INTERSIL LMP2015

LMP2015 Single/LMP2016 Dual
High Precision, Rail-to-Rail Output Operational Amplifier
General Description
Features
The LMP2015/LMP2016 are the first members of National's
new LMPTM precision amplifier family. The LMP2015/
LMP2016 offer unprecedented accuracy and stability in
space-saving miniature packaging at an affordable price.
These devices utilize patented techniques to measure and
continually correct the input offset error voltage. The result is
a series of amplifiers which are ultra stable over time and
temperature. They have excellent CMRR and PSRR ratings,
and do not exhibit the familiar 1/f voltage and current noise
increase that plagues traditional amplifiers. The combination
of characteristics makes the LMP2015/LMP2016 good choices for transducer amplifiers, high gain configurations, ADC
buffer amplifiers, DAC I-V conversion, or any other 2.7V-5V
application requiring precision and long term stability.
Other useful benefits of the LMP2015/LMP2016 are rail-to-rail
output, a low supply current of 930 µA, and a wide gain bandwidth product of 3 MHz. These extremely versatile features
provide high performance and ease of use.
(For VS = 5V, Typical unless otherwise noted)
■ Low guaranteed VOS over temperature
■ Low noise with no 1/f
■ High CMRR
■ High PSRR
■ High AVOL
■ Wide gain bandwidth product
■ High slew rate
■ Low supply current
■ Rail-to-Rail output
■ No external capacitors required
10 µV
35 nV/√Hz
130 dB
120 dB
130 dB
3 MHz
4 V/µs
930 µA
30 mV
Applications
■
■
■
■
Precision instrumentation amplifiers
Thermocouple amplifiers
Strain gauge bridge amplifier
ADC driver
Connection Diagrams
5-Pin SOT23
8-Pin SOIC
8-Pin MSOP
20212538
20212502
Top View
Top View
20212542
Top View
Ordering Information
Package
5-Pin SOT23
Part Number
Temperature
Range
LMP2015MF
AD5A
LMP2015MFX
LMP2015MA
8-Pin SOIC
LMP2015MAX
LMP2016MA
LMP2015MA
−40°C to 125°C
LMP2016MA
LMP2016MAX
8-Pin MSOP
LMP2016MM
AE5A
LMP2016MMX
© 2007 National Semiconductor Corporation
Package Marking
202125
Transport Media
1k Units Tape and Reel
3k Units Tape and Reel
NSC Drawing
MF05A
95 Units/Rail
2.5k Units Tape and Reel
95 Units/Rail
M08A
2.5k Units Tape and Reel
1k Units Tape and Reel
3.5k Units Tape and Reel
MUA08A
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LMP2015 Single/LMP2016 Dual High Precision, Rail-to-Rail Output Operational Amplifier
December 18, 2007
LMP2015 Single/LMP2016 Dual
Differential Input Voltage
Current at Input Pin
Current at Output Pin
Current at Power Supply Pin
Absolute Maximum Ratings (Note 1)
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
ESD Tolerance (Note 2)
Human Body Model
Machine Model
Supply Voltage
Common Mode Input Voltage
−0.3 ≤ VCM ≤ VCC +0.3V
Lead Temperature (soldering
10 sec.)
+300°C
±Supply Voltage
30 mA
30 mA
50 mA
Operating Ratings
2000V
200V
5.8V
(Note 1)
Supply Voltage
Storage Temperature Range
Temperature Range (Note 3)
2.7V to 5.25V
−65°C to 150°C
−40°C to 125°C
2.7V DC Electrical Characteristics
Unless otherwise specified, all limits guaranteed for TA = 25°C,
V+ = 2.7V, V− = 0V, V CM = 1.35V, VO = 1.35V and RL > 1 MΩ. Boldface limits apply at the temperature extremes.
Symbol
Typ
(Note 4)
Max
(Note 5)
Input Offset Voltage
(LMP2015 only)
0.8
5
10
Input Offset Voltage
(LMP2016 only)
0.8
5
10
Offset Calibration Time
0.5
10
12
ms
Input Offset Voltage
0.015
.05
μV/°C
Long Term Offset Drift
0.006
μV/month
Lifetime VOS Drift
2.5
μV
IIN
Input Current
-3
pA
IOS
Input Offset Current
6
pA
RIND
Input Differential Resistance
9
MΩ
CMRR
Common Mode Rejection Ratio
VOS
TCVOS
Parameter
Conditions
−0.3 ≤ VCM ≤ 0.9V
95
90
0 ≤ VCM ≤ 0.9V
CMVR
Input Common Mode Range
Min
(Note 5)
130
−0.3
0.9
CMRR ≥ 90 dB
0
0.9
95
90
120
2.665
2.655
2.68
Power Supply Rejection Ratio
V+ – V− = 2.7V to 5V, VCM = 0V
VO
Output Swing
(LMP2015 only)
RL = 10 kΩ to 1.35V
VIN(diff) = ±0.5V
0.033
2.630
2.615
RL = 2 kΩ to 1.35V
VIN(diff) = ±0.5V
RL = 10 kΩ to 1.35V
VIN(diff) = ±0.5V
2.64
2.63
2.615
2.6
2
0.060
0.075
V
0.085
0.105
V
0.060
0.075
V
2.65
0.061
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dB
2.68
0.033
RL = 2 kΩ to 1.35V
VIN(diff) = ±0.5V
dB
2.65
0.061
Output Swing
(LMP2016 only)
μV
dB
CMRR ≥ 95 dB
PSRR
Units
0.085
0.105
V
AVOL
IO
Parameter
Open Loop Voltage Gain
Output Current
IS
Conditions
Min
(Note 5)
Typ
(Note 4)
RL = 10 kΩ
95
90
130
RL = 2 kΩ
90
85
124
Sourcing, VO = 0V
VIN(diff) = ±0.5V
5
3
12
Sinking, VO = 5V
VIN(diff) = ±0.5V
5
3
18
Supply Current per Channel
0.919
Max
(Note 5)
Units
dB
mA
1.20
1.50
mA
2.7V AC Electrical Characteristics
TA = 25°C, V+ = 2.7V, V− = 0V, VCM = 1.35V, VO = 1.35V, and
RL > 1 MΩ. Boldface limits apply at the temperature extremes.
Symbol
Parameter
Conditions
Min
(Note 5)
Typ
(Note 4)
Max
(Note 5)
Units
GBWP
Gain Bandwidth Product
3
MHz
SR
Slew Rate
4
V/μs
θm
Phase Margin
60
Deg
Gm
Gain Margin
−14
dB
en
Input Referred Voltage Noise
35
in
Input Referred Current Noise
enp-p
Input Referred Voltage Noise
trec
Input Overload Recovery Time
nV/
pA/
RS = 100Ω, DC to 10 Hz
850
nVPP
50
ms
5V DC Electrical Characteristics
Unless otherwise specified, all limits guaranteed for TA = 25°C, V+ = 5V,
V− = 0V, V CM = 2.5V, VO = 2.5V and RL > 1 MΩ. Boldface limits apply at the temperature extremes.
Symbol
VOS
TCVOS
Parameter
Conditions
Min
(Note 5)
Typ
(Note 4)
Max
(Note 5)
Input Offset Voltage
(LMP2015 only)
0.12
5
10
Input Offset Voltage
(LMP2016 only)
0.12
5
10
Offset Calibration Time
0.5
10
12
Input Offset Voltage
0.015
.05
Long Term Offset Drift
0.006
Units
μV
ms
μV/°C
μV/month
Lifetime VOS Drift
2.5
μV
IIN
Input Current
−3
pA
IOS
Input Offset Current
6
pA
RIND
Input Differential Resistance
9
MΩ
CMRR
Common Mode Rejection Ratio
−0.3 ≤ VCM ≤ 3.2
100
90
CMRR ≥ 100 dB
−0.3
3.2
CMRR ≥ 90 dB
0
3.2
V+ – V− = 2.7V to 5V, VCM = 0V
95
90
0 ≤ VCM ≤ 3.2
CMVR
PSRR
Input Common Mode Range
Power Supply Rejection Ratio
3
130
120
dB
dB
dB
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LMP2015 Single/LMP2016 Dual
Symbol
LMP2015 Single/LMP2016 Dual
Symbol
VO
Parameter
Output Swing
(LMP2015 only)
Conditions
RL = 10 kΩ to 2.5V
VIN(diff) = ±0.5V
Min
(Note 5)
Typ
(Note 4)
4.96
4.95
4.978
0.040
4.895
4.875
RL = 2 kΩ to 2.5V
VIN(diff) = ±0.5V
4.92
4.91
RL = 10 kΩ to 2.5V
VIN(diff) = ±0.5V
4.875
4.855
IO
Open Loop Voltage Gain
Output Current
IS
RL = 10 kΩ
105
100
130
RL = 2 kΩ
95
90
132
Sourcing, VO = 0V
VIN(diff) = ±0.5V
8
6
15
Sinking, VO = 5V
V IN(diff) = ±0.5V
8
6
17
Supply Current per Channel
0.930
5V AC Electrical Characteristics
0.115
0.140
V
0.080
0.095
V
4.919
0.0.91
AVOL
V
4.978
0.040
RL = 2 kΩ to 2.5V
VIN(diff) = ±0.5V
0.070
0.085
Units
4.919
0.091
Output Swing
(LMP2016 only)
Max
(Note 5)
0.125
0.150
V
dB
mA
1.20
1.50
mA
TA = 25°C, V+ = 5V, V− = 0V, VCM = 2.5V, VO = 2.5V, and RL > 1 MΩ.
Boldface limits apply at the temperature extremes.
Symbol
Parameter
Conditions
Min
(Note 5)
Typ
(Note 4)
Max
(Note 5)
Units
GBW
Gain-Bandwidth Product
3
MHz
SR
Slew Rate
4
V/μs
θm
Phase Margin
60
deg
Gm
Gain Margin
−15
dB
en
Input-Referred Voltage Noise
35
in
Input-Referred Current Noise
enp-p
Input-Referred Voltage Noise
trec
Input Overload Recovery Time
nV/
pA/
RS = 100Ω, DC to 10 Hz
850
nVPP
50
ms
Note 1: Absolute Maximum Ratings indicate limits beyond which damage may occur. Operating Ratings indicate conditions for which the device is intended to
be functional, but specific performance is not guaranteed. For guaranteed specifications and test conditions, see the Electrical Characteristics.
Note 2: Human Body Model, applicable std. MIL-STD-883, Method 3015.7. Machine Model, applicable std. JESD22-A115-A (ESD MM std. of JEDEC)
Field-Induced Charge-Device Model, applicable std. JESD22-C101-C (ESD FICDM std. of JEDEC).
Note 3: The maximum power dissipation is a function of TJ(MAX), θJA. The maximum allowable power dissipation at any ambient temperature is PD = (TJ(MAX) –
TA)/ θJA. All numbers apply for packages soldered directly onto a PC Board.
Note 4: Typical values represent the most likely parametric norm as determined at the time of characterization. Actual typical values may vary over time and will
also depend on the application and configuration. The typical values are not tested and are not guaranteed on shipped production material.
Note 5: Limits are 100% production tested at 25°C. Limits over the operating temperature range are guaranteed through correlations using statistical quality
control (SQC) method.
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4
LMP2015 Single/LMP2016 Dual
Typical Performance Characteristics
TA = 25°C, VS = 5V unless otherwise specified.
Supply Current vs. Supply Voltage
Offset Voltage vs. Supply Voltage
20212523
20212555
Offset Voltage vs. Common Mode Voltage (VS = +5V)
Offset Voltage vs. Common Mode Voltage (VS = +2.7V)
20212525
20212524
Voltage Noise vs. Frequency
Input Bias Current vs. Common Mode
20212503
20212504
5
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LMP2015 Single/LMP2016 Dual
PSRR vs. Frequency
PSRR vs. Frequency
20212507
20212506
Output Sourcing @ 2.7V
Output Sourcing @ 5V
20212559
20212560
Output Sinking @ 2.7V
Output Sinking @ 5V
20212561
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20212562
6
Maximum Output Swing vs. Supply Voltage
20212563
20212564
Minimum Output Swing vs. Supply Voltage
Minimum Output Swing vs. Supply Voltage
20212565
20212566
CMRR vs. Frequency
Open Loop Gain and Phase vs. Supply Voltage
20212508
20212505
7
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LMP2015 Single/LMP2016 Dual
Maximum Output Swing vs. Supply Voltage
LMP2015 Single/LMP2016 Dual
Open Loop Gain and Phase vs. Resistive Load @ 2.7V
Open Loop Gain and Phase vs. Resistive Load @ 5V
20212509
20212510
Open Loop Gain and Phase vs. Capacitive Load @ 2.7V
Open Loop Gain and Phase vs. Capacitive Load @ 5V
20212512
20212511
Open Loop Gain and Phase vs. Temperature @ 2.7V
Open Loop Gain and Phase vs. Temperature @ 5V
20212536
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20212537
8
LMP2015 Single/LMP2016 Dual
THD+N vs. Amplitude
THD+N vs. Frequency
20212514
20212513
0.1 Hz − 10 Hz Noise vs. Time
20212515
9
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LMP2015 Single/LMP2016 Dual
Application Information
THE BENEFITS OF THE LMP2015/LMP2016's
NO 1/f NOISE
Using patented methods, the LMP2015/LMP2016 eliminate
the 1/f noise present in other amplifiers. That noise, which
increases as frequency decreases, is a major source of measurement 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 10 nV/
and a noise corner of 10 Hz, the RMS noise at 0.001 Hz is 1
. This is equivalent to a 0.50 µV peak-to-peak error, in
µV/
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 LMP2015/LMP2016 will have only 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 frequencies. 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 LMP2015/LMP2016 eliminate 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 thermocouple
noise that is equal to the LMP2015/LMP2016 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 LMP2015/LMP2016 is
made of copper. This results in equal and opposite junctions
which cancel this effect. The extremely small size of the
SOT23 package results in the leads being very close together. This further reduces the probability of temperature differences and hence decreases thermal noise.
20212516
FIGURE 1. Overload Recovery Test
The wide bandwidth of the LMP2015/LMP2016 enhance performance when it is used as an amplifier to drive loads that
inject transients back into the output. ADCs (Analog-to-Digital
Converters) 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 860 ns. This rapid recovery is due to
the wide bandwidth of the output stage and large total GBWP.
NO EXTERNAL CAPACITORS REQUIRED
The LMP2015/LMP2016 do not need external capacitors.
This eliminates the problems caused by capacitor leakage
and dielectric absorption, which can cause delays of several
seconds from turn-on until the amplifier's error has settled.
MORE BENEFITS
The LMP2015/LMP2016 offer the benefits mentioned above
and more. These parts have rail-to-rail outputs and consume
only 950 µA of supply current while providing excellent DC
and AC electrical performance. In DC performance, the
LMP2015/LMP2016 achieve 130 dB of CMRR, 120 dB of
PSRR and 130 dB of open loop gain. In AC performance, the
LMP2015/LMP2016 provide 3 MHz of gain bandwidth product
and 4 V/µs of slew rate.
HOW THE LMP2015/LMP2016 WORK
The LMP2015/LMP2016 use new, patented techniques to
achieve the high DC accuracy traditionally associated with
chopper-stabilized amplifiers without the major drawbacks
produced by chopping. The LMP2015/LMP2016 continuously
monitor the input offset and correct this error. The conventional chopping process produces many mixing products,
both sums and differences, between the chopping frequency
and the incoming signal frequency. This mixing causes a
large amount 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. To explain this Figure 2 shows
a plot, 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 LMP2015/LMP2016.
This data was taken under the exact same conditions. The
auto-zero action is visible at about 30 kHz but note the absence of mixing products at other frequencies. As a result, the
LMP2015/LMP2016 have very low distortion of 0.02% and
very low mixing products.
OVERLOAD RECOVERY
The LMP2015/LMP2016 recover from input overload much
faster than most chopper-stabilized op amps. Recovery from
driving 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.
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10
20212517
FIGURE 2. The Output of a Chopper Stabilized Op Amp
(MAX432)
20212518
FIGURE 4. Precision Strain Gauge Amplifier
Extending Supply Voltages and Output Swing by Using a
Composite Amplifier Configuration
In cases where substantially higher output swing is required
with higher supply voltages, arrangements such as those
shown in Figure 5 and Figure 6 can be used. These configurations utilize the excellent DC performance of the LMP2015
while allowing the superior voltage and frequency capabilities
of the LM6171 to set the dynamic performance of the overall
amplifier. For example, it is possible to achieve ±12V output
swing with 300 MHz of overall GBW (AV = 100) while keeping
the worst case output shift due to VOS less than 4 mV. The
LMP2015 output voltage is kept at about mid-point of its overall supply voltage, and its input common mode voltage range
allows the V− terminal to be grounded in one case (Figure 5,
inverting operation) and tied to a small non-critical negative
bias in another (Figure 6, non-inverting operation). Higher
closed loop gains are also possible with a corresponding reduction in realizable bandwidth. Table 1 shows some other
closed loop gain possibilities along with the measured performance in each case.
20212504
FIGURE 3. The Output of the LMP2015/LMP2016
INPUT CURRENTS
The LMP2015/LMP2016 input currents are different than
standard bipolar or CMOS input currents in that it appears as
a current flowing in one input and out the other. Under most
operating conditions, these currents are in the picoamp level
and will have little or no effect in most circuits. These currents
tend to increase slightly when the common-mode voltage is
near the minus supply. (See the typical curves.) At high temperatures such as 85°C, the input currents become larger,
0.5 nA typical, and are both positive except when the VCM is
near V−. If operation is expected at low common-mode voltages and high temperature, do not add resistance in series
with the inputs to balance the impedances. Doing this can
cause an increase in offset voltage. A small resistance such
as 1 kΩ can provide some protection against very large transients or overloads, and will not increase the offset significantly.
11
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LMP2015 Single/LMP2016 Dual
PRECISION STRAIN GAUGE AMPLIFIER
This strain gauge amplifier (Figure 4) provides high gain
(1006 or ~60 dB) with very low offset and drift. Using the resistors' tolerances as shown, the worst case CMRR will be
greater than 108 dB. The CMRR is directly related to the resistor mismatch. The rejection of common-mode error, at the
output, is independent of the differential gain, which is set by
R3. The CMRR is further improved, if the resistor ratio matching is improved, by specifying tighter-tolerance resistors, or
by trimming.
LMP2015 Single/LMP2016 Dual
It should be kept in mind that in order to minimize the output
noise voltage for a given closed loop gain setting, one could
minimize the overall bandwidth. As can be seen from Equation 1, the output noise has a square root relationship to the
bandwidth.
In the case of the inverting configuration, it is also possible to
increase the input impedance of the overall amplifier by raising the value of R1. This can be done without having to
increase the feedback resistor, R2, to impractical values, by
utilizing a "Tee" network as feedback. See the LMC6442
datasheet (Application Information section) for more details
on this.
20212519
FIGURE 5. Composite Amplifier Configuration
TABLE 1. Composite Amplifier Measured Performance
20212521
AV
R1
Ω
R2
Ω
C2
pF
BW
MHz
SR
(V/μs)
en p-p
(mVPP)
FIGURE 7. AC Coupled ADC Driver
50
200
10k
8
3.3
178
37
100
100
10k
10
2.5
174
70
100
1k
100k
0.67
3.1
170
70
500
200
100k
1.75
1.4
96
250
1000
100
100k
2.2
0.98
64
400
LMP2015 AS AN ADC DRIVER
The LMP2015 is a great choice for an amplifier stage immediately before the input of an ADC (Analog-to-Digital Converter) as an ADC driver, whether AC or DC coupled. See
Figure 7 and Figure 8. This is because of the following important characteristics:
A) Very low offset voltage and offset voltage drift over time
and temperature allow a high closed loop gain setting
without introducing any short term or long term errors. For
example, when set to a closed loop gain of 100 as the
analog input amplifier for a 12-bit A/D converter, the overall conversion error over full operation temperature and
30 year life of the part (operating at 50°C) would be less
than 5 LSBs.
B) Fast large signal settling time to 0.01% of final value
(1.4 μs) allows 12-bit accuracy at a sampling rate of 100
kHz or more.
C) No flicker (1/f) noise means unsurpassed data accuracy
over any measurement period of time, no matter how
long. Consider the following op amp performance, based
on a typical low noise, high performance commerciallyavailable device, for comparison:
Op amp flatband noise = 8 nV/
1/f corner frequency = 100 Hz
AV = 2000
Measurement time = 100 sec
Bandwidth = 2 Hz
This example will result in about 2.2 mVPP (1.9 LSB) of
output noise contribution due to the op amp alone, compared to about 594 μVPP (less than 0.5 LSB) when that
op amp is replaced with the LMP2015 which has no 1/f
contribution. If the measurement time is increased from
100 seconds to 1 hour, the improvement realized by using
the LMP2015 would be a factor of about 4.8 times
(2.86 mVPP compared to 596 μV when LMP2015 is used).
This is mainly because the LMP2015 accuracy is not
compromised by increasing the observation time.
In terms of the measured output peak-to-peak noise, the following relationship holds between output noise voltage;
en p-p, the closed-loop gain; AV, and −3 dB bandwidth; BW:
(1)
20212520
FIGURE 6. Composite Amplifier Configuration
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12
E) Rail-to-Rail output swing maximizes the ADC dynamic
range in 5V single supply converter applications. Figure
7and Figure 8 are typical block diagrams showing the
LMP2015 used as an ADC driver.
20212522
FIGURE 8. DC Coupled ADC Driver
13
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LMP2015 Single/LMP2016 Dual
D) Copper leadframe construction minimizes any thermocouple effects which would degrade low level/high gain
data conversion application accuracy (see discussion in
"The Benefits of the LMP2015" section).
LMP2015 Single/LMP2016 Dual
Physical Dimensions inches (millimeters) unless otherwise noted
5-Pin SOT23
NS Package Number MF0A5
8-Pin SOIC
NS Package Number M08A
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LMP2015 Single/LMP2016 Dual
8-Pin MSOP
NS Package Number MUA08A
15
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LMP2015 Single/LMP2016 Dual High Precision, Rail-to-Rail Output Operational Amplifier
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