Solution for designing a 400 W fixed-off-time controlled
PFC preregulator with the L6563S and L6563H
Introduction
In addition to the transition mode (TM) and fixed-frequency continuous conduction mode
(FF-CCM) operation of PFC preregulators, a third approach is proposed that couples the
simplicity and affordability of TM operation with the high-current capability of FF-CCM
operation. This solution is a peak current-mode control with fixed-off-time (FOT). Design
equations are given and a practical design for a 400 W board is illustrated and evaluated.
Two methods of controlling power factor corrector (PFC) preregulators based on boost
topology are currently in use: the fixed-frequency (FF) PWM and the transition mode (TM)
PWM (fixed on-time, variable frequency). The first method employs average current-mode
control, a relatively complex technique requiring sophisticated controller ICs (e.g. the
L4981A/B from STMicroelectronics) and a considerable component count. The second uses
the simpler peak current-mode control, which is implemented with cheaper controller ICs
(e.g. the L6561, L6562, L6562A and L6563S from STMicroelectronics), and far fewer
external parts, therefore it is far less expensive. In the first method the boost inductor works
in continuous conduction mode (CCM), while TM makes the inductor work on the boundary
between continuous and discontinuous mode, by definition. For a given power throughput,
TM operation involves higher peak currents as compared to FF-CCM (Figure 1 and
Figure 2).
Figure 1.Line, inductor, switch and diode
currents in FF-CCM PFC
AN3142
Application note
Figure 2.Line, inductor, switch and diode
currents in TM PFC
This demonstration, consistent with the above mentioned cost considerations, suggests the
use of TM in a lower power range, while FF-CCM is recommended for higher power levels.
This criterion, though always true, is sometimes difficult to apply, especially for a midrange
power level, around 150-300 W. The assessment of which approach gives the better
cost/performance trade-off needs to be done on a case-by-case basis, considering the cost
and the stress of not only power semiconductors and magnetic but also of the EMI filter. At
the same power level, the switching frequency component to be filtered out in a TM system
is twice the line current, whereas it is typically 1/3 or 1/4 in a CCM system.
In this area where the TM/CCM usability boundary is uncertain, a third approach that
couples the simplicity and affordability of TM operation with the high-current capability of
CCM operation may be a solution to the dilemma. Generally speaking, FF PWM is not the
only alternative when CCM operation is desired. FF PWM modulates both switch ON and
OFF times (their sum is constant by definition), and a given converter operates in either
CCM or DCM depending on the input voltage and the loading conditions. Exactly the same
result can be achieved if the on-time only is modulated and the off-time is kept constant, in
which case, however, the switching frequency is no longer fixed (Figure 3 and Figure 4).
This is referred to as “fixed-off-time” (FOT) control. Peak-current-mode control can still be
used.
Figure 3.Basic waveforms for fixed
frequency PWM
An important factor is that FOT control does not need a specialized control IC. A simple
modification of a standard TM PFC controller operation, requiring just a few additional
passive parts and no significant extra cost, is all that is needed.
Figure 4.Basic waveforms for fixed-off-time
PWM
4/44Doc ID 17005 Rev 3
AN3142Operation of an FOT-controlled PFC preregulator
2 Operation of an FOT-controlled PFC preregulator
Figure 5 shows a block diagram of an FOT-controlled PFC preregulator. An error amplifier
(VA) compares a portion of the preregulator's output voltage Vout with a reference VREF
and generates an error signal V
hypothesis, is fed into an input of the multiplier block and multiplied by a portion of the
rectified input voltage V
V
, which has an amplitude proportional to that of V
CSREF
MULT
the sinusoidal reference for PWM modulation. V
comparator that, on the non-inverting input, receives the voltage V
R
, proportional to the current flowing through switch M (typically a MOSFET) and the L
sense
inductor during the on-time of M. When the two voltages are equal, the comparator resets
the PWM latch and M, supposedly already ON, is switched OFF.
Figure 5.Block diagram of an FOT-controlled PFC pre-regulator
proportional to their difference. VC, a DC voltage by
C
. At the output of the multiplier, there is a rectified sinusoid,
and to VC, which represents
MULT
is fed into the inverting input of a
CSREF
on the sense resistor
CS
As a result, V
V
is a rectified sinusoid, the inductor peak current is also enveloped by a rectified
CSREF
determines the peak current through the M and the L inductor. As
CSREF
sinusoid. The line current Iin is the average inductor current that is the low-frequency
component of the inductor current resulting from the low-pass filtering operated by the EMI
filter. The PWM latch output Q going high activates the timer that, after a predetermined
time in which T
another switching cycle. If T
has elapsed, sets the PWM latch, therefore turning M on and starting
OFF
is such that the inductor current does not fall to zero, the
OFF
system operates in CCM. It is apparent that FOT control requires almost the same
architecture as TM control, just the way the off-time of M is determined also changes. It is
not a difficult task to modify externally the operation of the standard TM PFC controller so
that the off-time of M is fixed. As a controller we refer to the L6563S [4], which is suitable for
power applications of a few hundred watts because of its gate drive capability and its high
noise immunity. For a more detailed and complex description of the fixed off-time technique
and in particular the line modulated FOT, please refer to [5].
Doc ID 17005 Rev 35/44
The circuit implementing the line-modulated fixed-off-time with the new L6563SAN3142
3 The circuit implementing the line-modulated fixed-
off-time with the new L6563S
The circuit that implements LM-FOT control with the L6563S is shown in Figure 6. During
the on-time of the MOSFET the gate voltage V
biased and the voltage at the ZCD pin is internally clamped at V
off-time of M V
= 10 V is low, the D diode is reverse-biased and the voltage at the pin
GD
decays with an exponential law until it reaches the triggering threshold (V
that causes the switch to turn on. The time needed for the ZCD voltage to go from V
to V
ZCDtrigger
defines the duration of the off-time T
Figure 6.Circuit implementing FOT control with the L6563S
= 15 V is high, the D diode is forward
GD
OFF
ZCDclamp
.
5.7 V. During the
ZCDtrigger
0.7 V)
ZCDclamp
The circuit in Figure 6. makes T
a function of the RMS line voltage thanks to the peak
OFF
holding effect of T1 (which acts as a buffer) along with R and C whose time constant is
significantly longer than a line half-cycle. With the addition of R0 and T1, as long as the
voltage on the ZCD pin during T
is above V
OFF
mult+VBE
following the law:
Equation 1
As V’
′
(t) falls below V
ZCD
⎡
⎢
⎣
V)t(V
ZCDclampZCD
mult+VBE
R
()
−=
+
RR
0
+⋅
, T1 is cut off and C is discharged through R only, so that
its evolution from that point on is described by:
Equation 2
′′
ZCD
V'
(t) decreases from V
ZCD
6/44Doc ID 17005 Rev 3
ZCDclamp
R
)t(V
=
RR
+
0
= 5.7 V to V
()
⎤
eVV
⎥
BEmult
⎦
mult+VBE
, C is discharged through R and R0,
)RR(t
+⋅
0
−
()
⋅
0
eVV
⋅+⋅
BEmult
R
CRR
+⋅
t
−
CR
⋅
()
RR
+
0
VV
+⋅
BEmult
in the following time period t':
AN3142The circuit implementing the line-modulated fixed-off-time with the new L6563S
Equation 3
⎤
⎥
⋅+−+⋅
RVV)RR(V
⎥
BEmult0ZCDclamp
⎦
and V''
′
t
(t) decreases from V
ZCD
⋅
RR
0
−=
+
RR
0
⎡
⋅⋅
lnC
⎢
⎢
⎣
mult+VBE
to V
()
⋅+
RVV
0BEmult
()
ZCDtrigger
= 0.7 V level in the following time
period t'':
Equation 4
Figure 7
V
⎡
′′
⋅−=
lnRCt
⎢
ZCDtrigger
⎣
illustrates the signal on the ZCD pin with the two discharging time constants
⎤
⎥
+
VV
BEmult
⎦
depending on the two resistors R, R0 and the L6563S parameters, particularly the upper
clamp voltage and the triggering voltage of the ZCD pin.
Figure 7.ZCD pin signal with the fixed off-time generator circuit
The sum of the two time periods is the off-time function:
Equation 5
OFF
⎡
R
⎢
RCT
⋅−=
+
⎢
⎣
⎡
0
ln
⋅
⎢
RR
⎢
0
⎣
()
RVV
⋅+
0BEmult
()
In this way, once the multiplier operating point (that is, the V
proper selection of R and R0 it is possible to increase T
maximum line voltage, it is always T
ON>TONmin
= 450 ns for the L6563S [4]. This is a
condition needed in order to avoid line distortion [
Doc ID 17005 Rev 37/44
OFF
5].
⎤
⎥
RVV)RR(V
⋅+−+⋅
⎥
BEmult0ZCDclamp
⎦
/ VAC ratio) is fixed, with a
mult
V
⎛
ZCDtrigger
⎜
+
ln
⎜
()
⎝
+
⎤
⎞
⎟
⎥
⎟
VV
⎥
BEmult
⎠
⎦
with the line voltage so that, at
The circuit implementing the line-modulated fixed-off-time with the new L6563SAN3142
It is easy to see that T
technique as “line-modulated fixed-off-time” (LM-FOT) [
is now a function of the instantaneous line voltage. We refer to this
OFF
5].
This modification, though simple, introduces profound changes in the timing relationships,
with a positive influence on the energetic relationships. From the control point of view,
modulating T
is a feedforward term that modifies the gain but does not change its
OFF
characteristics. Consequently, all of the properties of the standard FOT control are
maintained. Due to the highly non-linear nature of the T
modulation introduced by T1
OFF
and R0, its effects are discussed only qualitatively and the quantitative aspects are provided
graphically for a specific case in [
5].
As a practical rule, it is convenient to first select a capacitor and then to calculate the resistor
needed to achieve the desired T
As the gate voltage V
as possible up to V
goes high, the Rs resistor charges the timing capacitor C as quickly
GD
ZCDclamp
, without exceeding clamp rating (I
(see Section 4.3.7 on page 20).
OFF
=10 mA). Then it must
ZCDx
fulfill the following inequalities:
Equation 6
−−
VVV−−
I
ZCDx
V
+
FZCDclampGDx
ZCDclamp
R
RRs
⋅<<
V
ZCDclamp
where VGD (assume VGD = 10 V) is the voltage delivered by the gate driver, V
VVV
FZCDclampGD
= 15 V its
GDx
maximum value, and VF the forward drop on D.
When working at high line/light load the on-time of the power switch becomes very short and
the Rs resistor alone is no longer able to charge C up to V
ZCDclamp
. The speed-up capacitor
Cs is then used in parallel to Rs. This capacitor causes an almost instantaneous charge of C
up to a level, after that Rs completes the charge up to V
ZCDclamp
. It is important that the
steep edge caused by Cs does not reach the clamp level, otherwise the internal clamp of the
L6563S undergoes uncontrolled current spikes (limited only by the dynamic resistance of
the 1N4148 and the ESR of Cs) that could overstress the IC. Cs must then be:
Equation 7
V
CCs−−<
ZCDclamp
VVV
FZCDclampGDx
8/44Doc ID 17005 Rev 3
AN3142Designing a fixed-off-time PFC
4 Designing a fixed-off-time PFC
4.1 Input specification
This first part is a detailed specification of the operating conditions of the circuit that is
needed for the following calculations in
wide input range mains PFC circuit has been considered. Some design criteria are also
given.
Section 4.2 on page 11. In this example a 400 W,
●Mains voltage range (VAC rms):(1)
●Minimum mains frequency:(2)
●Rated output power (W):(3)
out
min
Hz47fl=
=
Vac90VAC
=
max
W400P
Vac265VAC
=
Because the PFC is a boost topology, the regulated output voltage depends strongly on the
maximum AC input voltage. In fact, for correct boost operation the output voltage must
always be higher than the input and therefore, because Vin max is V
, the output has been
pk
set at 400 Vdc as the typical value. If the input voltage is higher, as typical in ballast
applications, the output voltage must be set higher accordingly. As a rule of thumb the
output voltage must be set 6/7% higher than the maximum input voltage peak.
●Regulated DC output voltage (Vdc)(4)
out
=
V400V
The target efficiency and PF are set here at minimum input voltage and maximum load.
They are used for the following operating condition calculation of the PFC. Of course at high
input voltage the efficiency is higher.
P
●Expected efficiency (%):(5)
out
P
in
%90
==η
●Expected power factor:(6)
99.0PF =
Because of the narrow loop voltage bandwidth, the PFC output can face overvoltages at
startup or in case of load transients. To protect from excessive output voltage that can
overstress the output components and the load, in the L6563S a device pin (PFC_OK, pin
#6) has been dedicated to monitor the output voltage with a separate resistor divider,
selected so that the voltage at the pin reaches 2.5 V if the output voltage exceeds a preset
value (Vovp), usually larger than the maximum Vout that can be expected, also including
worst-case load/line transients.
V430V
●Maximum. output voltage (Vdc):(7)
Doc ID 17005 Rev 39/44
OVP
=
Designing a fixed-off-time PFCAN3142
The mains frequency generates a 2fL voltage ripple on the output voltage at full load. The
ripple amplitude determines the current flowing into the output capacitor and the ESR.
Additionally, a certain holdup capability in case of mains dips can be requested from the
PFC in which case the output capacitor must also be dimensioned, taking into account the
required minimum voltage value (V
) after the elapsed holdup time (t
out min
Hold
).
●Maximum output low frequency ripple:(8)
●Minimum output voltage after line drop (Vdc):(9)
ms20t
●Holdup capability (ms):(10)
Hold
=
out
V10V
=∆
V300V
=
minout
The PFC minimum switching frequency is one of the main parameters used to dimension
the boost inductor. Here we consider the switching frequency at low mains on the top of the
sinusoid and at full load conditions. As a rule of thumb, it must be higher than the audio
bandwidth in order to avoid audible noise and additionally it must not interfere with the
L6563S minimum internal starter period, as given in the datasheet. On the other hand, if the
minimum frequency is set too high the circuit shows excessive losses at higher input voltage
and probably operates skipping switching cycles not only at light load. Typical minimum
frequency range is55-95 kHz for wide range operation.
●Minimum switching frequency (kHz)(11)
Where f
= 1/(T+220 nsec) due to the ZCD - gate drive signal delay typical of the
swmin
minsw
kHz80f
=
L6563S.
The design is to be done on the basis of a ripple factor (the ratio of the maximum current
ripple amplitude to the inductor peak current at minimum line voltage) kr=0.34.
●Ripple factor(12)
In order to properly select the power components of the PFC and dimension the heat sinks
in case they are needed, the maximum operating ambient temperature around the PFC
circuitry must be known. Please note that this is not the maximum external operating
temperature of the entire equipment, but it is the local temperature at which the PFC
components are working.
●Maximum ambient temperature (°C):(13)
10/44Doc ID 17005 Rev 3
ambx
34.0kr=
C50T
°=
AN3142Designing a fixed-off-time PFC
4.2 Operating condition
The first step is to define the main parameters of the circuit, using the specification points
given in
Rated DC output current:
Equation 8
Section 4.1 on page 9:
I=
out
P
out
I
out
V
out
W400
V400
A00.1
==
Maximum input power:
Equation 9
P
out
=
P
in
P
in
η
90
W400
=⋅=
W44.444100
Referring to the main currents shown in Figure 1, the following formula expresses the
maximum value of current circulating in the boost cell which means at minimum line voltage
of the selected range:
RMS input current:
Equation 10
P
I
=
in
out
min
I
=
in
PFVAC
⋅
W400
99.0Vac90
⋅
A99.4
=
It is important to define the following ratios in order to continue describing the energetic
relationships in the PFC:
Equation 11
min
2k=
Equation 12
VAC
max
2k=
From Equation 11 and Equation 12:
Line peak current:
Equation 13
I
maxPK
⋅
=
Inductor Ripple-∆ILpk:
Doc ID 17005 Rev 311/44
VAC
V
V
out
P2
in
Vk
⋅
outmin
out
min
max
Vac90
min
max
I
maxPK
2k
Vac265
2k
⋅
=
⋅
32.0
==
V400
94.0
==
V400
W44.4442
V40032.0
A98.6
=
Designing a fixed-off-time PFCAN3142
Equation 14
k6
⋅
IL⋅
=∆
pk
r
k38
⋅−
r
I
IL
maxPK
=∆
pk
34.06
⋅
34.038
⋅−
A04.2A98.6
=⋅
Inductor peak current:
Equation 15
IL⋅
maxpk
8
=
k38
⋅−
r
I
IL
maxPK
maxpk
8
=
34.038
⋅−
A01.8A98.6
=⋅
It is also possible to calculate the RMS current flowing into the switch and into the diode,
needed to calculate the losses of these two elements.
RMS switch current:
Equation 16
⋅
ISW
rms
P
in
=
⋅
Vk
2
outmin
k16
min
−⋅
3
ISW
π
rms
=
W400
⋅
2
−⋅
V40032.0
32.016
⋅
3
π
A22.4
=
RMS diode current:
Equation 17
ID
rms
P
in
=
⋅
Vk
outmin
k16
min
⋅
ID
=
π
3
rms
W400
⋅
V40032.0
⋅
32.016
⋅
3
π
A57.2
=
It is worth remembering that the accuracy of the approximate energetic relationships
described here is quite good at maximum load for low values of parameter k, that is, at low
line voltage, but worsens at high line and as the power throughput is reduced. Since in the
design phase current stress is calculated at maximum load and minimum line voltage, their
accuracy is acceptable for design purposes.
12/44Doc ID 17005 Rev 3
AN3142Designing a fixed-off-time PFC
4.3 Power section design
4.3.1 Bridge rectifier
The input rectifier bridge can use standard slow recovery, low-cost devices.
Typically a 600 V device is selected in order to have good margin against mains surges. An
NTC resistor limiting the current at turn-on is required to avoid overstress to the diode
bridge.
The rectifier bridge power dissipation can be calculated using
and
Equation 20. The threshold voltage (V
diode of the bridge can be found in the component datasheet.
Equation 18
Equation 19
The power dissipated on the bridge is:
Equation 20
4.3.2 Input capacitor
bridge
I
inrms
I
Equation 18, Equation 19,
) and dynamic resistance (Rdiode) of a single
th
I2
⋅
in
=
=
avg_in
=
2
I2
⋅
in
=
π
2
diodebridge
inrms
2
A99.42
⋅
2
A99.42
⋅
π
A53.3
=
A25.2
=
IV4IR4P⋅⋅+⋅⋅=
avg_inth
W53.7A25.2V7.04)A53.3(025.04P
=⋅⋅+⋅Ω⋅=
The input filter capacitor (Cin) is placed across the diode bridge output. This capacitor must
smooth the high-frequency ripple and must sustain the maximum instantaneous input
voltage. In a typical application an EMI filter is placed between the mains and the PFC
circuit. In this application the EMI filter is reinforced by a differential mode Pi-filter after the
bridge to reject the differential noise coming from the whole switching circuit. The design of
the EMI filter (common mode and differential mode) is not described here. The value of the
input filter capacitor can be calculated as follows, simply considering the output power that
the PFC should deliver at full load:
Equation 21
−
3
in
P105.2C⋅⋅=
out
in
3
−
F1W400105.2C
µ=⋅⋅=
The maximum value of this capacitor is limited to avoid line current distortion. The value
chosen for this design is 1µF.
Doc ID 17005 Rev 313/44
Designing a fixed-off-time PFCAN3142
4.3.3 Output capacitor
The output bulk capacitor (Co) selection depends on the DC output voltage (4), the allowed
maximum voltage
The 100/120 Hz (twice the mains frequency) voltage ripple (∆Vout = peak-to-peak ripple
(8) is a function of the capacitor impedance and the peak capacitor current:
value)
Equation 22
(7), and the converter output power (3).
I2V+
⋅⋅=∆
outout
1
2
)Cf22(
⋅⋅π
Ol
ESR
2
With a low ESR capacitor the capacitive reactance is dominant, therefore:
Equation 23
I
C
O
out
≥
=
∆⋅⋅π
Vf2
outl
P
out
∆⋅⋅⋅π
C
≥
VVf2
O
outoutl
W400
V10V400Hz472
⋅⋅⋅π
F338
µ=
Vout is usually selected in the range of 1.5% of the output voltage. Although ESR does not
usually affect the output ripple, it should be taken into account for power loss calculations.
The total RMS capacitor ripple current, including mains frequency and switching frequency
components, is:
Equation 24
Crms
2
2
rms
IIDI−=
out
Crms
()()
22
A36.2A0.1A56.2I
=−=
If the PFC stage must guarantee a specified holdup time, the selection criterion of the
capacitance changes. Co has to deliver the output power for a certain time (t
specified maximum dropout voltage (V
(which takes load regulation and output ripple into account). V
) that is the minimum output voltage value
out min
is the minimum output
out min
Hold
) with a
operating voltage before the 'power fail' detection and consequent stopping by the
downstream system supplied by the PFC.
Equation 25
⋅⋅
tP2
out
Holdout
2
2
−∆−
VVV
C
=
O
minout
()()
=
C
O
()
out
A 20% tolerance on the electrolytic capacitors must be taken into account for the right
dimensioning.
Following the relationship (
Equation 25), for this application a capacitor Co = 330 µF (450 V)
has been selected in order to maintain a holdup capability for 22 ms. The actual output
voltage ripple with this capacitor is also calculated. In detail:
14/44Doc ID 17005 Rev 3
ms20W4002
⋅⋅
22
V300V10V400
−−
F3.242
µ=
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