LMR12010
VIN VIN
EN
BOOST
SW
FB
GND
VOUT
C3 L1
C1
C2
R1
R2
D1
D2
ON
OFF
LMR12010
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SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
LMR12010 SIMPLE SWITCHER
®
20Vin, 1A Step-Down Voltage Regulator in SOT-23
Check for Samples: LMR12010
1FEATURES DESCRIPTION
The LMR12010 regulator is a monolithic, high
23 Input Voltage Range of 3V to 20V frequency, PWM step-down DC/DC converter in a 6-
Output Voltage Range of 0.8V to 17V pin Thin SOT-23 package. It provides all the active
Output Current Up to 1A functions to provide local DC/DC conversion with fast
transient response and accurate regulation in the
1.6MHz (LMR12010X) and 3 MHz (LMR12010Y) smallest possible PCB area.
Switching Frequencies With a minimum of external components and online
Low Shutdown Iq, 30 nA Typical design support through WEBENCH, the LMR12010 is
Internal Soft-start easy to use. The ability to drive 1A loads with an
Internally Compensated internal 300mNMOS switch using state-of-the-art
Current-Mode PWM Operation 0.5µm BiCMOS technology results in the best power
density available. The world class control circuitry
Thermal Shutdown allows for on-times as low as 13ns, thus supporting
Thin SOT-23-6 Package (2.97 x 1.65 x 1mm) exceptionally high frequency conversion over the
Fully Enabled for WEBENCH®Power Designer entire 3V to 20V input operating range down to the
minimum output voltage of 0.8V. Switching frequency
is internally set to 1.6 MHz (LMR12010X) or 3 MHz
APPLICATIONS (LMR12010Y), allowing the use of extremely small
Point-of-Load Conversions from 3.3V, 5V, and surface mount inductors and chip capacitors. Even
12V Rails though the operating frequencies are very high,
Space Constrained Applications efficiencies up to 90% are easy to achieve. External
shutdown is included, featuring an ultra-low stand-by
Battery Powered Equipment current of 30nA. The LMR12010 utilizes current-mode
Industrial Distributed Power Applications control and internal compensation to provide high-
Power Meters performance regulation over a wide range of
operating conditions. Additional features include
Portable Hand-Held Instruments internal soft-start circuitry to reduce inrush current,
pulse-by-pulse current limit, thermal shutdown, and
PERFORMANCE BENEFITS output over-voltage protection.
Extremely Easy to Use
Tiny Overall Solution Reduces System Cost
1Please 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.
2SIMPLE SWITCHER, WEBENCH are registered trademarks of Texas Instruments.
3All other trademarks are the property of their respective owners.
PRODUCTION DATA information is current as of publication date. Copyright © 2011, Texas Instruments Incorporated
Products conform to specifications per the terms of the Texas
Instruments standard warranty. Production processing does not
necessarily include testing of all parameters.
1
2
3
6
5
4
1
2
3
6
5
4
BOOST
GND
FB
SW
VIN
EN
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
System Performance Efficiency Efficiency
vs vs
Load Current - "X" VOUT = 5V Load Current - "Y" VOUT = 5V
Connection Diagram
Figure 1. 6-Lead SOT
Package Number DDC0006A
Figure 2. Pin 1 Identification
PIN DESCRIPTIONS
Pin Name Function
1 BOOST Boost voltage that drives the internal NMOS control switch. A bootstrap
capacitor is connected between the BOOST and SW pins.
2 GND Signal and Power ground pin. Place the bottom resistor of the feedback
network as close as possible to this pin for accurate regulation.
3 FB Feedback pin. Connect FB to the external resistor divider to set output
voltage.
4 EN Enable control input. Logic high enables operation. Do not allow this pin to
float or be greater than VIN + 0.3V.
5 VIN Input supply voltage. Connect a bypass capacitor to this pin.
6 SW Output switch. Connects to the inductor, catch diode, and bootstrap
capacitor.
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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(1)(2)
VIN -0.5V to 24V
SW Voltage -0.5V to 24V
Boost Voltage -0.5V to 30V
Boost to SW Voltage -0.5V to 6.0V
FB Voltage -0.5V to 3.0V
EN Voltage -0.5V to (VIN + 0.3V)
Junction Temperature 150°C
ESD Susceptibility (3) 2kV
Storage Temp. Range -65°C to 150°C
For soldering specifications: see product folder at www.ti.com and literature number SNOA549
(1) Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for
which the device is intended to be functional, but specific performance is not ensured. For ensured specifications and the test
conditions, see Electrical Characteristics.
(2) If Military/Aerospace specified devices are required, please contact the Texas Instruments Sales Office/Distributors for availability and
specifications.
(3) Human body model, 1.5kin series with 100pF.
OPERATING RATINGS(1)
VIN 3V to 20V
SW Voltage -0.5V to 20V
Boost Voltage -0.5V to 25V
Boost to SW Voltage 1.6V to 5.5V
Junction Temperature Range 40°C to +125°C
Thermal Resistance θJA(2) 118°C/W
(1) Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for
which the device is intended to be functional, but specific performance is not ensured. For ensured specifications and the test
conditions, see Electrical Characteristics.
(2) Thermal shutdown will occur if the junction temperature exceeds 165°C. 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 onto a 3” x 3” PC board with 2oz. copper on 4 layers in still air. For a 2 layer board using 1 oz. copper in still
air, θJA = 204°C/W.
ELECTRICAL CHARACTERISTICS
Specifications with standard typeface are for TJ= 25°C, and those in boldface type apply over the full Operating
Temperature Range (TJ= -40°C to 125°C). VIN = 5V, VBOOST - VSW = 5V unless otherwise specified. Datasheet min/max
specification limits are specified by design, test, or statistical analysis. Min Typ Max
Symbol Parameter Conditions Units
(1) (2) (1)
VFB Feedback Voltage 0.784 0.800 0.816 V
ΔVFB/ΔVIN Feedback Voltage Line Regulation VIN = 3V to 20V 0.01 % / V
IFB Feedback Input Bias Current Sink/Source 10 250 nA
Undervoltage Lockout VIN Rising 2.74 2.90
UVLO Undervoltage Lockout VIN Falling 2.0 2.3 V
UVLO Hysteresis 0.30 0.44 0.62
LMR12010X 1.2 1.6 1.9
FSW Switching Frequency MHz
LMR12010Y 2.2 3.0 3.6
LMR12010X 85 92
DMAX Maximum Duty Cycle %
LMR12010Y 78 85
(1) Specified to TI’s Average Outgoing Quality Level (AOQL).
(2) Typicals represent the most likely parametric norm.
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ELECTRICAL CHARACTERISTICS (continued)
Specifications with standard typeface are for TJ= 25°C, and those in boldface type apply over the full Operating
Temperature Range (TJ= -40°C to 125°C). VIN = 5V, VBOOST - VSW = 5V unless otherwise specified. Datasheet min/max
specification limits are specified by design, test, or statistical analysis. Min Typ Max
Symbol Parameter Conditions Units
(1) (2) (1)
LMR12010X 2
DMIN Minimum Duty Cycle %
LMR12010Y 8
RDS(ON) Switch ON Resistance VBOOST - VSW = 3V 300 600 m
ICL Switch Current Limit VBOOST - VSW = 3V 1.2 1.7 2.5 A
IQQuiescent Current Switching 1.5 2.5 mA
Quiescent Current (shutdown) VEN = 0V 30 nA
LMR12010X (50% Duty Cycle) 2.5 3.5
IBOOST Boost Pin Current mA
LMR12010Y (50% Duty Cycle) 4.25 6.0
Shutdown Threshold Voltage VEN Falling 0.4
VEN_TH V
Enable Threshold Voltage VEN Rising 1.8
IEN Enable Pin Current Sink/Source 10 nA
ISW Switch Leakage 40 nA
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TYPICAL PERFORMANCE CHARACTERISTICS
All curves taken at VIN = 5V, VBOOST - VSW = 5V, L1 = 4.7 µH ("X"), L1 = 2.2 µH ("Y") and TA= 25°C, unless specified
otherwise.
Efficiency Efficiency
vs vs
Load Current - "X" VOUT = 5V Load Current - "Y" VOUT = 5V
Figure 3. Figure 4.
Efficiency Efficiency
vs vs
Load Current - "X" VOUT = 3.3V Load Current - "Y" VOUT = 3.3V
Figure 5. Figure 6.
Efficiency
vs
Load Current - "X" VOUT = 1.5V Efficiency vs Load Current - "Y" VOUT = 1.5V
Figure 7. Figure 8.
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TYPICAL PERFORMANCE CHARACTERISTICS (continued)
All curves taken at VIN = 5V, VBOOST - VSW = 5V, L1 = 4.7 µH ("X"), L1 = 2.2 µH ("Y") and TA= 25°C, unless specified
otherwise.
Oscillator Frequency vs Temperature - "X" Oscillator Frequency vs Temperature - "Y"
Figure 9. Figure 10.
Current Limit vs Temperature Current Limit vs Temperature
VIN = 5V VIN = 20V
Figure 11. Figure 12.
VFB vs Temperature RDSON vs Temperature
Figure 13. Figure 14.
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TYPICAL PERFORMANCE CHARACTERISTICS (continued)
All curves taken at VIN = 5V, VBOOST - VSW = 5V, L1 = 4.7 µH ("X"), L1 = 2.2 µH ("Y") and TA= 25°C, unless specified
otherwise. Line Regulation - "X"
IQSwitching vs Temperature VOUT = 1.5V, IOUT = 500mA
Figure 15. Figure 16.
Line Regulation - "Y" Line Regulation - "X"
VOUT = 1.5V, IOUT = 500mA VOUT = 3.3V, IOUT = 500mA
Figure 17. Figure 18.
Line Regulation - "Y"
VOUT = 3.3V, IOUT = 500mA
Figure 19.
Copyright © 2011, Texas Instruments Incorporated Submit Documentation Feedback 7
Product Folder Links: LMR12010
L
R
1
R
2
D
1
D2
BOOST
Output
Control
Logic
Current
Limit
Thermal
Shutdown
Under
Voltage
Lockout
Corrective Ramp
Reset
Pulse
PWM
Comparator
Current-Sense Amplifier RSENSE
+
+
Internal
Regulator
and
Enable
Circuit
Oscillator
Driver 0.3:
Switch
Internal
Compensation
SW
EN
FB
GND
Error Amplifier -
+VREF
0.8V
COUT
ON
OFF
VBOOST
IL
VSW
+
-
CBOOST
VOUT
CIN
VIN
VIN
ISENSE
+
-
+
-
+
-0.88V
-
+
OVP
Comparator
Error
Signal
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
BLOCK DIAGRAM
Figure 20.
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0
0
VIN
VD
TON
t
t
Inductor
Current
D = TON/TSW
VSW
TOFF
TSW
IL
IPK
SW
Voltage
LMR12010
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SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
APPLICATION INFORMATION
Theory of Operation
The LMR12010 is a constant frequency PWM buck regulator IC that delivers a 1A load current. The regulator
has a preset switching frequency of either 3 MHz (LMR12010Y) or 1.6MHz (LMR12010X). These high
frequencies allow the LMR12010 to operate with small surface mount capacitors and inductors, resulting in
DC/DC converters that require a minimum amount of board space. The LMR12010 is internally compensated, so
it is simple to use, and requires few external components. The LMR12010 uses current-mode control to regulate
the output voltage.
The following operating description of the LMR12010 will refer to the Simplified Block Diagram (Figure 20) and to
the waveforms in Figure 21. The LMR12010 supplies a regulated output voltage by switching the internal NMOS
control switch at constant frequency and variable duty cycle. A switching cycle begins at the falling edge of the
reset pulse generated by the internal oscillator. When this pulse goes low, the output control logic turns on the
internal NMOS control switch. During this on-time, the SW pin voltage (VSW) swings up to approximately VIN, and
the inductor current (IL) increases with a linear slope. ILis measured by the current-sense amplifier, which
generates an output proportional to the switch current. The sense signal is summed with the regulator’s
corrective ramp and compared to the error amplifier’s output, which is proportional to the difference between the
feedback voltage and VREF. When the PWM comparator output goes high, the output switch turns off until the
next switching cycle begins. During the switch off-time, inductor current discharges through Schottky diode D1,
which forces the SW pin to swing below ground by the forward voltage (VD) of the catch diode. The regulator
loop adjusts the duty cycle (D) to maintain a constant output voltage.
Figure 21. LMR12010 Waveforms of SW Pin Voltage and Inductor Current
BOOST Function
Capacitor CBOOST and diode D2 in Figure 22 are used to generate a voltage VBOOST. VBOOST - VSW is the gate
drive voltage to the internal NMOS control switch. To properly drive the internal NMOS switch during its on-time,
VBOOST needs to be at least 1.6V greater than VSW. Although the LMR12010 will operate with this minimum
voltage, it may not have sufficient gate drive to supply large values of output current. Therefore, it is
recommended that VBOOST be greater than 2.5V above VSW for best efficiency. VBOOST VSW should not exceed
the maximum operating limit of 5.5V.
5.5V > VBOOST VSW > 2.5V for best performance.
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LMR12010
BOOST
SW
GND
L
D1
D2
COUT
CBOOST
VOUT
CIN
VIN
VIN
VBOOST
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
Figure 22. VOUT Charges CBOOST
When the LMR12010 starts up, internal circuitry from the BOOST pin supplies a maximum of 20mA to CBOOST.
This current charges CBOOST to a voltage sufficient to turn the switch on. The BOOST pin will continue to source
current to CBOOST until the voltage at the feedback pin is greater than 0.76V.
There are various methods to derive VBOOST:
1. From the input voltage (VIN)
2. From the output voltage (VOUT)
3. From an external distributed voltage rail (VEXT)
4. From a shunt or series zener diode
In the Simplifed Block Diagram of Figure 20, capacitor CBOOST and diode D2 supply the gate-drive current for the
NMOS switch. Capacitor CBOOST is charged via diode D2 by VIN. During a normal switching cycle, when the
internal NMOS control switch is off (TOFF) (refer to Figure 21), VBOOST equals VIN minus the forward voltage of D2
(VFD2), during which the current in the inductor (L) forward biases the Schottky diode D1 (VFD1). Therefore the
voltage stored across CBOOST is
VBOOST - VSW = VIN - VFD2 + VFD1 (1)
When the NMOS switch turns on (TON), the switch pin rises to
VSW = VIN (RDSON x IL), (2)
forcing VBOOST to rise thus reverse biasing D2. The voltage at VBOOST is then
VBOOST = 2VIN (RDSON x IL) VFD2 + VFD1 (3)
which is approximately
2VIN - 0.4V (4)
for many applications. Thus the gate-drive voltage of the NMOS switch is approximately
VIN - 0.2V (5)
An alternate method for charging CBOOST is to connect D2 to the output as shown in Figure 22. The output
voltage should be between 2.5V and 5.5V, so that proper gate voltage will be applied to the internal switch. In
this circuit, CBOOST provides a gate drive voltage that is slightly less than VOUT.
In applications where both VIN and VOUT are greater than 5.5V, or less than 3V, CBOOST cannot be charged
directly from these voltages. If VIN and VOUT are greater than 5.5V, CBOOST can be charged from VIN or VOUT
minus a zener voltage by placing a zener diode D3 in series with D2, as shown in Figure 23. When using a
series zener diode from the input, ensure that the regulation of the input supply doesn’t create a voltage that falls
outside the recommended VBOOST voltage.
(VINMAX VD3) < 5.5V
(VINMIN VD3) > 1.6V
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LMR12010
VIN BOOST
SW
GND
L
D1
D2
D3
R3
C4
VBOOST
CBOOST
VZ
VOUT
VIN
COUT
CIN
LMR12010
VIN BOOST
SW
GND
CBOOST
L
D1
D2
D3
VBOOST
VOUT
COUT
CIN
VIN
LMR12010
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SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
Figure 23. Zener Reduces Boost Voltage from VIN
An alternative method is to place the zener diode D3 in a shunt configuration as shown in Figure 24. A small
350mW to 500mW 5.1V zener in a SOT-23 or SOD package can be used for this purpose. A small ceramic
capacitor such as a 6.3V, 0.1µF capacitor (C4) should be placed in parallel with the zener diode. When the
internal NMOS switch turns on, a pulse of current is drawn to charge the internal NMOS gate capacitance. The
0.1 µF parallel shunt capacitor ensures that the VBOOST voltage is maintained during this time.
Resistor R3 should be chosen to provide enough RMS current to the zener diode (D3) and to the BOOST pin. A
recommended choice for the zener current (IZENER) is 1 mA. The current IBOOST into the BOOST pin supplies the
gate current of the NMOS control switch and varies typically according to the following formula for the X version:
IBOOST = 0.56 x (D + 0.54) x (VZENER VD2) mA (6)
IBOOST can be calculated for the Y version using the following:
IBOOST = (D + 0.5) x (VZENER - VD2) mA
where
D is the duty cycle
VZENER and VD2 are in volts
IBOOST is in milliamps (7)
VZENER is the voltage applied to the anode of the boost diode (D2), and VD2 is the average forward voltage across
D2. Note that this formula for IBOOST gives typical current. For the worst case IBOOST, increase the current by 40%.
In that case, the worst case boost current will be
IBOOST-MAX = 1.4 x IBOOST (8)
R3 will then be given by
R3 = (VIN - VZENER) / (1.4 x IBOOST + IZENER) (9)
For example, using the X-version let VIN = 10V, VZENER = 5V, VD2 = 0.7V, IZENER = 1mA, and duty cycle D = 50%.
ThenIBOOST = 0.56 x (0.5 + 0.54) x (5 - 0.7) mA = 2.5mA (10)
R3 = (10V - 5V) / (1.4 x 2.5mA + 1mA) = 1.11k(11)
Figure 24. Boost Voltage Supplied from the Shunt Zener on VIN
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LMR12010
VIN VIN
EN
BOOST
SW
FB
GND
VOUT
C3 L1
C2
R1
R2
D1
D2
ON
OFF
C1 R3
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
Figure 25. VBOOST Derived from VIN
Figure 26. VBOOST Derived from Series Zener Diode (VOUT)
Enable Pin / Shutdown Mode
The LMR12010 has a shutdown mode that is controlled by the enable pin (EN). When a logic low voltage is
applied to EN, the part is in shutdown mode and its quiescent current drops to typically 30nA. Switch leakage
adds another 40nA from the input supply. The voltage at this pin should never exceed VIN + 0.3V.
SOFT-START
This function forces VOUT to increase at a controlled rate during start up. During soft-start, the error amplifier’s
reference voltage ramps from 0V to its nominal value of 0.8V in approximately 200µs. This forces the regulator
output to ramp up in a more linear and controlled fashion, which helps reduce inrush current. Under some
circumstances at start-up, an output voltage overshoot may still be observed. This may be due to a large output
load applied during start up. Large amounts of output external capacitance can also increase output voltage
overshoot. A simple solution is to add a feed forward capacitor with a value between 470pf and 1000pf across
the top feedback resistor (R1).
Output Overvoltage Protections
The overvoltage comparator compares the FB pin voltage to a voltage that is 10% higher than the internal
reference Vref. Once the FB pin voltage goes 10% above the internal reference, the internal NMOS control
switch is turned off, which allows the output voltage to decrease toward regulation.
Undervoltage Lockout
Undervoltage lockout (UVLO) prevents the LMR12010 from operating until the input voltage exceeds 2.74V(typ).
The UVLO threshold has approximately 440mV of hysteresis, so the part will operate until VIN drops below
2.3V(typ). Hysteresis prevents the part from turning off during power up if VIN is non-monotonic.
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r = 'iL
lO
D = VO + VD
VIN + VD - VSW
D = VO
VIN
LMR12010
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SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
Current Limit
The LMR12010 uses cycle-by-cycle current limiting to protect the output switch. During each switching cycle, a
current limit comparator detects if the output switch current exceeds 1.7A (typ), and turns off the switch until the
next switching cycle begins.
Thermal Shutdown
Thermal shutdown limits total power dissipation by turning off the output switch when the IC junction temperature
exceeds 165°C. After thermal shutdown occurs, the output switch doesn’t turn on until the junction temperature
drops to approximately 150°C.
Design Guide
Inductor Selection
The Duty Cycle (D) can be approximated quickly using the ratio of output voltage (VO) to input voltage (VIN):
(12)
The catch diode (D1) forward voltage drop and the voltage drop across the internal NMOS must be included to
calculate a more accurate duty cycle. Calculate D by using the following formula:
(13)
VSW can be approximated by:
VSW = IOx RDS(ON) (14)
The diode forward drop (VD) can range from 0.3V to 0.7V depending on the quality of the diode. The lower VDis,
the higher the operating efficiency of the converter.
The inductor value determines the output ripple current. Lower inductor values decrease the size of the inductor,
but increase the output ripple current. An increase in the inductor value will decrease the output ripple current.
The ratio of ripple current (ΔiL) to output current (IO) is optimized when it is set between 0.3 and 0.4 at 1A. The
ratio r is defined as:
(15)
One must also ensure that the minimum current limit (1.2A) is not exceeded, so the peak current in the inductor
must be calculated. The peak current (ILPK) in the inductor is calculated by:
ILPK = IO+ΔIL/2 (16)
If r = 0.5 at an output of 1A, the peak current in the inductor will be 1.25A. The minimum specified current limit
over all operating conditions is 1.2A. One can either reduce r to 0.4 resulting in a 1.2A peak current, or make the
engineering judgement that 50mA over will be safe enough with a 1.7A typical current limit and 6 sigma limits.
When the designed maximum output current is reduced, the ratio r can be increased. At a current of 0.1A, r can
be made as high as 0.9. The ripple ratio can be increased at lighter loads because the net ripple is actually quite
low, and if r remains constant the inductor value can be made quite large. An equation empirically developed for
the maximum ripple ratio at any current below 2A is:
r = 0.387 x IOUT-0.3667 (17)
Note that this is just a guideline.
The LMR12010 operates at frequencies allowing the use of ceramic output capacitors without compromising
transient response. Ceramic capacitors allow higher inductor ripple without significantly increasing output ripple.
See the Output Capacitor section for more details on calculating output voltage ripple.
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'VO = 'iL x (RESR + 1
8 x fS x CO)
IRMS-IN = IO x D x r2
12
1-D +
L = VO + VD
IO x r x fSx (1-D)
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
Now that the ripple current or ripple ratio is determined, the inductance is calculated by:
where
fsis the switching frequency
IOis the output current (18)
When selecting an inductor, make sure that it is capable of supporting the peak output current without saturating.
Inductor saturation will result in a sudden reduction in inductance and prevent the regulator from operating
correctly. Because of the speed of the internal current limit, the peak current of the inductor need only be
specified for the required maximum output current. For example, if the designed maximum output current is 0.5A
and the peak current is 0.7A, then the inductor should be specified with a saturation current limit of >0.7A. There
is no need to specify the saturation or peak current of the inductor at the 1.7A typical switch current limit. The
difference in inductor size is a factor of 5. Because of the operating frequency of the LMR12010, ferrite based
inductors are preferred to minimize core losses. This presents little restriction since the variety of ferrite based
inductors is huge. Lastly, inductors with lower series resistance (DCR) will provide better operating efficiency. For
recommended inductors see Example Circuits.
Input Capacitor
An input capacitor is necessary to ensure that VIN does not drop excessively during switching transients. The
primary specifications of the input capacitor are capacitance, voltage, RMS current rating, and ESL (Equivalent
Series Inductance). The recommended input capacitance is 10µF, although 4.7µF works well for input voltages
below 6V. The input voltage rating is specifically stated by the capacitor manufacturer. Make sure to check any
recommended deratings and also verify if there is any significant change in capacitance at the operating input
voltage and the operating temperature. The input capacitor maximum RMS input current rating (IRMS-IN) must be
greater than:
(19)
It can be shown from the above equation that maximum RMS capacitor current occurs when D = 0.5. Always
calculate the RMS at the point where the duty cycle, D, is closest to 0.5. The ESL of an input capacitor is usually
determined by the effective cross sectional area of the current path. A large leaded capacitor will have high ESL
and a 0805 ceramic chip capacitor will have very low ESL. At the operating frequencies of the LMR12010,
certain capacitors may have an ESL so large that the resulting impedance (2πfL) will be higher than that required
to provide stable operation. As a result, surface mount capacitors are strongly recommended. Sanyo POSCAP,
Tantalum or Niobium, Panasonic SP or Cornell Dubilier ESR, and multilayer ceramic capacitors (MLCC) are all
good choices for both input and output capacitors and have very low ESL. For MLCCs it is recommended to use
X7R or X5R dielectrics. Consult capacitor manufacturer datasheet to see how rated capacitance varies over
operating conditions.
Output Capacitor
The output capacitor is selected based upon the desired output ripple and transient response. The initial current
of a load transient is provided mainly by the output capacitor. The output ripple of the converter is:
(20)
When using MLCCs, the ESR is typically so low that the capacitive ripple may dominate. When this occurs, the
output ripple will be approximately sinusoidal and 90° phase shifted from the switching action. Given the
availability and quality of MLCCs and the expected output voltage of designs using the LMR12010, there is really
no need to review any other capacitor technologies. Another benefit of ceramic capacitors is their ability to
bypass high frequency noise. A certain amount of switching edge noise will couple through parasitic
capacitances in the inductor to the output. A ceramic capacitor will bypass this noise while a tantalum will not.
Since the output capacitor is one of the two external components that control the stability of the regulator control
loop, most applications will require a minimum at 10 µF of output capacitance. Capacitance can be increased
significantly with little detriment to the regulator stability. Like the input capacitor, recommended multilayer
ceramic capacitors are X7R or X5R. Again, verify actual capacitance at the desired operating voltage and
temperature.
14 Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated
Product Folder Links: LMR12010
R1 =VO- 1
VREF x R2
IRMS-OUT = IO x r
12
LMR12010
www.ti.com
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
Check the RMS current rating of the capacitor. The RMS current rating of the capacitor chosen must also meet
the following condition:
(21)
Catch Diode
The catch diode (D1) conducts during the switch off-time. A Schottky diode is recommended for its fast switching
times and low forward voltage drop. The catch diode should be chosen so that its current rating is greater than:
ID1 = IOx (1-D) (22)
The reverse breakdown rating of the diode must be at least the maximum input voltage plus appropriate margin.
To improve efficiency choose a Schottky diode with a low forward voltage drop.
BOOST Diode
A standard diode such as the 1N4148 type is recommended. For VBOOST circuits derived from voltages less than
3.3V, a small-signal Schottky diode is recommended for greater efficiency. A good choice is the BAT54 small
signal diode.
BOOST Capacitor
A ceramic 0.01µF capacitor with a voltage rating of at least 6.3V is sufficient. The X7R and X5R MLCCs provide
the best performance.
Outup Voltage
The output voltage is set using the following equation where R2 is connected between the FB pin and GND, and
R1 is connected between VOand the FB pin. A good value for R2 is 10k.
(23)
PCB Layout Considerations
When planning layout there are a few things to consider when trying to achieve a clean, regulated output. The
most important consideration when completing the layout is the close coupling of the GND connections of the CIN
capacitor and the catch diode D1. These ground ends should be close to one another and be connected to the
GND plane with at least two through-holes. Place these components as close to the IC as possible. Next in
importance is the location of the GND connection of the COUT capacitor, which should be near the GND
connections of CIN and D1.
There should be a continuous ground plane on the bottom layer of a two-layer board except under the switching
node island.
The FB pin is a high impedance node and care should be taken to make the FB trace short to avoid noise pickup
and inaccurate regulation. The feedback resistors should be placed as close as possible to the IC, with the GND
of R2 placed as close as possible to the GND of the IC. The VOUT trace to R1 should be routed away from the
inductor and any other traces that are switching.
High AC currents flow through the VIN, SW and VOUT traces, so they should be as short and wide as possible.
However, making the traces wide increases radiated noise, so the designer must make this trade-off. Radiated
noise can be decreased by choosing a shielded inductor.
The remaining components should also be placed as close as possible to the IC. Refer to the LMR12010 demo
board as an example of a good layout.
Copyright © 2011, Texas Instruments Incorporated Submit Documentation Feedback 15
Product Folder Links: LMR12010
D = VO + VD + VDCR
VIN + VD - VSW
D = VOUT + VD
VIN + VD - VSW
K = POUT
POUT + PLOSS
K = POUT
PIN
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
Calculating Efficiency, and Junction Temperature
The complete LMR12010 DC/DC converter efficiency can be calculated in the following manner.
(24)
Or
(25)
Calculations for determining the most significant power losses are shown below. Other losses totaling less than
2% are not discussed.
Power loss (PLOSS) is the sum of two basic types of losses in the converter, switching and conduction.
Conduction losses usually dominate at higher output loads, where as switching losses remain relatively fixed and
dominate at lower output loads. The first step in determining the losses is to calculate the duty cycle (D).
(26)
VSW is the voltage drop across the internal NFET when it is on, and is equal to:
VSW = IOUT x RDSON (27)
VDis the forward voltage drop across the Schottky diode. It can be obtained from the Electrical Characteristics
section. If the voltage drop across the inductor (VDCR) is accounted for, the equation becomes:
(28)
This usually gives only a minor duty cycle change, and has been omitted in the examples for simplicity.
The conduction losses in the free-wheeling Schottky diode are calculated as follows:
PDIODE = VDx IOUT(1-D) (29)
Often this is the single most significant power loss in the circuit. Care should be taken to choose a Schottky
diode that has a low forward voltage drop.
Another significant external power loss is the conduction loss in the output inductor. The equation can be
simplified to:
PIND = IOUT2x RDCR (30)
The LMR12010 conduction loss is mainly associated with the internal NFET:
PCOND = IOUT2x RDSON x D (31)
Switching losses are also associated with the internal NFET. They occur during the switch on and off transition
periods, where voltages and currents overlap resulting in power loss. The simplest means to determine this loss
is to empirically measuring the rise and fall times (10% to 90%) of the switch at the switch node:
PSWF = 1/2(VIN x IOUT x freq x TFALL) (32)
PSWR = 1/2(VIN x IOUT x freq x TRISE) (33)
PSW = PSWF + PSWR (34)
Table 1. Typical Rise and Fall Times vs Input Voltage
VIN TRISE TFALL
5V 8ns 4ns
10V 9ns 6ns
15V 10ns 7ns
Another loss is the power required for operation of the internal circuitry:
PQ= IQx VIN (35)
IQis the quiescent operating current, and is typically around 1.5mA. The other operating power that needs to be
calculated is that required to drive the internal NFET:
PBOOST = IBOOST x VBOOST (36)
16 Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated
Product Folder Links: LMR12010
RT = 'T
Power
6PCOND + PSW + PDIODE + PIND + PQ + PBOOST = PLOSS
LMR12010
www.ti.com
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
VBOOST is normally between 3VDC and 5VDC. The IBOOST rms current is approximately 4.25mA. Total power
losses are: (37)
Design Example 1:
Operating Conditions
VIN 5.0V POUT 2.5W
VOUT 2.5V PDIODE 151mW
IOUT 1.0A PIND 75mW
VD0.35V PSWF 53mW
Freq 3MHz PSWR 53mW
IQ1.5mA PCOND 187mW
TRISE 8ns PQ7.5mW
TFALL 8ns PBOOST 21mW
RDSON 330mPLOSS 548mW
INDDCR 75m
D0.568
η= 82%
Calculating the LMR12010 Junction Temperature
Thermal Definitions:
TJ=Chip junction temperature
TA=Ambient temperature
RθJC =Thermal resistance from chip junction to device case
RθJA =Thermal resistance from chip junction to ambient air
Figure 27. Cross-Sectional View of Integrated Circuit Mounted on a Printed Circuit Board.
Heat in the LMR12010 due to internal power dissipation is removed through conduction and/or convection.
Conduction: Heat transfer occurs through cross sectional areas of material. Depending on the material, the
transfer of heat can be considered to have poor to good thermal conductivity properties (insulator vs conductor).
Heat Transfer goes as:
siliconpackagelead framePCB.
Convection: Heat transfer is by means of airflow. This could be from a fan or natural convection. Natural
convection occurs when air currents rise from the hot device to cooler air.
Thermal impedance is defined as:
(38)
Copyright © 2011, Texas Instruments Incorporated Submit Documentation Feedback 17
Product Folder Links: LMR12010
RTJA = 165oC - TA
PINTERNAL
6PCOND + PSWF + PSWR + PQ + PBOOST = PINTERNAL
PINTERNAL = 322 mW
TJ = (RTJC x Power) + TC = 80oC/W x 322 mW + TC
RTJA = TJ - TC
Power
RTJA = TJ - TA
Power
LMR12010
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
www.ti.com
Thermal impedance from the silicon junction to the ambient air is defined as:
(39)
This impedance can vary depending on the thermal properties of the PCB. This includes PCB size, weight of
copper used to route traces and ground plane, and number of layers within the PCB. The type and number of
thermal vias can also make a large difference in the thermal impedance. Thermal vias are necessary in most
applications. They conduct heat from the surface of the PCB to the ground plane. Place two to four thermal vias
close to the ground pin of the device.
The datasheet specifies two different RθJA numbers for the Thin SOT-23–6 package. The two numbers show the
difference in thermal impedance for a four-layer board with 2oz. copper traces, vs. a four-layer board with 1oz.
copper. RθJA equals 120°C/W for 2oz. copper traces and GND plane, and 235°C/W for 1oz. copper traces and
GND plane.
Method 1:
To accurately measure the silicon temperature for a given application, two methods can be used. The first
method requires the user to know the thermal impedance of the silicon junction to case. (RθJC) is approximately
80°C/W for the Thin SOT-23-6 package. Knowing the internal dissipation from the efficiency calculation given
previously, and the case temperature, which can be empirically measured on the bench we have:
(40)
Therefore:
TJ= (RθJC x PLOSS) + TC(41)
Design Example 2:
Operating Conditions
VIN 5.0V POUT 2.5W
VOUT 2.5V PDIODE 151mW
IOUT 1.0A PIND 75mW
VD0.35V PSWF 53mW
Freq 3MHz PSWR 53mW
IQ1.5mA PCOND 187mW
TRISE 8ns PQ7.5mW
TFALL 8ns PBOOST 21mW
RDSON 330mPLOSS 548mW
INDDCR 75m
D0.568
(42)
The second method can give a very accurate silicon junction temperature. The first step is to determine RθJA of
the application. The LMR12010 has over-temperature protection circuitry. When the silicon temperature reaches
165°C, the device stops switching. The protection circuitry has a hysteresis of 15°C. Once the silicon
temperature has decreased to approximately 150°C, the device will start to switch again. Knowing this, the RθJA
for any PCB can be characterized during the early stages of the design by raising the ambient temperature in the
given application until the circuit enters thermal shutdown. If the SW-pin is monitored, it will be obvious when the
internal NFET stops switching indicating a junction temperature of 165°C. Knowing the internal power dissipation
from the above methods, the junction temperature and the ambient temperature, RθJA can be determined.
(43)
Once this is determined, the maximum ambient temperature allowed for a desired junction temperature can be
found.
18 Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated
Product Folder Links: LMR12010
RTJA = 165oC - 94oC
322 mW = 220oC/W
6PCOND + PSWF + PSWR + PQ + PBOOST = PINTERNAL
PINTERNAL = 322 mW
LMR12010
www.ti.com
SNVS731A SEPTEMBER 2011REVISED SEPTEMBER 2011
Design Example 3:
Operating Conditions
Package SOT-23-6
VIN 12.0V POUT 2.475W
VOUT 3.30V PDIODE 523mW
IOUT 750mA PIND 56.25mW
VD0.35V PSWF 108mW
Freq 3MHz PSWR 108mW
IQ1.5mA PCOND 68.2mW
IBOOST 4mA PQ18mW
VBOOST 5V PBOOST 20mW
TRISE 8ns PLOSS 902mW
TFALL 8ns
RDSON 400m
INDDCR 75m
D30.3%
(44)
Using a standard TI Thin SOT-23-6 demonstration board to determine the RθJA of the board. The four layer PCB
is constructed using FR4 with 1/2oz copper traces. The copper ground plane is on the bottom layer. The ground
plane is accessed by two vias. The board measures 2.5cm x 3cm. It was placed in an oven with no forced
airflow.
The ambient temperature was raised to 94°C, and at that temperature, the device went into thermal shutdown.
(45)
If the junction temperature was to be kept below 125°C, then the ambient temperature cannot go above 54.2°C.
TJ- (RθJA x PLOSS) = TA(46)
Copyright © 2011, Texas Instruments Incorporated Submit Documentation Feedback 19
Product Folder Links: LMR12010
PACKAGE OPTION ADDENDUM
www.ti.com 28-Feb-2017
Addendum-Page 1
PACKAGING INFORMATION
Orderable Device Status
(1)
Package Type Package
Drawing Pins Package
Qty Eco Plan
(2)
Lead/Ball Finish
(6)
MSL Peak Temp
(3)
Op Temp (°C) Device Marking
(4/5)
Samples
LMR12010XMK/NOPB ACTIVE SOT-23-THIN DDC 6 1000 Green (RoHS
& no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF7B
LMR12010XMKE/NOPB ACTIVE SOT-23-THIN DDC 6 250 Green (RoHS
& no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF7B
LMR12010XMKX/NOPB ACTIVE SOT-23-THIN DDC 6 3000 Green (RoHS
& no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF7B
LMR12010YMK/NOPB ACTIVE SOT-23-THIN DDC 6 1000 Green (RoHS
& no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF8B
LMR12010YMKE/NOPB ACTIVE SOT-23-THIN DDC 6 250 Green (RoHS
& no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF8B
LMR12010YMKX/NOPB ACTIVE SOT-23-THIN DDC 6 3000 Green (RoHS
& no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF8B
(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) Eco Plan - The planned eco-friendly classification: Pb-Free (RoHS), Pb-Free (RoHS Exempt), or Green (RoHS & no Sb/Br) - please check http://www.ti.com/productcontent for the latest availability
information and additional product content details.
TBD: The Pb-Free/Green conversion plan has not been defined.
Pb-Free (RoHS): TI's terms "Lead-Free" or "Pb-Free" mean semiconductor products that are compatible with the current RoHS requirements for all 6 substances, including the requirement that
lead not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, TI Pb-Free products are suitable for use in specified lead-free processes.
Pb-Free (RoHS Exempt): This component has a RoHS exemption for either 1) lead-based flip-chip solder bumps used between the die and package, or 2) lead-based die adhesive used between
the die and leadframe. The component is otherwise considered Pb-Free (RoHS compatible) as defined above.
Green (RoHS & no Sb/Br): TI defines "Green" to mean Pb-Free (RoHS compatible), and free of Bromine (Br) and Antimony (Sb) based flame retardants (Br or Sb do not exceed 0.1% by weight
in homogeneous material)
(3) MSL, Peak Temp. - The Moisture Sensitivity Level rating according to the JEDEC industry standard classifications, and peak solder temperature.
(4) There may be additional marking, which relates to the logo, the lot trace code information, or the environmental category on the device.
(5) Multiple Device Markings will be inside parentheses. Only one Device Marking contained in parentheses and separated by a "~" will appear on a device. If a line is indented then it is a continuation
of the previous line and the two combined represent the entire Device Marking for that device.
PACKAGE OPTION ADDENDUM
www.ti.com 28-Feb-2017
Addendum-Page 2
(6) Lead/Ball Finish - Orderable Devices may have multiple material finish options. Finish options are separated by a vertical ruled line. Lead/Ball Finish values may wrap to two lines if the finish
value exceeds the maximum column width.
Important Information and Disclaimer:The information provided on this page represents TI's knowledge and belief as of the date that it is provided. TI bases its knowledge and belief on information
provided by third parties, and makes no representation or warranty as to the accuracy of such information. Efforts are underway to better integrate information from third parties. TI has taken and
continues to take reasonable steps to provide representative and accurate information but may not have conducted destructive testing or chemical analysis on incoming materials and chemicals.
TI and TI suppliers consider certain information to be proprietary, and thus CAS numbers and other limited information may not be available for release.
In no event shall TI's liability arising out of such information exceed the total purchase price of the TI part(s) at issue in this document sold by TI to Customer on an annual basis.
TAPE AND REEL INFORMATION
*All dimensions are nominal
Device Package
Type Package
Drawing Pins SPQ Reel
Diameter
(mm)
Reel
Width
W1 (mm)
A0
(mm) B0
(mm) K0
(mm) P1
(mm) W
(mm) Pin1
Quadrant
LMR12010XMK/NOPB SOT-
23-THIN DDC 6 1000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3
LMR12010XMKE/NOPB SOT-
23-THIN DDC 6 250 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3
LMR12010XMKX/NOPB SOT-
23-THIN DDC 6 3000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3
LMR12010YMK/NOPB SOT-
23-THIN DDC 6 1000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3
LMR12010YMKE/NOPB SOT-
23-THIN DDC 6 250 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3
LMR12010YMKX/NOPB SOT-
23-THIN DDC 6 3000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3
PACKAGE MATERIALS INFORMATION
www.ti.com 3-Mar-2017
Pack Materials-Page 1
*All dimensions are nominal
Device Package Type Package Drawing Pins SPQ Length (mm) Width (mm) Height (mm)
LMR12010XMK/NOPB SOT-23-THIN DDC 6 1000 210.0 185.0 35.0
LMR12010XMKE/NOPB SOT-23-THIN DDC 6 250 210.0 185.0 35.0
LMR12010XMKX/NOPB SOT-23-THIN DDC 6 3000 210.0 185.0 35.0
LMR12010YMK/NOPB SOT-23-THIN DDC 6 1000 210.0 185.0 35.0
LMR12010YMKE/NOPB SOT-23-THIN DDC 6 250 210.0 185.0 35.0
LMR12010YMKX/NOPB SOT-23-THIN DDC 6 3000 210.0 185.0 35.0
PACKAGE MATERIALS INFORMATION
www.ti.com 3-Mar-2017
Pack Materials-Page 2
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