LMR12010_14 [TI]

SIMPLE SWITCHER® 20Vin, 1A Step-Down Voltage Regulator in SOT-23;
LMR12010_14
型号: LMR12010_14
厂家: TEXAS INSTRUMENTS    TEXAS INSTRUMENTS
描述:

SIMPLE SWITCHER® 20Vin, 1A Step-Down Voltage Regulator in SOT-23

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LMR12010  
LMR12010 SIMPLE SWITCHER ® 20Vin, 1A Step-Down Voltage Regulator in  
SOT-23  
Literature Number: SNVS731A  
September 29, 2011  
LMR12010  
SIMPLE SWITCHER® 20Vin, 1A Step-Down Voltage  
Regulator in SOT-23  
Applications  
Point-of-Load Conversions from 3.3V, 5V, and 12V Rails  
Space Constrained Applications  
Battery Powered Equipment  
Industrial Distributed Power Applications  
Power Meters  
Portable Hand-Held Instruments  
System Performance  
30166501  
Efficiency vs Load Current - "X" VOUT = 5V  
Features  
Input voltage range of 3V to 20V  
Output voltage range of 0.8V to 17V  
Output current up to 1A  
1.6MHz (LMR12010X) and 3 MHz (LMR12010Y)  
switching frequencies  
Low shutdown Iq, 30 nA typical  
Internal soft-start  
Internally compensated  
Current-Mode PWM operation  
Thermal shutdown  
Thin SOT23-6 package (2.97 x 1.65 x 1mm)  
Fully enabled for WEBENCH® Power Designer  
Performance Benefits  
30166536  
Extremely easy to use  
Efficiency vs Load Current - "Y" VOUT = 5V  
Tiny overall solution reduces system cost  
30166534  
WEBENCH® is a registered trademark of National Semiconductor Corp.  
© 2011 National Semiconductor Corporation  
301665  
www.national.com  
Connection Diagrams  
30166560  
30166505  
Pin 1 Indentification  
6-Lead TSOT  
NS Package Number MK06A  
Ordering Information  
NSC Package  
Drawing  
Order Number  
Package Type  
Package Marking  
Supplied As  
LMR12010XMKE  
LMR12010XMK  
LMR12010XMKX  
LMR12010YMKE  
LMR12010YMK  
LMR12010YMKX  
SF7B  
250 Units on Tape and Reel  
1000 Units on Tape and Reel  
3000 Units on Tape and Reel  
250 Units on Tape and Reel  
1000 Units on Tape and Reel  
3000 Units on Tape and Reel  
TSOT-6  
MK06A  
SF8B  
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
4
FB  
EN  
Feedback pin. Connect FB to the external resistor divider to set output  
voltage.  
Enable control input. Logic high enables operation. Do not allow this  
pin to float or be greater than VIN + 0.3V.  
5
6
VIN  
Input supply voltage. Connect a bypass capacitor to this pin.  
SW  
Output switch. Connects to the inductor, catch diode, and bootstrap  
capacitor.  
www.national.com  
2
Absolute Maximum Ratings (Note 1)  
Operating Ratings (Note 1)  
If Military/Aerospace specified devices are required,  
please contact the National Semiconductor Sales Office/  
Distributors for availability and specifications.  
VIN  
3V to 20V  
-0.5V to 20V  
-0.5V to 25V  
SW Voltage  
Boost Voltage  
Boost to SW Voltage  
Junction Temperature Range  
Thermal Resistance θJA (Note 3)  
VIN  
-0.5V to 24V  
-0.5V to 24V  
-0.5V to 30V  
-0.5V to 6.0V  
-0.5V to 3.0V  
-0.5V to (VIN + 0.3V)  
150°C  
1.6V to 5.5V  
SW Voltage  
Boost Voltage  
Boost to SW Voltage  
FB Voltage  
EN Voltage  
−40°C to +125°C  
118°C/W  
Junction Temperature  
ESD Susceptibility (Note 2)  
Storage Temp. Range  
2kV  
-65°C to 150°C  
For soldering specifications: see product folder at  
www.national.com and www.national.com/ms/MS/MS-  
SOLDERING.pdf  
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  
guaranteed by design, test, or statistical analysis.  
Min  
(Note 4)  
Typ  
(Note 5)  
Max  
(Note 4)  
Symbol  
Parameter  
Feedback Voltage  
Conditions  
Units  
VFB  
0.784  
0.800  
0.01  
10  
0.816  
V
VIN = 3V to 20V  
ΔVFBVIN Feedback Voltage Line Regulation  
% / V  
nA  
IFB  
Sink/Source  
VIN Rising  
VIN Falling  
Feedback Input Bias Current  
Undervoltage Lockout  
Undervoltage Lockout  
UVLO Hysteresis  
250  
2.74  
2.3  
0.44  
1.6  
3.0  
92  
2.90  
UVLO  
V
2.0  
0.30  
1.2  
2.2  
85  
0.62  
1.9  
LMR12010X  
FSW  
DMAX  
DMIN  
Switching Frequency  
Maximum Duty Cycle  
Minimum Duty Cycle  
MHz  
%
LMR12010Y  
3.6  
LMR12010X  
LMR12010Y  
78  
85  
LMR12010X  
2
%
LMR12010Y  
8
RDS(ON)  
ICL  
Switch ON Resistance  
Switch Current Limit  
VBOOST - VSW = 3V  
VBOOST - VSW = 3V  
Switching  
300  
1.7  
1.5  
30  
600  
2.5  
2.5  
mΩ  
A
1.2  
1.8  
IQ  
Quiescent Current  
mA  
nA  
Quiescent Current (shutdown)  
VEN = 0V  
LMR12010X (50% Duty Cycle)  
LMR12010Y (50% Duty Cycle)  
VEN Falling  
2.5  
4.25  
3.5  
6.0  
0.4  
IBOOST  
Boost Pin Current  
mA  
V
Shutdown Threshold Voltage  
Enable Threshold Voltage  
Enable Pin Current  
VEN_TH  
VEN Rising  
IEN  
Sink/Source  
10  
40  
nA  
nA  
ISW  
Switch Leakage  
Note 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 guaranteed. For guaranteed specifications and the test conditions, see Electrical Characteristics.  
Note 2: Human body model, 1.5kin series with 100pF.  
Note 3: 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.  
Note 4: Guaranteed to National’s Average Outgoing Quality Level (AOQL).  
Note 5: Typicals represent the most likely parametric norm.  
3
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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 vs Load Current - "X" VOUT = 5V  
Efficiency vs Load Current - "Y" VOUT = 5V  
30166534  
30166536  
Efficiency vs Load Current - "X" VOUT = 3.3V  
Efficiency vs Load Current - "Y" VOUT = 3.3V  
30166551  
30166552  
Efficiency vs Load Current - "X" VOUT = 1.5V  
Efficiency vs Load Current - "Y" VOUT = 1.5V  
30166537  
30166535  
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4
Oscillator Frequency vs Temperature - "X"  
Oscillator Frequency vs Temperature - "Y"  
30166527  
30166528  
Current Limit vs Temperature  
VIN = 5V  
Current Limit vs Temperature  
VIN = 20V  
30166529  
30166547  
VFB vs Temperature  
RDSON vs Temperature  
30166533  
30166530  
5
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IQ Switching vs Temperature  
Line Regulation - "X"  
VOUT = 1.5V, IOUT = 500mA  
30166546  
30166556  
Line Regulation - "Y"  
VOUT = 1.5V, IOUT = 500mA  
Line Regulation - "X"  
VOUT = 3.3V, IOUT = 500mA  
30166554  
30166555  
Line Regulation - "Y"  
VOUT = 3.3V, IOUT = 500mA  
30166553  
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6
Block Diagram  
30166506  
FIGURE 1.  
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.  
General Description  
The LMR12010 regulator is a monolithic, high frequency,  
PWM step-down DC/DC converter in a 6-pin Thin SOT23  
package. It provides all the active functions to provide local  
DC/DC conversion with fast transient response and accurate  
regulation in the smallest possible PCB area.  
With a minimum of external components and online design  
support through WEBENCH®, the LMR12010 is easy to  
use. The ability to drive 1A loads with an internal 300mΩ  
NMOS switch using state-of-the-art 0.5µm BiCMOS technol-  
ogy results in the best power density available. The world  
class control circuitry allows for on-times as low as 13ns, thus  
supporting exceptionally high frequency conversion over the  
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 (LMR12010Y), allowing  
the use of extremely small surface mount inductors and chip  
capacitors. Even though the operating frequencies are very  
high, efficiencies up to 90% are easy to achieve. External  
shutdown is included, featuring an ultra-low stand-by current  
of 30nA. The LMR12010 utilizes current-mode control and in-  
ternal compensation to provide high-performance regulation  
over a wide range of operating conditions. Additional features  
include internal soft-start circuitry to reduce inrush current,  
pulse-by-pulse current limit, thermal shutdown, and output  
over-voltage protection.  
The following operating description of the LMR12010 will refer  
to the Simplified Block Diagram (Figure 1) and to the wave-  
forms in Figure 2. The LMR12010 supplies a regulated output  
voltage by switching the internal NMOS control switch at con-  
stant 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 con-  
trol logic turns on the internal NMOS control switch. During  
this on-time, the SW pin voltage (VSW) swings up to approxi-  
mately VIN, and the inductor current (IL) increases with a linear  
slope. IL is 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 propor-  
tional to the difference between the feedback voltage and  
VREF. When the PWM comparator output goes high, the out-  
put 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.  
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  
7
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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  
When the NMOS switch turns on (TON), the switch pin rises  
to  
VSW = VIN – (RDSON x IL),  
forcing VBOOST to rise thus reverse biasing D2. The voltage at  
VBOOST is then  
VBOOST = 2VIN – (RDSON x IL) – VFD2 + VFD1  
which is approximately  
2VIN - 0.4V  
for many applications. Thus the gate-drive voltage of the  
NMOS switch is approximately  
VIN - 0.2V  
30166507  
An alternate method for charging CBOOST is to connect D2 to  
the output as shown in Figure 3. 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  
FIGURE 2. LMR12010 Waveforms of SW Pin Voltage and  
Inductor Current  
a gate drive voltage that is slightly less than VOUT  
.
BOOST FUNCTION  
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 volt-  
age by placing a zener diode D3 in series with D2, as shown  
in Figure 4. 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.  
Capacitor CBOOST and diode D2 in Figure 3 are used to gen-  
erate a voltage VBOOST. VBOOST - VSW is the gate drive voltage  
to the internal NMOS control switch. To properly drive the in-  
ternal NMOS switch during its on-time, VBOOST needs to be at  
least 1.6V greater than VSW. Although the LMR12010 will op-  
erate 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.  
(VINMAX – VD3) < 5.5V  
(VINMIN – VD3) > 1.6V  
5.5V > VBOOST – VSW > 2.5V for best performance.  
30166509  
30166508  
FIGURE 4. Zener Reduces Boost Voltage from VIN  
FIGURE 3. VOUT Charges CBOOST  
An alternative method is to place the zener diode D3 in a  
shunt configuration as shown in Figure 5. 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 capac-  
itance. The 0.1 µF parallel shunt capacitor ensures that the  
VBOOST voltage is maintained during this time.  
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)  
Resistor R3 should be chosen to provide enough RMS current  
to the zener diode (D3) and to the BOOST pin. A recom-  
mended 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:  
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 1, 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 2), VBOOST equals  
IBOOST = 0.56 x (D + 0.54) x (VZENER – VD2) mA  
IBOOST can be calculated for the Y version using the following:  
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8
 
 
 
IBOOST = (D + 0.5) x (VZENER - VD2) mA  
where D is the duty cycle, VZENER and VD2 are in volts, and  
IBOOST is in milliamps. 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 typ-  
ical 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  
R3 will then be given by  
R3 = (VIN - VZENER) / (1.4 x IBOOST + IZENER  
)
30166550  
For example, using the X-version let VIN = 10V, VZENER = 5V,  
VD2 = 0.7V, IZENER = 1mA, and duty cycle D = 50%. Then  
FIGURE 7. VBOOST Derived from Series Zener Diode  
(VOUT  
)
IBOOST = 0.56 x (0.5 + 0.54) x (5 - 0.7) mA = 2.5mA  
R3 = (10V - 5V) / (1.4 x 2.5mA + 1mA) = 1.11kΩ  
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 dur-  
ing start up. During soft-start, the error amplifier’s reference  
voltage ramps from 0V to its nominal value of 0.8V in approx-  
imately 200µs. This forces the regulator output to ramp up in  
a more linear and controlled fashion, which helps reduce in-  
rush current. Under some circumstances at start-up, an out-  
put 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 volt-  
age overshoot. A simple solution is to add a feed forward  
capacitor with a value between 470pf and 1000pf across the  
top feedback resistor (R1).  
30166548  
FIGURE 5. Boost Voltage Supplied from the Shunt Zener  
on VIN  
OUTPUT OVERVOLTAGE PROTECTION  
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 refer-  
ence, 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). Hys-  
teresis prevents the part from turning off during power up if  
VIN is non-monotonic.  
30166542  
FIGURE 6. VBOOST Derived from VIN  
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 ap-  
proximately 150°C.  
9
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Now that the ripple current or ripple ratio is determined, the  
inductance is calculated by:  
Design Guide  
INDUCTOR SELECTION  
The Duty Cycle (D) can be approximated quickly using the  
ratio of output voltage (VO) to input voltage (VIN):  
where fs is the switching frequency and IO is the output cur-  
rent. When selecting an inductor, make sure that it is capable  
of supporting the peak output current without saturating. In-  
ductor saturation will result in a sudden reduction in induc-  
tance 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 maxi-  
mum 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 re-  
striction since the variety of ferrite based inductors is huge.  
Lastly, inductors with lower series resistance (DCR) will pro-  
vide better operating efficiency. For recommended inductors  
see Example Circuits.  
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:  
VSW can be approximated by:  
VSW = IO x RDS(ON)  
The diode forward drop (VD) can range from 0.3V to 0.7V de-  
pending on the quality of the diode. The lower VD is, the higher  
the operating efficiency of the converter.  
The inductor value determines the output ripple current. Low-  
er 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:  
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 rat-  
ing 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 ca-  
pacitor maximum RMS input current rating (IRMS-IN) must be  
greater than:  
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  
If r = 0.5 at an output of 1A, the peak current in the inductor  
will be 1.25A. The minimum guaranteed 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 in-  
creased. 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 empiri-  
cally developed for the maximum ripple ratio at any current  
below 2A is:  
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.  
-0.3667  
r = 0.387 x IOUT  
Note that this is just a guideline.  
The LMR12010 operates at frequencies allowing the use of  
ceramic output capacitors without compromising transient re-  
sponse. Ceramic capacitors allow higher inductor ripple with-  
out significantly increasing output ripple. See the output  
capacitor section for more details on calculating output volt-  
age ripple.  
OUTPUT CAPACITOR  
The output capacitor is selected based upon the desired out-  
put ripple and transient response. The initial current of a load  
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10  
transient is provided mainly by the output capacitor. The out-  
put ripple of the converter is:  
PCB Layout Considerations  
When planning layout there are a few things to consider when  
trying to achieve a clean, regulated output. The most impor-  
tant 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 con-  
nection of the COUT capacitor, which should be near the GND  
connections of CIN and D1.  
When using MLCCs, the ESR is typically so low that the ca-  
pacitive 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 ca-  
pacitor 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 capaci-  
tances 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. Capaci-  
tance 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 tem-  
perature.  
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 de-  
signer must make this trade-off. Radiated noise can be de-  
creased by choosing a shielded inductor.  
Check the RMS current rating of the capacitor. The RMS cur-  
rent rating of the capacitor chosen must also meet the follow-  
ing condition:  
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.  
Calculating Efficiency, and Junction  
Temperature  
The complete LMR12010 DC/DC converter efficiency can be  
calculated in the following manner.  
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 = IO x (1-D)  
The reverse breakdown rating of the diode must be at least  
the maximum input voltage plus appropriate margin. To im-  
prove efficiency choose a Schottky diode with a low forward  
voltage drop.  
Or  
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 effi-  
ciency. A good choice is the BAT54 small signal diode.  
Calculations for determining the most significant power loss-  
es 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).  
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.  
OUTPUT 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 VO and the FB pin. A good value for R2  
is 10kΩ.  
VSW is the voltage drop across the internal NFET when it is  
on, and is equal to:  
VSW = IOUT x RDSON  
11  
www.national.com  
VD is 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:  
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  
)
PSWR = 1/2(VIN x IOUT x freq x TRISE  
)
PSW = PSWF + PSWR  
Typical Rise and Fall Times vs Input Voltage  
VIN  
5V  
TRISE  
8ns  
TFALL  
4ns  
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:  
10V  
15V  
9ns  
6ns  
10ns  
7ns  
PDIODE = VD x IOUT(1-D)  
Another loss is the power required for operation of the internal  
circuitry:  
Often this is the single most significant power loss in the cir-  
cuit. Care should be taken to choose a Schottky diode that  
has a low forward voltage drop.  
PQ = IQ x VIN  
IQ is 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:  
Another significant external power loss is the conduction loss  
in the output inductor. The equation can be simplified to:  
PIND = IOUT2 x RDCR  
PBOOST = IBOOST x VBOOST  
The LMR12010 conduction loss is mainly associated with the  
internal NFET:  
VBOOST is normally between 3VDC and 5VDC. The IBOOST rms  
current is approximately 4.25mA. Total power losses are:  
PCOND = IOUT2 x RDSON x D  
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.  
Design Example 1:  
Operating Conditions  
VIN  
5.0V  
2.5V  
1.0A  
0.35V  
3MHz  
1.5mA  
8ns  
POUT  
PDIODE  
PIND  
2.5W  
VOUT  
IOUT  
VD  
151mW  
75mW  
53mW  
53mW  
187mW  
7.5mW  
21mW  
548mW  
PSWF  
PSWR  
PCOND  
PQ  
Freq  
IQ  
TRISE  
TFALL  
RDSON  
INDDCR  
D
8ns  
PBOOST  
PLOSS  
330mΩ  
75mΩ  
0.568  
η = 82%  
Calculating the LMR12010 Junction Temperature  
RθJC = Thermal resistance from chip junction to device case  
RθJA = Thermal resistance from chip junction to ambient air  
Thermal Definitions:  
TJ = Chip junction temperature  
TA = Ambient temperature  
www.national.com  
12  
30166573  
FIGURE 8. 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.  
ature, which can be empirically measured on the bench we  
have:  
Conduction: Heat transfer occurs through cross sectional ar-  
eas of material. Depending on the material, the transfer of  
heat can be considered to have poor to good thermal con-  
ductivity properties (insulator vs conductor).  
Heat Transfer goes as:  
Therefore:  
siliconpackagelead framePCB.  
TJ = (RθJC x PLOSS) + TC  
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.  
Design Example 2:  
Operating Conditions  
Thermal impedance is defined as:  
VIN  
5.0V  
2.5V  
1.0A  
0.35V  
3MHz  
1.5mA  
8ns  
POUT  
PDIODE  
PIND  
2.5W  
VOUT  
IOUT  
VD  
151mW  
75mW  
53mW  
53mW  
187mW  
7.5mW  
21mW  
548mW  
PSWF  
PSWR  
PCOND  
PQ  
Thermal impedance from the silicon junction to the ambient  
air is defined as:  
Freq  
IQ  
TRISE  
TFALL  
RDSON  
INDDCR  
D
8ns  
PBOOST  
PLOSS  
330mΩ  
75mΩ  
0.568  
This impedance can vary depending on the thermal proper-  
ties 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 SOT23–6 package. The two numbers show the differ-  
ence 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.  
The second method can give a very accurate silicon junction  
temperature. The first step is to determine RθJA of the appli-  
cation. The LMR12010 has over-temperature protection cir-  
cuitry. When the silicon temperature reaches 165°C, the  
device stops switching. The protection circuitry has a hys-  
teresis 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 dur-  
ing 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 obvi-  
Method 1:  
To accurately measure the silicon temperature for a given  
application, two methods can be used. The first method re-  
quires the user to know the thermal impedance of the silicon  
junction to case. (RθJC) is approximately 80°C/W for the Thin  
SOT23-6 package. Knowing the internal dissipation from the  
efficiency calculation given previously, and the case temper-  
13  
www.national.com  
ous 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.  
TFALL  
RDSON  
INDDCR  
D
8ns  
400mΩ  
75mΩ  
30.3%  
Once this is determined, the maximum ambient temperature  
allowed for a desired junction temperature can be found.  
Using a standard National Semiconductor Thin SOT23-6  
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.  
Design Example 3:  
Operating Conditions  
Package  
VIN  
SOT23-6  
12.0V  
3.30V  
750mA  
0.35V  
3MHz  
1.5mA  
4mA  
POUT  
PDIODE  
PIND  
2.475W  
523mW  
56.25mW  
108mW  
108mW  
68.2mW  
18mW  
VOUT  
IOUT  
The ambient temperature was raised to 94°C, and at that  
temperature, the device went into thermal shutdown.  
VD  
PSWF  
PSWR  
PCOND  
PQ  
Freq  
IQ  
IBOOST  
VBOOST  
TRISE  
If the junction temperature was to be kept below 125°C, then  
the ambient temperature cannot go above 54.2°C.  
5V  
PBOOST  
PLOSS  
20mW  
TJ - (RθJA x PLOSS) = TA  
8ns  
902mW  
www.national.com  
14  
Physical Dimensions inches (millimeters) unless otherwise noted  
6-Lead TSOT Package  
NS Package Number MK06A  
15  
www.national.com  
Notes  
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