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Updated Operational Amplifier Selection Guide for
Optimum Noise Performance – Design Note 140
Frank Cox
Eight years ago, George Erdi wrote a very useful Design
Note (DN6) that presented information to aid in the selec-
tion of op amps for optimum noise performance, in both
graphical and tabular form. Design Note 140 is an update of
DN6. It covers new low noise op amps as well as some high
speed op amps. Although a great deal has changed in eight
years, especially in electronics, noise is still a critical issue
in op amp circuit design and the LT
®
1028 is still the lowest
noise op amp for low source impedance applications.
The amount of noise an op amp circuit will produce is
determined by the device used, the total resistance in the
circuit, the bandwidth of the measurement, the tempera-
ture of the circuit and the gain of the circuit. A convenient
figure of merit for the noise performance of an op amp is the
spectral density or spot noise. This is obtained by normaliz-
ing the measurement to a unit of bandwidth. Here the unit is
1Hz and the noise is reported as “nV/Hz.” The noise in a
particular application bandwidth can be calculated by mul-
tiplying the spot noise by the square root of the application
bandwidth.
Some other simplifications are made to facilitate compari-
son. For instance, the noise is referred to the input of the
circuit so that the effect of the circuit gain, which will vary
with application, does not confuse the issue. Also, the
calculations assume a temperature of 27°C or 300°K.
The formula used to calculate the spot noise and the
schematic of the circuit used are shown in Figure 1. Figures
2 through 4 plot the spot noise of selected op amps vs the
equivalent source resistance. The first two plots show
precision op amps intended for low frequency applica-
tions, whereas the last plot shows high speed voltage-
feedback op amps. There are two plots for the low
frequency op amps because at very low frequencies (less
than about 200Hz) an additional noise mechanism, which
is inversely proportional to frequency, becomes important.
This is called 1/f or flicker noise. Figure 2 shows slightly
higher levels of noise due to this contribution.
, LTC and LT are registered trademarks of Linear Technology Corporation.
WHERE: V
TR1
, V
TR2
AND V
TR3
ARE THERMAL NOISE FROM RESISTORS
R
eq
=
4kT = (16.56)(10)
–21
J
R2 + (R1)(R3)
R1 + R3
)
)
AND V
n
IS THE VOLTAGE SPOT NOISE AND I
n
IS THE CURRENT SPOT NOISE OF THE
OP AMP AS GIVEN ON THE DATA SHEET.
V =
(4kT)Req + Vn2 + In2(Req2)
IS THE INPUT REFERRED SPOT NOISE IN A 1Hz BANDWIDTH.
Figure 1
Studying the formula and the plots leads to several conclu-
sions. The values of the resistors used should be as small as
possible to minimize noise, but since the feedback resistor
is a load on the output of the op amp, it must not be too small.
For a small equivalent source resistance, the voltage noise
dominates. As the resistance increases, the resistor noise
becomes most important. When the source resistance is
greater than 100k, the current noise dominates because the
contribution of the current noise is proportional to R
eq
,
whereas the resistor noise is proportional to the R
eq
.
For low frequency applications and a source resistance
greater than 100k, the LT1169 JFET input op amp is the
obvious choice. Not only does the LT1169 have an ex-
tremely low current noise of 0.8fA/Hz , it also has a very
low voltage noise of 6nV/Hz. The LT1169 also has excel-
lent DC specifications, with a very low input bias current of
3pA (typical), which is maintained over the input common
mode range, and a high gain of 120dB.
+
I
n
V
n
V
TR2
R2
V
TR3
R3
V
TR1
DN140 F01
R1
LINEAR TECHNOLOGY CORPORATION 1996
LT/GP 1096 155K • PRINTED IN THE USA
Linear Technology Corporation
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900
FAX
: (408) 434-0507
TELEX
: 499-3977
For literature on our Operational Amplifiers,
call 1-800-4-LINEAR. For applications help,
call (408) 432-1900, Ext. 2593
Table 1. Best Op Amp for Lowest Noise vs Source Resistance
BEST OP AMP
SOURCE R (R
eq
) 10Hz PRECISION 1000Hz PRECISION 10kHz HIGH SPEED
0 to 500LT1028, LT1115, LT1128 LT1028, LT1115, LT1128 LT1220/21/22/24/25/26
500 to 1.5k LT1007, LT1037 LT1028, LT1115, LT1128 LT1220/21/22/24/25/26
1.5k to 3k LT1124/25/26/27 LT1028, LT1115, LT1128 LT1220/21/22/24/25/26
3k to 5k LT1124/25/26/27 LT1007, LT1037 LT1220/21/22/24/25/26
5k to 10k LT1124/25/26/27 LT1124/25/26/27 LT1354/57/60/63
10k to 20k LT1001/02 LT1113, LT1124/25/26/27 LT1354/57/60/63
20k to 100k LT1001/02 LT1055/56/57/58, LT1113, LT1169 LT1351
100k to 1M LT1022, LT1055/56/57/58, LT1022, LT1055/56/57/58, LT1113 LT1351
LT1113, LT1122, LT1169 LT1122, LT1169, LT1457
1M to 10M LT1022, LT1055/56/57/58, LT1022, LT1055/56/57/58, LT1113
LT1113, LT1122, LT1169 LT1122, LT1169, LT1457
High speed op amps, here defined by slew rates greater than
100V/µs, are plotted in Figure 4. These op amps come in a
wider range of speeds than the precision op amps plotted in
Figures 2 and 3. The faster parts will generally have slightly
more spot noise, but because they will most likely be
selected on the basis of speed, a selection of parts is plotted.
For example, the LT1354–LT1363 (these are single op
amps; duals and quads are available) are close in noise
performance and consequently cluster close together on the
plot, but have a speed range of 12MHz GBW to 70MHz GBW.
The same information is presented in tabular form in
Table 1.
EQUIVALENT SOURCE RESISTANCE ()
1
3
30
300
SPOT NOISE (nV/Hz)
100
1000
10 100k 10M
DN140 F03
0.3 1k 10k 1M100
10
LT1028
LT1128 LT1124
LT1169
RESISTOR NOISE ONLY
LT1007
LT1037
EQUIVALENT SOURCE RESISTANCE ()
1
3
30
300
SPOT NOISE (nV/Hz)
100
1000
10 100k 10M
DN140 F02
0.3 1k 10k 1M100
10
LT1028
LT1128 LT1001
LT1124
LT1169
LT1007
LT1037
RESISTOR NOISE ONLY
Figure 4. 10kHz Spot Noise vs Equivalent Source Resistance
(High Speed Amplifiers)
EQUIVALENT SOURCE RESISTANCE ()
1
3
30
300
SPOT NOISE (nV/Hz)
100
1000
10 100k 1M
DN140 F04
0.3 1k 10k100
10
LT1351
RESISTOR NOISE ONLY
LT1220
LT1221
LT1222
LT1224
LT1225
LT1226
LT1334
LT1357
LT1360
LT1363
Figure 3. 1kHz Spot Noise vs Equivalent Source Resistance
Figure 2. 10Hz Spot Noise vs Equivalent Source Resistance