Fairchild FPS service manual

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Application Note AN4140
Transformer Design Consideration for off-line Flyback Converters using Fairchild Power Switch (FPS
1. Introduction
For flyback coverters, the transformer is the most important factor that determines the performance such as the efficiency, output regulation and EMI. Contrary to the normal transformer, the flyback transformer is inherently an inductor that provides energy storage, coupling and isolation for the flyback converter. In the general transformer, the current flo ws in bot h the prim ary and se condary wi nding at the same time. However, in the flyback transformer, the current flows only in the primary winding while the energy in the core is charged and in the secondary windin g while the energy in the core is discharged. Usually gap is introduced between the core to increase the energy storage capacity.
This paper presents practical design considerations of transformers for off-line flyback converters employing Fairchild Power Switch (FPS). In order to give insight to th e reader, practical design examples are also provided.
2. General Transformer design procedure
(1) Choose the proper core Core type
for commercial SMPS (Switchied mode power supply) applications. Various ferrite cores and bobbins are shown in Figure 1. The type of the core should be chosen with regard to system requirements including number of outputs, physical height, cost and so on. Table 1 shows features and typical application of various cores.
: Ferrite is the most widely used core material
Core Features Typical Applications EEEI-Low cost Aux. power
EFD
-Low profile LCD Monitor
EPC EER -Large winding window area
-Various bobbins for multiple output
PQ -Large cross sectional area
-Relatively expensive
Table 1. Features and typical applications of various cores
Core size : Actually, the initial selection of the core is
bound to be crude since there are too many variables. One way to select the proper core is to refer to the manufacture's core selection guide. If there is no proper reference, use the table 2 as a starting point. The core recommended in table 1 is typical for the universal input range, 67kHz switching frequency and 12V singl e outp ut app lication . When th e in put voltage range is 195-265 Vac (European input range) or the switching frequency is higher than 67 kHz, a small er core can be used. For an application with low voltage and/or mul tiple outputs, usually a larger core should be used than recommended in the table.
Output Power
0-10W EI12.5
10-20W EI22 EE19 EPC19 20-30W EI25 EE22 EPC25 EER25.5 30-50W EI28
50-70W EI35 EE30 EER28L 70-100W EI40 EE35 EER35 100-150W EI50 EE40 EER40
150-200W EI60 EE50
EI core EE core EPC core EER core
EE8 EI16 EI19
EI30
EE10
EE13
EE16
EE25 EPC30 EER28
EE60
TM
)
Battery charger
CRT monitor, C-TV DVDP, STB
EPC10 EPC13 EPC17
EER42 EER49
Figure 1. Ferrite core (TDK)
©2003 Fairchild Semiconductor Corporation
Table 2. Core quick selection table (For universal input range, fs=67kHz and 12V single output)
AN4140 APPLICATION NOTE
I
I
Once the core type and size are determined, the following variables are obtained from the core data sheet.
- A
: The cross-sectional area of the core (mm2)
e
- A
: Winding window area (mm2)
w
- B
: Core saturation flux density (tesla)
sat
Figure 2 shows the Ae and A
of a core. The typical B-H
w
characteristics of ferrite core from TDK (PC40) are shown in Figure 3. Since the saturation flux density (B
) decreases as
sat
the temperature increases, the high temperature character­istics should be considered. If there is no reference data, use
B
=0.3~0.35 T.
sat
Aw
Aw
AwAw
Ae
Ae
AeAe
(2) Determine the primary side inductance (Lm) of the transformer
In order to determine the primary side inductance, the following variables should be determined first. (For a detailed design procedure, please refer to the application note AN4137.)
- P
: Maximum input power
in
- f
: Switching frequency of FPS device
s
min
- V
- D
- K
: Minimum DC link voltage
DC
: Maximum duty cycle
max
: Ripple factor, which is defined at the minimum input
RF
voltage and full load condition, as shown in Figure 4. For DCM opera tion, K
= 1 and for CCM operation KRF < 1.
RF
The ripple factor is closely related with the transformer size and the RMS value of the MOSFET current. Even though the conduction loss in the MOSFET can be reduced through reducing the ripple factor, too small a ripple factor forces an increase in transformer size. Considering both efficiency and core size, it is reasonable to set K universal input range and K
= 0.4-0.8 for the European
RF
= 0.3-0.5 for the
RF
input range. Meanwhile, in the case of low power applications below 5W where size is most critical, a relatively large ripple factor is used in order to minimize the transformer size. In that case, it is typical to set K
0.7 for the universal input range and K
= 1.0 for the
RF
= 0.5-
RF
European input range.
Figure 2. Window Area and Cross Sectional Area
Magnetization Curves (typical)
Material :PC40
500
400
300
200
Flux density B (mT)
100
0
0
Figure 3. Typical B-H characteristics of ferrite core
(TDK/PC40)
800 1600
Magnetic field H (A/m)
25 ℃℃℃
60 ℃℃℃
100 ℃℃℃
120 ℃℃℃
peak
I
I
EDC
I
ds
peak
I
ds
I
EDC
=
K
RF
I
2
EDC
D
max
D
max
Figure 4. MOSFET Drain Current and Ripple Factor (KRF)
CCM operation : KRF < 1
K
=
RF
2
I
I
EDC
DCM operation : KRF =1
With the given variables, the primary side inductance, Lm is obtained as
min
V
()
L
m
DC
--------------------------------------------- -= (1) 2PinfsK
2
D
max
RF
2
©2002 Fairchild Semiconductor Corporation
APPLICATION NOTE AN4140
I
I
where V maximum duty cycle, P the switching frequency of the FPS device and K
min
is the minimum DC input voltage, D
DC
is the maximum input power, fs is
in
max
RF
is the
is the
ripple factor. Once L
is determined, the maximum peak cur rent and RMS
m
current of the MOSFET in normal operation are obtained as
peak
I
ds
rms
I
ds
where I
and
3I
()
I
I
-----+= (2)
I
EDC
2
2
2
+
EDC
------------------------------------- -=4()
EDC
V
min
V
DC
-----------------------------------= (5) Lmf
D
I
 
DC
D
s
max
-----
------------- -=3()
2
3
P
in
min
D
max
max
With the chosen core, the minimum number of turns for the transformer primary side to avoid the core saturation is given by
LmI
min
N
P
over
-------------------
= (6)
B
satAe
10
×
6
(turns)
(3) Determine the number of turns for each output
Figure 6 shows the simplified diagram of the transformer, whrere V by the feedback control while V
stands for the reference output th at is regulated
o1
stands for the n-th
o(n)
output. First, determine the turns ratio (n) between the primary side
and the feedback controlled secondary side as a reference.
V
R0
--------------------------
n
Vo1VF1+
where N
and Ns1 are the number of turns for primary side
p
and reference output, respectively, V and V
is the diode (DR1) forward voltage drop of the
F1
N
P
---------= = (7) N
s1
is the output voltage
o1
reference output that is regulated by the feedback control. Then, determine the proper integer for N
resulting Np is larger than N
min
obtained from equation (6).
p
so that the
s1
The number of turns for the other output (n-th output) is determined as
V
+
N
sn()
on()VFn()
---------------------------------=N V
o1VF1
+
s1
turns() 8()
The number of turns for Vcc winding is determined as
where L
is the primary side inductance, I
m
pulse-by-pulse current limit level, A area of the core and B
is the saturation flux density in
sat
is the cross-sectional
e
is the FPS
over
tesla. If the pulse-by-pulse current limit lev el of FPS is larger than
the peak drain current of the power supply design, it may result in excessive transformer size since I
is used in
over
determining the minimum primary side turns as shown in equation (6). Therefore, it is required to choose a FPS with proper current limit specifications or to adjust the peak drain current close to I in Figure 5. It is reasonable to design I
I
considering the transient response and tolerance of I
over
by increasing the ripple factor as shown
over
peak
to be 70-80% of
ds
over
Pulse-by-pulse current limit of FPS (I
70-80% of I
I
ds
Increasing ripple
factor (K
)
RF
over
peak
I
ds
peak
Decreasing pirmary
=
side Inductance (L
)
over
I
EDC
)
m
Vcc*V
+
--------------------------- -=N
N
a
V
where V FPS device, and V
* is the nominal value of the supply voltage of the
cc
is the forward voltage drop of Da as
Fa
defined in Figure 6. Since V increases, it is proper to set V
Fa
+
o1VF1
cc
cc
s1
turns() 9()
increases as the output load
* as Vcc start voltage (refer to
the data sheet) to avoid trigge ring the ov er voltage pro tectio n during normal operation.
S(n)
F(n)
D
R(n)
-
V
.
+ V
-
V
RO
Np
N
+
D
F1
R1
-
N
+ V
S1
- V
D
+
*
V
cc
+
Fa
a
N
a
-
+
O(n)
-
+
V
O1
-
Figure 5. Adjustment peak drain current
©2002 Fairchild Semiconductor Corporation
Figure 6. Simplified diagram of the transformer
3
AN4140 APPLICATION NOTE
other windings can act as Faraday shields. When the primary Once the number of turns on the primary side have been determined, the gap length of the core is obtained through approximation as
2
N
=mm() 10()
G40

πA
-------------------- -

e
1000L

1
P
-----­A
m
L
side winding has more than t wo layers, the innermost layer
winding should start from th e drain pin of FPS as show n in
Figure 7. This allows the winding driven by the highest
voltage to be shielded by other windings, thereby
maximizing the shielding effect.
where A
is the AL-value with no gap in nH/turns2, Ae is the
L
cross sectional area of the core as shown in Figure 2, L specified in equation (1) and N
is the number of turns for
p
the primary side of the transformer
(4) Determine the wire diameter for each winding
The wire diameter is determined based on the rms current through the wire. The current density is typically 5A/mm when the wire is long (>1m). When the wire is short with a small number of turns, a current density of 6-10 A/mm also acceptable. A void using wire with a diameter larger than 1 mm to avoid severe eddy current losses as well as to make winding easier. For high current output, it is better to use parallel windings with multiple strands of thinner wire to minimize skin effect.
3. Transformer Construction Method.
(1) Winding Sequence
(b) Vcc winding
is
m
In general, the voltage of each winding is influenced by the
voltage of the adjacent winding. The optimum placement of
the Vcc winding is determined by the over voltage pro tection
(OVP) sensitivity, the Vcc operating range and control
scheme.
-Over voltage protection (OVP) sensitivity : When the
2
output voltage goes above its normal operation value due to
some abnormal situation, Vcc voltage also increases. FPS
2
uses Vcc voltage to indirectly monitor the over voltage
is
situation in the secondary side. However, a RCD snubber
network acts as an another output as shown in Figure 8 and
Vcc voltage is also influenced by the snubber capacitor
voltage. Because the snubber voltage increases as the drain
current increases, OVP of FPS can be triggered not only by
the output over voltage condition, but also by the over load
condition.
The sensitivity of over voltage protection is closely related to
the physical distance between windings. If the Vcc winding
is close to the secondary side output winding, Vcc voltage
will change sensitively to the variation of th e output voltage.
Meanwhile, if the Vcc winding is placed close to the primar y
side winding, Vcc voltage will vary sensitively as the
snubber capacitor voltage changes.
(a) Primary winding
3mm 3mm
Barrier tape
Insulation tape
...... Na ...
.......... Ns .........
....... Np/2 .....
........ Np/2 ..... .
Bobbin
To FPS Drain pin
Figure 7. Primary side winding
It is typical to place all the primary winding or a portion of the primary winding innermost on the bobbin. This minimizes the length of wire, reducing the conduction loss in the wire. The EMI noise radiation can be reduced, since the
-
V
sn
+
Np
+
V
cc
N
a
-
Figure 8. Primary side winding
N
S2
N
S1
+
V
O2
-
+
V
O1
-
4
©2002 Fairchild Semiconductor Corporation
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