May 1998 Low Distortion Rail-to-Rail Op Amps Have 0.003% THD with 100kHz Signal

DESIGN FEATURES
Low Distortion Rail-to-Rail Op Amps
Have 0.003% THD with 100kHz Signal
by Danh Tran
Introduction
Device Characteristics
The LT1630/LT1632 duals and
LT1631/LT1633 quads are the newest members of Linear Technology’s
family of rail-to-rail op amps, which
provide the best combination of AC
performance and DC precision over
the widest range of supply voltages.
The LT1630/LT1631 deliver a 30MHz
gain-bandwidth product, a 10V/µs
slew rate and 6nV/√Hz input-voltage
noise. Optimized for higher speed
applications, the LT1632/LT1633
have a 45MHz gain-bandwidth product, a 45V/µs slew rate and 12nV/√Hz
input voltage noise. In a low supply
environment, these op amps maximize system dynamic range and
precision. The very large open loop
gain of these devices (a few million)
virtually eliminates gain error.
Because input offset error is so important on low supplies, it is
guaranteed over the whole rail-to-rail
input range. To achieve this, these
amplifiers use an LTC proprietary
trim algorithm to minimize the input
offset at two common mode voltages,
one at the negative supply and the
other at the positive supply. To make
designing with these amplifiers
straightforward, their performance is
fully specified for 3V, 5V and ±15V
supplies.
The LT1630/LT1631 have a gainbandwidth product of 30MHz, a
10V/µ s slew rate and a low input
noise voltage of 6nV/√Hz. With a
4.1mA typical supply current per
amplifier, the LT1630/LT1631 can
sink or source currents in excess of
50mA on a ±15V supply, allowing
them to drive low impedance loads.
Input offset voltage with a 5V supply
is specified at 525µV maximum over
the entire input range; a minimum
open loop gain of 500,000 ensures a
very small gain error. To maximize
common mode rejection, the LT1630/
LT1631 also employ a patented trim
technique that keeps the input offset
shift to less than 525µV when the
input common mode voltage is varied
from rail-to-rail. The output can swing
to within 40mV to either rail while
providing 0.5mA output current. Furthermore, the device’ s characteristics
change very little over the supply range
of 3V to ±15V: the worst-case supply
rejection is 87dB and the typical gainbandwidth product is constant at
30MHz. The LT1630/LT1631 have
only 0.003% THD with a 100kHz signal while operating on a low supply
voltage, as shown in Figure 1.
Optimized for higher frequency and
slew rate applications, the LT1632/
LT1633 deliver a gain-bandwidth
product of 45MHz, a slew rate of
45V/µs and an input voltage noise of
12nV/√Hz. These devices consume
4.6mA of supply current per amplifier
and have a short-circuit current of
70mA operating on a ±15V supply.
The input offset voltage is guaranteed
to be less than 1350µV over the whole
input range and the open loop gain is
specified to be greater than 450,000
on a 5V supply. Also, using the proprietary trim technique, the LT1632/
LT1633 is guaranteed to have an
input-offset shift of less than 1500µV
when the input common mode voltage
is varied from rail-to-rail. Like the
L T1630/L T1631, the L T1632/
LT1633’s characteristics don’t change
much over the specified supply range
of 3V to ±15V. Figure 2 illustrates the
large-signal response of LT1632 with
various loads for a 5V supply. Figure
3 shows the harmonic distortion of
LT1632 with a 1.25MHz sinusoidal
signal. Table 1 summarizes the performance of these newest rail-to-rail
amplifiers.
The LT1630/LT1632 dual amplifiers are available in either 8-pin SO
or 8-pin miniDIP packages. The
LT1631/LT1633 quad amplifiers are
available in the 14-pin SO.
1
VIN = 2VP-P
RL = 10k
THD + NOISE (%)
0.01
0.001
RL = 150Ω
0.3V
VS = 3V, 0V
AV = 1
RL = 1k
0.3V
VS = 5V, 0V AND 3V, 0V
AV = –1
10
1
FREQUENCY (kHz)
–30
–68.4dB
–71dB
–60
200ns/DIV
–70
1
2.5
FREQUENCY (MHz)
4
1630_03.EPS
163031 G23
14
–20
–50
100
Figure 1. LT1630 total harmonic distortion
+ noise vs frequency
0
VS = 5V
RL = 600Ω
AV = 1
VIN = 2VP-P AT 1.25MHz
–10
–40
RL = 10k
0.3V
VS = 5V, 0V
AV = 1
0.0001
0.1
VS = 5V
AV = 1
AMPLITUDE (dB)
1V/DIV
0.1
10
Figure 2. LT1632 large-signal response
Figure 3. LT1632 harmonic distortion
Linear Technology Magazine • May 1998
DESIGN FEATURES
exceeds either supply by approximately 700mV, D1–D2 or D3–D4 will
turn on and force the output to the
proper polarity.
The collector currents of the input
pairs are combined at the intermediate stage, consisting of Q8–Q12. Most
of the voltage gain of the amplifier is
generated in this stage. Its output is
then buffered and applied to output
transistors Q14 and Q15. Capacitors
C1 and C2 form local feedback loops
at the output stage to lower the output impedance at high frequency.
Table 1. Amplifier characteristics: VS = 5V, 25°C
Parameter
Gain-Bandwidth Product
Slew Rate
VS = ±15V
Input Noise Voltage
Offset Voltage
VCM = V–, V+
Offset Voltage Shift
VCM = V–, V+
Open Loop Gain
RL = 10k
Input Bias Current
VCM = V–, V+
Input Offset Current VCM = V–, V+
No Load
Output Voltage
Swing to Rail
IO = 20mA
VS = 5V
Short-Circuit Current
VS = ±15V
Operating Supply Voltage Range
Specified Supply Voltages
LT1630/LT1631 LT1632/LT1633
30MHz
45MHz
10V/µs
45V/µs
6nV/ Hz
12nV/ Hz
<525µV
<1350µV
<525µV
<1500µV
500k
450k
1µA
2.2µA
150nA
440nA
15mV
15mV
900mV
900mV
±40mA
±40mA
±70mA
±70mA
2.7V–30V
2.7V–30V
3V, 5V, ±15V
3V, 5V, ±15V
The Rail-to-Rail Architecture
Figure 4 shows the simplified schematic of these amplifiers. The circuit
is composed of three distinct stages:
an input stage, an intermediate stage
and an output stage. The input stage
consists of two differential amplifiers,
a PNP stage (Q1–Q2) and an NPN
stage (Q3–Q4), that are active over
different portions of the input common mode range. Each input stage is
trimmed for minimum offset voltage
and maximum common mode rejection. The intermediate stage is a folded
cascode configuration formed by Q8–
Q12, which provides most of the
voltage gain. A pair of complementary
common emitter devices, Q14–Q15,
creates an output stage which can
swing from rail to rail. The amplifiers
are fabricated on Linear Technology’s
proprietary complementary bipolar
process, which ensures that the
output devices, Q14 and Q15, possess a very similar DC and AC
characteristics.
Let’s first examine the input stage.
Transistor Q5 switches tail current I1
between the two input stages. When
the input common mode voltage, VCM,
is between the negative supply and
1.5V below positive supply, Q5 is
reverse biased and the PNP differential pair Q1–Q2 is active. As VCM moves
further toward the positive supply,
Q5 will be forward biased and steer
Linear Technology Magazine • May 1998
Typ
Typ
Typ
Max
Max
Min
Max
Max
Typ
Typ
Typ
Typ
Applications
the tail current I1 through the current
mirror Q6–Q7 to activate the NPN
differential pair. The PNP pair becomes
inactive for the rest of the input common mode range, up to the positive
supply. The input stages are protected by a pair of back-to-back diodes
D5–D6. When a differential voltage of
more than 0.7V is applied to the
inputs, these diodes will turn on,
preventing the emitter-base breakdown of the input transistors. To
prevent the output from reversing
polarity when the input voltage
exceeds the power supplies, two pairs
of crossing diodes, D1–D4, are
employed. When the input voltage
The ability to accommodate any input
and output signals that fall within the
device’ s supplies makes these amplifiers very easy to use. They exhibit a
very good transient response and can
drive low impedance loads, which
makes them suitable for high performance applications. The following
applications demonstrate the versatility of these amplifiers.
400kHz 4th Order Butterworth
Filter for 3V Operation
The circuit shown in Figure 5 makes
use of the low voltage operation and
the wide bandwidth of the LT1630 to
create a 400kHz 4th order lowpass
filter with a 3V supply. The amplifiers
are configured in the inverting mode
for the lowest distortion and the output can swing rail-to-rail for the
V+
R3
+
I1
D1
R6
+ IN 225Ω
R4
Q12
Q11
R5
Q15
Q13
+
D5
Q5
D6
VBIAS
I2
D2
R7
– IN 225Ω
V
Q4
Q3
–
C2
CC
OUT
Q2
Q1
D3
Q9
Q8
D4
Q7
V–
BUFFER
AND
OUTPUT BIAS
C1
Q6
R1
R2
Q14
1630/31 F01
Figure 4. LT1630 simplified schematic
15
DESIGN FEATURES
10
0
–10
47pF
2.32k
2.32k
GAIN (dB)
–20
–
6.65k
VIN
–
5.62k
2.74k
220pF
22pF 3V
2.74k
1/2 LT1630
+
470pF
–30
–40
–50
–60
1/2 LT1630
+
–70
VOUT
VS = 3V, 0V
VIN = 2.25VP-P
–80
VS/2
–90
0.1k
1630/31 TA01
1k
10k
100k
FREQUENCY (Hz)
1M
10M
1630/31 TA02
Figure 6. Frequency response of filter
in Figure 5
Figure 5. Single-supply, 400kHz, 4th order Butterworth filter
maximum dynamic range. Figure 6
displays the frequency response of
the filter. Stopband attenuation is
greater than 85dB at 10MHz. With a
2.25VP-P, 100kHz input signal, the
filter has harmonic distortion products of less than –87dBc.
the two inputs multiplied by the gain
of 100. Common mode range can be
calculated by the equations shown
with Figure 7. For example, the common mode range is from 0.15V to
2.65V if the output voltage is at onehalf of the 3V supply. The common
mode rejection is greater than 110dB
at 100Hz when trimmed with resistor
R1. Figure 8 shows the amplifier’s
cutoff frequency of 550kHz.
40dB Gain, 550kHz
Instrumentation Amplifier
An instrumentation amplifier with a
rail-to-rail output swing, operating
from a 3V supply, can be constructed
with the LT1632, as shown in Figure
7. The amplifier has a nominal gain of
100, which can be adjusted with
resistor R5. The DC output level is
equal to the input voltage (VIN) between
Conclusion
The LT1630–LT1633 family of railto-rail amplifiers extends the performance of rail-to-rail operation by
offering high speed characteristics
R5 450Ω
combined with precision. The combination of low distortion, high slew
rate and wide bandwidth allows these
amplifiers to be used in applications
where the signal amplitude could be
as large as the power supplies, and
where both AC and DC performance
are required. These amplifiers maintain their precision by specifying the
input offset over the whole input common mode range and by having the
typical open loop gain of a few million.
These characteristics, combined with
a wide supply operation and a large
output current capability, make these
amplifiers truly versatile and ideal for
demanding applications.
R4 20k
R2 2k
3V
R1 20k
50
–
+
–IN
( (
VOUT(DC) R2
AV
+ 0.1V
R5
1.0
1.1
( (
VOUT(DC) R2
AV
R5
OUT
AV =
R4
R3
(
1+
R2
R1
+
R3 + R2
R5
(
+ 2.85V
1.0
1.1
BW = 550kHz
VOUT(DC) = (+IN – (–IN))DC × GAIN
Figure 7. Single-supply instrumentation amplifier
16
= 100
10
VS = 3V
AV = 100
0
–10
COMMON MODE
INPUT
–20
–30
–40
–50
–60
UPPER LIMIT COMMON MODE INPUT VOLTAGE
VCMH =
20
+
LOWER LIMIT COMMON MODE INPUT VOLTAGE
DIFFERENTIAL
INPUT
30
1/2
LT1632
+IN
VCML =
40
–
VOLTAGE GAIN (dB)
R3 2k
1/2
LT1632
–70
100
1k
10k
100k
FREQUENCY (Hz)
1M
10M
1562 TA09
Figure 8. Frequency response of Figure 7’s
instrumentation amplifier
Linear Technology Magazine • May 1998