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Transcript
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Fast Op Amps Operate Rail-to-Rail on 2.7V – Design Note 241
Glen Brisebois
The new LT®1806 and LT1809 are fast operational amplifiers with rail-to-rail inputs and outputs. The LT1806 is
optimized for low noise (3.5nV/√Hz) and offset (100µV
typical, 550µV max) and has a 325MHz gain bandwidth
product. The LT1809 is optimized for low distortion
(– 90dBc to 5MHz) and has a 180MHz gain bandwidth
product. Both amplifiers have 85mA output drive capability and are fully specified over commercial and industrial
temperature ranges on 3V, 5V and ±5V supplies.
Parallel Composite Amplifier Achieves
Low Distortion into Heavy Loads
Achieving low distortion is difficult enough and driving
heavy loads only makes the undertaking more difficult.
Figure 1 shows a parallel composite topology where each
amplifier is given a different responsibility. Amplifier U1 is
configured in a standard gain of 2 to account for the
eventual attenuation caused by the 50Ω output divider.
Amplifier U1 alone can drive the load, but its distortion
figures would suffer. Therefore, amplifier U2 is added in
a slightly higher gain and its output is coupled to the
circuit output through the attenuating 10Ω resistor, with
the product of the gain and the attenuation set to match
U1’s gain of 2. In this way, the heavy load current is
supplied by U2’s output and is not seen by U1. Although
the heavy load current on U2 will cause it to generate
higher distortion, these distortion products are decoupled
by the 10Ω resistor and corrected by U1. Basically, U2
supplies the power and U1 supplies the precision.
While this provides improvement, it is still possible to do
better. Normally, lower distortion is achieved by putting
the output into “Class A” operation, in which the bias
current is higher than the peak load current. This is often
done with a simple load resistor to one of the supply rails.
Unfortunately, in cases where load current is already high,
additional load current will only make matters worse.
However, a kind of “tracking” Class A operation can be
achieved by putting a small offset voltage into the power
amplifier, U2. This causes a slight DC shift in its output
and increases the bias current of U1’s output stage. The
DC offset is injected at VA through R7 and can be dynamically adjusted to suit real-time requirements. Table 1
shows results achieved with a 1VP-P input signal at
2.5MHz with ±5V supplies, with the last entry showing
, LTC and LT are registered trademarks of Linear Technology Corporation.
VA
1k
619Ω
5V
49.9Ω
453Ω
2
3
7
–
6
U2
LT1806
+
4
1
R1
10Ω
–5V
AV = 2.2
AV = 2.0
5V
VIN
3
2
S1
7
+
6
U1
LT1806
–
4
1
49.9Ω
VOUT
50Ω COAX
CABLE
–5V
499Ω
DN241 F01
499Ω
Figure 1. Parallel Composite Amplifier: U2 Provides
the Current, Easing the Load on U1. U1 Provides Only
a Correction Current
Table 1. Distortion of Figure 1 at 2.5MHz, VSUPPLY = ±5V
HARMONICS
2nd
3rd
VIN
S1
VA
RL
VOUT
ISUPPLY
NOTE
1VP-P
Open
0V
1M
2VP-P
– 92dBc
– 98dBc
22mA
Low distortion at light load
1VP-P
Open
0V
50Ω
1VP-P
– 80dBc
– 84dBc
24mA
Load increases, distortion worse
1VP-P
Closed
0V
50Ω
1VP-P
– 90dBc
– 99dBc
25mA
U2 helps, distortion better
1VP-P
Closed
1.5V
50Ω
1VP-P
– 94dBc
– 99dBc
28mA
Add offset, distortion better yet
3VP-P
Closed
1.5V
50Ω
3VP-P
– 85dBc
– 77dBc
36mA
Results at higher amplitude
10/00/241
RL
www.BDTIC.com/Linear
3VP-P throughput. Note that because the circuit shown is
noninverting, its input impedance is high and is easy to
drive.
Among the benefits of this parallel composite topology
over series composite topologies is that it does not
require onerous attention to compensation and does not
reduce the effective bandwidth of the op amps. The tradeoff is that supply current increases, but the designer
should remember that a 3VP-P signal requires ±30mA of
peak current itself, so a 36mA supply current is modest
considering the low distortion levels being achieved. This
example was shown using two LT1806’s for low noise and
high bandwidth, but depending on the requirements other
amplifiers can be configured in this topology as well.
Rail-to-Rail Pulse Width Modulator
Using the LT1809
Binary modulation schemes are used in order to improve
efficiency and reduce physical circuit size. They do this by
reducing the power dissipation in the output driver transistors. In a normal Class A or Class AB amplifier, voltage
drop and current flow exist simultaneously in the output
transistors and power losses proportional to V • I occur.
In a binary modulation scheme, the output transistors,
whether bipolar or FET, are switched hard-on and hard-off
so that voltage drops do not occur simultaneously with
current flow. The circuit of Figure 2 shows an example of
a binary modulation scheme, in this case pulse width
modulation.
The LT1809 is configured as an integrator in order to
generate nice linear rail-to-rail voltage ramps. The polarity
of the ramp is determined by the output of comparator A
R1
26.1Ω
V+
R2
2k
R3
2k
2
4
+
A
1/2 LT1714
1
–
14
R4
13 499Ω
2
16
–
7
LT1809
3
3
V+
R5
1k
+
C2
0.01µF
V + = 2.7V TO 7V
4
R6
1k
C4
0.001µF
6
21Ω
C3
100pF
1MHz
TRIANGLE
WAVE
16kHz ANALOG FILTER
FOR LINEARITY MEASUREMENT
V+
7
V+
1
15
The linearity of the pulse width modulated signal can
easily be ascertained by putting a simple 2-pole RC filter
at the output (as shown in Figure 2). This demodulates the
signal which can then be viewed and compared with the
original input signal on an oscilloscope. Using a spectrum
analyzer and a 1kHz reference signal, this circuit’s distortion products were measured as better than – 50dBc
(0.3%) to about 3.5VP-P, degrading to – 30dBc (3%) as
the circuit clips at 5VP-P on a single 5V supply.
ANTIALIASING
1k FILTER
ANALOG
INPUT
C1
500pF
V+
into R4. The heavy hysteresis of R1 around comparator A
combined with the feedback of the LT1809 force the
devices to perpetually reverse each other, resulting in a
1MHz triangle wave. This constitutes the usual first half of
any pulse width modulator, but the forte of this particular
implementation is that it is rail-to-rail allowing a full-scale
analog input. Once the triangle wave is achieved, the
remainder of the pulse width modulator is easy, and is
constituted by doing a simple comparison using the
second half of the LT1714. The triangle wave and the
relatively slow moving analog signal (the one to be modulated or to do the modulation, depending on how you look
at it) are fed into the inputs of comparator B, whose output
is then the PWM representation of the analog input
voltage. The higher the analog input voltage, the wider the
output pulse. The time averaged output level is thus
proportional to the analog input voltage. This binary
output can then be fed into power transistors with direct
control over motor or speaker winding current, for
example, with their inherent lowpass characteristic. Care
must be taken to avoid cross conduction in the output
power transistors.
5
+
B
1/2 LT1714
8
–
1k
11
10
12
C5
0.01µF
10k
C6
0.001µF
9
6
DN241 F02
COMPLEMENTARY
1MHz PWM
OUTPUTS
Figure 2. Rail-to-Rail 1MHz Pulse Width Modulator
Data Sheet Download
http://www.linear-tech.com/go/dnLT1806
http://www.linear-tech.com/go/dnLT1809
Linear Technology Corporation
For literature on our Op Amps,
call 1-800-4-LINEAR. For applications help,
call (408) 432-1900, Ext. 2456
dn241 LT/TP 1000 340K • PRINTED IN THE USA
1630 McCarthy Blvd., Milpitas, CA 95035-7417
www.BDTIC.com/Linear
(408)432-1900 ● FAX: (408) 434-0507 ● www.linear-tech.com
 LINEAR TECHNOLOGY CORPORATION 2000