In the most recent developments regarding energy saving, optimization and correct
selection of design components are considered a must in order to have improved electric
efficiency. An increasing sensitivity regarding energy problems has made companies and
consumers more demanding. In this context, cooperation and support between silicon
makers and customers is paramount: an exchange of experience leads to a better and
quicker way to realize new projects. In this article, we present an electronic ballast project
designed thanks to customer input. This application note describes the demonstration board
for 2X28 W electronic lamp ballast with active PFC. The ballast is formed by a part of the
PFC section and a self-oscillating half bridge converter. The circuit has been designed for a
nominal input voltage of 230 Vrms±15% and 50-60 Hz. The key components are the power
bipolar transistor (STD845DN40), the MOSFET device (STD3N62K3), and an ST power
switching driver for the PFC section. The purpose of this application note is to show a simple
and cheap lighting application optimized in terms of power factor (PFC), THD harmonic
distortion, and electric efficiency. The DC-AC converter section presents a layout solution
that offers the customer the possibility of using a bipolar transistor, or DIP 8 or SOT-82
package.
The system description is subdivided into two main sections, namely the PFC boost section
and half bridge converter. The system description starts with the PFC section and then
continues with the DC-AC converter. In the PFC section the method and the electrical
elements concerning the optimization of PFC and THD parameters are pointed out. In the
DC-AC converter section, the focus is the optimization of transistor bipolar driving.
4/24Doc ID 022164 Rev 1
AN3973Power factor section
2 Power factor section
The PFC section (boost converter) mainly consists of STD3N62K3 MOSFET SuperMESH3
technology and the L6562A power switching driver. The new SuperMESH3 technology is
obtained through the combination of fine tuning between standard SuperMESH and
MDMESH technology. This has resulted in the development of a new technology that
represents the optimization of the basic standard SuperMESH in terms of R
dynamic features. SuperMesh has integrated Zener diodes gate-to-source in order to
protect its gate-oxide from voltage spikes. The L6562A is a current-mode PFC controller
operating in transition mode. It has an improved performance compared to its predecessor,
the L6561.
Figure 2 shows the PFC section schematic plus the component values.
Figure 2.PFC section, boost converter diagram
DS(on)
* area and
!-V
The power factor consists of the displacement factor related to phase angle and the
distortion factor related to wave shape. The displacement factor is the ratio between the real
power (transferred to the output) and the apparent power (RMS line voltage times RMS line
current) drawn from the main, while the distortion factor is the ratio between the
fundamental component of the current and the total current:
Equation 1
Therefore, the section is designed in order to minimize input current distortion and forces the
input current to be in phase with the input voltage.
This system operates in transition mode, the boundary between continuous and
discontinuous current mode. The control simplicity and the inductor size, due to the low
inductance value needed, are the main advantages of this conduction current mode.
Doc ID 022164 Rev 15/24
Power factor sectionAN3973
2.1 PFC section design
The first step is to define the converter specifications that the user must set for the new PFC
boost topology project.
Table 1.Converter specification data and fixed parameters
NameSymbolValue
Input voltage rangeV
Nominal output voltageV
Nominal output powerP
INmin-VINmax
out
out
Target efficiencyn∼
Minimum switching frequencyf
s
180 Vac to 264 Vac
400 V
60 W
90%
35 kHz
Expected power factorPF0.99
At switching frequency, the inductor current is a triangle shape and the average value is half
of the peak of triangle. The resulting inductor current is shown in Figure 3, where it is also
shown that, by geometric relationships, the average value is the peak of sinewave input
current. The system operates the boundary between continuous and discontinuous
(transition mode current):
Figure 3.Inductor and input current waveform. MOSFET timing
Therefore the main operating conditions are:
●RMS input current
●Peak inductor current
●RMS inductor current
6/24Doc ID 022164 Rev 1
I
in
P
IL=
P
in
==
PFV
minAC
I22IL=
inpk
2
3
out
η
minAC
I
inRMS
AM10586v1
A374.0
=
PFV*
AN3973Power factor section
2.1.1 Input capacitor
The input filter capacitor (Cin) must reduce the high frequency voltage ripple across Cin and
the switching noise due to the high frequency inductor current ripple. The input capacitor
depends on the voltage ripple (r) and it is usually between 5% and 20% of the minimum
input voltage:
●Ripple voltage coefficient (%):
●Input capacitor
=
C
IN
π
1.0r =
I
in
r*V*f2
minACminSW
nF100
≈
In the applicative conditions, a polyester capacitor was chosen. It offers benefits in terms of
voltage stability and power factor (PF).
2.1.2 Output capacitor
The output capacitor is a function of voltage ripple (ΔV
ΔV
is usually selected at around 1.5% of the output voltage capacitor:
out
●Output capacitor
An electrolytic capacitor has been selected because it has low impedance (ESR) and
therefore provides good energy storage and improves the transient performance.
2.1.3 Boost inductor
The inductor boost depends on the several parameters and different approaches which can
be used. First, the inductor value is usually calculated so that the minimum switching
frequency is greater than the maximum frequency of the L6562A internal starter. Assuming
unity PF, it is possible to write:
●Instantaneous switching frequency
Therefore, the inductor value is determined at the top of the sinusoid () where the
switching frequency is the minimum:
●Inductor value
The optimum dynamic performances of the MOSFET device, selected for this application,
have allowed higher operation minimum frequency and consequently lower boost
inductance. In this case a 1.8 mH boost inductance was selected.
) and of the capacitor impedance.
out
C
=
Out
)V(L
=
AC
2
AC
P
out
−
VV*f4
Δπ
fθ−=
sw
outoutmain
P*Vf2
uF47
≈
2
1
AC
LP2
IN
)V2V(V
ACOut
INoutminSW
ACOut
V
out
))sin(V2V(V
π
=θ
2
2.1.4 Power MOSFET selection
MOSFET SuperMESH3 technology perfectly matches boost converter characteristics. In
fact, this technology has got a dynamic performance better than that of the standard
SuperMESH but not as good as MDMESH. That translates into having low switching power
losses and commutation which is not so fast that it implies ringing phenomenon such as
decreased PF and THD factors. MOSFET selection is based mainly on maximum voltage
rating, total power losses, and maximum operating temperature. In this case a MOSFET
device with minimum voltage rating 500 V (1.2*V
Doc ID 022164 Rev 17/24
=480 V) must be selected: 20% of V
BUS
BUS
Power factor sectionAN3973
indicates the safe margin. In the end, the MOSFET selection depended on power losses
and maximum operating temperature. MOSFET total power losses depend on conduction
and switching losses. The conduction losses at minimum input voltage are calculated by:
●Conduction losses
●RMS switch current
PcR
DS on()
2
I
⋅=
SWrms
senV2V
min
θ−
*senII
θ=
LpkSWrms
V3
inBUS
BUS
The switching losses in the MOSFET occur only during turn-off, because this boost topology
works in transition mode. Basically they can be expressed by:
●Switching power losses
Psw
where Qgd is the gate drain charge, I
f
s(ILRMS
) is switch frequency calculated for value.
=
is RMS inductor current, Ig is the gate current and
LRMS
I*V*Q
LBUSgd
RMS
I*2
g
)I(f
Ls
RMS
Based on the information above, the MOSFET choice was the STD3N62K3 device. The final
results show that STD3N62K3 ensures good performance in terms of electrical and thermal
behavior.
2.1.5 L6562A biasing circuitry
The dimensioning of biasing circuitry of the L6562A driver is reported for only a few
elements. In particular, the dimensioning is shown for those components that have been
relevant in terms of THD harmonic distortion and power factor (PF).
Figure 4.PFC section, relevant elements for THD and PFC factor
!-V
Pin2 (COMP). A feedback compensation network is put between this pin and INV in order to
fix narrow bandwidth and avoid high distortion of the input current waveform. In this way a
8/24Doc ID 022164 Rev 1
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