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IRFR3707ZTRLPbF Datasheet(PDF) 8 Page - Infineon Technologies AG |
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IRFR3707ZTRLPbF Datasheet(HTML) 8 Page - Infineon Technologies AG |
8 / 12 page IRFR/U3707ZPbF 8 2016-5-31 Power MOSFET Selection for Non-Isolated DC/DC Converters Control FET Special attention has been given to the power losses in the switching elements of the circuit - Q1 and Q2. Power losses in the high side switch Q1, also called the Control FET, are impacted by the Rds(on) of the MOSFET, but these conduction losses are only about one half of the total losses. Power losses in the control switch Q1 are given by; Ploss = Pconduction+ Pswitching+ Pdrive+ Poutput This can be expanded and approximated by; This simplified loss equation includes the terms Qgs2 and Qoss which are new to Power MOSFET data sheets. Qgs2 is a subelement of traditional gate-source charge that is included in all MOSFET data sheets. The importance of splitting this gate-source charge into two sub elements, Qgs1 and Qgs2, can be seen from Fig 16. Qgs2 indicates the charge that must be supplied by the gate driver between the time that the threshold voltage has been reached and the time the drain current rises to Id max at which time the drain voltage begins to change. Minimizing Qgs2 is a critical factor in reducing switching losses in Q1. Qoss is the charge that must be supplied to the output capacitance of the MOSFET during every switching cycle. Figure A shows how Qoss is formed by the parallel combination of the voltage dependent (non-linear) capacitance’s Cds and Cdg when multiplied by the power supply input buss voltage. P loss Irms 2 R ds(on) I Q gd i g V in f I Q gs2 i g V in f Q g Vg f Qoss 2 V in f Synchronous FET The power loss equation for Q2 is approximated by; *dissipated primarily in Q1 For the synchronous MOSFET Q2, Rds(on) is an important characteristic; however, once again the importance of gate charge must not be overlooked since it impacts three critical areas. Under light load the MOSFET must still be turned on and off by the control IC so the gate drive losses become much more significant. Secondly, the output charge Qoss and reverse recovery charge Qrr both generate losses that are transferred to Q1 and in- crease the dissipation in that device. Thirdly, gate charge will impact the MOSFETs’ susceptibility to Cdv/dt turn on. The drain of Q2 is connected to the switching node of the converter and therefore sees transitions between ground and Vin. As Q1 turns on and off there is a rate of change of drain voltage dV/dt which is capacitive coupled to the gate of Q2 and can induce a voltage spike on the gate that is sufficient to turn the MOSFET on, resulting in shoot-through current . The ratio of Qgd/Qgs1 must be min- imized to reduce the potential for Cdv/dt turn on. Figure A: Qoss Characteristic P loss Pconduction Pdrive Poutput * P loss Irms 2 R ds(on) Q g Vg f Qoss 2 V in f Q rr Vin f |
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