ÇUKUROVA UNIVERSITY INSTITUTE OF NATURAL AND APPLIED ...
ÇUKUROVA UNIVERSITY INSTITUTE OF NATURAL AND APPLIED ... ÇUKUROVA UNIVERSITY INSTITUTE OF NATURAL AND APPLIED ...
3. FUNDAMENTALS OF DVR Mustafa İNCİ V i i [ k ( V −V ) + k k ( V −V ) − i ] = k { } (3.22) f ref s c v ref l c The load side voltage for this control configuration is given by (3.23) Vload Gclose 1 Vref + Gclose2 = V (3.23) s Where G close1 is the closed-loop transfer function from the reference signal V ref to V load while G close2 is the closed-loop transfer function from the supply voltage V s to V load . These transfer functions (3.24) and (3.25) (Vilathgamuwa et al., 2002) : G ( nk k k + nk )( L s + r ) i c v i l l close1 ( s) = (3.24) 3 2 a1 ncvs + a2ncvs + a3ncvs + a4ncv G close 2 ( s) LL C s + 2 ( L r + Lr + kk L ) C s + ( r rC + (1− nk) L + kk rC ) s+ ( 1−nk) 3 l f f f l l f i c l f f l f i l i c l f i l = (3.25) 3 2 a1 ncvs + a2 ncvs + a3 ncvs + a4 ncv r Following a similar analysis as in open loop control method, it can be seen the real root of the characteristics equation can be approximately located at − 2 2 ( r + n r )/( L + n L ) l t L (Vilathgamuwa et al., 2006). t . Factorization of the characteristics equation yields 2 2 2 ( L + n L ) s + ( r + n r ) ( s + b s bncv) 3 2 a1 ncv s + a2ncvs + a3 ncvs + a4ncv ≈ b1 ncv{ l t l t } 2ncv + (3.26) Where b b ncv 2ncv 1 , and b 3 ncv are given in the Appendix. The expressions for the coefficients b b ncv 2ncv 1 , and b 3 ncv show that the two dominant complex poles depend largely on the values of the filter inductance, filter resistance as well as the capacitor current loop gain k c . Furthermore it can be shown that the real part of these poles is − ( rf + kikc )/ 2L f . This is a very useful feature 41
3. FUNDAMENTALS OF DVR Mustafa İNCİ because there is now an additional flexibility in the design introduced by the factor k c . For a given k i , the value of k c can be chosen such that k k >> r and a corresponding increase in the real part of the complex poles is obtained. Thus the damping level can be increased with an increase of the capacitor current gain (Vilathgamuwa et al., 2006). The resulting system can be seen to have the natural damping frequency ω nncv i c f r + n r + n r + nk k k r 1 2 2 l t f i c v l 1+ nk k k ω nncv = ≈ == 1+ nk k k . (3.27) i c v 2 i c v ( rl + n rt ) Lf C f Lf C f Lf C f The natural damping frequency of the closed loop system is therefore approximately 1 + nk k k times filter resonance frequency(Vilathgamuwa et al., i c v 2002). System damping and stability margin can be improved by properly selecting the gains k c and k v . These gains are determined for a given design specification by deriving transfer function between load and the reference voltage. Further analysis reveals that the increase of current gain tends to increase the damping level while the increase of voltage gain k v , tends to decrease it. As the feed forward gain presents only in the numerator of the transfer function it does not contribute to improve system damping and stability margin. However it can be independently adjusted to decrease steady state error of compensated load voltage. However it can be independently adjusted to decrease steady state error of compensated load voltage (Vilathgamuwa et al., 2006). k f , 3.3.6. Gate Signal Generation Gate signals are used to control of the electrical switches in inverter. The rms value of output voltage in inverter is controlled by turning the solid-state devices. 42
- Page 9 and 10: VII
- Page 12 and 13: LIST OF FIGURES PAGES Figure 1.1. D
- Page 14 and 15: Figure 5.3. Injected voltages by us
- Page 16 and 17: LIST OF SYMBOLS C : DC Link Capacit
- Page 18 and 19: LIST OF ABBREVATIONS A AC APF ASD C
- Page 20: 1. INTRODUCTION Mustafa İNCİ 1. I
- Page 23 and 24: 1. INTRODUCTION Mustafa İNCİ 4
- Page 25 and 26: 2. POWER QUALITY Mustafa İNCİ 2.1
- Page 27 and 28: 2. POWER QUALITY Mustafa İNCİ 2.2
- Page 29 and 30: 2. POWER QUALITY Mustafa İNCİ 2.2
- Page 31 and 32: 2. POWER QUALITY Mustafa İNCİ •
- Page 34 and 35: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 36 and 37: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 38 and 39: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 42 and 43: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 44 and 45: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 46: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 49 and 50: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 51 and 52: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 53 and 54: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 55 and 56: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 58: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 63: 3. FUNDAMENTALS OF DVR Mustafa İNC
- Page 66 and 67: 4. MODELING OF PROPOSED DVR Mustafa
- Page 68 and 69: 4. MODELING OF PROPOSED DVR Mustafa
- Page 70 and 71: 4. MODELING OF PROPOSED DVR Mustafa
- Page 72 and 73: 4. MODELING OF PROPOSED DVR Mustafa
- Page 74 and 75: 4. MODELING OF PROPOSED DVR Mustafa
- Page 76 and 77: 4. MODELING OF PROPOSED DVR Mustafa
- Page 78 and 79: 4. MODELING OF PROPOSED DVR Mustafa
- Page 81 and 82: 4. MODELING OF PROPOSED DVR Mustafa
- Page 83 and 84: 4. MODELING OF PROPOSED DVR Mustafa
- Page 85 and 86: 4. MODELING OF PROPOSED DVR Mustafa
- Page 88 and 89: 4. MODELING OF PROPOSED DVR Mustafa
- Page 90 and 91: 4. MODELING OF PROPOSED DVR Mustafa
- Page 92: 4. MODELING OF PROPOSED DVR Mustafa
- Page 95 and 96: 4. MODELING OF PROPOSED DVR Mustafa
- Page 97 and 98: 4. MODELING OF PROPOSED DVR Mustafa
- Page 100 and 101: 4. MODELING OF PROPOSED DVR Mustafa
- Page 102 and 103: 5. SIMULATION RESULTS AND CASE STUD
- Page 104 and 105: 5. SIMULATION RESULTS AND CASE STUD
- Page 106 and 107: 5. SIMULATION RESULTS AND CASE STUD
- Page 108 and 109: 5. SIMULATION RESULTS AND CASE STUD
3. FUNDAMENTALS <strong>OF</strong> DVR Mustafa İNCİ<br />
V<br />
i<br />
i<br />
[ k ( V −V<br />
) + k k ( V −V<br />
) − i ]<br />
= k<br />
{ }<br />
(3.22)<br />
f<br />
ref<br />
s<br />
c<br />
v<br />
ref<br />
l<br />
c<br />
The load side voltage for this control configuration is given by (3.23)<br />
Vload<br />
Gclose<br />
1<br />
Vref<br />
+ Gclose2<br />
= V<br />
(3.23)<br />
s<br />
Where G<br />
close1<br />
is the closed-loop transfer function from the reference signal<br />
V<br />
ref<br />
to V<br />
load<br />
while G<br />
close2<br />
is the closed-loop transfer function from the supply voltage<br />
V<br />
s<br />
to V<br />
load<br />
. These transfer functions (3.24) and (3.25) (Vilathgamuwa et al., 2002) :<br />
G<br />
( nk k k + nk )( L s + r )<br />
i c v i l l<br />
close1 ( s)<br />
= (3.24)<br />
3<br />
2<br />
a1<br />
ncvs<br />
+ a2ncvs<br />
+ a3ncvs<br />
+ a4ncv<br />
G<br />
close 2<br />
( s)<br />
LL C s +<br />
2<br />
( L r + Lr + kk L ) C s + ( r rC + (1−<br />
nk)<br />
L + kk rC ) s+<br />
( 1−nk)<br />
3<br />
l f f f l l f i c l f f l f i l i c l f<br />
i l<br />
= (3.25)<br />
3 2<br />
a1<br />
ncvs<br />
+ a2<br />
ncvs<br />
+ a3<br />
ncvs<br />
+ a4<br />
ncv<br />
r<br />
Following a similar analysis as in open loop control method, it can be seen<br />
the real root of the characteristics equation can be approximately located at<br />
−<br />
2<br />
2<br />
( r + n r )/( L + n L )<br />
l<br />
t<br />
L<br />
(Vilathgamuwa et al., 2006).<br />
t<br />
. Factorization of the characteristics equation yields<br />
2<br />
2 2<br />
( L + n L ) s + ( r + n r ) ( s + b s bncv)<br />
3 2<br />
a1 ncv<br />
s + a2ncvs<br />
+ a3<br />
ncvs<br />
+ a4ncv<br />
≈ b1<br />
ncv{ l t l t<br />
}<br />
2ncv<br />
+ (3.26)<br />
Where<br />
b b ncv 2ncv<br />
1<br />
, and b 3 ncv<br />
are given in the Appendix.<br />
The expressions for the coefficients<br />
b b ncv 2ncv<br />
1<br />
, and b 3 ncv<br />
show that the two<br />
dominant complex poles depend largely on the values of the filter inductance, filter<br />
resistance as well as the capacitor current loop gain k<br />
c<br />
. Furthermore it can be shown<br />
that the real part of these poles is − ( rf<br />
+ kikc<br />
)/<br />
2L<br />
f<br />
. This is a very useful feature<br />
41