Solution for designing a 400 W fixed-off-time controlled
PFC preregulator with the L6562A
Introduction
In addition to the transition mode (TM) and fixed-frequency continuous conduction mode
(FF-CCM) operation of PFC pre-regulators, 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) pre-regulators 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 one
uses the simpler peak current-mode control, which is implemented with cheaper controller
ICs (e.g. the L6561, L6562, L6562A from STMicroelectronics), much fewer external parts
and is therefore much 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 2).
Figure 1.Line, inductor, switch and diode
currents in FF-CCM PFC
AN2782
Application note
Figure 2.Line, inductor, switch and diode
currents in TM PFC
"CCM" type
IL
"TM" type
IL
IAC
IAC
ON
MOSFET
OFF
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.
Figure 32.EVL6562A-400W: input current waveform at 100 V - 50 Hz - 400 W load . . . . . . . . . . . . . 34
Figure 33.EVL6562A-400W: input current waveform at 230 V -50 Hz - 400 W load . . . . . . . . . . . . . 34
Figure 34.EVL6562A-400W: input current waveform at 100 V - 50 Hz - 200 W load . . . . . . . . . . . . . 34
Figure 35.EVL6562A-400W: input current waveform at 230 V - 50 Hz - 200 W load . . . . . . . . . . . . . 34
Figure 36.EVL6562A-400W: input current waveform at 100 V - 50 Hz - 70 W load . . . . . . . . . . . . . . 35
Figure 37.EVL6562A-400W: input current waveform at 230 V - 50 Hz - 70 W load . . . . . . . . . . . . . . 35
Doc ID 14763 Rev 23/39
Introduction to FOT controlAN2782
1 Introduction to FOT control
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 can 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-
Gate drive
signal
frequency PWM
TON'
TON'
TOFF'
TOFF'
TON
TON
TOFF
TOFF
TSWTSW
TSW TSW
TON'
TON'
TON
TON
TOFF'
TOFF'
TOFF
TOFF
TON'
TON'
TON
TON
An important point 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
Gate drive
signal
TON'TON'TON'
TON'TON'TON'
TOFF TOFF
TOFF TOFF
TSW'TSW'
TSW'TSW'
TONTON TONTOFF TOFF
TON TON TON TOFF TOFF
TSW TSW
TSW TSW
4/39Doc ID 14763 Rev 2
AN2782Operation of an FOT-controlled PFC pre-regulator
2 Operation of an FOT-controlled PFC pre-regulator
Figure 5 shows a block diagram of an FOT-controlled PFC pre-regulator. An error amplifier
(VA) compares a portion of the pre-regulator'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
, whose amplitude is proportional to that of V
CSREF
MULT
sinusoidal reference for PWM modulation. V
comparator that, on the non-inverting input, receives the voltage V
Rsense, proportional to the current flowing through the switch M (typically a MOSFET) and
the inductor L 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 will be a rectified sinusoid,
and to VC, which represents the
MULT
is fed into the inverting input of a
CSREF
on the sense resistor
CS
As a result, V
determines the peak current through M and the inductor L. As V
CSREF
CSREF
is
a rectified sinusoid, the inductor peak current is enveloped by a rectified sinusoid as well.
The line current Iin will be 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
T
has elapsed, sets the PWM latch, thus turning M on and starting another switching
OFF
cycle. If T
is such that the inductor current does not fall to zero, the system operates in
OFF
CCM. It is apparent that FOT control requires nearly the same architecture as TM control,
just the way the off-time of M is determined 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 will refer to the L6562A [4], which is suitable for a few hundred watts
power applications 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 [7].
Doc ID 14763 Rev 25/39
The circuit implementing the line-modulated fixed off-time with the new L6562AAN2782
(
3 The circuit implementing the line-modulated fixed
off-time with the new L6562A
The circuit that implements LM-FOT control with the L6562A 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 diode D 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 L6562A
= 15 V is high, the diode D is forward-
GD
OFF
ZCDclamp
.
≈ 5.7 V. During the
ZCDtrigger
≈ 0.7 V)
ZCDclamp
The circuit ofFigure 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 R
voltage on the ZCD pin during T
is above V
OFF
mult+VBE
, C is discharged through R and R0,
and T, as long as the
0
following the law:
)RR(t
+⋅
0
−
′
As V’
⎡
V)t(V
⎢
ZCDclampZCD
⎣
(t) falls below V
ZCD
−=
0
mult+VBE
R
()
RR
+
, T1 is cut off and C is discharged through R only, so that
⎤
()
⋅
0
+⋅
eVV
⎥
BEmult
⎦
R
CRR
+⋅
()
RR
+
0
+⋅
(1)
VV
BEmult
its evolution from that point on is described by:
V'
(t) decreases from V
ZCD
′
t
′′
ZCD
ZCDclamp
⋅
RR
0
−=
+
RR
0
R
)t(V
=
()
RR
+
0
= 5.7 V to V
BEmult
mult+VBE
⎡
⋅⋅
lnC
⎢
⎢
⎣
t
−
CR
⋅
eVV
⋅+⋅
(2)
in the following time period t':
)
⋅+
RVV
0BEmult
()
⎤
⎥
⋅+−+⋅
RVV)RR(V
⎥
BEmult0ZCDclamp
⎦
(3)
6/39Doc ID 14763 Rev 2
AN2782The circuit implementing the line-modulated fixed off-time with the new L6562A
and V''
(t) decreases from V
ZCD
mult+VBE
to V
ZCDtriggering
= 0.7 V level in the following time
period t'':
V
⎡
′′
⋅−=
lnRCt
ZCDtrigger
⎢
⎣
⎤
⎥
+
VV
BEmult
⎦
(4)
Figure 7 illustrates the signal on the ZCD pin with the two discharging time constants
depending on the two resistors R, R
and the L6562A parameters, particularly the upper
0
clamp voltage and the triggering voltage of the ZCD pin.
Figure 7.ZCD pin signal with the fixed off-time generator circuit
6
6
6
ZCDclamp
ZCDclamp
ZCDclamp
5
5
5
4
4
4
3
3
3
Vzcd (V)
Vzcd (V)
Vzcd (V)
2
2
2
′
′
′
ZCD
ZCD
ZCD
)(tV
)(tV
)(tV
′′
′′
′′
)(tV
)(tV
)(tV
ZCD
ZCD
ZCD
VV
7.5=
VV
7.5=
VV
7.5=
VV+
VV+
VV+
BEmult
BEmult
BEmult
1
1
1
0
0
0
02468
02468
02468
′
′
′
t
t
t
usec
usec
usec
′′
′′
′′
t
t
t
T
T
T
OFF
OFF
OFF
ZCDtrigger
ZCDtrigger
ZCDtrigger
VV
7.0=
VV
7.0=
VV
7.0=
The sum of the two time periods is the OFF-time function:
⎤
⎞
(5)
⎟
⎥
⎟
VV
⎥
BEmult
⎠
⎦
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 R
maximum line voltage, it is always T
condition needed in order to avoid line distortion[
It is easy to see that T
OFF
it is possible to increase T
0
ON>TONmin
= 450 ns for the L6562A [4]. This is a
OFF
7].
is now a function of the instantaneous line voltage. We will refer to
this technique as “line-modulated fixed off-time” (LM-FOT) [
⎤
⎥
⋅+−+⋅
RVV)RR(V
⎥
BEmult0ZCDclamp
⎦
/VAC ratio) is fixed, with a
mult
V
⎛
ZCDtrigger
⎜
+
ln
⎜
()
⎝
+
with the line voltage so that, at
7].
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
Doc ID 14763 Rev 27/39
The circuit implementing the line-modulated fixed off-time with the new L6562AAN2782
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 and R0, its
OFF
effects are discussed only qualitatively and the quantitative aspects are provided graphically
for a specific case in [
7].
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 resistor Rs charges the timing capacitor C as quickly
GD
ZCDclamp
, without exceeding clamp rating (I
(see Section 4.3.7).
OFF
=10 mA). Then it must
ZCDx
fulfill the following inequalities:
VVV
FZCDclampGD
(6)
= 15 V its
GDx
I
ZCDx
where V
(assume VGD = 10 V) is the voltage delivered by the gate driver, V
GD
maximum value, and V
VVV−−
−−
FZCDclampGDx
V
ZCDclamp
+
R
the forward drop on D.
F
RRs
⋅<<
V
ZCDclamp
When working at high line/light load the on-time of the power switch becomes very short and
the resistor Rs 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
L6562A 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:
V
CCs−−<
ZCDclamp
VVV
FZCDclampGDx
(7)
8/39Doc ID 14763 Rev 2
AN2782Designing a fixed off-time PFC
=
=
=
=
=
=
Δ
4 Designing a fixed off-time PFC
4.1 Input specification
The following is a possible design flowchart in reference to a fixed off-time mode PFC using
the L6562A. This first part is a detailed specification of the operating conditions of the circuit
that is needed for the following calculations in
input range mains PFC circuit has been considered. Some design criteria are also given.
Section 4.2. In this example a 400 W, wide
●Mains voltage range (Vac rms):
●Minimum mains frequency:
●Rated output power (W):
min
Vac90VAC
l
out
max
Hz47f
W400P
Vac265VAC
=
(8)
(9)
(10)
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 thus, because Vin max is V
VAC
max
2374=⋅
pk
, the
output has been 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):
out
V400V
(11)
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 (%):
●Expected power factor:
out
P
in
%90
==η
99.0PF
(12)
(13)
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, the L6562A integrates an OVP. The
overvoltage protection sets the extra voltage overimposed to Vout:
●Maximum output overvoltage (Vdc):
Doc ID 14763 Rev 29/39
V40OVP
(14)
Designing a fixed off-time PFCAN2782
=
Δ
=
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 (Vout min) after the elapsed holdup time (t
●Maximum output low frequency ripple:
●Minimum output voltage after line drop (Vdc):
●Holdup capability (ms):
out
Hold
V10V
=
minout
=
).
Hold
(15)
V300V
ms20t
(16)
(17)
The PFC minimum switching frequency is the 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
L6562A 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 is 55÷95 kHz for wide range operation.
●Minimum switching frequency (kHz):
Where f
= 1/(T+220 nsec) due to the ZCD - gate drive signal delay typical of the
swmin
kHz72f
=
minsw
(18)
L6562A.
The design will 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) k
●Ripple factor
=0.36.
r
34.0k
r
(19)
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)
ambx
C50T
°=
(20)
10/39Doc ID 14763 Rev 2
AN2782Designing 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
●Maximum input power
Section 4.1:
P
out
out
I
out
V
out
P
in
W400
90
I=
P
out
=
P
in
η
W400
==
V400
=⋅=
(21)
A00.1
(22)
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
P
I
=
in
out
min
I
=
in
PFVAC
⋅
W400
=
99.0Vac90
⋅
(23)
A99.4
It is important to define the following ratios in order to continue describing the energetic
relationships in the PFC:
VAC
min
min
max
2k=
2k=
V
VAC
V
out
max
out
min
max
Vac90
2k
Vac265
2k
32.0
==
V400
94.0
==
V400
(24)
(25)
From (24), (25):
P2
●Line peak current:
⋅
I
=
maxPK
in
I
Vk
⋅
outmin
maxPK
⋅
=
)W44.444(2
=
V400318.0
⋅
(26)
A98.6
●Inductor ripple-
ΔILpk:
IL⋅
=Δ
pk
Doc ID 14763 Rev 211/39
k6
⋅
r
I
k38
⋅−
r
IL
maxPK
=Δ
pk
34.06
⋅
34.038
⋅−
=⋅
(27)
A18.2A98.6
Designing a fixed off-time PFCAN2782
●Inductor peak
current:
IL⋅
maxpk
8
=
I
k38
⋅−
r
IL
maxPK
maxpk
8
=
34.038
⋅−
=⋅
(28)
A07.8A98.6
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:
●RMS
diode
current:
ISW
ID
rms
rms
P
in
=
⋅
Vk
outmin
P
in
=
⋅
Vk
outmin
It is worth reminding that the accuracy of the approximate energetic relationships described
here is quite good at maximum load for low values of the 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.
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.
⋅
k16
min
ISW
rms
rms
=
=
−⋅
2
π
3
k16
min
⋅
3
ID
π
W400
⋅
W400
⋅
2
V400318.0
⋅
V400318.0
318.016
⋅
−⋅
⋅
3
=
3
π
318.016
=
π
A22.4
A57.2
(29)
(30)
The rectifier bridge power dissipation can be calculated using equations
threshold voltage and dynamic resistance of a single diode of the bridge can be found in the
component datasheet.
I2
⋅
I
=
inrms
I
avg_in
in
2
I2
⋅
=
in
π
⋅
=
2
⋅
=
The power dissipated on the bridge is:
12/39Doc ID 14763 Rev 2
(31), (32), (33). The
A99.42
=
A99.42
π
A53.3
=
A25.2
(31)
(32)
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