LM26400Y Dual 2A, 500kHz Wide Input Range Buck Regulator General Description Features The LM26400Y is a monolithic, two-output fixed frequency PWM step-down DC/DC regulator in a 16-pin LLP or thermally enhanced ETSSOP package. With a minimum number of external components and internal loop compensation, the LM26400Y is easy to use. The ability to drive 2A loads with an internal 175mΩ NMOS switch using state-of-the-art 0.5µm BiCMOS technology results in a high-power density design. The world class control circuitry allows for an ON-time as low as 40 ns, thus supporting high-frequency conversion over the entire input range of 3V to 20V and down to an output voltage of only 0.6V. The LM26400Y utilizes peak current-mode control and internal compensation to provide high-performance regulation over a wide range of line and load conditions. Switching frequency is internally set to 500kHz, optimal for a broad range of applications in terms of size versus thermal tradeoffs. Given a non-synchronous architecture, efficiencies above 90% are easy to achieve. External shutdown is included, enabling separate turn-on and turn-off of the two channels. Additional features include programmable soft-start circuitry to reduce inrush current, pulse-by-pulse current limit and frequency foldback, integrated bootstrap structure and thermal shutdown. ■ ■ ■ ■ ■ ■ ■ ■ ■ ■ ■ ■ ■ Input voltage range of 3-20V Dual 2A output Output voltage down to 0.6V Internal compensation 500kHz PWM frequency Separate enable pins Separate soft start pins Frequency foldback protection 175mΩ NMOS switch Integrated bootstrap diodes Over-current protection ETSSOP and LLP packages Thermal shutdown Applications ■ ■ ■ ■ ■ ■ ■ DTV-LCD Set-Top Box XDSL Automotive Computing Peripherals Industrial Controls Point of Load Typical Application 20200252 © 2007 National Semiconductor Corporation 202002 www.national.com LM26400Y Dual 2A, 500kHz Wide Input Range Buck Regulator August 2007 LM26400Y Connection Diagrams 16-Lead ETSSOP (top view) 16-Lead LLP (top view) 20200202 20200203 NS Package Drawing MXA16A NS Package Drawing SDA16A Ordering Information www.national.com NSC Package Supplied As Drawing Order Number Package Type LM26400YMH ETSSOP-16 MXA16A Rail of 92 Units LM26400YMHX ETSSOP-16 MXA16A 2500 Units on Tape and Reel LM26400YSD LLP-16 SDA16A 1000 Units on Tape and Reel LM26400YSDX LLP-16 SDA16A 4500 Units on Tape and Reel LM26400YSDE LLP-16 SDA16A 250 Units on Tape and Reel 2 Pin Name Description 1 FB1 Feedback pin of Channel 1. Connect FB1 to an external voltage divider to set the output voltage of Channel 1. 2 SS1 Soft start pin of Channel 1. Connect a capacitor between this pin and ground to program the start up speed. 3 EN1 Enable control input for Channel 1. Logic high enables operation. Do not allow this pin to float or be greater than VIN + 0.3V. 4 AVIN Input supply for generating the internal bias used by the entire IC and for generating the internal bootstrap bias. Needs to be locally bypassed. 5 GND Signal and Power ground pin. Kelvin connect the lower resistor of the feedback voltage divider to this pin for good load regulation. 6 EN2 Enable control input for Channel 2. Logic high enables operation. Do not allow this pin to float or be greater than VIN + 0.3V. 7 SS2 Soft start pin of Channel 2. Connect a capacitor between this pin and ground to program the start up speed. 8 FB2 Feedback pin of Channel 2. Connect FB2 to an external voltage divider to set the output voltage of Channel 2. 9 BST2 Supply rail for the gate drive of Channel 2's NMOS switch. A bootstrap capacitor should be placed between the BST2 and SW2 pins. 10 SW2 Switch node of Channel 2. Connects to the inductor, catch diode, and bootstrap capacitor. 11, 12, 13,14 PVIN Input voltage of the power supply. Directly connected to the drain of the internal NMOS switch. Tie these pins together and connect to a local bypass capacitor. 15 SW1 Switch node of Channel 1. Connects to the inductor, catch diode, and bootstrap capacitor. 16 BST1 Supply rail for the gate drive of Channel 1's NMOS switch. A bootstrap capacitor should be placed between the BST1 and SW1 pins. DAP Die Attach Pad Must be connected to system ground for low thermal impedance and low grounding inductance. 3 www.national.com LM26400Y Pin Descriptions LM26400Y SSx Voltage Junction Temperature ESD Susceptibility Human Body Model (Note 3) Storage Temperature Range Absolute Maximum Ratings (Note 1) If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/ Distributors for availability and specifications. AVIN, PVIN SWx Voltage BSTx Voltage BSTx to SW Voltage FBx Voltage ENx Voltage (Note 2) −0.5V to 22V −0.5V to 22V −0.5V to 26V −0.5V to 6V −0.5V to 3V −0.5V to 22V Operating Ratings −0.5V to 3V +150°C 2kV -65°C to 150°C (Note 1) VIN Junction Temperature 3V to 20V −40°C to +125°C Electrical Characteristics Unless otherwise stated, the following conditions apply: AVIN = PVIN = VIN = 5V. Limits in standard type are for TJ = 25°C only; limits in boldface type apply over the junction temperature (TJ) range of -40°C to 125°C. Minimum and Maximum limits are guaranteed through test, design, or statistical correlation. Typical values represent the most likely parametric norm at TJ = 25°C, and are provided for reference purposes only. Symbol Parameter Conditions VFB 0°C to 85°C. Feedback Loop Closed. Voltages at FB1 and FB2 Pins -40°C to 125°C. Feedback Loop Closed. ΔVFB_LINE Line Regulation of FB1 and FB2 Voltages, Expressed as PPM VIN = 3V to 20V Change Per Volt of VIN Variation IFB Current in FB1 and FB2 Pins VFB = 0.6V VUVLO Under Voltage Lockout Threshold VIN Rises From 0V VUVLO_HYS fSW Min Typ 0.591 0.585 Max 0.611 0.6 0.617 66 VIN Falls From 3.3V Units V ppm/V 0.4 250 2.7 2.9 nA V 2.0 2.3 Hysteresis of UVLO Threshold 0.2 0.36 0.55 V Switching Frequency 0.39 0.52 0.65 MHz DMAX Maximum Duty Cycle 90 96 % DMIN Minimum Duty Cycle 2 % RDS_ON ON Resistance of Internal Power MOSFET ICL Peak Current Limit of Internal MOSFET ISD Shutdown Current of AVIN Pin EN1 = EN2 = 0V IQ Quiescent Current of AVIN Pin (both channels are enabled but EN1 = EN2 = 5V, FB1 = FB2 = 0.7V not switching) VEN_IH Input Logic High of EN1 and EN2 Pins VEN_IL Input Logic Low of EN1 and EN2 Pins IEN EN1 and EN2 Currents (sink or source) ISW_LEAK Switch Leakage Current Measured at SW1 and SW2 Pins ΔΦ Phase Shift Between SW1 and Feedback Loop Closed. Continuous SW2 Rising Edges Conduction Mode. 170 180 190 deg ISS SSx Pin Current 11 16 21 µA www.national.com ETSSOP, 2A Drain Current 175 320 LLP, 2A Drain Current 194 350 3 4.5 2.5 2 mA V 2.5 0.4 4 A nA 4 EN1 = EN2 = SWx = 0 mΩ V 5 nA 1 µA Parameter ΔISS Difference Between SS1 and SS2 Currents VFB_F FB1 and FB2 Frequency Foldback Threshold Conditions Min Typ Max Units 3 µA 0.35 V Thermal Characteristics Symbol Description Conditions Typical Value TSSOP LLP θJA Junction-to-Ambient Thermal Mount package on a standard board (Note 5) and Resistance (Note 4) test per JESD51-7 standard. 28 26 θJC Junction-to-Case-Bottom Thermal Resistance 3 2.8 TSD Thermal Shutdown Threshold Junction temperature rises. 165 TSD_HYS Thermal Shutdown Hysteresis Junction temperature falls from above TSD. 15 Unit °C/W °C Note 1: Absolute maximum ratings indicate limits beyond which damage to the device may occur. Operating Ratings are conditions under which the device is intended to be functional, but specific performance is not guaranteed. For guaranteed performance limits and associated test conditions, see Electrical Characteristics table. Note 2: EN1 and EN2 pins should never be higher than VIN + 0.3V. Note 3: The human body model is a 100pF capacitor discharged through a 1.5 kΩ resistor into each pin. Test method is per JESD-22-A114. Note 4: Value is highly board-dependent. For comparison of package thermal performance only. Not recommended for prediction of junction temperature in real applications. See THERMAL CONSIDERATIONS for more information. Note 5: A standard board refers to a four-layer PCB with the size 4.5”x3”x0.063”. Top and bottom copper is 2 oz. Internal plane copper is 1 oz. For details refer to JESD51-7 standard. 5 www.national.com LM26400Y Symbol LM26400Y Typical Performance Characteristics Unless otherwise specified or thermal-shutdown related, TA = 25° C for efficiency curves, loop gain plots and waveforms, and TJ = 25°C for all others. Efficiency, VOUT = 5V Efficiency, VOUT = 3.3V 20200237 20200216 Efficiency, VOUT = 2.5V Efficiency, VOUT = 1.2V 20200217 20200218 AVIN Shutdown Current vs. Temperature VIN Shutdown Current vs. VIN 20200206 www.national.com 20200238 6 LM26400Y Switching Frequency vs. Temperature Feedback Voltage vs. Temperature 20200207 20200208 Feedback Voltage vs. VIN Frequency Foldback 20200210 20200209 SS-Pin Current vs. Temperature FET RDS_ON vs. Temperature 20200278 20200221 7 www.national.com LM26400Y Switch Current Limit vs. Temperature Loop Gain, CCM 20200234 20200219 Loop Gain, DCM Loop Gain, CCM 20200220 20200236 Loop Gain, DCM Load Step Response 20200222 www.national.com 20200223 8 LM26400Y Load Step Response Line Transient Response 20200224 20200227 Start-Up (No Load) Start-Up (No Load) 20200228 20200239 Shutdown Thermal Shutdown 20200229 20200230 9 www.national.com LM26400Y Recovery from Thermal Shutdown Short-circuit Triggering 20200240 20200231 Short-circuit Release 20200232 www.national.com 10 LM26400Y Block Diagram 20200204 11 www.national.com LM26400Y reference and the level of the soft-start reference will be the lower of SS voltage and 0.6V. When the output is pre-biased, the LM26400Y can usually start up successfully if there is at least a 2-Volt difference between the input voltage and the pre-bias. An output pre-bias condition refers to the case when the output is sitting at a nonzero voltage at the beginning of a start-up. The key to a successful start-up under such a situation is enough initial voltage across the bootstrap capacitor. When an output prebias condition is anticipated, the power supply designer should check the start-up behavior under the highest potential pre-bias. A pre-bias condition caused by a glitch in the enable signal after start-up or by an input brown-out condition normally is not an issue because the bootstrap capacitor holds its charge much longer than the output capacitor(s). Due to the frequency foldback mechanism, the switching frequency during start-up will be lower than the normal value before VFB reaches 0.35V or so. See Frequency Foldback plot in the Typical Performance Characteristics section. It is generally okay to connect the EN pin to VIN to simplify the system design. However, if the VIN ramp is slow and the load current is relatively high during soft-start, the VOUT ramp may have a notch in it and a slight overshoot at the end of startup. This is due to the reduced load current handling capability of the LM26400Y for VIN lower than 5V. If this kind of behavior is a problem for the system designer, there are two solutions. One is to control the EN pin with a logic signal and do not pull the EN high until VIN is above 5V or so. Make sure the logic signal is never higher than VIN by 0.3V. The other is to use an external 5V bootstrap bias if it is ready before VIN hits 2.7V or so. See LOW INPUT VOLTAGE CONSIDERATIONS section for more information. Application Hints GENERAL The LM26400Y is a dual PWM peak-current mode buck regulator with two integrated power MOSFET switches. The part is designed to be easy to use. The two regulators are mostly identical and share the same input voltage and the same reference voltage (0.6V). The two PWM clocks are of the same frequency but 180° out of phase. The two channels can have different soft-start ramp slopes and can be turned on and off independently. Loop compensation is built in. The feedback loop design is optimized for ceramic output capacitors. Since the power switches are built in, the achievable output current level also has to do with thermal environment of the specific application. The LM26400Y enters thermal shutdown when the junction temperature exceeds 165°C or so. START-UP AND SHUTDOWN During a soft-start, the ramp of the output voltage is proportional to the ramp of the SS pin. When the EN pin is pulled high, an internal 16µA current source starts to charge the corresponding SS pin. The capacitance between the SS pin and ground determines how fast the SS voltage ramps up. The non-inverting input of the transconductance error amplifier, i.e. the moving reference during soft-start, will be the lower of SS voltage and the 0.6V reference (VREF). So before SS reaches 0.6V, the reference to the error amplifier will be the SS voltage. When SS exceeds 0.6V, the non-inverting input of the transconductance amplifier will be a constant 0.6V and that will be the time soft-start ends. The SS voltage will continue to ramp all the way up to the internal 2.7V supply voltage before leveling off. To calculate the needed SS capacitance for a given soft-start duration, use the following equation. OVER-CURRENT PROTECTION The instantaneous switch current is limited to a typical of 3 Amperes. Any time the switch current reaches that value, the switch will be turned off immediately. This will result in a smaller duty cycle than normal, which will cause the output voltage to dip. The output voltage will continue drooping until the load draws a current that is equal to the peak-limited inductor current. As the output voltage droops, the FB pin voltage will also droop proportionally. When the FB voltage dips below 0.35V or so, the PWM frequency will start to decrease. The lower the FB voltage the lower the PWM frequency. See Frequency Foldback plot in the Typical Performance Characteristics section. The frequency foldback helps two things. One is to prevent the switch current from running away as a result of the finite minimum ON time (40 ns or so for the LM26400Y) and the small duty cycle caused by lowered output voltage due to the current limit. The other is it also helps reduce thermal stress both in the IC and the external diode. The current limit threshold of the LM26400Y remains constant over all duty cycles. One thing to pay attention to is that recovery from an overcurrent condition does not go through a soft-start process. This is because the reference voltage at the non-inverting input of the error amplifier always sits at 0.6V during the overcurrent protection. So if the over-current condition is suddenly removed, the regulator will bring the FB voltage back to 0.6V as quickly as possible. This may cause an overshoot in the output voltage. Generally, the larger the inductor or the lower the output capacitance the more the overshoot, and vice versa. If the amount of such overshoot exceeds the allowed limit for a system, add a CFF capacitor in parallel with the upper ISS is SS pin charging current, typically 16µA. VREF is the internal reference voltage, typically 0.6V. tSS is the desired softstart duration. For example, if 1ms is the desired soft-start time, then the nominal SS capacitance should be 25nF. Apply tolerances if necessary. Use the VFB entry in the Electrical Characteristic table for the VREF tolerance. Inductor current during soft-start can be calculated by the following equation. VOUT is the target output voltage, IOUT is the load current during start-up, and COUT is the output capacitance. For example, if the output capacitor is 10µF, output voltage is 2.5V, softstart capacitor is 10nF and there is no load, then the average inductor current during soft-start will be 62.5mA. When EN pin is pulled below 0.4V or so, the 16µA current source will stop charging the SS pin. The SS pin will be discharged through a 330Ω internal FET to ground. During this time, the internal power switch will remain turned off while the output is discharged by the load. If EN is again pulled high before SS and output voltage are completely discharged, soft-start will begin with a non-zero www.national.com 12 LM26400Y feedback resistor to eliminate the overshoot. See the section LOAD STEP RESPONSE for more details on CFF. When one channel gets into over-current protection mode, the operation of the other channel will not be affected. The above analysis serves as a starting point. It is a good practice to always verify loop gain on bench. LOOP STABILITY To the first order approximation, the LM26400Y has a VFB-toInductor Current transfer admittance (i.e. ratio of inductor current to FB pin voltage, in frequency domain) close to the plot in Figure 1. The transfer admittance has a DC value of 104dBS (dBS stands for decibel Siemens. The equivelant of 0dBS is 1 Siemens.). There is a pole at 1Hz and a zero at approximately 8kHz. The plateau after the 8kHz zero is about 27dBS. There are also high frequency poles that are not shown in the figure. They include a double pole at 1.2MHz or so, and another double pole at half the switching frequency. Depending on factors such as inductor ripple size and duty cycle, the double pole at half the switching frequency may become two separate poles near half the switching frequency. LOAD STEP RESPONSE In general, the excursion in output voltage caused by a load step can be reduced by increasing the output capacitance. Besides that, increasing the small-signal loop bandwidth also helps. This can be achieved by adding a 27nF or so capacitor (CFF) in parallel with the upper feedback resistor (assuming the lower feedback resistor is 5.9kΩ). See Figure 2 for an illustration. 20200251 FIGURE 2. Adding a CFF Capacitor The responses to a load step between 0.2A and 2A with and without a CFF are shown in Figure 3. The higher loop bandwidth as a result of CFF reduces the total output excursion by about 80mV. 20200250 FIGURE 1. VFB-to-Inductor Current Transfer Admittance An easy strategy to build a stable loop with reasonable phase margin is to try to cross over between 20kHz and 100kHz, assuming the output capacitor is ceramic. When using pure ceramic capacitors at the output, simply use the following equation to find out the crossover frequency. where 22S (22 Siemens) is the equivelant of the 27dBS transfer admittance mentioned above and r is the ratio of 0.6V to the output voltage. Use the same equation to find out the needed output capacitance for a given crossover frequency. Phase margin is typically between 50° and 60°. Notice the above equation is only good for a crossover between 20kHz and 100kHz. A crossover frequency outside this range may result in lower phase margin and less accurate prediction by the above equation. Example: VOUT = 2.5V, COUT = 36µF, find out the crossover frequency. Assume the crossover is between 20kHz and 100kHz. Then 20200242 FIGURE 3. CFF Improves Load Step Response Use the following equation to calculate the new loop bandwidth: Again, the assumption is the crossover is between 20kHz and 100kHz. In an extreme case where the load goes to less than 100mA during a large load step, output voltage may exhibit extra un- 13 www.national.com LM26400Y dershoot. This usually happens when the load toggles high at the time VOUT just ramps down to its regulation level from an overshoot. Figure 4 shows such a case where the load toggles between 1.7A and only 50mA. The recommended voltage for the external bias is 5V. Due to the absolute maximum rating of VBST - VSW, the external 5V bias should not be higher than 6V. THERMAL SHUTDOWN Whenever the junction temperature of the LM26400Y exceeds 165°C, the MOSFET switch will be kept off until the temperature drops below 150°C, at which point the regulator will go through a hard-start to quickly raise the output voltage back to normal. Since it is a hard-start, there will be an overshoot at the output. See Thermal Shutdown in the Typical Performance Characteristics section. POWER LOSS ESTIMATION The total power loss in the LM26400Y comprises of three parts - the power FET conduction loss, the power FET switching loss and the IC's housekeeping power loss. Use the following equation to estimate the conduction loss. where TJ is the junction temperature or the target junction temperature if the former is unknown. RDS is the ON resistance of the internal FET at room temperature. Use 180mΩ for RDS if the actual value is unknown. Use the following equation to estimate the switching loss. 20200241 FIGURE 4. Extreme Load Step In the example, the load first goes down to 50mA quickly (0.9A/µs), causing a 90µs no-switching period, and then quickly goes up to 1.7A when VOUT1 just hits its regulation level (1.2V), resulting in a large dip of 440mV in the output voltage. If it is known in a system design that the load can go down to less than 100mA during a load step, and that the load can toggle high any time after it toggles low, take the following measures to minimize the potential extra undershoot. First is to add the Cff mentioned above. Second is to increase the output capacitance. For example, to meet a ±10% VOUT excursion requirement for a 100mA to 2A load step, approximately 200µF output capacitance is needed for a 1.2V output, and about 44µF is needed for a 5V output. Another loss in the IC is the housekeeping loss. It is the power dissipated by circuitry in the IC other than the power FETs. The equation is: The 15mW is gate drive loss. Do the calculation for both channels and find out the total power loss in the IC. LOW INPUT VOLTAGE CONSIDERATIONS When VIN is between 3V and 5V, it is recommended that an external bootstrap bias voltage and a Schottky diode be used to handle load currents up to 2A. See Figure 5 for an illustration. The power loss calculation can help estimate the overall power supply efficiency. Example: VIN = 12V, VOUT1 = 1.2V, IOUT1 = 2A, VOUT2 = 2.5V, IOUT2 = 2A. Target junction temperature is 90°C. So conduction loss in Channel 1 is: Conduction loss in Channel 2 is: 20200244 Switching loss in either channel is: FIGURE 5. External Bootstrap for Low VIN www.national.com 14 LM26400Y House keeping loss is: Finally the total power loss in the LM26400Y is: Choose 1% resistors. R2 = 5.90kΩ. PROGRAMMING OUTPUT VOLTAGE First make sure the required maximum duty cycle in steady state is less than 80% so that the regulator will not lose regulation. The datasheet lower limit for maximum duty cycle is about 90% over temperature (see Electrical Characteristics table for the accurate value). The maximum duty cycle in steady state happens at low line and full load. The output voltage is programmed through the feedback resistors R1 and R2, as illustrated in Figure 6. INDUCTOR SELECTION An inductance value that gives a peak-to-peak ripple current of 0.4A to 0.8A is recommended. Too large a ripple current can reduce the maximum achievable DC load current because the peak current of the switch is limited to a typical of 3A. Too small a ripple current can cause the regulator to oscillate due to the lack of inductor current ramp signal, especially under high input voltages. Use the following equation to determine inductance: where VIN_MAX is the maximum input voltage of the application. The rated current of the inductor should be higher than the maximum DC load current. Generally speaking, the lower the DC resistance of the inductor winding, the higher the overall regulator efficiency. Ferrite core inductors are recommended for less AC loss and less fringing magnetic flux. The drawback of ferrite core inductors is their quick saturation characteristic. Once the inductor gets saturated, its current can spike up very quickly if the switch is not turned off immediately. The current limit circuit has a propagation delay and so is oftentimes not fast enough to stop the saturated inductor from going above the current limit. This has the potential to damage the internal switch. So to prevent a ferrite core inductor from getting into saturation, the inductor saturation current rating should be higher than the switch current limit ICL. The LM26400Y is quite robust in handling short pulses of current that is a few amps above the current limit. When a compromise has to be made, pick an inductor with a saturation current just above the lower limit of the ICL. Be sure to validate the short-circuit protection over the intended temperature range. To prevent the inductor from saturating over the entire -40°C to 125°C range, pick one with a saturation current higher than the upper limit of ICL in the Electrical Characteristics table. Inductor saturation current is usually lower when hot. So consult the inductor vendor if the saturation current rating is only specified at room temperature. Soft saturation inductors such as the iron powder types can also be used. Such inductors do not saturate suddenly and therefore are safer when there is a severe overload or even shorted output. Their physical sizes are usually smaller than the Ferrite core inductors. The downside is their fringing flux and higher power dissipation due to relatively high AC loss, especially at high frequencies. Example: VOUT = 1.2V; VIN = 9V to 14V; IOUT = 2A max; Peak-to-peak Ripple Current ΔI = 0.6A. 20200258 FIGURE 6. Programming Output Voltage It is recommended that the lower feedback resistor R2 always be 5.9kΩ. This simplifies the selection of the CFF value (For an explanation of CFF, please refer to the section LOAD STEP RESPONSE). The 5.9kΩ is also a suitable R2 value in applications that need to increase the output voltage on the fly by paralleling another resistor with R2. Since the FB pin is 0.6V during normal operation, the current through the feedback resistors is normally 0.6V / 5.9kΩ = 0.1mA and the power dissipation in R2 is 0.6V x 0.6V / 5.9kΩ = 61µW - low enough for 0402 size or smaller resistors. Use the following equation to determine the upper feedback resistor R1. To determine the maximum allowed resistor tolerance, use the following equation: where TOL is the set point accuracy of the regulator, Φ is the tolerance of VFB. Example: VOUT = 1.2V, with a set point accuracy of +/-3.5%. 15 www.national.com LM26400Y ripple current by the impedance of the output capacitors. For example, if the inductor ripple current is 0.6A peak-to-peak, and the output capacitance is 44µF, then the output voltage ripple should be close to 0.6A x (6.28 x 500kHz x 44µF)-1 = 4.3mV. Sometimes when a large ceramic capacitor is used, the switching frequency may be higher than the capacitor's self resonance frequency. In that case, find out the true impedance at the switching frequency and then multiply that value by the ripple current to get the ripple voltage. The amount of output capacitance also impacts the stability of the feedback loop. Refer to the LOOP STABILITY section for guidelines. Choose a 5µH or so ferrite core inductor that has a saturation current around 3A at room temperature. For example, Sumida's CDRH6D26NP-5R0NC. If the maximum load current is significantly lower than 2A, pick an inductor with the same saturation rating as a 2A design but with a lowered DC current rating. That should result in a smaller inductor. There are not many choices, though. Another possibility is to use a soft saturation type inductor, whose size will be dominated by the DC current rating. INPUT CAPACITOR SELECTION The input capacitors provide the AC current needed by the nearby power switch so that current provided by the upstream power supply does not carry a lot of AC content, generating less EMI. To the buck regulator in question, the input capacitor also prevents the drain voltage of the FET switch from dipping when the FET is turned on, therefore providing a healthy line rail for the LM26400Y to work with. Since typically most of the AC current is provided by the local input capacitors, the power loss in those capacitors can be a concern. In the case of the LM26400Y regulator, since the two channels operate 180° out of phase, the AC stress in the input capacitors is less than if they operated in phase. The measure for the AC stress is called input ripple RMS current. It is strongly recommended that at least one 4.7µF ceramic capacitor be placed next to the PVIN pins. Bulk capacitors such as electrolytic capacitors or OSCON capacitors can be added to help stabilize the local line voltage, especially during large load transient events. As for the ceramic capacitors, use X7R , X6S or X5R types. They maintain most of their capacitance over a wide temperature range. Try to avoid sizes smaller than 0805. Otherwise significant drop in capacitance may be caused by the DC bias voltage. See OUTPUT CAPACITOR SELECTION section for more information. The DC voltage rating of the ceramic capacitor should be higher than the highest input voltage. Capacitor temperature is a major concern in board designs. While using a 4.7µF or higher MLCC as the input capacitor is a good starting point, it is a good idea to check the temperature in the real thermal environment to make sure the capacitors are not over heated. Capacitor vendors may provide curves of ripple RMS current vs. temperature rise, based on a designated thermal impedance. In reality, the thermal impedance may be very different. So it is always a good idea to check the capacitor temperature on the board. Since the duty cycles of the two channels may overlap, calculation of the input ripple RMS current is a little tedious. Use the following equation. OUTPUT CAPACITOR SELECTION Output capacitors in a buck regulator handles the AC current from the inductor and so have little ripple RMS current and their power dissipation is not a concern. The concern usually revolves around loop stability and capacitance retention. The LM26400Y's internal loop compensation was designed around ceramic output capacitors. From a stability point of view, the lower the output voltage, the more capacitance is needed. Below is a quick summary of temperature characteristics of some commonly used ceramic capacitors. So an X7R ceramic capacitor means its capacitance can vary ±15% over the temperature range of -55°C to +125°C. Capacitance Variation Over Temperature (Class II Dielectric Ceramic Capacitors) Low Temperature High Temperature Capacitance Change Range X: -55°C 5: +85°C R: ±15% Y: -30°C 6: +105°C S: ±22% Z: +10°C 7: +125°C U: +22%, -56% 8: +150°C V: +22%, -82% Besides the variation of capacitance over temperature, the actual capacitance of ceramic capacitors also vary, sometimes significantly, with applied DC voltage. Figure 7 illustrates such a characteristic of several ceramic capacitors of various physical sizes from Murata. Unless the DC voltage across the capacitor is going to be small relative to its rated value, going to too small a physical size will have the penalty of losing significant capacitance during circuit operation. I1 is Channel 1's maximum output current. I2 is Channel 2's maximum output current. d1 is the non-overlapping portion of Channel 1's duty cycle D1. d2 is the non-overlapping portion of Channel 2's duty cycle D2. d3 is the overlapping portion of the two duty cycles. Iav is the average input current. Iav= I1·D1 + I2·D2. To quickly determine the values of d1, d2 and d3, refer to the decision tree in Figure 8. To determine the duty cycle of each channel, use D = VOUT/VIN for a quick result or use the following equation for a more accurate result. 20200245 FIGURE 7. Capacitance vs. Applied DC Voltage The amount of output capacitance directly contributes to the output voltage ripple magnitude. A quick way to estimate the output voltage ripple is to multiply the inductor peak-to-peak www.national.com 16 RDC is the winding resistance of the inductor. RDS is the ON resistance of the MOSFET switch. Example: VIN = 5V, VOUT1 = 3.3V, IOUT1 = 2A, VOUT2 = 1.2V, IOUT2 = 1.5A, RDS = 170mΩ, RDC = 30mΩ. (IOUT1 is the same as I1 in the input ripple RMS current equation, IOUT2 is the same as I2). 20200246 FIGURE 8. Determining d1, d2 and d3 In boards that have internal ground planes, extending the toplayer thermal pad outside the body of the package to form a "dogbone" shape offers little performance improvement. However, for two-layer boards, the dogbone shape on the top layer will provide significant help. Predicting on paper with reasonable accuracy the junction temperature of the LM26400Y in a real-world application is still an art. Major factors that contribute to the junction temperature but not directly associated with the thermal performance of the LM26400Y itself include air speed, air temperature, nearby heating elements and arrangement of PCB copper connected to the DAP of the LM26400Y. The θJA value published in the datasheet is based on a standard board design in a single heating element mode and measured in a standard environment. The real application is usually completely different from those conditions. So the actual θJA will be significantly different from the datasheet number. The best approach is still to assign as much copper area as allowed to the DAP and prototype the design. When prototyping the design, it is necessary to know the junction temperature of the LM26400Y to assess the thermal margin. The best way to measure the LM26400Y's junction temperature when the board is working in its usual mode is to measure the package-top temperature using an infrared thermal imaging camera. Look for the highest temperature reading across the case-top. Add two degrees to the measurement result and the number should be a pretty good estimate of the junction temperature. Due to the high temperature gra- CATCH DIODE SELECTION The catch diode should be at least 2A rated. The most stressful operation for the diode is usually when the output is shorted under high line. Always pick a Schottky diode for its lower forward drop and higher efficiency. The reverse voltage rating of the diode should be at least 25% higher than the highest input voltage. The diode junction temperature is a main concern here. Always validate the diode's junction temperature in the intended thermal environment to make sure its thermally derated maximum current is not exceeded. There are a few 2A, 30V surface mount Schottky diodes available in the market. Notice that diodes have a negative temperature coefficient, so do not put two diodes in parallel to achieve a lower temperature rise. Current will be hogged by one of the diodes instead of shared by the two. Use a larger package for that purpose. THERMAL CONSIDERATIONS Due to the low thermal impedance from junction to the dieattach pad (or DAP, exposed metal at the bottom of the package), thermal performance heavily depends on PCB copper arrangement. The minimum requirement is to have a top-layer thermal pad that is exactly the same size as the DAP. There should be at least nine 8-mil thermal vias in the pad. The thermal vias should be connected to internal ground plane(s) (if available) and to a ground plane on the bottom layer that is as large as allowed. 17 www.national.com LM26400Y First, find out the duty cycles. Plug the numbers into the duty cycle equation and we get D1 = 0.75, and D2 = 0.33. Next, follow the decision tree in Figure 8 to find out the values of d1, d2 and d3. In this case, d1 = 0.5, d2 = D2 + 0.5 - D1 = 0.08, and d3 = D1 - 0.5 = 0.25. Iav = IOUT1·D1 + IOUT2·D2 = 1.995A. Plug all the numbers into the input ripple RMS current equation and the result is Iirrm = 0.77A. LM26400Y dient across the case-top, the use of a thermal couple is generally not recommended. If a thermal couple has to be used, try to locate the hottest spot on the case-top first and then secure the thermal couple at exactly the same location. The thermal couple needs to be a light-gauge type (such as 40-gauge). Apply a small blob of thermal compound to the contact point and then secure the thermal couple on the casetop using thermally non-conductive glue. If the maximum allowed junction temperature is exceeded, load current has to be lowered to bring the temperature back in specification. Or better thermal management such as more air flow needs to be provided. As a summary, here is a list of important items to consider: 1. Use multi-layer PC boards with internal ground planes. 2. Use nine or more thermal vias to connect the top-layer thermal pad to internal ground plane(s) and ground copper on the bottom layer. 3. Generate as large a ground plane as allowable on outer layers, especially near the package. 4. Use 2 oz. copper whenever possible. 5. Try to spread out heat generating components. 6. The inductors and diodes are heat generating components and should be connected to power or ground planes using many vias. 3. The SW pins are high current carrying pins so traces connected to them should be short and fat. 4. Keep feedback resistors close to the FB pins. 5. Keep the AVIN RC filter close to the AVIN pin. 6. Keep the voltage feedback traces away from the switch nodes. 7. Use six or more vias next to the ground pad of the catch diode. 8. Use at least four vias next to the ground pad of output capacitors. 9. Use at least four vias next to each pad of the input capacitors. For low EMI emission, try not to assign large areas of copper to the noisy switch nodes as a heat sinking method. Instead, assign a lot of copper to the output nodes. LAYOUT GUIDELINES There are mainly two considerations for PCB layout - thermal and electrical. For thermal details, refer to the section THERMAL CONSIDERATIONS. Electrical wise, follow the rules below as much as possible. In general, the LM26400Y is a quite robust part in terms of insensitivity to different layout patterns or even abuses. 1. Keep the input ceramic capacitor(s) as close to the PVIN pins as possible. 2. Use internal ground planes when available. www.national.com 20200243 FIGURE 9. PCB Layout Example 18 LM26400Y LM26400Y Design Examples 20200253 FIGURE 10. Example Circuit 1 Bill of Materials (Circuit 1, VIN = 12V±10%, Output1 = 1.2V/2A, Output2 = 2.5V/2A) Part Description Part Values Physical Size Part Number Manufacturer C1 Capacitor, Ceramic 10µF, 16V, X5R 1210 GRM32DR61C106KA01 Murata C2 Capacitor, Ceramic 0.22µF, 16V, X5R 0603 EMK107BJ224KA-T Taiyo Yuden C3 Capacitor, Ceramic 0.1µF, 6.3V, X5R 0402 C1005X5R0J104K TDK C4 Capacitor, Ceramic 0.1µF, 6.3V, X5R 0402 C1005X5R0J104K TDK C5 Capacitor, Ceramic 100µF, 6.3V, X5R 1210 GRM32ER60J107ME20L Murata C6 Capacitor, Ceramic 47µF, 6.3V, X5R 1210 GRM32ER60J476ME20L Murata C7 Capacitor, Ceramic 0.012µF, 6.3V, X5R 0402 C0402C123K9PACTU Kemet C8 Capacitor, Ceramic 0.012µF, 6.3V, X5R 0402 C0402C123K9PACTU Kemet C9 Capacitor, Ceramic 0.027µF, 6.3V, X5R 0402 C0402C273K9PACTU Kemet C10 Capacitor, Ceramic 0.027µF, 6.3V, X5R 0402 C0402C273K9PACTU Kemet D1 Diode, Schottky 2A, 30V SMB MBRS230LT3G ON Semiconductor D2 Diode, Schottky 2A, 30V SMB MBRS230LT3G ON Semiconductor L1 Inductor 5µH, 2.2A 7x7x2.8 mm3 CDRH6D26NP-5R0NC Sumida mm3 L2 Inductor 8.7µH, 2.2A 7x7x4 CDRH6D38NP-8R7NC Sumida R1 Resistor 10.0Ω, 1% 0402 CRCW040210R0FK Vishay R2 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay R3 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay R4 Resistor 18.7kΩ, 1% 0402 CRCW040218K7FK Vishay R5 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay U1 Regulator Dual 2A Buck ETSSOP-16 LM26400YMH National Semiconductor 19 www.national.com LM26400Y LM26400Y Design Examples Bill of Materials (Circuit 1, VIN = 7V to 20V, Output1 = 3.3V/2A, Output2 = 5V/2A) Part Description Part Values Physical Size Part Number Manufacturer C1 Capacitor, Ceramic 10µF, 25V, X5R 1812 GRM43DR61E106KA12 Murata C2 Capacitor, Ceramic 0.22µF, 25V, X5R 0603 TMK107BJ224KA-T Taiyo Yuden C3 Capacitor, Ceramic 0.1µF, 6.3V, X5R 0402 C1005X5R0J104K TDK C4 Capacitor, Ceramic 0.1µF, 6.3V, X5R 0402 C1005X5R0J104K TDK C5 Capacitor, Ceramic 47µF, 6.3V, X5R 1210 GRM32ER60J476ME20 Murata C6 Capacitor, Ceramic 33µF, 6.3V, X5R 1210 GRM32DR60J336ME19 Murata C7 Capacitor, Ceramic 0.012µF, 6.3V, X5R 0402 C0402C123K9PACTU Kemet C8 Capacitor, Ceramic 0.012µF, 6.3V, X5R 0402 C0402C123K9PACTU Kemet C9 Capacitor, Ceramic 0.027µF, 6.3V, X5R 0402 C0402C273K9PACTU Kemet C10 Capacitor, Ceramic 0.027µF, 6.3V, X5R 0402 C0402C273K9PACTU Kemet D1 Diode, Schottky 2A, 30V SMB MBRS230LT3G ON Semiconductor D2 Diode, Schottky 2A, 30V SMB MBRS230LT3G ON Semiconductor L1 Inductor 10µH, 3A 8.3x8.3x4 mm3 CDRH8D38NP-100NC Sumida mm3 L2 Inductor 15µH, 3A 8.3x8.3x4 CDRH8D43/HP-150NC Sumida R1 Resistor 10.0Ω, 1% 0402 CRCW040210R0FK Vishay R2 Resistor 26.7kΩ, 1% 0402 CRCW040226K7FK Vishay R3 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay R4 Resistor 43.2kΩ, 1% 0402 CRCW040218K7FK Vishay R5 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay U1 Regulator Dual 2A Buck ETSSOP-16 LM26400YMH National Semiconductor www.national.com 20 LM26400Y LM26400Y Design Examples 20200255 FIGURE 11. Example Circuit 2 Bill of Materials (Circuit 2, VIN = 3V to 5V, Output1 = 1.2V/2A, Output2 = 1.8V/2A) Part Description Part Values Physical Size Part Number Manufacturer C1 Capacitor, Ceramic 10µF, 6.3V, X5R 1206 GRM319R60J106KE19 Murata C2 Capacitor, Ceramic 0.22µF, 6.3V, X5R 0402 JMK105BJ224KV-F Taiyo Yuden C3 Capacitor, Ceramic 0.1µF, 6.3V, X5R 0402 C1005X5R0J104K TDK C4 Capacitor, Ceramic 0.1µF, 6.3V, X5R 0402 C1005X5R0J104K TDK C5 Capacitor, Ceramic 100µF, 6.3V, X5R 1210 GRM32ER60J107ME20L Murata C6 Capacitor, Ceramic 100µF, 6.3V, X5R 1210 GRM32ER60J107ME20L Murata C7 Capacitor, Ceramic 0.012µF, 6.3V, X5R 0402 C0402C123K9PACTU Kemet C8 Capacitor, Ceramic 0.012µF, 6.3V, X5R 0402 C0402C123K9PACTU Kemet C9 Capacitor, Ceramic 0.027µF, 6.3V, X5R 0402 C0402C273K9PACTU Kemet C10 Capacitor, Ceramic 0.027µF, 6.3V, X5R 0402 C0402C273K9PACTU Kemet D1 Diode, Schottky 2A, 30V SMB MBRS230LT3G ON Semiconductor D2 Diode, Schottky 2A, 30V SMB MBRS230LT3G ON Semiconductor L1 Inductor 5µH, 2.2A 7x7x2.8 mm3 CDRH6D26NP-5R0NC Sumida mm3 L2 Inductor 5µH, 2.2A 7x7x2.8 CDRH6D26NP-5R0NC Sumida R1 Resistor 10.0Ω, 1% 0402 CRCW040210R0FK Vishay R2 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay R3 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay R4 Resistor 11.8kΩ, 1% 0402 CRCW040211K8FK Vishay R5 Resistor 5.90kΩ, 1% 0402 CRCW04025K90FK Vishay U1 Regulator Dual 2A Buck ETSSOP-16 LM26400YMH National Semiconductor 21 www.national.com LM26400Y Physical Dimensions inches (millimeters) unless otherwise noted 16-Lead ETSSOP Package NS Package Number MXA16A 16-Lead LLP Package NS Package Number SDA16A www.national.com 22 LM26400Y Notes 23 www.national.com LM26400Y Dual 2A, 500kHz Wide Input Range Buck Regulator Notes THE CONTENTS OF THIS DOCUMENT ARE PROVIDED IN CONNECTION WITH NATIONAL SEMICONDUCTOR CORPORATION (“NATIONAL”) PRODUCTS. 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