# On the Measurement of Switching Energy

The way to identify the transient starting and ending points varies between manufacturers and researchers. Some manufacturers define the starting point of the turn-on transient as when gate-to-source voltage v

_{gs}increases to 10% of its steady-state value VDR, and the ending point to be when the drain-to-source voltage v

_{ds}decreases to 2% of its steady-state value V

_{CC}. The turn-off transient is defined to begin when v

_{gs}decreases to 90% of VDR and ends when the drain current id decreases to 2% of the steady-state value I

_{D}.

Other manufacturers consider the starting point of the turn-on transient to be when v

_{gs}in-creases to 10% of V

_{DR}and ends when v

_{ds}decreases to 10% of V

_{CC}. The starting point of the turn-off transient is defined to be when v

_{gs}decreases to 90% of V

_{DR}and ends when v

_{ds}increases to 90% of V

_{CC}.

Both of these methods ignore the losses caused by the switching ringing, which are consid-ered by some researchers. The turn-on transient is defined as starting when the id is non-zero and ending when the peak-to-peak current of the ringing is 10% of I

_{D}. The turn-off transient is defined as beginning when id begins to decrease and ends when the peak-to-peak current of the ringing is 10% of I

_{D}. This method includes the ringing loss but also contains part of the conduction loss. The proportions of the conduction losses that are included are different for different devices under various test conditions. This would make a comparison of the devices unfair.

This work describes a method to calculate the switching energy independent of transient timing. The total loss energy E is calculated from switching energy E

_{switch}, conduction energy E

_{cond}, steady-state current I, resistance R

_{ds(on)}when the MOSFET is fully on, and on-time T

_{on}by

*E*=

*E*+

_{switch}*E*=

_{cond}*E*+

_{switch}*I*. Constant I is realized by a current source in simulation or large inductor in practice. "Constant R

^{2}R_{ds(on)}T_{on}_{ds(on)}" is approximated by "negligible variation in R

_{ds(on)}" by limiting the temperature rise induced by the power pulses in one period. By assigning T

_{on}to be a chosen on-time T

_{on1}, the associated total energy in one cycle E

_{1}could be obtained by simulation or experiment. By assigning Ton to be value T

_{on2}, the associated E

_{2}becomes known. The switching energy is then calculated by E

_{switch}= (E

_{1}T

_{on2}- E

_{2}T

_{on1})/(T

_{on2}- T

_{on1}). The switching energy calculated by the previous three existing methods based on the simulated power waveform differs from the simulated channel energy by more than 9%. The difference is reduced to 0.3% by using the proposed method.