FEATURES
Very Low Noise 5 nV/
Excellent Input Offset Voltage 75 V Max
Low Offset Voltage Drift 1 V/ⴗC Max
Very High Gain 1500 V/mV Min
Outstanding CMR 106 dB Min
Slew Rate 2.4 V/s Typ
Gain Bandwidth Product 5 MHz Typ
Industry-Standard 8-Lead Dual Pinout
GENERAL DESCRIPTION
The OP270 is a high performance, monolithic, dual operational
amplifier with exceptionally low voltage noise, 5 nV/÷Hz max at
1 kHz. It offers comparable performance to ADI’s industry
standard OP27.
The OP270 features an input offset voltage below 75 mV and an
offset drift under 1 mV/∞C, guaranteed over the full military tem-
perature range. Open-loop gain of the OP270 is over 1,500,000
into a 10 kW load, ensuring excellent gain accuracy and linearity,
even in high gain applications. Input bias current is under 20 nA,
which reduces errors due to signal source resistance. The OP270’s
CMR of over 106 dB and PSRR of less than 3.2 mV/V signifi-
cantly reduce errors due to ground noise and power supply
fluctuations. Power consumption of the dual OP270 is one-third
less than two OP27s, a significant advantage for power conscious
applications. The OP270 is unity-gain stable with a gain bandwidth
product of 5 MHz and a slew rate of 2.4 V/ms.
÷÷
÷Hz @ 1 kHz Max
÷÷
Operational Amplifier
OP270
CONNECTION DIAGRAMS
16-Lead SOIC
(S-Suffix)
1
–IN A
2
+IN A
3
NC
4
V–
5
NC
+IN B
6
–IN B
7
NC
8
NC = NO CONNECT
OP270
16
15
14
13
12
11
10
9
OUT A
NC
NC
V+
NC
NC
OUT B
NC
The OP270 offers excellent amplifier matching, which is important
for applications such as multiple gain blocks, low noise instrumentation amplifiers, dual buffers, and low noise active filters.
The OP270 conforms to the industry-standard 8-lead DIP pinout.
It is pin compatible with the MC1458, SE5532/A, RM4558, and
HA5102 dual op amps, and can be used to upgrade systems
using those devices.
For higher speed applications, the OP271, with a slew rate of
8V/ms, is recommended. For a quad op amp, see the OP470.
8-Lead PDIP (P-Suffix)
8-Lead CERDIP
(Z-Suffix)
OUT A
–IN A
+IN A
1
2
A
3
4
V–
OP270
8
V+
7
OUT B
B
6
–IN B
5
+IN B
SIMPLIFIED SCHEMATIC
(One of Two Amplifiers Is Shown)
–IN
+IN
REV. C
Information furnished by Analog Devices is believed to be accurate and
reliable. However, no responsibility is assumed by Analog Devices for its
use, nor for any infringements of patents or other rights of third parties that
may result from its use. 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 companies.
Stresses above those listed under Absolute Maximum Ratings may cause permanent damage to the device. This is a stress rating only; functional operation of the
device at these or any other conditions above those listed in the operational
sections of this specification is not implied. Exposure to absolute maximum rating
conditions for extended periods may affect device reliability.
2
The OP270’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 +10 V, the input current should be limited to ±25 mA.
*θJA is specified for worst-case mounting conditions, i.e., θJA is specified for device
in socket for CERDIP and PDIP packages; θJA is specified for device soldered to
printed circuit board for SOIC package.
For military processed devices, please refer to the Standard
Microcircuit Drawing (SMD) available at
www.dscc.dla.mil/programs/milspec/default.asp.
SMD Part NumberADI Equivalent
5962-8872101PAOP270AZMDA
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 OP270 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.
WARNING!
ESD SENSITIVE DEVICE
–4–
REV. C
Page 5
COMMON-MODE VOLTAGE (V)
INPUT BIAS CURRENT (nA)
7
–12.5
2
4
3
6
TA = 25ⴗC
V
S
= ⴞ15V
5
–10.0
–7.5
–5.0
–2.5
0.0
2.5
5.0
7.5
10.0
12.5
Typical Performance Characteristics–
OP270
10
TA = 25ⴗC
9
VS = ⴞ15V
8
7
6
5
4
3
1/f CORNER = 5Hz
101001k
FREQUENCY (Hz)
VOLTA G E NOISE (nV/ Hz)
2
1
1
TPC 1. Voltage Noise Density
vs. Frequency
10
TA = 25ⴗC
= ⴞ15V
V
S
1.0
CURRENT NOISE (pA/ Hz)
0.1
1010010k
1/f CORNER = 200Hz
1k
FREQUENCY (Hz)
TPC 4. Current Noise Density
vs. Frequency
5
T
= 25ⴗC
A
4
AT 10Hz
3
2
VOLTA G E NOISE (nV/ Hz)
1
0ⴞ5ⴞ15ⴞ20
SUPPLY VOLTAGE (V)
AT 1kHz
ⴞ10
TPC 2. Voltage Noise Density
vs. Supply Voltage
40
VS = ⴞ15V
30
20
10
0
–10
VOLTA G E NOISE (nV/ Hz)
–20
–30
–50 –25 025 50 75 100 125
–75
TEMPERATURE (ⴗC)
TPC 5. Input Offset Voltage vs.
Temperature
0.1Hz TO 10Hz NOISE
NOISE VOLTAGE (100nV/DIV)
TA = 25ⴗC
= ⴞ15V
V
S
TIME (1sec/DIV)
TPC 3. 0.1 Hz to 10 Hz Input
Voltage Noise
5
TA = 25ⴗC
= ⴞ15V
V
S
4
3
2
1
CHANGE IN OFFSET VOLTAGE (A)
0
12345
0
TIME (Minutes)
TPC 6. Warm-Up Offset Voltage
Drift
7
6
5
4
INPUT BIAS CURRENT (nA)
3
2
–75
TPC 7. Input Bias Current vs.
Temperature
REV. C
VS = ⴞ15V
= 0V
V
CM
–50050100 125
–252575
TEMPERATURE (ⴗC)
5
VS = ⴞ15V
= 0V
V
CM
4
3
2
1
INPUT OFFSET CURRENT (nA)
0
–75
–50050100 125
–252575
TEMPERATURE (ⴗC)
TPC 8. Input Offset Current vs.
Temperature
–5–
TPC 9. Input Bias Current vs.
Common-Mode Voltage
Page 6
OP270
TEMPERATURE (ⴗC)
TOTA L SUPPLY CURRENT (mA)
8
0
2
–75–252575125
6
4
VS = ⴞ15V
–50050100
7
1
5
3
130
120
110
100
90
80
70
60
CMR (dB)
50
40
30
20
10
1101001k10k 100k 1M
FREQUENCY (Hz)
TA = 25ⴗC
V
TPC 10. CMR vs. Frequency
140
120
100
80
60
PSR (dB)
40
20
–PSR
+PSR
= ⴞ15V
S
TA = 25ⴗC
6
5
4
+125ⴗC
+25ⴗC
–55ⴗC
3
TOTA L SUPPLY CURRENT (mA)
2
0ⴞ5ⴞ10ⴞ15ⴞ20
SUPPLY VOLTAGE (V)
TPC 11. Total Supply Current
vs. Supply Voltage
140
120
100
80
60
VOLTA GE GAIN (dB)
40
20
TA = 25ⴗC
V
= ⴞ15V
S
TPC 12. Total Supply Current
vs. Temperature
80
60
40
20
CLOSED-LOOP GAIN (dB)
0
TA = 25ⴗC
V
S
= ⴞ15V
0
110010k1M100M
101k100k10M
FREQUENCY (Hz)
TPC 13. PSR vs. Frequency
25
20
15
10
5
GAIN (dB)
0
–5
–10
1
TPC 16. Open-Loop Gain Phase
Shift vs. Frequency
PHASE
GAIN
2345678910
FREQUENCY (Hz)
TA = 25ⴗC
= ⴞ15V
V
S
PHASE
MARGIN = 62ⴗ
80
100
120
140
160
180
5000
4000
3000
2000
PHASE SHIFT (Degrees)
OPEN-LOOP GAIN (V/mV)
1000
TPC 17. Open-Loop Gain vs.
Supply Voltage
0
110010k1M100M
101k100k10M
FREQUENCY (Hz)
TPC 14. Open-Loop Gain vs.
Frequency
0
0
ⴞ5ⴞ10ⴞ15ⴞ20ⴞ25
SUPPLY VOLTAGE (V)
–6–
–20
1k10k
100k10M
FREQUENCY (Hz)
1M
TPC 15. Closed-Loop Gain vs.
Frequency
80
70
60
50
PHASE MARGIN (Degrees)
40
–75
⌽
GBP
–50 –25 0 25 50 75 100 125 150
TEMPERATURE (ⴗC)
TPC 18. Gain-Bandwidth Phase
Margin vs. Temperature
REV. C
8
7
6
5
GAIN BANDWIDTH PRODUCT (MHz)
4
Page 7
OP270
28
24
20
16
12
8
PEAK-TO-PEAK AMPLITUDE (V)
4
0
1k
10k100k1M10M
FREQUENCY (Hz)
TA = 25ⴗC
VS = ⴞ15V
THD = 1%
TPC 19. Maximum Output
Swing vs. Frequency
100
TA = +25ⴗC
= ⴞ15V
V
S
75
50
AV = 100
25
OUTPUT IMPEDANCE (⍀)
0
1k100k10M
10k1M
FREQUENCY (Hz)
AV = 1
AV = 10
TPC 22. Output Impedance vs.
Frequency
15
TA = 25ⴗC
VS = ⴞ15V
14
13
12
11
10
9
8
MAXIMUM OUTPUT ( V)
7
6
5
1k10k100k
POSITIVE
SWING
NEGATIVE
SWING
LOAD RESISTANCE (⍀)
TPC 20. Maximum Output
Voltage vs. Load Resistance
2.8
VS = ⴞ15V
2.7
2.6
2.5
2.4
SLEW RATE (V/s)
2.3
2.2
–7525125
–2575
TEMPERATURE (ⴗC)
–SR
+SR
0100–5050
TPC 23. Slew Rate vs.
Temperature
50
TA = 25ⴗC
= ⴞ15V
V
S
VIN = 100mV
AV = +1
40
30
20
OVERSHOOT (%)
10
0
200600800
04001000
CAPACITIVE LOAD (pF)
TPC 21. Small-Signal Overshoot
vs. Capacitive Load
190
180
170
160
150
140
130
120
110
100
CHANNEL SEPARATION (dB)
90
TA = 25ⴗC
V
= ⴞ15V
80
S
VO = 20V p-p TO 10kHz
70
11k1M
100100k10
FREQUENCY (Hz)
10k
TPC 24. Channel Separation vs.
Frequency
0.1
TA = 25ⴗC
VS = ⴞ15V
VO = 20V p-p
R
=2k⍀
L
A
V
0.01
DISTORTION (%)
0.001
1010k
100
FREQUENCY (Hz)
AV = 1
1k
TPC 25. Total Harmonic Distortion vs. Frequency
REV. C
= 10
20s
TA = 25ⴗC
VS = ⴞ15V
AV = +1
RL = 2k⍀
5V
TPC 26. Large Signal Transcient
Response
–7–
50mV200nS
TA = 25ⴗC
VS = ⴞ15V
AV = +1
RL = 2k⍀
TPC 27. Small-Signal
Transient Response
Page 8
OP270
5k⍀
500⍀
50⍀
1/2
OP270
5k⍀
1/2
OP270
CHANNEL SEPARATION = 20 log
20V
V
1
p-p
V
2
Figure 1. Channel Separation Test Circuit
+18V
8
100k⍀
200k⍀
100k⍀
2
1/2
OP270
3
6
1/2
OP270
5
4
1
7
V
1
V2/1000
TOTAL NOISE AND SOURCE RESISTANCE
The total noise of an op amp can be calculated by:
EeiR e
nnnS t
222
=
()+()
+
()
where:
E
= total input referred noise
n
e
= op amp voltage noise
n
i
= op amp current noise
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.
Figure 3 shows the relationship between total noise at 1 kHz
and source resistance. For R
by the voltage noise of the OP270. As R
< 1 kW the total noise is dominated
S
rises above 1 kW, total
S
noise increases and is dominated by resistor noise rather than by
the voltage or current noise of the OP270. When R
exceeds
S
20 kW, current noise of the OP270 becomes the major contributor
to total noise.
100
OP200
10
–18V
Figure 2. Burn-In Circuit
APPLICATIONS INFORMATION
VOLTAGE AND CURRENT NOISE
The OP270 is a very low noise dual op amp, exhibiting atypical
voltage noise of only 3.2 nV/
÷÷
÷Hz @ 1 kHz. The exceptionally
÷÷
low noise characteristic of the OP270 is achieved in part 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 OP270 is gained
at the expense of current noise performance, which is normal 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 (nV/ Hz)
OP270
RESISTOR
NOISE ONLY
1
1001k10k100k
RS – SOURCE RESISTANCE (⍀)
Figure 3. Total Noise vs. Source Resistance
(Including Resistor Noise) at 1 kHz
Figure 4 also shows the relationship between total noise and
source resistance, but at 10 Hz. Total noise increases more
quickly than shown in Figure 3 because current noise is inversely
proportional to the square root of frequency. In Figure 4, current
noise of the OP270 dominates the total noise when R
> 5 kW.
S
Figures 3 and 4 show that to reduce total noise, source resistance
must be kept to a minimum. In applications with a high source
resistance, the OP200, with lower current noise than the OP270,
will provide lower total noise.
–8–
REV. C
Page 9
OP270
100
10
OP200
OP270
TOTAL NOISE (nV/ Hz)
RESISTOR
NOISE ONLY
1
1001k10k100k
RS – SOURCE RESISTANCE (⍀)
Figure 4. Total Noise vs. Source Resistance
(Including Resistor Noise) at 10 Hz
1000
OP200
100
OP270
PEAK-TO-PEAK NOISE (nV)
RESISTOR
NOISE ONLY
Figure 5 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 voltage
S
noise of the OP270 is the major contributor to peak-to-peak
noise, with current noise the major contributor as R
increases.
S
The crossover point between the OP270 and the OP200 for
peak-to-peak noise is at R
=17kW.
S
The OP271 is a higher speed version of the OP270, with a slew
rate of 8 V/ms. Noise of the OP271 is slightly higher than that of
the OP270. Like the OP270, the OP271 is unity-gain stable.
For reference, typical source resistances of some signal sources
are listed in Table I.
Table I.
Source
DeviceImpedanceComments
Strain gage<500 WTypically used in low
frequency applications.
Magnetic<1500 WLow I
very important to reduce
B
tapehead,self-magnetization problems
microphonewhen direct coupling is used.
OP270 IB can be neglected.
Magnetic<1500 WSimilar need for low I
in
B
phonographdirect coupled applications.
cartridgeOP270 will not introduce any
self-magnetization problem.
Linear variable <1500 WUsed in rugged servo-feedback
differentialapplications. Bandwidth of
transformerinterest is 400 Hz to 5 kHz.
10
1001k10k100k
RS – SOURCE RESISTANCE (⍀)
Figure 5. Peak-to-Peak Noise (0.1 Hz to 10 Hz) vs.
Source Resistance (Includes Resistor Noise)
R3
1.24k⍀
R1
5⍀
R2
5⍀
–
OP270
DUT
+
+
OP27E
–
R4
200⍀
R5
909⍀
C1
2F
R6
600⍀
D1, D2
1N4148
R8
10k⍀
Figure 6. Peak-to-Peak Voltage Noise Test Circuit (0.1 Hz to 10 Hz)
+
OP27E
–
0.032F
R9
306k⍀
C2
R10
65.4k⍀
R11
65.4k⍀
C4
0.22F
C3
0.22F
+
OP42E
–
R12
10k⍀
R13
5.9k⍀
R14
4.99k⍀
GAIN = 50,000
= ⴞ15V
V
S
C5
1F
e
OUT
REV. C
–9–
Page 10
OP270
eee
OUTnA
2
nB
2
=
()+()
Ê
Ë
Á
ˆ
¯
˜
101
NOISE MEASUREMENTS
Peak-to-Peak Voltage Noise
The circuit of Figure 6 is a test setup for measuring peak-to-peak
voltage noise. To measure the 200 nV peak-to-peak noise specification of the OP270 in the 0.1 Hz to 10 Hz range, the following
precautions must be observed:
1. The device has to be warmed up for at least five minutes. As
shown in the warm-up drift curve, the offset voltage typically
changes 2 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 has to be well shielded from
air currents. Shielding also minimizes thermocouple effects.
3. Sudden motion in the vicinity of the device can also “feed
through” to increase the observed noise.
4. The test time to measure noise of 0.1 Hz to 10 Hz should not
exceed 10 seconds. As shown in the noise-tester frequency
response curve of Figure 7, 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.
100
80
60
GAIN (dB)
40
20
0
0.010.11.010100
FREQUENCY (Hz)
Figure 7. 0.1 Hz to 10 Hz Peak-to-Peak Voltage
Noise Test Circuit Frequency Response
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. They will minimize output
noise introduced via the amplifier supply pins.
Noise Measurement — Noise Voltage Density
The circuit of Figure 8 shows a quick and reliable method of
measuring the noise voltage density of dual op amps. The first
amplifier is in unity-gain, with the final amplifier in a noninverting
gain of 101. As noise voltages of each amplifier are uncorrelated,
they add in rms fashion to yield:
The OP270 is a monolithic device with two identical amplifiers. The noise voltage density of each individual amplifier will
match, giving:
2
Ê
ˆ
eee
=
1012101 2
OUTn
R1
100⍀
–
1/2
OP270
+
Á
Ë
e
(nV/ Hz) = 101 ( 2
OUT
V
= 15V
S
=
˜
()
¯
R2
10k⍀
–
1/2
OP270
+
TO SPECTRUM ANALYZER
苲
苲
e
e
)
n
n
OUT
Figure 8. Noise Voltage Density Test Circuit
R3
1.24k⍀
R2
R1
100k⍀
5⍀
–
OP270
DUT
+
200⍀
–
OP27E
+
R4
R5
8.06k⍀
e
nOUT
TO SPECTRUM ANALYZER
GAIN = 10,000
VS = ⴞ15V
Figure 9. Current Noise Density Test Circuit
Noise Measurement — Current Noise Density
The test circuit shown in Figure 9 can be used to measure current noise density. The formula relating the voltage output to
current noise density is:
2
ˆ
Ê
e
nOUT
Á
Ë
i
=
n
-
nVHz
40/
˜
G
()
¯
R
S
2
where:
G = gain of 10,000
= 100 kW source resistance
R
S
–10–
REV. C
Page 11
OP270
CAPACITIVE LOAD DRIVING AND POWER SUPPLY
CONSIDERATIONS
The OP270 is unity-gain stable and 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 OP270.
In the standard feedback amplifier, the op amp’s output resistance combines with the load capacitance to form a low-pass
filter that adds phase shift in the feedback network and reduces
stability. A simple circuit to eliminate this effect is shown in
Figure 10. 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 10 are for a
load capacitance of up to 1,000 pF when used with the OP270.
V+
+
C3
0.1FC210F
R2
V–
C1
200pF
C5
0.1FC410F
R3
50⍀
+
PLACE SUPPLY DECOUPLING
CAPACITOR AT OP270
V
OUT
C1
1000pF
R1
V
IN
–
OP270
+
Figure 10. Driving Large Capacitive Loads
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 like the one
in Figure 11.
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
capable of handling the current requirements (I
≥ 500 W, the output is
f
£ 20 mA at 10 V);
L
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 (3 pF) creates additional phase shift and reduces
phase margin. A small capacitor (20 pF to 50 pF) in parallel
with R
helps eliminate this problem.
f
APPLICATIONS
Low Phase Error Amplifier
The simple amplifier depicted in Figure 12 utilizes a monolithic
dual operational amplifier 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 V
Vo/(K1 + 1) = V
of V
O/VIN
/(K1 + 1) = VIN. The A2 feedback loop forces
2
/(K1 + 1), yielding an overall transfer function
2
= K1 + 1. The dc gain is determined by the resistor
divider at the output, VO, and is not directly affected by the resistor divider around A2. Note that like 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.
R2
K1
–
1/2
OP270E
A2
+
–
1/2
OP270E
A1
V
IN
ASSUME A1 AND A1 ARE MATCHED.
+
T
(s) =
A
O
s
R2
R2
R2 = R1
V
2
R1
K1
VO = (K1 + 1) V
V
O
IN
Figure 12. Low Phase Error Amplifier
Figure 13 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 w/bw
occurs at 0.002 w/bw
0.11 w/bw
for the low phase error amplifier.
T
< 0.1. For example, phase error of –0.1∞
T
for the single op amp amplifier, but at
T
REV. C
Figure 11. Pulsed Operation
–11–
Page 12
OP270
0
–1
–2
–3
–4
–5
PHASE SHIFT (Degrees)
–6
–7
0.0010.010.11.0
SINGLE OP AMP.
CONVENTIONAL DESIGN
CASCADED
(TWO STAGES)
LOW PHASE ERROR
0.0050.050.5
FREQUENCY RATIO (1/)(/T)
AMPLIFIER
Figure 13. Phase Error Comparison
C1
0.47F
V
IN
47k⍀
R3
680⍀
R5
680⍀
R7
680⍀
R9
680⍀
R11
680⍀
R1
+
1/2
OP270E
–
C2
6.8F
+
TANTALUM
C3
1F
+
TANTALUM
C4
0.22F
C5
0.047F
C6
0.022F
3.3k⍀
L1
1H
L2
600mH
L3
180mH
L4
60mH
L5
10mH
R2
+
1/2
R4
1k⍀
R6
1k⍀
R8
1k⍀
R10
1k⍀
R12
1k⍀
60Hz
200Hz
800Hz
3kHz
10kHz
OP270E
–
3.3k⍀
R13
Figure 14. 5-Band Low Noise Graphic Equalizer
R14
100⍀
FIVE-BAND LOW NOISE STEREO GRAPHIC EQUALIZER
The graphic equalizer circuit shown in Figure 14 provides 15 dB of
boost or cut over a 5-band range. Signal-to-noise ratio over a 20 kHz
bandwidth is better than 100 dB and referred to a 3 V rms input.
Larger inductors can be replaced by active inductors, but this
reduces the signal-to-noise ratio.
DIGITAL PANNING CONTROL
Figure 15 uses a DAC8221, a dual 12-bit CMOS DAC, to pan
a signal between two channels. One channel is formed by the
current output of DAC A driving one-half of an OP270 in a
current-to-voltage converter configuration. The other channel is
formed by the complementary output current of DAC A, which
normally flows to ground through the AGND pin. This complementary current is converted to a voltage by the other half of the
OP-270, which also holds AGND at virtual ground.
Gain error due to mismatching between the internal DAC ladder
resistors and the current-to-voltage feedback resistors is eliminated by using feedback resistors internal to the DAC8221. Only
DAC A passes a signal; DAC B provides the second feedback
resistor. With V
V
OUT
ing DAC B. Distortion of the digital panning control is less than
using R
B, is accurate and not influenced by digital data reach-
FB
B unconnected, the current-to-voltage converter,
REF
0.002% over the 20 Hz to 20 kHz audio range. Figure 16 shows
the complementary outputs for a 1 kHz input signal and a digital
ramp applied to the DAC data input.
DUAL PROGRAMMABLE GAIN AMPLIFIER
The dual OP270 and the DAC8221, a dual 12-bit CMOS
DAC, can be combined to form a space-saving dual programmable amplifier. The digital code present at the DAC, which is
easily set by a microprocessor, determines the ratio between the
internal feedback resistor and the resistance the DAC ladder
presents to the op amp feedback loop. Gain of each amplifier is
V
OUT
Vn
IN
= –
4096
where n equals the decimal equivalent of the 12-bit digital code
present at the DAC. If the digital code present at the DAC
consists of all zeros, the feedback loop will open, causing the op
amp output to saturate. A 20 MW resistor placed in parallel with
the DAC feedback loop eliminates this problem with only a very
small reduction in gain accuracy.
–12–
REV. C
Page 13
OP270
V
IN
DAC DATA BUS
PINS 6 (MSB) - 17 (LSB)
NC
WRITE
CONTROL
+5V
2
–
1/2
OP270GP
3
+
6
–
1/2
OP270GP
5
+
+15V
–15V
DAC8221HP
V
4
REF
V
22
REF
18
DAC A/DAC B
19
CS
20
WR
21
V
DD
RFBA
3
A
DAC A
B
DAC B
DGND
I
A
2
OUT
AGND 1
RFBB
23
I
B
24
OUT
5
Figure 15. Digital Panning Control
8
4
0.01F
+
10F
–
1
7
OUT
–
0.1F10F
+
OUT
WRITE
CONTROL
20M⍀
2
3
6
5
+15V
–
1/2
OP270EZ
+
–15V
–
1/2
OP270GP
+
DAC8221HP
3
VINA
23
VINB
DAC DATA BUS
PINS 6 (MSB) - 17 (LSB)
18
19
20
RFBA
RFBB
DGND
+5V
V
DAC A
DAC B
5
21
DD
V
A
4
REF
A
I
2
OUT
AGND
1
I
B
24
OUT
20M⍀
V
B
22
REF
Figure 17. Dual Programmable Gain Amplifier
0.01F
+
10F
–
8
1
4
0.1F10F
7
V
A
OUT
–
+
V
B
OUT
A OUT
A OUT
5V1ms5V
Figure 16. Digital Panning Control Output
REV. C
–13–
Page 14
OP270
OUTLINE DIMENSIONS
8-Lead Ceramic Dual In-Line Package [CERDIP]
Z-Suffix
(Q-8)
Dimensions shown in inches and (millimeters)
0.005 (0.13)
PIN 1
0.200 (5.08)
MAX
0.200 (5.08)
0.125 (3.18)
0.023 (0.58)
0.014 (0.36)
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETERS DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
0.055 (1.40)
MIN
0.100 (2.54) BSC
0.405 (10.29) MAX
MAX
85
1
4
0.070 (1.78)
0.030 (0.76)
0.310 (7.87)
0.220 (5.59)
0.060 (1.52)
0.015 (0.38)
0.150 (3.81)
MIN
SEATING
PLANE
0.320 (8.13)
0.290 (7.37)
15
0
0.015 (0.38)
0.008 (0.20)
8-Lead Plastic Dual In-Line Package [PDIP]
P-Suffix
(N-8)
Dimensions shown in inches and (millimeters)
0.375 (9.53)
0.365 (9.27)
0.355 (9.02)
8
1
0.100 (2.54)
0.180
(4.57)
MAX
0.150 (3.81)
0.130 (3.30)
0.110 (2.79)
0.022 (0.56)
0.018 (0.46)
0.014 (0.36)
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
COMPLIANT TO JEDEC STANDARDS MO-095AA
BSC
5
4
0.295 (7.49)
0.285 (7.24)
0.275 (6.98)
0.015
(0.38)
MIN
SEATING
PLANE
0.060 (1.52)
0.050 (1.27)
0.045 (1.14)
0.325 (8.26)
0.310 (7.87)
0.300 (7.62)
0.150 (3.81)
0.135 (3.43)
0.120 (3.05)
0.015 (0.38)
0.010 (0.25)
0.008 (0.20)
16-Lead Standard Small Outline Package [SOIC]
Wide Body
S-Suffix
(RW-16)
Dimensions shown in millimeters and (inches)
10.50 (0.4134)
10.10 (0.3976)
16
1
1.27 (0.0500)
BSC
0.30 (0.0118)
0.10 (0.0039)
COPLANARITY
0.10
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN