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AN4107 Datasheet, PDF (5/14 Pages) Fairchild Semiconductor – Design of Power Factor Correction
APPLICATION NOTE
AN4107
toff
=
L
----I--L---(--p---e--a---k---)-(---t--)----
VO – sin(ωt)
=
L
-------2---I--i--n---(--p--e---a--k---)--s---i-n----(--ω-----t--)-------
VO – Vin(peak) sin (ωt)
Iin(peak) = -η-----⋅-2--V--V--i--nO---(-Ip--O-e---a--k---)
(2)
(3)
TS = ton + toff
=
2
LIi
n
(p
ea
k
)



-------------1---------------
Vin(peak)
+
-V----O------–----V-----i-n--s--(-i--np---e(---ω-a---t-k--)--)--s---i--n----(--ω-----t--)
(4)
= -4---L----V----O------I-ηO------(--m------a---x----) V-----2---i--n----(-1-p----e----a----k----) + V-----i--n---(---p---e----a----k----)--(---V----O-1-----–----V-----i-n----(---p---e----a----k----)--)
TS ( m a x )
=
-4---L----V----O------I-O------(--m-----a----x----)
η



---------------1-----------------
V2in(peak)
+
V-----i-n----(---p---e----a----k----)--(--V-----O-1-----–----V-----i-n----(---p---e----a----k---)---)
(5)
L = --------------------------------------------------------------------------------------------η---------------------------------------------------------------------------------------------- (6)
4fsw(m
i
n)
VOIO
(
ma
x)



---------------1-----------------
V2in(peak)
+
V-----i--n---(---p----e---a----k----)--(---V----O-1-----–----V-----i--n---(---p----e---a----k----)--)
2) Auxiliary winding design
The auxiliary winding voltage is lowest at the highest line.
So the number of auxiliary winding can be obtained by (7).
A small resistor is connected to the auxiliary winding to
suppress the high frequency ringing voltage.
Naux = --------------V----C----C-----⋅--N-----P---------------
(7)
 V O
–
2----π----2--
Vi

n ( H L )
3) Input capacitor design
The voltage ripple of the input capacitor is maximum when
the line is lowest and the load is heaviest. If fsw(min) >> fac ,
the input current can be assumed to be constant during a
switching period.
Inductor
Current
Input
Current
2 ⋅ I in( peak _ max)
I in( peak _ max)
ton / 2
t on
Figure 7. Input Current and Inductor Current Waveform during a Switching Cycle
∫ Cin
≥
------------2------------
∆Vin(max)
⋅
t---o---n-
2
0
 I i n ( p e a k _max )
–
2-----⋅---I--i--n---(-p---e---a--k---_--m----a--x--)
ton
t
dt
≥
-t-o---n----⋅---I--i--n---(-p---e---a--k---_--m----a--x--)
2 ⋅ ∆Vin(max)
(8)
≥
-----------L------⋅---I--2--O----(--m----a--x---)---⋅---V-----2--O-------------
∆Vin(max) ⋅ V3in(peak_max)
The input capacitor must be larger than the value calculated
by (8). And the maximum input capacitance is limited by the
input displacement factor(IDF), defined as IDF≡cosθ .
Therefore the input capacitor must be smaller than Cin(max)
calculated by (12).
©2001 Fairchild Semiconductor Corporation
Va = VA = Vin(peak) cos (ωt)
(9)
ia = Ia cos(ωt)
iA = ia + ic = Ia cos (ωt) – ωCinVin(peak) sin(ωt)
( 10 )
θ
=
tan
–1 ω-----C----i--n---V----i--n---(-p---e---a--k--)
Ia
(11)
Cin(max)
=
------------I--a------------
ωVin(peak)
tan
(
cos
–1(IDF))
=
------------2---V-----O----I--O-------------
ω V 2 i n ( p e a k _max )
tan
(
cos
–1(IDF))
( 12 )
5