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AN4242 Datasheet(PDF) 5 Page - STMicroelectronics |
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AN4242 Datasheet(HTML) 5 Page - STMicroelectronics |
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5 / 26 page ![]() DocID024196 Rev 1 5/26 AN4242 Features of the SiC diodes After simplification and introduction of the junction capacitance variation versus the reverse voltage Cj(V), Qc is defined by the following formula: Equation 3 This relation demonstrates that Qc is defined by the integral of the junction capacitance Cj between 0 and VR, the voltage reapplied on the diode. This theoretical approach allows the direct and accurate evaluation of Qc, avoiding the inaccuracy introduced by potential measurement problems. The strict expression of the energy stocked in the junction capacitor for a given reverse voltage can be determined by: Equation 4 Due to the non-linearity of the junction capacitance versus the reverse voltage, this relation is different from the traditional energy formula ½ · C · V² (or ½ · Q · V), which is valid only when considering a constant capacitance. 1.2 Forward characteristics Another main feature of SiC diodes is the variation of the forward voltage drop (VF) with the junction temperature. Figure 3 shows the forward current versus forward voltage drop characteristics for 3 different junction temperature levels. A crossing-point can be observed at a certain level of current IC. When the current is lower than this level, the temperature coefficient of the forward voltage drop ( V F) is negative. When the current is higher, it becomes positive. The same crossing point exists for traditional silicon diodes, but it appears at a much higher current level (>10 times the nominal current). This is linked to the higher forward current density of SiC diodes. ò Qc(V ) = R VR 0 Cj(V) dV ò Qc(V ) = R VR 0 Cj(V) · V dV |
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