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THAT 1583 Low-Noise Page 6 of 16 Document 600173 Rev 03
Differential Audio Preamplifier IC
THAT Corporation; 45 Sumner Street; Milford, Massachusetts 01757-1656; USA
Tel: +1 508 478-9200; Fax +1 508 478-0990; Web: www.thatcorp.com
Copyright © 2016, THAT Corporation; All rights reserved.
Amplifier Overview
Referring to Figure 15, the THAT1583's differential
voltage gain (G) is set by the feedback resistors (R
A
and R
B
) and R
G
, as shown in the following equation.
The amplifier's minimum gain is unity (0 dB), which
occurs with infinite R
G
. The feedback resistors
should nominally be equal, though tight tolerance
matching is not required.
= 1 +
+
In low-noise current-feedback amplifiers like the
1583, many performance characteristics depend
critically on the impedance of the feedback network
(R
A
, R
B
, and R
G
).
The 1583 (and 1570) offers a novel approach to an
integrated microphone preamplifier in that all three
gain resistors are external. This gives the designer
freedom to select the optimal values for the best
noise performance at the desired gain setting(s).
Noise versus Gain
The noise performance of a preamplifier based on
the 1583 is determined as the sum of several noise
sources. These are as follows (refer to Figure 15 for
component reference designators):
1. the amplifier's own input voltage noise;
2. the voltage noise of the gain-setting resistor
network (R
G
in parallel with R
A
and R
B
);
3. the voltage noise of the external source im-
pedance, connected to the 1583's input (R
M
in
parallel with R
1
+ R
2
):,
4. the current noise from IN+ and IN-, developed
across the source impedance (R
M
in parallel
with R
1
+R
2
), and
5. the current noise from R
G1
and R
G2
, translated
to a voltage when drawn across the equivalent
impedance of the external gain-setting resistor
network (R
G
in parallel with R
A
and R
B
).
Since all these sources are uncorrelated, mostly
random (Gaussian) noise, these sources all add in
root-mean-square fashion. But which one is most
important changes with gain, so predicting how noise
varies can be complex.
A complete discussion of these sources and their
interaction is beyond the scope of this data sheet.
For more information, see "De-Integrating Integrated
Circuit Preamps", available from THAT Corporation's
web site, especially pages 13 through 20 However,
the following discussion covers the highlights.
At high gains (above 40 dB or so), the system noise
is typically dominated by the first three factors in the
above list. At high gains, for practical values of R
A
,
R
B
, and R
G
(where R
G
is typically less 100Ω) and
typical external source impedances (microphones are
generally around 150Ω), the amplifier's input voltage
noise will be the largest contributor. However, at
1.9 nV/√Hz (-128.9 dBu unweighted, 22 kHz
bandwidth) the amplifier's own input noise is only
1.5 dB higher than that of a 150 Ω microphone (-
130.4 dBu). So, the external source impedance R
M
is
a significant contributor to the total noise of the
system.
At low gains (under about 20 dB), the dominant
noise sources are factors 2 and 5. An important case
occurs at 0 dB (unity) differential gain. In order to
reach 0 dB gain, R
G
is open (infinite resistance). In
this case, the current noise in R
G1
and R
G2
is drawn
across the highest possible impedance (R
A
and R
B
alone, without any shunting effect of R
G
). The only
way to mitigate this noise is to use lower values for
R
A
and R
B
.
Of course, there is a continuum of relative impor-
tances here as gain goes from minimum (0 dB) to
maximum (over 70 dB). As gain varies, the im-
portance of each factor will vary in its own way, each
contributing a different relative amount to the total.
In general, to minimize low-gain noise, we suggest to
keep R
A
and R
B
as small as possible.
Another perspective on noise performance is gained
by measuring the noise using an A-weighting filter.
Figure 3 compares equivalent input noise for various
gains in a 22 kHz bandwidth vs. using an A-weighting
filter. The A-weighting filter improves input noise
performance by about 3 dB.
Bandwidth
An important characteristic of current-feedback
amplifiers is that the amplifier bandwidth is inversely
proportional to the feedback resistance R
A
and R
B
.
The bandwidth decreases with increasing feedback
resistance. As mentioned before, the minimum value
of R
A
and R
B
is determined by the amplifier's stability
and cannot be under any condition lower than 2 kΩ.
Figure 5 shows typical bandwidth versus gain for a
few selected values of feedback resistance.
Theory of Operation
Figure 15. Simple THAT1583 Amplifier Circuit
A
R
B
R
G
R
M
R
1
R
2
IN1 OUT+
OUT-
OUT1
OUT2
R
G
1
R
G
2
IN2