Averaged Modeling of Non-ideal Boost Converter Operating ... - ijcee
Averaged Modeling of Non-ideal Boost Converter Operating ... - ijcee
Averaged Modeling of Non-ideal Boost Converter Operating ... - ijcee
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International Journal <strong>of</strong> Computer and Electrical Engineering, Vol.3, No.1, February, 2011<br />
1793-8163<br />
di dTv ( D+ dˆ<br />
) ( V+<br />
vˆ<br />
) T<br />
d d 2L 2L<br />
d vap<br />
d d vap<br />
D dˆ<br />
Vap<br />
vˆ<br />
1<br />
+ 1−<br />
1<br />
−<br />
2<br />
=<br />
1<br />
+<br />
1<br />
+<br />
⎡ 2L( IL<br />
+ iˆ<br />
L<br />
) ⎤<br />
+ ⎢1<br />
−<br />
( Vzp<br />
+ vˆ<br />
zp)<br />
( D d )( Vi<br />
vˆ<br />
⎥<br />
⎣ 1<br />
+<br />
1<br />
+<br />
i<br />
) Ts<br />
⎦<br />
2 2<br />
1 L<br />
1<br />
s i 1 1 i i s<br />
= =<br />
1 2<br />
+ (3)<br />
( ) ( )( )<br />
ap<br />
(4)<br />
C. AC Small-Signal Model<br />
If we suppose that, the small-signal component is much<br />
less than the direct component, make the direct component is<br />
zero, and neglect the secondary small-signal product term.<br />
Then the (3) and (4) can be predigested to the (5) and (6). So<br />
we can get the small-signal linear equivalent model <strong>of</strong><br />
non-<strong>ideal</strong> <strong>Boost</strong> converter in discontinuous conduction<br />
model, shown in fig.2.<br />
( )<br />
2<br />
2<br />
d i d T v D + dˆ<br />
( V + vˆ<br />
)<br />
1<br />
1 L<br />
d + d<br />
1<br />
2<br />
2<br />
1<br />
= a vˆ<br />
+ a dˆ<br />
i<br />
=<br />
2L<br />
1<br />
s<br />
i<br />
=<br />
dv 1 ap + (1 −d1−d2)<br />
vzp<br />
= −<br />
⎡<br />
⎢1<br />
−<br />
⎢⎣<br />
( D + dˆ<br />
)( V + vˆ<br />
)<br />
1<br />
( I + iˆ<br />
)<br />
L L<br />
( D + dˆ<br />
)( V + vˆ<br />
)<br />
1<br />
2L<br />
[( V − V − V − I R ) + ( vˆ<br />
− vˆ<br />
− R iˆ<br />
)]<br />
i<br />
1<br />
1<br />
E<br />
1<br />
2 L<br />
1<br />
o<br />
o<br />
i<br />
L<br />
o<br />
i<br />
E<br />
+<br />
T<br />
∧ ∧ ∧ ∧<br />
= b vi<br />
+ b2<br />
d1+<br />
b3<br />
iL<br />
+ b4<br />
vo<br />
s<br />
⎤<br />
⎥<br />
⎥⎦<br />
1<br />
(6)<br />
Fig.2. small-signal model <strong>of</strong> <strong>Boost</strong> converter in DCM<br />
Form fig.2, we can calculate the input-to-output transfer<br />
function<br />
Gvi( s)<br />
and the control-to-output transfer function<br />
Gvd( s)<br />
are<br />
vˆ o( s)<br />
Gvi( s)<br />
=<br />
vˆ i( s )<br />
dˆ1( s ) = 0<br />
i<br />
i<br />
o<br />
i<br />
T<br />
s<br />
E<br />
L<br />
(5)<br />
1 −b1− a1( sL+ RE<br />
+ b3)<br />
E 3 C<br />
=<br />
( sL + R + b )( sR C + sRC + 1)<br />
1+ b4<br />
+<br />
RsRC ( C + 1)<br />
tt 1 4 (1 + swz1)(1 + swz2)<br />
= ⋅<br />
tt 2 3+<br />
tt 0 4 s s 2<br />
1 + + ( )<br />
Qw0 w0<br />
(7)<br />
G<br />
vd<br />
vˆ () s<br />
() s =<br />
o<br />
dˆ 1 ()ˆ s v i () s = 0<br />
b2+ a2( sL+ RE<br />
+ b3)<br />
=−<br />
( sL + RE+ b3)( sRCC + sRC + 1)<br />
1+ b4<br />
+<br />
RsRC ( C + 1)<br />
tt 4 5 (1 + swz2)(1 −swz3)<br />
= ⋅<br />
tt 2 3+<br />
tt 0 4 s s 2<br />
1 + + ( )<br />
Qw0 w0<br />
(8)<br />
The parameters <strong>of</strong> the actual <strong>Boost</strong> converter as following:<br />
input-voltage Vi<br />
= 5V<br />
, output-voltage Vo<br />
= 10V<br />
, Load<br />
current Io<br />
= 0.2A<br />
, R = 50Ω ,<br />
L=<br />
19.2μH<br />
,<br />
RL<br />
= 3.6mΩ ,<br />
C = 1000μF<br />
, RC<br />
= 2mΩ . The model<br />
number <strong>of</strong> the MOSFET which we used in this paper is<br />
2SK2690. Ron<br />
= 10mΩ , for Schottky diode RF<br />
= 1mΩ ,<br />
switching frequency<br />
fs<br />
= 50kHz<br />
, PWM outputs the Peak<br />
voltage is Vm<br />
= 1V<br />
. Then there parameters are put into the<br />
formulas as following<br />
R<br />
V<br />
E<br />
4 DR 1 on DR 2 F<br />
= ( RL+ + )<br />
3( D1+ D2)<br />
D1+ D2 D1+ D2<br />
,<br />
ap =− Vo<br />
,<br />
2LIL<br />
2= −D1<br />
1 s i<br />
IO<br />
D<br />
IL<br />
= ( D1+<br />
D2)<br />
DTV and D2<br />
R is the total equivalent resistance <strong>of</strong> the three parasitic<br />
E<br />
resistances which were calculated to branch <strong>of</strong> inductance.<br />
Then we can get<br />
D1 ≈ 0.35 , RE<br />
≈22.69mΩ , VE<br />
≈ 0.184V<br />
,<br />
IL<br />
≈ 0.43A<br />
.<br />
Put the four parameters into formula(7)and (8), then we<br />
can get formula (9) and (10).<br />
s s<br />
(1 + )(1 − )<br />
G ( ) 2.112 500000 913333<br />
vi s = ×<br />
2<br />
s ⎛ s ⎞<br />
1+ + ⎜ ⎟<br />
58.42 ⎝ 4502 ⎠ (9)<br />
s s<br />
(1 + )(1 − )<br />
G ( ) 23.696 500000 307433<br />
vd s = ×<br />
2<br />
s ⎛ s ⎞<br />
1+ + ⎜ ⎟<br />
58.42 ⎝ 4502 ⎠ (10)<br />
80