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LTC4265 Datasheet(PDF) 35 Page - Linear Technology |
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LTC4265 Datasheet(HTML) 35 Page - Linear Technology |
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35 / 42 page ![]() LTC4278 35 4278fc APPLICATIONS INFORMATION CMILLER is calculated from the gate charge curve included on most MOSFET data sheets (Figure 16). The secondary-side power MOSFETs typically operate at substantially lower VDS, so you can neglect transition losses. The dissipation is calculated using: PDIS(SEC) = IRMS(SEC)2 • RDS(ON)(1 + d) With power dissipation known, the MOSFETs’ junction temperatures are obtained from the equation: TJ = TA + PDIS • θJA whereTAistheambienttemperatureandθJAistheMOSFET junction to ambient thermal resistance. Once you have TJ iterate your calculations recomputing d and power dissipations until convergence. Gate Drive Node Consideration The PG and SG gate drivers are strong drives to minimize gate drive rise and fall times. This improves efficiency, but the high frequency components of these signals can cause problems. Keep the traces short and wide to reduce parasitic inductance. The parasitic inductance creates an LC tank with the MOSFET gate capacitance. In less than ideal layouts, a series resistance of 5Ω or more may help to dampen the ringing at the expense of slightly slower rise and fall times and poorer efficiency. The LTC4278 gate drives will clamp the max gate voltage to roughly 7.5V, so you can safely use MOSFETs with maximum VGS of 10V and larger. Synchronous Gate Drive There are several different ways to drive the synchronous gateMOSFET.Fullconverterisolationrequiresthesynchro- nousgatedrivetobeisolated.Thisisusuallyaccomplished by way of a pulse transformer. Usually the pulse driver is used to drive a buffer on the secondary, as shown in the application on the front page of this data sheet. However,otherschemesarepossible.Therearegatedrivers andsecondary-sidesynchronouscontrollersavailablethat provide the buffer function as well as additional features. QA VGS a b 4278 F16 QB MILLER EFFECT GATE CHARGE (QG) Figure 16. Gate Charge Curve The flat portion of the curve is the result of the Miller (gate to-drain)capacitanceasthedrainvoltagedrops.TheMiller capacitance is computed as: CMILLER = QB –QA VDS The curve is done for a given VDS. The Miller capacitance for different VDS voltages are estimated by multiplying the computed CMILLER by the ratio of the application VDS to the curve specified VDS. WithCMILLERdetermined,calculatetheprimary-sidepower MOSFET power dissipation: PD(PRI) =IRMS(PRI) 2 •R DS(ON) 1+ δ ( )+ VIN(MAX) • PIN(MAX) DCMIN •RDR • CMILLER VGATE(MAX) – VTH • fOSC where: RDR is the gate driver resistance (≈10Ω) VTH is the MOSFET gate threshold voltage fOSC is the operating frequency VGATE(MAX) = 7.5V for this part (1 + d) is generally given for a MOSFET in the form of a normalizedRDS(ON)vstemperaturecurve.Ifyoudon’thave a curve, use d = 0.005/°C • ΔT for low voltage MOSFETs. |
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