The electrical and thermal performances of switching converters are strongly influenced by
the behavior of the switching devices. Modern power devices design requires a trade-off in
terms of forward v oltage drop, breakdown voltage and switching speed. In AC-DC
converters such as PFC circuits, efficiency is strongly related to the switch perf ormances
and the diode recovery behavior (please refer to 1 in Bibliography on page 18). In the past
the benefits of the improved MOSFET performances have been generally spoiled by th e
diode current recovery behavior . In recent years the introduction of the Silicon Carbide (SiC)
Schottky diode has led to an effecti v e advantage in the switching transient losses reduction,
thanks to the very low re v erse reco v ery current with respect to the tr aditional fast diode. The
impact on the converter of the impro v ed ch aracteristics of bot h de vices lea ds to an increase
in efficiency.
In this application note the new generation of super-junction MOSFET (MDmesh
SiC diodes has been used to design a 200 W continuous PFC converter. The dynamic
characteristics of both super-junction MOSFET and SiC diodes , are investigated in the
actual application and compared with the traditional components in order to carry out the
qualitative and quantitative improvements in terms of switching performances and con v erter
efficiency. The presented experimental results allow analysis of inf ormation for the co nv erter
designers focusing on the determination of benefits and effectiveness of the de vices utiliz ed
in the considered application.
The following PFC design example is referred to as an experimental board, used for
demonstration purposes as described in AN628(please refer to 2 in Bibliography on
page 18). The design target specifications are:
●UNIVERSAL AC input supply voltage Vin
●DC output regulated voltage VO = 400 V
●Rated output power PO = 200 W
●Full-load output ripple ∆Vout-ripple = ±8 V
●Maximum overvoltage value ∆Vout = 50 V
●Switching frequency f
●Maximum Inductor current rip p le ∆IL = 35% of ILrms
The guidelines for controller design (L4981A) and power component selection can be found
in AN628 (please refer to 2 in Bibliography on page 18). In the next section instead we will
discuss the choice of the power MOSFET and boost diode.
= 88 V to 264 V
rms
4/20
AN2649Power MOSFET
2 Power MOSFET
Since the MOSFET device has to sustain a minimum blocking voltage value of 500 V
(V
= V
DSS
the R
DS(on)
+ VOUT - ripple + V
out
for its relation with the power dissipation.
The device STP12NM50N with its 500 V BV
T= 25 °C), is the best choice for the application. The losses at turn-on depend on the
selected boost diode and on the choice of the RG chosen to reduce the di/dt and therefore
the levels of EMI of the converter. As described in AN628 (please refer to 2) a gate
resistance of 15 Ω has been selected for turn-on, while a diode is used for a fast turn-off.
●The maximum "on state" power dissipation evaluated at the minimum input mains
voltage is:
), then the most important parameter for the se lection is
out
and the R
DSS
DS(on)
(R
DS(on)max
= 0.38 at
Equation 1
P
ON MAX–
●The switching (on + off) losses can be estimated as:
2
I
Qrmsmax
R
on max–
2.15()20.381.76 W=⋅=⋅=
Equation 2
where, P
while P
crossover
REC
In general P
P
SWPcrossoverPRECtcrVoutfswIrmsPREC
are the switching losses due to the crossover time of the power MOSFET
is the contribution due to the diode recovery.
depends on the di/dt value of the current MOSFET at turn-on (and this
REC
+⋅⋅⋅=+=
depends on the RG value selected and the intrinsic capacitance of the MOSFET) because
this di/dt sets the value of I
on the boost diode recovery current. To take into account the
RM
boost diode recovery effect, for the silicon diode, an easy approach is to compute two times
the current value (at turn-on). This means that P
is 1.5 times the P
SW
crossover
value, (see
AN628), but for the SiC diode we can suppose (thanks to superior switching performances)
that the P
value is negligible.
REC
Equation 3
P
SW
15ns 400V 100kHz 2.15A⋅⋅⋅()1.3 W==
The capacitive losses at turn-on to be added are:
Equation 4
P
capacitive
10
------
C
3
OSS
1.5
V
out
10
------
f
sw
230pF400()
3
1.5
100kHz0.6 W=⋅⋅⋅=⋅⋅ ⋅≈
where C
is the drain capacitance at VDS= 25 V.
oss
To reduce the switching losses at turn-off, a RCD snubber is used and in order to keep the
junction temperature at a saf e le vel at w orst case condition, lo w-line input v oltage (88 V) and
full load (200 W), a small heatsink is used.
5/20
Booster diodeAN2649
3 Booster diode
The booster diode is selected to withstand the output voltage and current. Moreover, it has
to be as fast as possible in order to reduce the power switch losses (please refer to 3 in
Bibliography on page 18). The STPSC806D (600 V/8 A) SiC diode matches these
specifications and is especially suitable for this application. This part offers the best so lution
for the continuous current mode operation due to its very fast recovery time, 15 ns typical.
The diode power losses can be split in two contributions: conduction losses and switching
losses.
The conduction losses can be estimated by:
Equation 5
⋅+⋅=
16 V
⋅
-------------------------- -=
3 π V
⋅⋅
I
2
lpk
Drms
out
with
Equation 6
P
DonVtoIoutRd
P
out
I
Drms
---------- -
V
lpk
The switching losses are:
Equation 7
P
swVout
Qrr f
⋅⋅=
SW
where
●V
●R
●V
●V
●I
●Qrr= total inverse recovery charge of diode
= threshold voltage
to
= differential resistance
d
= line voltage peak value
lpk
= DC output voltage
out
= RMS value of diode current
Drms
At low-line input voltage the conduction losses are bigger with respect to the case of highline voltage while the switching losses are always negligible due to the small value of Qrr f or
every value of di/ dt of curr ent im posed b y the MOSFET (at turn-on). The last instance is not
true for the silicon diode, because Qrr is bigger and greatly depends on the di/dt value.
Furthermore the silicon diode performance are temperature-dependent (Vf, recovery
current, etc.), while the SiC diode has the same behavior also for high temperature (please
refer to 1 in Bibliography on page 18). In the worst case:
Equation 8
P
DonVtoIoutRd
2
I
Drms
0.9V 0.5A0.065Ω 1.282A20.55 W=⋅+⋅=⋅+⋅=
Equation 9
Another important parameter to take into account for the choice of boost diode is the I
value. At startup the output capacitor sinks much current (it is discharged) and the boost
6/20
P
0W≅
SW
FSM
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