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SC2441AEVB датащи(PDF) 31 Page - Semtech Corporation |
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SC2441AEVB датащи(HTML) 31 Page - Semtech Corporation |
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31 / 37 page ![]() 31 2006 Semtech Corp. www.semtech.com POWER MANAGEMENT SC2441A Applications Information In Figure 21, Q gs1 is the gate charge needed to bring the gate-to-source voltage V gs to the threshold Vgs_th, Q gs2 is the additional gate charge required for the switch current to reach its full-scale value I ds . and Q gd is the charge needed to charge gate-to-drain (Miller) capacitance when V ds is falling. Switching losses occur during the time interval [t 1, t3]. Defining t r = t3-t1. tr can be approximated as . V V R ) Q Q ( t gsp cc gt gd 2 gs r - + = where R gt is the total resistance from the driver supply rail to the gate of the MOSFET. It includes the gate driver internal impedance R gi, external resistance Rge and the gate resistance R g within the MOSFET i.e. R gt = Rgi+Rge+Rg. V gsp is the Miller plateau voltage shown in Figure 21. Similarly an approximate expression for t f is . gsp gt gd gs2 f V )R Q (Q t + = Only a portion of the total losses P g = QgVccfs is dissipated in the MOSFET package. Here Q g is the total gate charge specified in the datasheet. The power dissipated within the MOSFET package is . f V Q R R P s cc g gt g tg = The total power loss of the top switch is then P t = Ptc+Pts+Ptg. If the input supply of the power converter varies over a wide range, then it will be necessary to weigh the relative importance of conduction and switching losses. This is because conduction loss is inversely proportional to the input voltage. Switching loss however increases with the input voltage. The total power loss of MOSFET should be calculated and compared for high-line and low-line cases. The worst case is then used for thermal design. Bottom Switch: The RMS current in bottom switch can be calculated . ) 1 )( D 1 ( I I 12 o rms , 2 Q 2 d + - = The conduction loss is then P bc=IQ2,rms 2 R ds(on), where R ds(on) is the channel resistance of bottom MOSFET. If the input voltage to output voltage ratio is high (e.g. V in=12V, Vo=1.5V), the duty ratio D will be small. Since the bottom switch conducts with duty ratio (1-D), the corresponding conduction losses can be quite high. Due to non-overlapping conduction between the top and the bottom MOSFET’s, the internal body diode or the external Schottky diode across the drain and source terminals always conducts prior to the turn on of the bottom MOSFET. The bottom MOSFET switches on with only a diode voltage between its drain and source terminals. The switching loss s d o 2 f r 2 1 bs f V I) 1 )( t t ( P d + + = is negligible due to near zero-voltage switching. The gate loss is estimated as . f V Q R R P s cc g gt g bg = The total bottom switch loss is then P b=Pbc+Pbs+Pbg. Once the power losses P loss for the top (Pt) and bottom (P b) MOSFET’s are known, thermal and package design at component and system level should be done to verify that the maximum die junction temperature (T j,max, usually 125oC) is not exceeded under the worst-case conditions. The equivalent thermal impedance from junction to ambient ( θ ja) should satisfy . P T T loss max , a max ,j ja - £ q θ ja depends on the die to substrate bonding, packaging material, the thermal contact surface, thermal compound property, the available effective heat sink area and the air flow condition (free or forced convection). Actual temperature measurement of the prototype should be carried out to verify the thermal design. Integrated Power MOSFET Drivers There are four internal MOSFET drivers in a dual- channel step-down converter. |
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