up will not present a
problem. A source resistance of at least 100 W in series with all
inputs (Figure 11) will limit the parasitic currents to a safe level
if V– is disconnected. It should be noted that any source resistance,
even 100 W, adds noise to the circuit. Where noise is required to
be kept at a minimum, a germanium or Schottky diode can be
used to clamp the V– pin and eliminate the parasitic current
flow instead of using series limiting resistors. For most applications, only one diode clamp is required per board or system.
R
f
OP471
8V/s
Figure 12. Pulsed Operation
Unity-Gain Buffer Applications
When Rf £ 100 W and the input is driven with a fast, large signal
pulse (>1 V), the output waveform will look as shown in Figure 12.
During the fast feedthrough-like portion of the output, the input
protection diodes effectively short the output to the input, and a
current, limited only by the output short-circuit protection, will
be drawn by the signal generator. With R
is capable of handling the current requirements (I
≥ 500 W , the output
f
£ 20 mA at
L
10 V); the amplifier will stay in its active mode and a smooth
transition will occur.
When R
> 3 kW, a pole created by Rf and the amplifier’s input
f
capacitance (2.6 pF) creates additional phase shift and reduces
phase margin. A small capacitor (20 pF to 50 pF) in parallel with
helps eliminate this problem.
R
f
APPLICATIONS
Low Noise Amplifier
A simple method of reducing amplifier noise by paralleling
amplifiers is shown in Figure 13. Amplifier noise, depicted in
Figure 14, is around 5 nV/÷Hz@ 1 kHz (R.T.I.). Gain for each
paralleled amplifier and the entire circuit is 100. The 200 W
resistors limit circulating currents and provide an effective output
resistance of 50 W. The amplifier is stable with a 10 nF capacitive
load and can supply up to 30 mA of output drive.
–10–
REV. A
Page 11
High-Speed Differential Line Driver
The circuit of Figure 15 is a unique line driver widely used in
professional audio applications. With ± 18 V supplies, the line
driver can deliver a differential signal of 30 V p-p
into a 1.5 kW
load. The output of the differential line driver looks exactly like
a transformer. Either output can be shorted to ground without
changing the circuit gain of 5, so the amplifier can easily be set
for inverting, noninverting, or differential operation. The line
driver can drive unbalanced loads, like a true transformer.
+15V
V
IN
R1
50
R4
50
R7
50
R10
50
1/4
OP471E
–15V
1/4
OP471E
1/4
OP471E
1/4
OP471E
R2
5k
R5
5k
R8
5k
R11
5k
R3
200
R6
200
R9
200
R12
200
V
= 100V
OUT
IN
OP471
100
90
REFERRED TO INPUT
10
0%
NOISE DENSITY – 0.58nV/ Hz/DIV
Figure 14. Noise Density of Low-Noise Amplifier, G = 100
R4
10k
R11
R8
10k
R5
10k
50
R10
50
R14
1k
R13
10k
R12
1k
–OUT
+OUT
1/4
OP471
R2
2k
R3
2k
R7
2k
R6
2k
R9
10k
1/4
OP471
IN
R1
1/4
10k
OP471
Figure 13. Low-Noise Amplifier
High-Output Amplifier
The amplifier shown in Figure 16 is capable of driving 20 V p-p
into a floating 400 W load. Design of the amplifier is based on a
bridge configuration. A1 amplifies the input signal and drives
the load with the help of A2. Amplifier A3 is a unity-gain inverter
which drives the load with help from A4. Gain of the high output
amplifier with the component values shown is 10, but can
easily be changed by varying R1 or R2.
+15V
C1
10F
+
C2
0.1F
R1
1k
1/4
OP471E
V
IN
C3
0.1F
C4
10F
+
A1
–15V
R2
9k
1/4
OP471E
A2
R3
50
R4
50
Figure 15. High-Speed Differential Line Driver
R5
5k
R6
5k
R7
50
R8
R
50
L
1/4
OP471E
A4
1/4
OP471E
A3
REV. A
Figure 16. High-Output Amplifier
–11–
Page 12
OP471
Quad Programmable Gain Amplifier
The combination of the quad OP471 and the DAC8408, a quad
8-bit CMOS DAC, creates a space-saving quad programmable gain
amplifier. The digital code present at the DAC, which is easily
set by a microprocessor, determines the ratio between the fixed
DAC feedback resistor and the impedance the DAC ladder presents
to the op amp feedback loop. Gain of each amplifier is:
V
OUT
V
IN
= –
VINA
VINB
256
n
DAC-8408ET
RFBA
RFBB
V
DD
DAC A
DAC B
where n equals the decimal equivalent of the 8-bit digital code
present at the DAC. If the digital code present at the DAC
consists of all zeros, the feedback loop will be open causing the
op amp output to saturate. The 20 MW resistors placed in parallel
with the DAC feedback loop eliminates this problem with a very
small reduction in gain accuracy.
V
A
REF
+15V
1/4
OP470E
–15V
1/4
OP470E
V
A
OUT
B
V
OUT
I
OUT1A
I
OUT2A/2B
V
REF
I
OUT1B
R1
20M
B
R2
20M
VINC
VIND
DAC DATA BUS
PINS 9 (LSB) – 16 (MSB)
RFBC
DAC C
RFBD
DAC D
DGND
V
REF
I
OUT1C
I
OUT2C/2D
V
REF
I
OUT1D
C
R3
20M
1/4
OP470E
D
R4
20M
1/4
OP470E
Figure 17. Quad Programmable Gain Amplifier
V
C
OUT
V
D
OUT
–12–
REV. A
Page 13
OP471
Low Phase Error Amplifier
The simple amplifier depicted in Figure 18 utilizes monolithic
matched operational amplifiers and a few resistors to substantially reduce phase error compared to conventional amplifier
designs. At a given gain, the frequency range for a specified phase
accuracy is over a decade greater than for a standard single op
amp amplifier.
The low phase error amplifier performs second-order frequency
compensation through the response of op amp A2 in the feedback loop of A1. Both op amps must be extremely well matched
in frequency response. At low frequencies, the A1 feedback loop
forces V2/(K1 + 1) = VIN. The A2 feedback loop forces Vo/(K1 +1)
= V
/(K1 + 1) yielding an overall transfer function of VO/VIN =
2
K1 + 1. The dc gain is determined by the resistor divider at
the output, V
, and is not directly affected by the resistor divider
O
around A2. Note that similar to a conventional single op amp
amplifier, the dc gain is set by resistor ratios only. Minimum
gain for the low phase error amplifier is 10.
Figure 19 compares the phase error performance of the low
phase error amplifier with a conventional single op amp amplifier
and a cascaded two-stage amplifier. The low phase error amplifier
shows a much lower phase error, particularly for frequencies where
/
< 0.1. For example, phase error of –0.1∞ occurs at 0.002 /
T
T
for the single op amp amplifier, but at 0.11 /T for the low
phase error amplifier.
For more detailed information on the low phase error amplifier,
see Application Note AN-107.