Application Information
THE BENEFITS OF LMP2014
NO 1/f NOISE
Using patented methods, the LMP2014 eliminates the 1/f
noise present in other amplifiers. That noise, which in-
creases as frequency decreases, is a major source of mea-
surement error in all DC-coupled measurements. Low-
frequency noise appears as a constantly-changing signal in
series with any measurement being made. As a result, even
when the measurement is made rapidly, this constantly-
changing noise signal will corrupt the result. The value of this
noise signal can be surprisingly large. For example: If a
conventional amplifier has a flat-band noise level of 10nV/
and a noise corner of 10 Hz, the RMS noise at 0.001
Hz is 1µV/ . This is equivalent to a 0.50 µV peak-to-
peak error, in the frequency range 0.001 Hz to 1.0 Hz. In a
circuit with a gain of 1000, this produces a 0.50 mV peak-
to-peak output error. This number of 0.001 Hz might appear
unreasonably low, but when a data acquisition system is
operating for 17 minutes, it has been on long enough to
include this error. In this same time, the LMP2014 will only
have a 0.21 mV output error. This is smaller by 2.4 x. Keep
in mind that this 1/f error gets even larger at lower frequen-
cies. At the extreme, many people try to reduce this error by
integrating or taking several samples of the same signal.
This is also doomed to failure because the 1/f nature of this
noise means that taking longer samples just moves the
measurement into lower frequencies where the noise level is
even higher.
The LMP2014 eliminates this source of error. The noise level
is constant with frequency so that reducing the bandwidth
reduces the errors caused by noise.
Another source of error that is rarely mentioned is the error
voltage caused by the inadvertent thermocouples created
when the common "Kovar type" IC package lead materials
are soldered to a copper printed circuit board. These steel-
based leadframe materials can produce over 35 µV/˚C when
soldered onto a copper trace. This can result in thermo-
couple noise that is equal to the LMP2014 noise when there
is a temperature difference of only 0.0014˚C between the
lead and the board!
For this reason, the lead-frame of the LMP2014 is made of
copper. This results in equal and opposite junctions which
cancel this effect.
OVERLOAD RECOVERY
The LMP2014 recovers from input overload much faster
than most chopper-stabilized op amps. Recovery from driv-
ing the amplifier to 2X the full scale output, only requires
about 40 ms. Many chopper-stabilized amplifiers will take
from 250 ms to several seconds to recover from this same
overload. This is because large capacitors are used to store
the unadjusted offset voltage.
The wide bandwidth of the LMP2014 enhances performance
when it is used as an amplifier to drive loads that inject
transients back into the output. ADCs (Analog-to-Digital Con-
verters) and multiplexers are examples of this type of load.
To simulate this type of load, a pulse generator producing a
1V peak square wave was connected to the output through a
10 pF capacitor. (Figure 1) The typical time for the output to
recover to 1% of the applied pulse is 80 ns. To recover to
0.1% requires 860ns. This rapid recovery is due to the wide
bandwidth of the output stage and large total GBW.
NO EXTERNAL CAPACITORS REQUIRED
The LMP2014 does not need external capacitors. This elimi-
nates the problems caused by capacitor leakage and dielec-
tric absorption, which can cause delays of several seconds
from turn-on until the amplifier’s error has settled.
MORE BENEFITS
The LMP2014 offers the benefits mentioned above and
more. It has a rail-to-rail output and consumes only 950 µA of
supply current while providing excellent DC and AC electrical
performance. In DC performance, the LMP2014 achieves
130 dB of CMRR, 120 dB of PSRR and 130 dB of open loop
gain. In AC performance, the LMP2014 provides 3 MHz of
gain-bandwidth product and 4 V/µs of slew rate.
HOW THE LMP2014 WORKS
The LMP2014 uses new, patented techniques to achieve the
high DC accuracy traditionally associated with chopper-
stabilized amplifiers without the major drawbacks produced
by chopping. The LMP2014 continuously monitors the input
offset and corrects this error. The conventional chopping
process produces many mixing products, both sums and
differences, between the chopping frequency and the incom-
ing signal frequency. This mixing causes large amounts of
distortion, particularly when the signal frequency approaches
the chopping frequency. Even without an incoming signal,
the chopper harmonics mix with each other to produce even
more trash. If this sounds unlikely or difficult to understand,
look at the plot (Figure 2), of the output of a typical (MAX432)
chopper-stabilized op amp. This is the output when there is
no incoming signal, just the amplifier in a gain of -10 with the
input grounded. The chopper is operating at about 150 Hz;
the rest is mixing products. Add an input signal and the noise
gets much worse. Compare this plot with Figure 3 of the
LMP2014. This data was taken under the exact same con-
ditions. The auto-zero action is visible at about 30 kHz but
note the absence of mixing products at other frequencies. As
a result, the LMP2014 has very low distortion of 0.02% and
very low mixing products.
20132916
FIGURE 1.
LMP2014MT
www.national.com 10