FEATURES
Single or Dual-Supply Operation
Excellent Sonic Characteristics
Low Noise: 7 nV/
Low THD: 0.0006%
Rail-to-Rail Output
High Output Current: ⴞ50 mA
Low Supply Current: 1.7 mA/Amplifier
Wide Bandwidth: 8 MHz
High Slew Rate: 12 V/s
No Phase Reversal
Unity Gain Stable
Stable Parameters Over Temperature
APPLICATIONS
Multimedia Audio
Professional Audio Systems
High Performance Consumer Audio
Microphone Preamplifier
MIDI Instruments
GENERAL DESCRIPTION
The SSM2275 and SSM2475 use the Butler Amplifier front
end, which combines both bipolar and FET transistors to offer
the accuracy and low noise performance of bipolar transistors
and the slew rates and sound quality of FETs. This product
family includes dual and quad rail-to-rail output audio amplifiers that achieve lower production costs than the industry standard OP275 (the first Butler Amplifier offered by Analog
Devices). This lower cost amplifier also offers operation from a
single 5 V supply, in addition to conventional ±15 V supplies.
The ac performance meets the needs of the most demanding au-
dio applications, with 8 MHz bandwidth, 12 V/µs slew rate and
extremely low distortion.
The SSM2275 and SSM2475 are ideal for application in high
performance audio amplifiers, recording equipment, synthesizers, MIDI instruments and computer sound cards. Where cascaded stages demand low noise and predictable performance,
SSM2275 and SSM2475 are a cost effective solution. Both are
stable even when driving capacitive loads.
The ability to swing rail-to-rail at the outputs (see Applications section) and operate from low supply voltages enables designers to attain high quality audio performance, even in single supply systems.
The SSM2275 and SSM2475 are specified over the extended
industrial (–40°C to +85°C) temperature range. The SSM2275 is
available in 8-lead plastic DIPs, SOICs, and microSOIC surfacemount packages. The SSM2475 is available in narrow body
SOICs and thin shrink small outline (TSSOP) surface-mount
packages.
*Protected by U.S. Patent No. 5,101,126.
√
Hz
Audio Amplifiers
SSM2275/SSM2475*
PIN CONFIGURATIONS
8-Lead Narrow Body SOIC 14-Lead Narrow Body SOIC
(SO-8) (R-14)
1
OUT A
2
–IN A
3
+IN A
+IN B
–IN B
OUT B
V+
SSM2475
4
(Not to Scale)
5
6
7
8-Lead microSOIC 14-Lead TSSOP
(RM-8) (RU-14)
OUT A
–IN A
+IN A
+IN B
–IN B
OUT B
V+
114
SSM2475
78
8-Lead Plastic DIP
(N-8)
OUT A
–IN A
+IN A
1
2
3
4
V–
SSM2275
(Not to
Scale)
8
7
6
5
V+
OUT B
–IN B
+IN B
14
13
12
11
10
9
8
OUT D
–IN D
+IN D
V–
+IN C
–IN C
OUT C
OUT D
–IN D
+IN D
V–
+IN C
–IN C
OUT C
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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
*θJA is specified for the worst case conditions, i.e., for device in socket for DIP
packages and soldered onto a circuit board for surface mount packages.
nent damage to the device. This is a stress rating only; the functional operation of
the device at these or any other conditions above those indicated in the opera tional
sections of this specification is not implied. Exposure to absolute maximum rating
conditions for extended periods may affect device reliability.
2
For supplies less than ±15 V, the input voltage and differential input voltage
must be less than ±15 V.
ORDERING GUIDE
TemperaturePackagePackage
ModelRangeDescriptionOptions
SSM2275P–40°C to +85°C8-Lead PDIPN-8
SSM2275S–40°C to +85°C8-Lead SOICSO-8
SSM2275RM–40°C to +85°C8-Lead microSOICRM-8
SSM2475S–40°C to +85°C14-Lead SOICR-14
SSM2475RU–40°C to +85°C14-Lead TSSOPRU-14
Units
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 SSM2275/SSM2475 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.
100
80
60
40
20
GAIN – dB
0
–20
–40
101M100
VS = 62.5V
= 2kV
R
L
= 10pF
C
L
1k10k100k
FREQUENCY – Hz
10M 40M
Figure 1. Phase/Gain vs. Frequency
225
180
135
90
45
PHASE – Degrees
0
–45
–90
100
80
60
40
20
GAIN – dB
0
–20
–40
101M100
1k10k100k
FREQUENCY – Hz
Figure 2. Phase/Gain vs. Frequency
VS = 62.5V
= 600V
R
L
= 10pF
C
L
10M 40M
225
180
135
90
45
PHASE – Degrees
0
–45
–90
REV. A–4–
Page 5
g
g
Typical Characteristics–SSM2275/SSM2475
100
80
60
40
20
GAIN – dB
0
–20
–40
101M100
100
80
60
40
VS = 615V
= 2kV
R
L
= 10pF
C
L
1k10k100k
FREQUENCY – Hz
10M 40M
Figure 3. Phase/Gain vs. Frequency
VS = 615V
= 600V
R
L
= 10pF
C
L
225
180
135
90
45
0
–45
–90
225
180
135
90
rees
PHASE – De
rees
60
VS = 615V
= 1258C
T
A
50
40
30
20
10
VOLTAGE NOISE DENSITY – nV/ Hz
0
10100k100
1k10k
FREQUENCY – Hz
Figure 6. SSM2275 Voltage Noise Density (Typical)
140
120
100
80
VS = 615V
= 1258C
T
A
20
GAIN – dB
0
–20
–40
101M100
1k10k100k
FREQUENCY – Hz
10M 40M
45
0
–45
–90
PHASE – De
Figure 4. Phase/Gain vs. Frequency
2.0
VS = 615V
= 1258C
T
1.8
A
1.6
1.4
1.2
1.0
0.8
0.6
CURRENT NOISE DENSITY – pA/ Hz
0.4
0.2
1010k100
FREQUENCY – Hz
1k
Figure 5. SSM2275 Current Noise Density vs. Frequency
60
40
COMMON MODE REJECTION – dB
20
0
10030M1k
10k1M10M
FREQUENCY – Hz
Figure 7. Common-Mode Rejection vs. Frequency
140
120
100
80
60
40
POWER SUPPLY REJECTION – dB
20
0
10010M1k
FREQUENCY – Hz
10k1M
VS = 615V
= 1258C
T
A
Figure 8. Power Supply Rejection vs. Frequency
REV. A–5–
Page 6
SSM2275/SSM2475–Typical Characteristics
29.5mV
0
200ns
20mV
0
SSM2275/SSM2475
–100
–110
–120
–130
–140
AMPLITUDE – dBV
–150
–160
VSY = +5V
A
R
V
0222
4 6 8 101214 161820
FREQUENCY – kHz
Figure 9. THD vs. Frequency (FFT)
= +1
V
= 100kV
L
= 0dBV
IN
11.0mV
1.0
0.9
0.8
0.7
0.6
0.5
0.4
(VOLTS-TO-RAIL) – V
OL
0.3
, V
OH
V
0.2
0.1
0
520
1015
LOAD CURRENT – mA
V
OUT –
(V+)
V
– (V–)
OUT
Figure 12. Headroom (VOH and VOL-to-Rails), TA = +25°C
00
20mV
200ns
Figure 10. Small Signal Response; RL = 600 Ω, CL = 0 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
22.5mV
00
20mV
200ns
Figure 13. Small Signal Response; RL = 600 Ω, CL = 200 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
35.5mV
00
20mV
200ns
Figure 11. Small Signal Response; RL = 600 Ω, CL = 100 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
Figure 14. Small Signal Response; RL = 600 Ω, CL = 300 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
REV. A–6–
REV. A–6–
Page 7
SSM2275/SSM2475
17.5mV
00
20mV
200ns
Figure 15. Small Signal Response; RL = 2 kΩ, CL = 0 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
31.0mV
00
43.0mV
00
20mV
200ns
Figure 18. Small Signal Response; RL = 2 kΩ, CL = 300 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
10.5mV
00
20mV
200ns
Figure 16. Small Signal Response; RL = 2 kΩ, CL = 100 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
38.0mV
00
20mV
200ns
Figure 17. Small Signal Response; RL = 2 kΩ, CL = 200 pF,
V
= ±2.5 V, AV = +1, VIN = 100 mV p-p
S
20mV
100ns
Figure 19. Small Signal Response; RL = 600 Ω, CL = 0 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
22.5mV
0
20mV
0
100ns
Figure 20. Small Signal Response; RL = 600 Ω, CL = 100 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
REV. A–7–
Page 8
SSM2275/SSM2475–Typical Characteristics
29.0mV
00
20mV
200ns
Figure 21. Small Signal Response; RL = 600 Ω, CL = 200 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
35.5mV
28.0mV
00
20mV
100ns
Figure 24. Small Signal Response; RL = 2 kΩ, CL = 100 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
36.5mV
00
20mV
200ns
Figure 22. Small Signal Response; RL = 600 Ω, CL = 300 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
13.0mV
00
20mV
100ns
Figure 23. Small Signal Response; RL = 2 kΩ, CL = 0 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
00
20mV
100ns
Figure 25. Small Signal Response; RL = 2 kΩ, CL = 200 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
42.0mV
00
20mV
200ns
Figure 26. Small Signal Response; RL = 2 kΩ, CL = 300 pF,
V
= ±15 V, AV = +1, VIN = 100 mV p-p
S
REV. A–8–
Page 9
SSM2275/SSM2475
THEORY OF OPERATION
The SSM2275 and SSM2475 are low noise and low distortion
rail-to-rail output amplifiers that are excellent for audio applications. Based on the OP275 audiophile amplifier, the SSM2275/
SSM2475 offers many similar performance characteristics with
the advantage of a rail-to-rail output from a single supply
source. Its low input voltage noise figure of 7 nV/√Hz allows the
device to be used in applications requiring high gain, such as
microphone preamplifiers. Its 11 V/µs slew rate also allows the
SSM2275/SSM2475 to produce wide output voltage swings
while maintaining low distortion. In addition, its low harmonic
distortion figure of 0.0006% makes the SSM2275 and
SSM2475 ideal for high quality audio applications.
Figure 27 shows the simplified schematic for a single amplifier.
The amplifier contains a Butler Amplifier at the input. This
front-end design uses both bipolar and MOSFET transistors in
the differential input stage. The bipolar devices, Q1 and Q2,
improve the offset voltage and achieve the low noise performance, while the MOS devices, M1 and M2, are used to obtain
higher slew rates. The bipolar differential pair is biased with a
proportional-to-absolute-temperature (PTAT) bias source, IB1,
while the MOS differential pair is biased with a non-PTAT
source, IB2. This results in the amplifier having a constant gainbandwidth product and a constant slew rate over temperature.
The amplifier also contains a rail-to-rail output stage that can
sink or source up to 50 mA of current. As with any rail-to-rail
output amplifier the gain of the output stage, and consequently
the open loop gain of the amplifier, is proportional to the load
resistance. With a load resistance of 50 kΩ, the dc gain of the
amplifier is over 110 dB. At load currents less than 1 mA, the
output of the amplifier can swing to within 30 mV of either supply rail. As load current increases, the maximum voltage swing
of the output will decrease. This is due to the collector to emitter saturation voltage of the output transistors increasing with an
increasing collector current.
Input Overvoltage Protection
The maximum input differential voltage that can be applied to
the SSM2275/SSM2475 is ±7 V. A pair of internal back-to-back
Zener diodes are connected across the input terminals. This
prevents emitter-base junction breakdown from occurring to the
input transistors, Q1 and Q2, when very large differential voltages are applied. If the device’s differential voltage could exceed
±7 V, then the input current should be limited to less than
±5 mA. This can be easily done by placing a resistor in series
with both inputs. The minimum value of the resistor can be
determined by:
V
IN
=
DIFF MAX
001
R
7
−
,
.
(1)
There are also ESD protection diodes that are connected from
each input to each power supply rail. These diodes are normally
reversed biased, but will turn on if either input voltage exceeds
either supply rail by more than 0.6 V. Again, should this condition occur the input current should be limited to less than
±5 mA. The minimum resistor value should then be:
V
IN MAX
R
IN
,
=
(2)
5
mA
In practice, RIN should be placed in series with both inputs to
reduce offset voltages caused by input bias current. This is
shown in Figure 28.
V+
R
IN
R
IN
V–
Figure 28. Using Resistors for Input Overcurrent Protection
Output Voltage Phase Reversal
The SSM2275/SSM2475 was designed to have a wide commonmode range and is immune to output voltage phase reversal with
an input voltage within the supply voltages of the device. However, if either of the device’s inputs exceeds 0.6 V above the positive voltage supply, the output could exhibit phase reversal.
This is due to the input transistor’s B–C junction becoming forward biased, causing the polarity of the input terminals of the
device to switch.
IB2
IN–Q1
M1
Q2IN+
M2
IB1
Figure 27. Simplified Schematic
REV. A–9–
CFI
V
CC
OUT
V
EE
Page 10
SSM2275/SSM2475
SSM2275
R
FB
V
OUT
R
L
V
IN
R1
0.1mF
10mF
V–
0.1mF
10mF
V+
R
B
SSM2275
R
FB
V
OUT
R
L
V
IN
R1
0.1mF
10mF
V–
0.1mF
10mF
V+
R
B
This phase reversal can be prevented by limiting the input current to +1 mA. This can be done by placing a resistor in series
with the input terminal that is expected to be overdriven. The
series resistance should be at least:
.
V
R
IN MAX
=
IN
06
−
,
1
mA
(3)
An equivalent resistor should be placed in series with both inputs to prevent offset voltages due to input bias currents, as
shown in Figure 28.
Output Short Circuit Protection
To achieve high quality rail-to-rail performance, the output of
the SSM2275/SSM2475 is not short-circuit protected. Shorting
the output may damage or destroy the device when excessive
voltages or currents are applied. To protect the output stage, the
maximum output current should be limited to ±40 mA. Placing
a resistor in series with the output of the amplifier as shown in
Figure 29, the output current can be limited. The minimum
value for R
can be found from Equation 4.
X
V
R
SY
=
X
(4)
mA
40
For a +5 V single supply application, RX should be at least
125 Ω. Because R
affected. The trade off in using R
is inside the feedback loop, V
X
is a slight reduction in output
X
voltage swing under heavy output current loads. R
is not
OUT
will also
X
increase the effective output impedance of the amplifier to
+ RX, where RO is the output impedance of the device.
R
O
R
FB
X
FEEDBACK
V
OUT
A1
125V
A1 = 1/2 SSM2275
R
Figure 29. Output Short Circuit Protection Configuration
Power Dissipation Considerations
While many designers are constrained to use very small and low
profile packages, reliable operation demands that the maximum
junction temperatures not be exceeded. A simple calculation
will ensure that your equipment will enjoy reliable operation
over a long lifetime. Modern IC design allows dual and quad
amplifiers to be packaged in SOIC and microSOIC packages,
but it is the responsibility of the designer to determine what the
actual junction temperature will be, and prevent it from exceed-
ing the 150°C. Note that while the θ
age options, the θ
for the SOIC and TSSOP are nearly double
JA
is similar between pack-
JC
the PDIP. The calculation of maximum ambient temperature is
relatively simple to make.
For example, with the 8-lead SOIC, the calculation gives a
maximum internal power dissipation (for all amplifiers, worst
case) of P
= (150°C – 85°C)/158°C/W = 0.41 W. For the
MAX
DIP package, a similar calculation indicates that 0.63 W (approximately 50% more) can be safely dissipated. Note that ambient temperature is defined as the temperature of the PC board
to which the device is connected (in the absence of radiated or
convected heat loss). It is good practice to place higher power
devices away from the more sensitive circuits. When in doubt,
measure the temperature in the vicinity of the SSM2275 with a
thermocouple thermometer.
Maximizing Low Distortion Performance
Because the SSM2275/SSM2475 is a very low distortion amplifier,
careful attention should be given to the use of the device to prevent
inadvertently introducing distortion. Source impedances seen by
both inputs should be made equal, as shown in Figure 28, with
= R1储RF for minimum distortion. This eliminates any offset
R
B
voltages due to varying bias currents. Proper power supply
decoupling reduces distortion due to power supply variations.
Because the open loop gain of the amplifier is directly dependent
on the load resistance, loads of less than 10 kΩ will increase the
distortion of the amplifier. This is a trait of any rail-to-rail op
amp. Increasing load capacitance will also increase distortion.
It is recommended that any unused amplifiers be configured as a
unity gain follower with the noninverting input tied to ground.
This minimizes the power dissipation and any potential crosstalk
from the unused amplifier.
As with many FET-type amplifiers, the PMOS devices in the
input stage exhibit a gate-to-source capacitance that varies with
the common mode voltage. In an inverting configuration, the inverting input is held at a virtual ground and the common-mode
voltage does not vary. This eliminates distortion due to input
capacitance modulation. In noninverting applications, the gateto-source voltage is not constant, and the resulting capacitance
modulation can cause a slight increase in distortion.
Figure 30 shows a unity gain inverter and a unity gain follower
configuration. Figure 31 shows an FFT of the outputs of these
amplifiers with a 1 kHz sine wave. Notice how the largest harmonic amplitude (2nd harmonic) is –120 dB below the fundamental (0.0001%) in the inverting configuration.
P
TT
=
MAX
−
I MAXA
,
θ
J
A
(5)
Figure 30. Basic Inverting and Noninverting Amplifiers
REV. A–10–
Page 11
SSM2275/SSM2475
R1
1kV
R
S
909V
R
F
10kV
+5V
–5V
R
L
10kV
V
OUT
V
IN
2V p-p
10kHz
–100
–110
–120
–130
–140
NOISE – dBV
–150
–160
022
–100
–110
–120
–130
–140
NOISE – dBV
–150
–160
022
VSY = 65V
= 11
A
V
= 100kV
R
L
= 0dBV
V
IN
VSY = 15V
= –1
A
V
= 100kV
R
L
= 0dBV
V
IN
1020
FREQUENCY – kHz
1020
FREQUENCY – kHz
Figure 31. Spectral Graph of Amplifier Outputs
Settling Time
The high slew rate and wide gain-bandwidth product of the
SSM2275 and SSM2475 amplifiers result in fast settling times
< 1 µs) that are suitable for 16- and 20-bit applications. The
(t
S
test circuit used to measure the settling time of the SSM2275/
SSM2475 is shown in Figure 32. This test method has advantages over false-sum node techniques of measuring settling times
in that the actual output of the amplifier is measured, instead of
an error voltage at the sum node. Common-mode settling effects are also taken into account in this circuit in addition to
slew rate and bandwidth factors.
The output waveform of the device under test is clamped by
Schottky diodes and buffered by the JFET source follower. The
signal is amplified by a factor of ten by the OP260 current feedback amplifier and then Schottky-clamped at the output to the
oscilloscope. The 2N2222 transistor sets up the bias current for
the JFET and the OP41 is configured as a fast integrator, providing overall dc offset nulling at the output.
10
8
6
4
2
0
–2
STEP SIZE – V
–4
–6
–8
–10
400600
10.1%10.01%
–0.01%
80010001200
SETTLING TIME – ns
Figure 33. Settling Time vs. Step Size
Overdrive Recovery
The overdrive, or overload, recovery time of an amplifier is the time
required for the output voltage to return to a rated output voltage
from a saturated condition. This recovery time can be important in
applications where the amplifier must recover quickly after a large
transient event, or overload. The circuit in Figure 34 was used to
evaluate the recovery time for the SSM2275/SSM2475. Also shown
are the input and output voltages. It takes approximately 0.5 µs for
the device to recover from output overload.
Figure 34. Overload Recovery Time Test Circuit
9V–15V
–+
0.1mF
0.1mF
+
9V–15V
65V
R
1kV
1N4148
L
D1D2
V+
DUT
V–
–
–15V
15kV
+15V
2N4416
2N2222A
1/2 OP260AJ
R
F
2kV
R
G
222V
1kV
D3
10kV
10kV
750V
SCHOTTKY DIODES D1–D4 ARE
HEWLETT-PACKARD HP5082-2835
IC1 IS 1/2 OP260AJ
IC2 IS PMI OP41EJ
D4
1mF
IC2
OUTPUT
(TO SCOPE)
Figure 32. Settling Time Test Fixture
REV. A–11–
Page 12
SSM2275/SSM2475
SSM2475-A
+12V
R2
10kV
R1
10kV
C3
33pF
R9
50V
R5
10kV
SSM2475-B
+12V
R8
10kV
R7
10kV
C4
33pF
R10
50V
R3
10kV
SSM2475-C
+5V
R4
10kV
C4
10mF
R12
10kV
R11
10kV
R13
100kV
C1*
10mF
R14
100kV
C2
10mF
+12V
V
IN
V
01
R6
10kV
C3
10mF
V
02
C1* IS OPTIONAL
Capacitive Loading
The output of the SSM2275/SSM2475 can tolerate a degree of
capacitive loading. However, under certain conditions, a heavy
capacitive load could create excess phase shift at the output and
put the device into oscillation. The degree of capacitive loading
is dependent on the gain of the amplifier. At unity gain, the amplifier could become unstable at loads greater than 600 pF. At
gain greater than unity, the amplifier can handle a higher degree
of capacitive load without oscillating. Figure 35 shows how to
configure the device to prevent oscillations from occurring.
C
FB
R
R
V
IN
R
B
50kV
INVERTING GAIN AMPLIFIER
FB
I
SSM2275
V
OUT
V
C
L
IN
50kV
NONINVERTING GAIN AMPLIFIER
R
R
B
I
C
FB
R
FB
SSM2275
V
OUT
C
L
Figure 35. Configurations for Driving Heavy Capacitive
Loads
R
should be at least 50 kΩ. To minimize offset voltage, the
B
parallel combination of R
ting a minimum C
of 15 pF bandlimits the amplifier enough to
F
and RI should be equal to RB. Set-
FB
eliminate any oscillation problems from any sized capacitive
load. The low-pass frequency is determined by:
For the values given in Figure 36, R
= 5 kΩ. With C1 omitted
IN
the circuit will provide a balanced output down to dc, otherwise
the –3 dB corner for the input frequency is set by:
=
2
π
1
(8)
RC
IN L
f
dB
−
3
The circuit can also be configured to provide additional gain if
desired. The gain of the circuit is:
where V
V
A
=
V
= VO1 – VO2, R1 = R3 = R5 = R7 and,
OUT
V
OUT
IN
2( R2)
=
(9)
R1
R2 = R4 = R6 = R8
Figure 37 shows the THD+N versus frequency response of the
circuit while driving a 600 Ω load at 1 V rms.
1
=
2
π
(6)
RC
FB F
= 15 pF, this results in an amplifier
With R
= 50 kΩ and C
FB
f
dB
−
3
F
with a 210 kHz bandwidth that can be used with any capacitive
load. If the amplifier is being used in a noninverting unity gain
configuration and R
If the offset voltage can be tolerated at the output, R
replaced by a short and C
typical input bias current of 200 nA and R
is omitted, CFB should be at least 100 pF.
I
can be removed entirely. With the
FB
= 50 kΩ, the in-
B
can be
FB
crease in offset voltage would be 10 mV. This configuration will
stabilize the amplifier under all capacitive loads.
Single Supply Differential Line Driver
Figure 36 shows a single supply differential line driver circuit
that can drive a 600 Ω load with less than 0.001% distortion.
The design mimics the performance of a fully balanced transformer based solution. However, this design occupies much less
board space while maintaining low distortion and can operate
down to dc. Like the transformer based design, either output
can be shorted to ground for unbalanced line driver applications
without changing the circuit gain of 1.
R13 and R14 set up the common-mode output voltage equal to
half of the supply voltage. C1 is used to couple the input signal
and can be omitted if the input’s dc voltage is equal to half of
the supply voltage. The minimum input impedance of the circuit as seen from V
is:
IN
RRRRRR
IN
=+
15 37 11||||
()
+
()
(7)
Figure 36. A Low Noise, Single Supply Differential
Line Driver
0.1
VSY = 12V
= 600V
R
L
0.01
THD + N – %
0.001
0.0001
2020k100
FREQUENCY – Hz
1k
10k
Figure 37. THD+N vs. Frequency of Differential Line Driver
REV. A–12–
Page 13
SSM2275/SSM2475
100pF
TO LPF
SSM2275-A
+12V
16
12
11
10
R
FB
(OPTIONAL)
V
CC
ACOM
I
OUT
R
F
AD1862
NOTE: ADDITIONAL PIN CONNECTIONS OMITTED FOR CLARITY
Multimedia Soundcard Microphone Preamplifier
The low distortion and low noise figures of the SSM2275 make
it an excellent device for amplifying low level audio signals. Figure 38 shows how the SSM2275 can be configured as a stereo
microphone preamplifier driving the input to a multimedia
sound codec, the AD1848. The SSM2275 can be powered from
the same +5 V single supply as the AD1848. The V
REF
pin on
the AD1848 provides a bias voltage of 2.25 V for the SSM2275.
This voltage can also be used to provide phantom power to a
condenser microphone through a 2N4124 transistor buffer and
2 kΩ resistors. The phantom power circuitry can be omitted for
dynamic microphones. The gain of SSM2275 amplifiers is set
by R2/R1 which is 100 (40 dB) as shown. Figure 39 shows the
1/2
7
RMS
+5V
0.1mF
output.
35/36
34/37
0.1mF
29
32
28
LMIC
V
CC
GND
V
REF
AD1848
RMIC
device’s THD+N performance with a 1 V
R2
10kV
+5V
L CHANNEL
MIC IN
R CHANNEL
MIC IN
10mF
2kV
+5V
2N4124
2kV
10mF
10kV
10kV
R1
100V
R1
100V
2
3
5
6
10mF
8
SSM2275
4
10mF
SSM2275
R2
10kV
1
1/2
Figure 38. Low Noise Microphone Preamplifier for
Multimedia Soundcard Codec
1
AV = +40dB
= ±2.5V
V
SY
= –40dBV
V
IN
> 10kV
R
L
= 22kHz
B
W
0.1
The AD1862 has a built in 3 kΩ resistor that is connected from
the inverting input to the output of the amplifier. The full-scale
output current of the AD1862 is ±1 mA, resulting in a maximum
output voltage of ±3 V. Additional feedback resistance can be
added in the feedback loop to increase the output voltage. With
connected the maximum output voltage will be:
R
FB
VmAkR
OUT MAXFB,
=× +
13Ω
()
(10)
Figure 40. A High Performance I-V Converter for a 20-Bit DAC
In Figure 41, the SSM2275 is used as a low-pass filter for one
channel of the AD1855, a 24-bit 96 kHz stereo sigma-delta
DAC, which uses a complementary voltage output. The filter is
configured as a second order low-pass Bessel filter with a cutoff
frequency of 50 kHz. This provides a phase linear response from
dc to 24 kHz, which is ideal for high quality audio applications.
The SSM2275 can be connected to the same +5 V power supply source, that the AD1855 is connected to, eliminating the
need for extra power circuitry. The FILT output (Pin 14) from
the AD1855 provides a common reference voltage equal to half
of the supply voltage for the SSM2275.
Amplifier A1 is used as a unity-gain inverter for the positive output of the AD1855. The output of A1 is combined with a negative output of the AD1855 into the active low pass filter around
A2. The output impedance of each output of the AD1855 is
100 Ω which must be taken into account to achieve proper dc
gain, which in Figure 41 is unity gain. In this configuration the
SSM2275 can drive reasonable capacitive loads, making the device suitable for the RCA jack line outputs found in most consumer audio equipment.
THD + N – %
0.01
0.001
2020k100
FREQUENCY – Hz
Figure 39. THD+N vs. Frequency (V
V
= 1 V rms)
OUT
High Performance I-V Converters and Filters for 20-Bit DACs
Because of the increasing resolution and lower harmonic distortions required by more audio applications, the need for high
quality amplifiers at the output of D/A converters becomes critical. The SSM2275 and SSM2475 can be used as current-tovoltage converters and smoothing filters for 18- and 20-bit
DACs, achieving 0.0006% THD+N figures while running from
the same +5 V or +12 V source used to power the D/A converter. Figure 40 shows how the SSM2275 can be used with the
AD1862, a current output 20-bit DAC.
REV. A–13–
1k
= +5 V, AV = 40 dB,
SY
10k
+5V
28
V
DD
V
OUT–
AD1855
OUT+
FILT
GND
GND
DD
18
13 OR 18
12 OR 17
14
1
15
+5V
1.05kV
1.15kV
1.05kV
A1
0.1mF
10mF
NOTE: ADDITIONAL PIN CONNECTIONS
OMITTED FOR CLARITY
562V
1.15kV
A1 AND A2 ARE SSM2275
OR 1/2 SSM2475
4.7nF
237V
A2
10mF
Figure 41. Low-Pass Filter for a 24-Bit Stereo SigmaDelta DAC
OUT
Page 14
SSM2275/SSM2475
SPICE Macro-model
The SPICE macro-model for the SSM2275 is shown in Listing
1 on the following page. This model is based on typical values
for the device and can be downloaded from Analog Devices’
Internet site at www.analog.com. The model uses a common
emitter output stage to provide rail-to-rail performance. A resistor and dc voltage source, in series with the collector, accurately
portray output dropout voltage versus output current. The
VCMH and VCML sources set the upper and lower limits of
the input common mode voltage range. Both are set up as a
function of the supply voltage to mimic the varying common
mode range with supply voltage. The EOS voltage source establishes the offset voltage and is also used to create the commonmode rejection and power supply rejection characteristics for
the model.
+5V SUPPLY
18-BIT
DAC
VL1
LL
2
3
4
5
6
7
8
DL
CK
DR
LR
DGND
VBR
18-BIT
SERIAL
REG.
18-BIT
SERIAL
REG.
18-BIT
DAC
V
REF
AD1868
V
REF
VBL
VOL
AGND
VOR
16
15
14
13
12
11
10
V
S
7.68kV
330pF
7.68kV
9
330pF
A secondary pole section is also set up to vary the gain bandwidth product and phase margin of the model based on the
supply voltage. The H1 and VR1 sources set up an equivalent
resistor that is linearly varied with supply voltage. This equivalent resistance, in parallel with C2, creates the secondary pole.
G2 is also linearly varied to increase the GBW at higher supply
voltages. With a supply voltage of 5 V, the gain bandwidth
product is 6.3 MHz with a 47 degree phase margin. At a 30 V
supply voltage, the GBW product moves out to 7.5 MHz with
48° phase margin.
The broadband input referred voltage noise for the model is
6.8 nV/√Hz. Flicker noise characteristics are also accurately
modeled with the 1/f corner frequency set through the KF and
AF terms in the input stage transistors. Finally, a voltage-controlled current source, GSY, is used to model the amplifier’s
supply current versus supply voltage characteristics.
1/2
SSM2275
9.76kV
9.76kV
3
2
7.68kV
7.68kV
6
5
8
4
100pF
100pF
1/2
SSM2275
220mF
1
47kΩ
220mF
7
47kV
LEFT
CHANNEL
OUTPUT
RIGHT
CHANNEL
OUTPUT
Figure 42. A Smoothing Filter for an 18-Bit Stereo DAC