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8/15/2019 Flyback Mathcad Example
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SWITCHING POWER SUPPLY DESIGN:DISCONTINUOUS MODE FLYBACK CONVERTER
Written by Michele Sclocchi
[email protected] Application Engineer National Semiconductor
Typical Flybac ! "#$p#$ p"%&' (#pply:
N"$&(: Write down the power supply requirements on :X :=!et the results on:"sults :=T)i( Ma$)ca* +il& )&lp( $)& calc#la$i", "+ $)& &-$&',al c".p",&,$( "+ a $ypical*i(c",$i,#"#( ."*& (%i$c)i,/ p"%&' (#pply0
I,p#$ 1"l$a/&:
#Minimum input $oltage: %imin 30 $olt⋅:=
Ma imum input $oltage: %ima 50 $olt⋅:=
O#$p#$:
N sp&
' &
(o &a
) &
(o &b
N sp*
' *
(o *a
) *
(o *b
N sp+
' +
(o +a
) +
(o +b
" sense
( s
" ,a
" ,*" ,+( ,+
( c
" c
( i*( i+- *
" +
' .+
( +%o+
%o*
%o&%input
)M&/00
1sen
comp
,b
agnd pgnd
dr
,a2sync2sd
%in
3Needed i, %in 4 /5%
36utput ,ilter
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Nominal output $oltage7 ma imum output ripple7 minimum output current7 ma imum outputcurrent
%o+ 5 $olt⋅:= %rp+ 10 m%⋅:= 1o+min 0.250 amp⋅:= 1o+ma 5 amp⋅:=
%o* 12 $olt⋅:= %rp* 20 m%⋅:= 1o*min 0.250 amp⋅:= 1o*ma 1 amp⋅:=
%o& 12 $olt⋅:= %rp& 20 m%⋅:= 1o&min 0.250 amp⋅:= 1o&ma 1 amp⋅:=8negati$e9
%d,w 0.6 $olt⋅:= 8 diode s ,orward drop $oltage9( ) ⋅ ( ) ⋅ ( ) ⋅: ( ) ⋅ ( ) ⋅ ( ) ⋅
S%i$c)i,/ F'&2#&,cy: ,sw 150
,sw: =
T'a,(+"'.&'3( E++ici&,cy: η 0.95:=
45 Ma-i.#. S$'&(( ", $)& (%i$c)i,/ ."(+&$ :
6 D&+i,& $)& +lybac 1"l$a/& ac'"(( $)& .#$#al i,*#c$a,c&: V+.
?,b 0.8:= 8?,b is a $alue between + to 5. 9
Nps+%o+ %d,w+
: =
6Ma-i.#. S%i$c)i,/ 1"l$a/& ", $)& (%i$c)i,/6."(+&$:
( ) ( )⋅:%ds ma 103.6 $olt=
Sa,e ,actor 8assume spi
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6C)""(& .i,i.#. *&a* $i.& *#$y cycl&: ' dt 0.1:=
6Ma-i.#. *'"p 1"l$a/& ac'"(( $)& (%i$c)i,/ ."(+&$ *#'i,/ $)& ", $i.&:O, '&(i($a,c& "+ $)& M"(+&$:"ds on 0.06 ohm⋅:=
%ds on η %imin⋅ "ds on⋅: =( )⋅
>on ma⋅ ⋅
%imin %ds on−( ) ?lon min⋅ ⋅
%ima %dson−( ) ?lhe energy stored is: E)p 1p 2⋅
2:= = and 1p
%omin >on ma⋅
)p:=
Edt 8.245 10 5−× $olt sec⋅=
- ;rimary inductance:
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)p1pp<
2: =
)p 9.105µ==
95 S&c",*a'y c#''&,$( a,* $#',( 'a$i"( (&c",*a'y;p'i.a'y5 : N(p4 < N(p7
Nsp+ %,b: = Nsp+ 0.233=
Nsp*%,b
: =Nsp* 0.525=
Nsp&%,b
: =Nsp& 0.525=
Nsp+4.286=
Nsp*1.905=
Nsp*1.905=
6Ma($&' "#$p#$:
# Secondary pea< current:1s+p<
⋅
1 ' ma− ' dt−: =
1s+p< 20.503 amp=
# Secondary "MS current:1s+rms
31 ' ma− ' dt−⋅: =
1s+rms 8.267 amp=
# Secondary A( current:
1s+ac 1s+rms2 1o+ma
2−: = 1s+ac 6.584amp=
# Secondary inductance :s sp p⋅: =
)s+ 0.496µ==
6Fi'($ (la1& "#$p#$:
# Secondary pea< current:1s*p<
1 ' ma− ' dt−: =
1s*p< 4.101amp=
# Secondary "MS current:1s*rms
31 ' ma− ' dt−⋅: =
1s*rms 1.653amp=
# Secondary A( current:
1s*ac 1s*rms2
1o*ma2
−: = 1s*ac 1.317 amp=
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# Secondary inductance :s sp p⋅: =
)s* 2.51µ==
6S&c",* (la1& "#$p#$:
# Secondary pea< current:1s&p< ⋅
1 ' ma− ' dt−: =
1s&p< 4.101 amp=
# Secondary "MS current:1s&rms
31 ' ma− ' dt−⋅: =
1s&rms 1.653 amp=
# Secondary A( current:
1s&ac 1s&rms2
1o&ma2
−: = 1s&ac 1.317amp=
# Secondary inductance:⋅: =
)s& 2.51µ==
=5 Ma-i.#. S$'&(( ac'"(( $)& "#$p#$ *i"*&(: V*i"*&Ma imum $oltage present on the cathode o, diodes
⋅
%diode+ ma 16.667 $olt=
⋅
%diode* ma 38.25 $olt=
⋅
%diode&ma
38.25 $olt=
Select a diode with %a#c44 %diode.ma 7 and ultra#,ast switching diode
>6a5 O#$p#$ 'ippl& Sp&ci+ica$i",( : O#$p#$ Capaci$"'(# Secondary inductance :
s sp p⋅: =)s* 2.51µ==
>o meet the output ripple speci,ications without using an e ternal )( ,ilter7 the output capacitorsha$e to meet two criteria:# satis,y the standard capacitance de,inition: I?C@*V;*$ where t is the >on time7 % is * B o, theallowable output ripple.# >he Equi$alent Series "esistance 8ES"9 o, the capacitor has to pro$ide less than H B o, thema imum output ripple. 8%rippleC1pea
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, c
2
'b
α
:=
6ne o, the critical ,actor o, a ,ilter design is the attenuating character at the corner ,requency.
>he damping ,actor 8 eta9 describes the gain at the corner ,requency and the time response o,the ,ilter. As the damping ,actor becomes smaller7 the gain at the corner ,requency becomeslarger.
or many ,ilters7 a damping ,actor o, + and a cuto,, ,requency within about an octa$e o, thecalculated ideal should pro$ide suitable ,iltering.'amping ,actor much greater than + may cause unacceptably high attenuation o, lower,requencies and a damping ,actor much less than .H5H may cause undesired ringing and the ,iltermay itsel, produce noise. 83 octa$eC inter$al that has the ,requency ratio *:+ 9# or each output:#6utput load resistance:"o+
1o+ma: =
#'esired damping ,actor: ζ .7:=
⋅ ⋅ ωc 5 .289 10×sec
=
#1nductance calculated:)+
⋅ ⋅
ωc: =
)+ 2.647µ==
#(apacitance calculated:
(o+b )+ ωc 2⋅: = (o+b 1.35µ=
#1nductance used: )+ used 10 µ=:=
#(apacitance used: (o+b used 50 µ:=
ωcu2 π⋅ )+ used (o+b used⋅⋅
: =
, i 10 0250: =
wi , i 2⋅ π⋅sec⋅: = ⋅
ωn)+ used (o+b used⋅
: = ωnc)+ (o+b⋅
: =
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ζ+2 "o+⋅ )+ used (o+b used⋅⋅
: =
ζ+c2 "o+⋅ )+ (o+b⋅⋅
: =
As+ i
1 i 2⋅ ζ+⋅wi
ωcu⋅+
wi
ωn
2
−
: = As+c i1 i 2⋅ ζ+c⋅
wi
ωc⋅+
wi
ωnc
2
−
: =
Mags+ i 20 log As+ i( )⋅:= Magsc+ i 20 log As+c i( )⋅:=
#(apacitor Selection:>he per,ormance o, a ,ilter critically depends on the capacitor used. Iesides the basic $oltageand capacity requirements7 select capacitors with low ES)7 ,or high ,requency attenuation7 andlow ES"7 ,or mid band attenuation and2or high ripple current capability.#(hohe input capacitor has to meet the ma imum ripple current rating 1p8rms9 and the ma imuminput $oltage ripple ES" $alue.
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other three important parameters o, a Mos,et are "ds8on97 gate threshold $oltage7 and gatecapacitance.>he switching Mos,et has three types o, losses7 conduction loss7 switching loss7 and gate chargeloss:#C",*#c$i", l"((&( are equal to: 1L*3" losses7 there,ore the total resistance between the sourceand drain during the on state7 "ds8on9 has to be as low as possible.#S%i$c)i,/ l"((&( are equal to: Switching#time3%ds313,requecy. >he switching time7 rise time and,all time is a ,unction o, the gate to drain Miller#charge o, the Mos,et7 -gd7 the internal resistanceo, the dri$er and the >hreshold %oltage7 %gs8th97 the minimum gate $oltage which enables thecurrent through drain source o, the Mos,et.6Ga$& c)a'/& l"((&( are caused by charging up the gate capacitance and then dumping thecharge to ground e$ery cycle. >he gate charge losses are equal to: ,requency -g8tot9 %dr Kn,ortunately7 the lowest on resistance de$ices tend to ha$e higher gate capacitance.Iecause this loss is ,requency dependent7 in $ery high current supplies with $ery large E>s7 withlarge gate capacitance7 a more optimal design may result ,rom reducing the operating ,requency.Switching losses are also e,,ected by gate capacitance. 1, the gate dri$er has to charge a largercapacitance7 then the time the Mos,et spends in the linear region increases and the lossesincrease. >he ,aster the rise time7 the lower the switching loss. Kn,ortunately this causes high,requency noise.
=
Mos,et: airchild -I+5N*5)# '*;A?"ds on 0.3 ohm⋅:=8>otal resistance between the source and drain during the on state9(oss 95 p⋅:=86utput capacitance9-g tot 13 n⋅ coul⋅:=8>otal gate charge9-gd miller 6.1 n⋅ coul⋅:=8!ate drain Miller charge9%gs th 2 $olt⋅:=
8>hreshold $oltage9#(onduction losses: ;condon rms⋅ ma⋅: =
#Switching losses: ;sw8ma 9>urn 6n time:tsw -gd miller
%dr %gs th−⋅: =
sw . × sec=
;sw ma tsw %ds ma⋅ 1pphe a$erage current required to dri$e the gate capacitor o, the Mos,et:⋅
aw g .=
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#>otal losses: ;tot8ma 9;tot ma 2.64watt=
#Ma imum unction temperature and heat sin< requirement:#Ma imum unction temperature desired:> ma 130:=
#Ma imum ambient temperature: >a ma 50:=
#>hermal resistance unction to ambient temperature:θ a
;tot ma: = θ a 30.305
watt=
(elsius
1, the thermal resistance calculated is lower than that one speci,ied on the Mos,et s data sheet aheat sin< or higher copper area is needed.
or E ample ,or a >5#*J& 8'*pahe )M&/00 uses a current mode control scheme. >he main ad$antages o, current mode controlare inherent cycle#by#cycle current limit ,or the switch7 and simple control loop characteristics.Since the )M&/00 has a ma imum duty cycle o, +55B7 and the power supply is designed to wor<in discontinuous mode with a 5B ma imum duty cycle7 the current limit should be designed sothat the pea< short circuit current limit is reached ust be,ore the 5B boundary is reached." sense
1pp< 1.1⋅: =
" sense 0.016 Ω=
445 T'a,(+"'.&' D&(i/,:
>he inductor# trans,ormer should be designed to minimi e the leahe total losses are minimi edwhen core losses and winding losses are appro imately the same $alue.
#(ore selection:>o reduce the core losses7 ,errite#; material is usually the pre,erred material ,or discontinuous
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#;rimary and secondaryOs inductance:
)p 9.105µ== )s+ 0.496µ== )s* 2.51µ== )s& 2.51µ==