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LTC3829 Datasheet(PDF) 23 Page - Linear Technology |
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LTC3829 Datasheet(HTML) 23 Page - Linear Technology |
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23 / 40 page ![]() LTC3829 3829f applicaTions inForMaTion where N is the number of output stages, δ is the tem- perature dependency of RDS(ON), RDR is the effective top driverresistance(approximately2ΩatVGS=VMILLER),VIN is the drain potential and the change in drain potential in the particular application. VTH(IL) is the data sheet speci- fied typical gate threshold voltage specified in the power MOSFET data sheet at the specified drain current. CMILLER is the calculated capacitance using the gate charge curve from the MOSFET data sheet and the technique described above. BothMOSFETshaveI2RlosseswhilethetopsideN-channel equation includes an additional term for transition losses, which peak at the highest input voltage. For VIN < 20V, the high current efficiency generally improves with larger MOSFETs, while for VIN > 20V, the transition losses rapidly increase to the point that the use of a higher RDS(ON)device with lower CMILLERactuallyprovideshigherefficiency.The synchronous MOSFET losses are greatest at high input voltage when the top switch duty factor is low or during a short-circuit when the synchronous switch is on close to 100% of the period. The term (1 + δ ) is generally given for a MOSFET in the form of a normalized RDS(ON) vs temperature curve, but δ = 0.005/°C can be used as an approximation for low voltage MOSFETs. The optional Schottky diodes conduct during the dead time between the conduction of the two large power MOSFETs. This prevents the body diode of the bottom MOSFET from turning on, storing charge during the dead time and requiring a reverse-recovery period which could cost as much as several percent in efficiency. A 2A to 8A Schottky is generally a good compromise for both regions of operation due to the relatively small average current. Larger diodes result in additional transition loss due to their larger junction capacitance. CIN and COUT Selection In continuous mode, the source current of each top N-channel MOSFET is a square wave of duty cycle VOUT/ VIN. A low ESR input capacitor sized for the maximum RMS current must be used. The details of a close form equation can be found in Application Note 77. Figure 10 showstheinputcapacitorripplecurrentfordifferentphase configurations with the output voltage fixed and input volt- age varied. The input ripple current is normalized against the DC output current. The graph can be used in place of tedious calculations. The minimum input ripple current can be achieved when the product of phase number and output voltage, N(VOUT), is approximately equal to the input voltage VIN or: V V k N where k N OUT IN = = , ,..., – 1 2 1 So the phase number can be chosen to minimize the input capacitor size for the given input and output voltages. In the graph of Figure 10, the local maximum input RMS capacitor currents are reached when: V V k N where k N OUT IN = = 2 1 1 2 – , ,..., Theseworst-caseconditionsarecommonlyusedfordesign becauseevensignificantdeviationsdonotoffermuchrelief. Note that capacitor manufacturer’s ripple current ratings are often based on only 2000 hours of life. This makes it advisable to further derate the capacitor or to choose a capacitor rated at a higher temperature than required. Several capacitors may also be paralleled to meet size or height requirements in the design. Always consult the capacitor manufacturer if there is any question. |
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