LMV751
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SNOS468E – AUGUST 1999 – REVISED MARCH 2013
LMV751 Low Noise, Low Vos, Single Op Amp
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FEATURES
DESCRIPTION
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The LMV751 is a high performance CMOS
operational amplifier intended for applications
requiring low noise and low input offset voltage. It
offers modest bandwidth of 4.5MHz for very low
supply current and is unity gain stable.
1
2
Low Noise 6.5nV/√Hz
Low VOS (0.05mV typ.)
Wideband 4.5MHz GBP typ.
Low Supply Current 500uA typ.
Low Supply Voltage 2.7V to 5.0V
Ground-Referenced Inputs
Unity Gain Stable
Small Package
APPLICATIONS
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Cellular Phones
Portable Equipment
Radio Systems
The output stage is able to drive high capacitance, up
to 1000pF and source or sink 8mA output current.
It is supplied in the space saving SOT-23-5 Tiny
package.
The LMV751 is designed to meet the demands of
small size, low power, and high performance required
by cellular phones and similar battery operated
portable electronics.
Connection Diagram
Figure 1. SOT-23-5 Top View
Figure 2. Voltage Noise
Figure 3. Gain/Phase
1
2
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of
Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.
All trademarks are the property of their respective owners.
PRODUCTION DATA information is current as of publication date.
Products conform to specifications per the terms of the Texas
Instruments standard warranty. Production processing does not
necessarily include testing of all parameters.
Copyright © 1999–2013, Texas Instruments Incorporated
LMV751
SNOS468E – AUGUST 1999 – REVISED MARCH 2013
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These devices have limited built-in ESD protection. The leads should be shorted together or the device placed in conductive foam
during storage or handling to prevent electrostatic damage to the MOS gates.
Absolute Maximum Ratings
ESD Tolerance
(1) (2)
(3)
Human Body Model
2000V
Machine Model
200V
Differential Input Voltage
±Supply Voltage
Supply Voltage (V+ - V−)
5.5V
Lead Temperature (Soldering, 10 sec.)
260°C
−65°C to 150°C
Storage Temperature Range
Junction Temperature (TJ)
(1)
(4)
150°C
Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Electrical specifications do not apply when
operating the device beyond its rated operating conditions.
If Military/Aerospace specified devices are required, please contact the Texas Instruments Sales Office/ Distributors for availability and
specifications.
Human body model, 1.5kΩ in series with 100pF. Machine model, 200Ω in series with 1000pF.
The maximum power dissipation is a function of TJ(MAX), θJA, and TA. The maximum allowable power dissipation at any ambient
temperature is PD = (TJ(MAX) - TA)/θJA. All numbers apply for packages soldered directly into a PC board.
(2)
(3)
(4)
Recommended Operating Conditions
Supply Voltage
2.7V to 5.0V
−40°C ≤ TJ ≤ 85°C
Temperature Range
Thermal Resistance (θJA)
(1)
DBV-5 Package, SOT-23-5
(1)
274°C/W
All numbers are typical, and apply to packages soldered directly onto PC board in still air.
2.7V Electrical Characteristics
V+ = 2.7V, V− = 0V, VCM = 1.35V, TA = 25°C unless otherwise stated. Boldface limits apply over the Temperature Range.
Symbol
Parameter
VOS
Input Offset Voltage
VCM
Input common-Mode Voltage Range
Condition
Typ
Limit
(2)
Units
0.05
1.0
1.5
mV
max
0
V
min
1.4
1.3
V
max
(1)
For CMRR ≥ 50dB
CMRR
Common Mode Rejection Ratio
0V < VCM < 1.3V
100
85
70
dB
min
PSRR
Power Supply Rejection Ratio
V+ = 2.7V to 5.0V
107
85
70
dB
min
IS
Supply Current
0.5
0.8
0.85
mA
max
IIN
Input Current
1.5
100
pA
max
IOS
Input Offset Current
AVOL
Voltage Gain
(1)
(2)
2
0.2
pA
RL = 10k Connect to V+/2
VO = 0.2V to 2.2V
120
110
95
RL = 2k Connect to V+/2
VO = 0.2V to 2.2V
120
100
85
dB
min
Typical values represent the most likely parametric norm.
All limits are ensured by testing or statistical analysis
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2.7V Electrical Characteristics (continued)
V+ = 2.7V, V− = 0V, VCM = 1.35V, TA = 25°C unless otherwise stated. Boldface limits apply over the Temperature Range.
Symbol
VO
Positive Voltage Swing
VO
Negative Voltage Swing
IO
Typ
Limit
RL = 10k Connect to V+/2
2.62
2.54
2.52
RL = 2k Connect to V+/2
2.62
2.54
2.52
RL = 10k Connect to V+/2
78
140
160
RL = 2k Connect to V+/2
78
160
180
Sourcing, VO = 0V
VIN (diff) = ±0.5V
12
6.0
1.5
Sinking, VO = 2.7V
VIN (diff) = ±0.5V
11
6.0
1.5
Parameter
Output Current
Condition
(1)
(2)
Units
V
min
mV
max
mA
min
en (10Hz)
Input Referred Voltage Noise
15.5
nV/√Hz
en (1kHz)
Input Referred Voltage Noise
7
nV/√Hz
en (30kHz)
Input Referred Voltage Noise
7
IN(1kHz)
Input Referred Current Noise
0.01
GBW
Gain-Bandwidth Product
4.5
SR
Slew Rate
10
nV/√Hz max
pA/√Hz
2
2
MHZ
min
V/µs
5.0V Electrical Characteristics
V+ = 5.0V, V− = 0V, VCM = 2.5V, TA = 25°C unless otherwise stated.Boldface limits apply over the Temperature Range.
Symbol
Parameter
Typ
Limit
(2)
Units
0.05
1.0
1.5
mV
max
103
85
70
dB
min
0
V
min
3.7
3.6
V
max
107
85
70
dB
min
(1)
VOS
Input Offset Voltage
CMRR
Common Mode Rejection Ratio
0V < VCM < 3.6V
VCM
Input Common-Mode Voltage Range
For CMRR ≥ 50dB
V+ = 2.7V to 5.0V
PSRR
Power Supply Rejection Ratio
IS
Supply Current
0.6
0.9
0.95
mA
max
IIN
Input Current
1.5
100
pA
max
IOS
Input offset Current
AVOL
Voltage Gain
VO
VO
(1)
(2)
Positive Voltage Swing
Negative Voltage Swing
0.2
pA
RL = 10k Connect to V+/2
VO = 0.2V to 4.5V
120
110
95
RL = 2k Connect to V+/2
VO = 0.2V to 4.5V
120
100
85
RL = 10k Connect to V+/2
4.89
4.82
4.80
RL = 2k Connect to V+/2
4.89
4.82
4.80
RL = 10k Connect to V+/2
86
160
180
RL = 2k Connect to V+/2
86
180
200
db
min
V
min
mV
max
Typical values represent the most likely parametric norm.
All limits are ensured by testing or statistical analysis
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5.0V Electrical Characteristics (continued)
V+ = 5.0V, V− = 0V, VCM = 2.5V, TA = 25°C unless otherwise stated.Boldface limits apply over the Temperature Range.
Symbol
IO
Typ
Limit
Sourcing, VO = 0V
VIN (diff) = ±0.5V
15
8.0
2.5
Sinking, VO = 5V
VIN (diff) = ±0.5V
20
8.0
2.5
Parameter
Output Current
(1)
en (10Hz)
Input Referred Voltage Noise
15
en (1kHz)
Input Referred Voltage Noise
6.5
en (30kHz)
Input Referred Voltage Noise
6.5
IN (1kHz)
Input Referred Current Noise
0.01
GBW
Gain-Bandwidth Product
SR
Slew Rate
4
5
2.3
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(2)
Units
mA
min
nV/ √Hz
nV/ √Hz
10
nV/ √Hz
max
pA/√Hz
2
MHz
min
V/µs
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Typical Performance Characteristics
Supply Current
vs.
Voltage
VOS
vs.
VCM, V+ = 2.7V
Figure 4.
Figure 5.
VOS
vs.
VCM, V+ = 5.0V
Source Current
vs.
Out, V+ = 2.7V
Figure 6.
Figure 7.
Source Current
vs.
VOUT, V+ = 5.0V
Gain/Phase
Figure 8.
Figure 9.
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Typical Performance Characteristics (continued)
Sinking Current
vs.
VOUT, V+ = 2.7V
Sinking Current
vs.
VOUT, V+ = 5.0V
Figure 10.
Figure 11.
VOS
vs.
V+
VIN
vs.
VOUT, V+ = 2.7V, RL = 2k
Figure 12.
Figure 13.
VIN
vs.
VOUT, V = 5.0V, RL = 2k
Input Bias
vs.
VCM, TA = 25°C
Figure 14.
Figure 15.
+
6
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Typical Performance Characteristics (continued)
Input Bias
vs.
VCM, TA = 85°C
PSRR +
Figure 16.
Figure 17.
PSRR −
Voltage Noise
Figure 18.
Figure 19.
CMRR
Figure 20.
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APPLICATION HINTS
Noise
There are many sources of noise in a system: thermal noise, shot noise, 1/f, popcorn noise, resistor noise, just to
name a few. In addition to starting with a low noise op amp, such as the LMV751, careful attention to detail will
result in the lowest overall noise for the system.
To invert or not invert?
Both inverting and non-inverting amplifiers employ feedback to stabilize the closed loop gain of the block being
designed. The loop gain (in decibels) equals the algebraic difference between the open loop and closed loop
gains. Feedback improves the Total Harmonic Distortion (THD) and the output impedance. The various noise
sources, when input referred, are amplified, not by the closed loop gain, but by the noise gain. For a noninverting amplifier, the noise gain is equal to the closed loop gain, but for an inverting amplifier, the noise gain is
equal to the closed loop gain plus one. For large gains, e.g., 100, the difference is negligible, but for small gains,
such as one, the noise gain for the inverting amplifier would be two. This implies that non-inverting blocks are
preferred at low gains.
Source impedance
Because noise sources are uncorrelated, the system noise is calculated by taking the RMS sum of the various
noise sources, that is, the square root of the sum of the squares. At very low source impedances, the voltage
noise will dominate; at very high source impedances, the input noise current times the equivalent external
resistance will dominate. For a detailed example calculation, refer to Note 1.
Bias current compensation resistor
In CMOS input op amps, the input bias currents are very low, so there is no need to use RCOMP (see Figure 21
and Figure 22) for bias current compensation that would normally be used with early generation bipolar op amps.
In fact, inclusion of the resistor would act as another thermal noise source in the system, increasing the overall
noise.
Figure 21. Bias Current Compensation Resistor
Figure 22. Bias Current Compensation Resistor
Resistor types
Thermal noise is generated by any passive resistive element. This noise is "white"; meaning it has a constant
spectral density. Thermal noise can be represented by a mean-square voltage generator eR2 in series with a
noiseless resistor, where eR2 is given by: Where:
eR2 = 4K TRB (volts)2
where
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T = temperature in °K
R = resistor value in ohms
B = noise bandwidth in Hz
K = Boltzmann's constant (1.38 x 10-23 W-sec/°K)
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(1)
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Actual resistor noise measurements may have more noise than the calculated value. This additional noise
component is known as excess noise. Excess noise has a 1/f spectral response, and is proportional to the
voltage drop across the resistor. It is convenient to define a noise index when referring to excess noise in
resistors. The noise index is the RMS value in uV of noise in the resistor per volt of DC drop across the resistor
in a decade of frequency. Noise index expressed in dB is:
NI = 20 log ((EEX/VDC) x 106) db
where
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EEX = resistor excess noise in uV per frequency decade
VDC = DC voltage drop across the resistor
(2)
Excess noise in carbon composition resistors corresponds to a large noise index of +10 dB to -20 dB. Carbon
film resistors have a noise index of -10 dB to -25 dB. Metal film and wire wound resistors show the least amount
of excess noise, with a noise index figure of -15 dB to -40 dB.
Other noise sources:
As the op amp and resistor noise sources are decreased, other noise contributors will now be noticeable. Small
air currents across thermocouples will result in low frequency variations. Any two dissimilar metals, such as the
lead on the IC and the solder and copper foil of the pc board, will form a thermocouple. The source itself may
also generate noise. An example would be a resistive bridge. All resistive sources generate thermal noise based
on the same equation listed above under "resistor types". (2)
Putting it all together
To a first approximation, the total input referred noise of an op amp is:
Et2 = en2 + ereq2 + (in*Req)2
where
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Req is the equivalent source resistance at the inputs
(3)
At low impedances, voltage noise dominates. At high impedances, current noise dominates. With a typical noise
current on most CMOS input op amps of 0.01 pA/√Hz, the current noise contribution will be smaller than the
voltage noise for Req less than one megohm.
Other Considerations
Comparator operation
Occasionally operational amplifiers are used as comparators. This is not optimum for the LMV751 for several
reasons. First, the LMV751 is compensated for unity gain stability, so the speed will be less than could be
obtained on the same process with a circuit specifically designed for comparator operation. Second, op amp
output stages are designed to be linear, and will not necessarily meet the logic levels required under all
conditions. Lastly, the LMV751 has the newer PNP-NPN common emitter output stage, characteristic of many
rail-to-rail output op amps. This means that when used in open loop applications, such as comparators, with very
light loads, the output PNP will saturate, with the output current being diverted into the previous stage. As a
result, the supply current will increase to the 20-30 mA. range. When used as a comparator, a resistive load
between 2kΩ and 10kΩ should be used with a small amount of hysteresis to alleviate this problem. When used
as an op amp, the closed loop gain will drive the inverting input to within a few millivolts of the non-inverting
input. This will automatically reduce the output drive as the output settles to the correct value; thus it is only when
used as a comparator that the current will increase to the tens of milliampere range.
Rail-to-Rail
Because of the output stage discussed above, the LMV751 will swing “rail-to-rail” on the output. This normally
means within a few hundred millivolts of each rail with a reasonable load. Referring to the Electrical
Characteristics table for 2.7V to 5.0V, it can be seen that this is true for resistive loads of 2kΩ and 10kΩ. The
input stage consists of cascoded P-channel MOSFETS, so the input common mode range includes ground, but
typically requires 1.2V to 1.3V headroom from the positive rail. This is better than the industry standard LM324
and LM358 that have PNP input stages, and the LMV751 has the advantage of much lower input bias currents.
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Loading
The LMV751 is a low noise, high speed op amp with excellent phase margin and stability. Capacitive loads up to
1000 pF can be handled, but larger capacitive loads should be isolated from the output. The most straightforward
way to do this is to put a resistor in series with the output. This resistor will also prevent excess power dissipation
if the output is accidentally shorted.
General Circuits
With the low noise and low input bias current, the LMV751 would be useful in active filters, integrators, current to
voltage converters, low frequency sine wave generators, and instrumentation amplifiers. (3)
NOTE
1. Sherwin, Jim “Noise Specs Confusing?” AN-104 (SNVA515), Texas Instruments.
2. Christensen, John, “Noise-figure curve ease the selection of low-noise op amps”, EDN, pp 8184, Aug. 4, 1994.
3. “Op Amp Circuit Collection”, AN-31 (SNLA140), Texas Instruments.
10
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SNOS468E – AUGUST 1999 – REVISED MARCH 2013
REVISION HISTORY
Changes from Revision D (March 2013) to Revision E
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Page
Changed layout of National Data Sheet to TI format .......................................................................................................... 10
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PACKAGE OPTION ADDENDUM
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30-Sep-2021
PACKAGING INFORMATION
Orderable Device
Status
(1)
Package Type Package Pins Package
Drawing
Qty
Eco Plan
(2)
Lead finish/
Ball material
MSL Peak Temp
Op Temp (°C)
Device Marking
(3)
(4/5)
(6)
LMV751M5
NRND
SOT-23
DBV
5
1000
Non-RoHS
& Green
Call TI
Level-1-260C-UNLIM
-40 to 85
A32A
LMV751M5/NOPB
ACTIVE
SOT-23
DBV
5
1000
RoHS & Green
SN
Level-1-260C-UNLIM
-40 to 85
A32A
LMV751M5X/NOPB
ACTIVE
SOT-23
DBV
5
3000
RoHS & Green
SN
Level-1-260C-UNLIM
-40 to 85
A32A
(1)
The marketing status values are defined as follows:
ACTIVE: Product device recommended for new designs.
LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect.
NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part in a new design.
PREVIEW: Device has been announced but is not in production. Samples may or may not be available.
OBSOLETE: TI has discontinued the production of the device.
(2)
RoHS: TI defines "RoHS" to mean semiconductor products that are compliant with the current EU RoHS requirements for all 10 RoHS substances, including the requirement that RoHS substance
do not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, "RoHS" products are suitable for use in specified lead-free processes. TI may
reference these types of products as "Pb-Free".
RoHS Exempt: TI defines "RoHS Exempt" to mean products that contain lead but are compliant with EU RoHS pursuant to a specific EU RoHS exemption.
Green: TI defines "Green" to mean the content of Chlorine (Cl) and Bromine (Br) based flame retardants meet JS709B low halogen requirements of