LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 LMR12010 SIMPLE SWITCHER® 20Vin, 1A Step-Down Voltage Regulator in SOT-23 Check for Samples: LMR12010 FEATURES DESCRIPTION • • • • The LMR12010 regulator is a monolithic, high frequency, PWM step-down DC/DC converter in a 6pin Thin SOT-23 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. 1 23 • • • • • • • 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 SOT-23-6 Package (2.97 x 1.65 x 1mm) Fully Enabled for WEBENCH® Power Designer 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 PERFORMANCE BENEFITS • • Extremely Easy to Use Tiny Overall Solution Reduces System Cost 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 technology 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 internal compensation to provide highperformance 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. D2 VIN BOOST VIN C3 C1 L1 SW LMR12010 ON OFF VOUT D1 EN C2 R1 FB GND R2 1 2 3 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. SIMPLE SWITCHER, WEBENCH are registered trademarks of Texas Instruments. All other 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 © 2011, Texas Instruments Incorporated LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com System Performance Efficiency vs Load Current - "X" VOUT = 5V Efficiency vs Load Current - "Y" VOUT = 5V Connection Diagram BOOST 1 6 SW GND 2 5 VIN FB 3 4 EN Figure 1. 6-Lead SOT Package Number DDC0006A 1 6 2 5 3 4 Figure 2. Pin 1 Identification PIN DESCRIPTIONS 2 Pin Name 1 BOOST Boost voltage that drives the internal NMOS control switch. A bootstrap capacitor is connected between the BOOST and SW pins. Function 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. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 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 ESD Susceptibility 150°C (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. 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. (2) (3) 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 −40°C to +125°C Junction Temperature Range Thermal Resistance θJA (2) (1) (2) 118°C/W 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. 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. Symbol VFB ΔVFB/ΔVIN IFB UVLO Parameter Conditions Feedback Voltage Feedback Voltage Line Regulation VIN = 3V to 20V Feedback Input Bias Current Sink/Source Undervoltage Lockout VIN Rising Undervoltage Lockout VIN Falling (1) (2) Switching Frequency DMAX Maximum Duty Cycle Typ Max 0.784 0.800 0.816 (1) (2) (1) Units 0.01 V %/V 10 250 2.74 2.90 2.0 2.3 0.30 0.44 0.62 LMR12010X 1.2 1.6 1.9 LMR12010Y 2.2 3.0 3.6 LMR12010X 85 92 LMR12010Y 78 85 UVLO Hysteresis FSW Min nA V MHz % Specified to TI’s Average Outgoing Quality Level (AOQL). Typicals represent the most likely parametric norm. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 3 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com 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. Symbol DMIN RDS(ON) Minimum Duty Cycle Conditions Min (1) Typ (2) LMR12010X 2 LMR12010Y 8 Max (1) Switch ON Resistance VBOOST - VSW = 3V Switch Current Limit VBOOST - VSW = 3V IQ Quiescent Current Switching Quiescent Current (shutdown) VEN = 0V 30 LMR12010X (50% Duty Cycle) 2.5 3.5 LMR12010Y (50% Duty Cycle) 4.25 6.0 Boost Pin Current Shutdown Threshold Voltage VEN Falling Enable Threshold Voltage VEN Rising IEN Enable Pin Current Sink/Source ISW Switch Leakage VEN_TH Submit Documentation Feedback 1.2 Units % ICL IBOOST 4 Parameter 300 600 1.7 2.5 A 1.5 2.5 mA nA 0.4 1.8 mΩ mA V 10 nA 40 nA Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 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 Figure 3. Figure 4. Efficiency vs Load Current - "X" VOUT = 3.3V Efficiency vs 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. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 5 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com 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. 6 Oscillator Frequency vs Temperature - "X" Oscillator Frequency vs Temperature - "Y" Figure 9. Figure 10. Current Limit vs Temperature VIN = 5V Current Limit vs Temperature VIN = 20V Figure 11. Figure 12. VFB vs Temperature RDSON vs Temperature Figure 13. Figure 14. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 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. IQ Switching vs Temperature Line Regulation - "X" VOUT = 1.5V, IOUT = 500mA Figure 15. Figure 16. Line Regulation - "Y" VOUT = 1.5V, IOUT = 500mA Line Regulation - "X" VOUT = 3.3V, IOUT = 500mA Figure 17. Figure 18. Line Regulation - "Y" VOUT = 3.3V, IOUT = 500mA Figure 19. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 7 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com BLOCK DIAGRAM VIN VIN Current-Sense Amplifier OFF EN Internal Regulator and Enable Circuit + - BOOST VBOOST Under Voltage Lockout Oscillator CIN D2 Thermal Shutdown Current Limit Output Control Logic Reset Pulse + ISENSE + + Corrective Ramp 0.3: Switch Driver SW OVP Comparator - ON RSENSE Error Signal D 1 + PWM Comparator CBOOST VSW L IL VOUT COUT 0.88V + - R 1 FB Internal Compensation + Error Amplifier + - VREF 0.8V R 2 GND Figure 20. 8 Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED 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. 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 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. VSW D = TON/TSW VIN SW Voltage TOFF TON 0 VD IL t TSW IPK Inductor Current 0 t 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. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 9 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com VBOOST D2 BOOST VIN VIN LMR12010 CIN CBOOST L SW VOUT GND D1 COUT 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 10 Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 D2 D3 BOOST VIN VIN LMR12010 CIN VBOOST CBOOST L SW VOUT GND COUT D1 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%. Then 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 (10) (11) VZ C4 D2 D3 R3 BOOST VIN VIN CIN VBOOST CBOOST LMR12010 L VOUT SW GND D1 COUT Figure 24. Boost Voltage Supplied from the Shunt Zener on VIN Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 11 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com D2 VIN BOOST VIN C3 C1 R3 L1 VOUT SW LMR12010 ON D1 C2 EN OFF R1 FB GND R2 Figure 25. VBOOST Derived from VIN D3 D2 VIN BOOST VIN C3 C1 R3 LMR12010 ON OFF L1 SW VOUT D1 EN C2 R1 FB GND R2 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. 12 Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED 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): VO D= 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: VO + VD D= VIN + VD - VSW (13) VSW can be approximated by: VSW = IO x 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 VD is, 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: r= 'iL lO (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. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 13 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com Now that the ripple current or ripple ratio is determined, the inductance is calculated by: L= VO + VD IO x r x fS x (1-D) where • • fs is the switching frequency IO is 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: IRMS-IN = IO x r2 D x 1-D + 12 (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: 'VO = 'iL x (RESR + 1 ) 8 x fS x CO (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 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 Check the RMS current rating of the capacitor. The RMS current rating of the capacitor chosen must also meet the following condition: IRMS-OUT = IO x r 12 (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 = IO x (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 VO and the FB pin. A good value for R2 is 10kΩ. R1 = VO VREF - 1 x R2 (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. Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 15 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com Calculating Efficiency, and Junction Temperature The complete LMR12010 DC/DC converter efficiency can be calculated in the following manner. POUT K= PIN (24) Or POUT K= POUT + PLOSS (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). VOUT + VD D= VIN + VD - VSW (26) VSW is the voltage drop across the internal NFET when it is on, and is equal to: VSW = IOUT x RDSON (27) 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: VO + VD + VDCR D= VIN + VD - VSW (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 = VD x 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 = IOUT2 x RDCR (30) The LMR12010 conduction loss is mainly associated with the internal NFET: PCOND = IOUT2 x 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) PSWR = 1/2(VIN x IOUT x freq x TRISE) PSW = PSWF + PSWR (32) (33) (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 = IQ x VIN (35) 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: PBOOST = IBOOST x VBOOST 16 (36) Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 VBOOST is normally between 3VDC and 5VDC. The IBOOST rms current is approximately 4.25mA. Total power losses are: 6PCOND + PSW + PDIODE + PIND + PQ + PBOOST = PLOSS (37) Design Example 1: Operating Conditions VIN 5.0V POUT 2.5W VOUT 2.5V PDIODE 151mW IOUT 1.0A PIND 75mW VD 0.35V PSWF 53mW Freq 3MHz PSWR 53mW IQ 1.5mA PCOND 187mW TRISE 8ns PQ 7.5mW TFALL 8ns PBOOST 21mW RDSON 330mΩ PLOSS 548mW INDDCR 75mΩ D 0.568 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: silicon→package→lead frame→PCB. 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: RT = 'T Power (38) Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 17 LMR12010 SNVS731A – SEPTEMBER 2011 – REVISED SEPTEMBER 2011 www.ti.com Thermal impedance from the silicon junction to the ambient air is defined as: TJ - TA RTJA = (39) Power 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: TJ - TC RTJA = (40) Power 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 VD 0.35V PSWF 53mW Freq 3MHz PSWR 53mW IQ 1.5mA PCOND 187mW TRISE 8ns PQ 7.5mW TFALL 8ns PBOOST 21mW RDSON 330mΩ PLOSS 548mW INDDCR 75mΩ D 0.568 6PCOND + PSWF + PSWR + PQ + PBOOST = PINTERNAL PINTERNAL = 322 mW TJ = (RTJC x Power) + TC = 80oC/W x 322 mW + TC (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. 165oC - TA RTJA = PINTERNAL (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 LMR12010 www.ti.com SNVS731A – SEPTEMBER 2011 – REVISED 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 VD 0.35V PSWF 108mW Freq 3MHz PSWR 108mW IQ 1.5mA PCOND 68.2mW IBOOST 4mA PQ 18mW VBOOST 5V PBOOST 20mW TRISE 8ns PLOSS 902mW TFALL 8ns RDSON 400mΩ INDDCR 75mΩ D 30.3% 6PCOND + PSWF + PSWR + PQ + PBOOST = PINTERNAL PINTERNAL = 322 mW (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. RTJA = 165oC - 94oC 322 mW = 220oC/W (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) Submit Documentation Feedback Copyright © 2011, Texas Instruments Incorporated Product Folder Links: LMR12010 19 PACKAGE OPTION ADDENDUM www.ti.com 11-Apr-2013 PACKAGING INFORMATION Orderable Device Status (1) Package Type Package Pins Package Drawing Qty Eco Plan Lead/Ball Finish (2) MSL Peak Temp Op Temp (°C) Top-Side Markings (3) (4) LMR12010XMK/NOPB ACTIVE SOT DDC 6 1000 Green (RoHS & no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF7B LMR12010XMKE/NOPB ACTIVE SOT DDC 6 250 Green (RoHS & no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF7B LMR12010XMKX/NOPB ACTIVE SOT DDC 6 3000 Green (RoHS & no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF7B LMR12010YMK/NOPB ACTIVE SOT DDC 6 1000 Green (RoHS & no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF8B LMR12010YMKE/NOPB ACTIVE SOT DDC 6 250 Green (RoHS & no Sb/Br) CU SN Level-1-260C-UNLIM -40 to 125 SF8B LMR12010YMKX/NOPB ACTIVE SOT 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) Multiple Top-Side Markings will be inside parentheses. Only one Top-Side 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 Top-Side Marking for that device. Addendum-Page 1 Samples PACKAGE OPTION ADDENDUM www.ti.com 11-Apr-2013 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. 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Addendum-Page 2 PACKAGE MATERIALS INFORMATION www.ti.com 14-Mar-2013 TAPE AND REEL INFORMATION *All dimensions are nominal Device Package Package Pins Type Drawing LMR12010XMK/NOPB SOT DDC 6 LMR12010XMKE/NOPB SOT DDC LMR12010XMKX/NOPB SOT DDC LMR12010YMK/NOPB SOT LMR12010YMKE/NOPB LMR12010YMKX/NOPB SPQ Reel Reel A0 Diameter Width (mm) (mm) W1 (mm) B0 (mm) K0 (mm) P1 (mm) W Pin1 (mm) Quadrant 1000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3 6 250 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3 6 3000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3 DDC 6 1000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3 SOT DDC 6 250 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3 SOT DDC 6 3000 178.0 8.4 3.2 3.2 1.4 4.0 8.0 Q3 Pack Materials-Page 1 PACKAGE MATERIALS INFORMATION www.ti.com 14-Mar-2013 *All dimensions are nominal Device Package Type Package Drawing Pins SPQ Length (mm) Width (mm) Height (mm) LMR12010XMK/NOPB SOT DDC 6 1000 210.0 185.0 35.0 LMR12010XMKE/NOPB SOT DDC 6 250 210.0 185.0 35.0 LMR12010XMKX/NOPB SOT DDC 6 3000 210.0 185.0 35.0 LMR12010YMK/NOPB SOT DDC 6 1000 210.0 185.0 35.0 LMR12010YMKE/NOPB SOT DDC 6 250 210.0 185.0 35.0 LMR12010YMKX/NOPB SOT DDC 6 3000 210.0 185.0 35.0 Pack Materials-Page 2 IMPORTANT NOTICE Texas Instruments Incorporated and its subsidiaries (TI) reserve the right to make corrections, enhancements, improvements and other changes to its semiconductor products and services per JESD46, latest issue, and to discontinue any product or service per JESD48, latest issue. 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