
advertisement
1096/140
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