Int
ern
at
i
onal
Journ
al of Ele
ctrical
an
d
Co
mput
er
En
gin
eeri
ng
(IJ
E
C
E)
Vo
l.
9
, No
.
3
,
J
un
e
201
9
, pp.
1496
~
15
05
IS
S
N:
20
88
-
8708
,
DOI: 10
.11
591/
ijece
.
v
9
i
3
.
pp
1496
-
15
05
1496
Journ
al h
om
e
page
:
http:
//
ia
es
core
.c
om/
journa
ls
/i
ndex.
ph
p/IJECE
Modifie
d
approach
for
h
ar
m
onic reduc
tion
in
three
-
ph
ase
t
o
seven
-
ph
ase
usin
g
t
ransforme
r wind
ing conn
ec
tion
s
Mehrd
ad
A
h
mad
i
Ka
m
arposh
ti
1
,
A
shk
an
A
byar
H
oss
eyni
2
1
Depa
rtment of
El
e
ct
ri
ca
l
Eng
in
ee
ring
,
Jou
y
bar
Branc
h
,
Islamic
Aza
d
Unive
rsit
y,
Ir
an
2
Depa
rtment of
El
e
ct
ri
ca
l
Eng
in
ee
ring
,
Univ
ers
ity
Co
llege
o
f
Ro
uzba
han
,
Ir
an
Art
ic
le
In
f
o
ABSTR
A
CT
Art
ic
le
history:
Re
cei
ved
Ma
y
15
, 201
8
Re
vised
N
ov
2
3
, 2
01
8
Accepte
d
Dec
12
, 201
8
Thre
e
phase
su
ppl
y
is
av
ai
l
able
in
the
g
ene
r
ating
station
or
g
rid,
wer
e
as
seve
n
phase
suppl
y
is
req
uir
ed
for
m
any
indu
stria
l
applic
at
io
ns
such
as,
ae
rospac
e,
railwa
y
and
aut
om
obi
le
app
lications.
The
re
are
diff
er
ent
m
et
hods
in
which
we
can
conve
rt
3
to
7
p
hase
using
2
4
-
Puls
e
Converter,
Car
rie
r
Based
PW
M
Te
chni
que
,
m
ult
ile
vel
conve
r
te
r
an
d
Multi
phase
Tr
ansform
er.
The
above
said
m
et
hods
which
are
m
ore
complic
a
te
d
to
design
for
highe
r
rat
ings
or
a
pur
e
sine
wave
wil
l
not
be
obt
ai
ned
or
har
m
onic
s
will
be
m
ore
.
For
Multi
phase
power
tra
nsm
ission
sy
stem
m
ult
ipha
se
tra
nsf
orm
ers
are
nee
ded
.
In
th
e
m
ult
ipha
se
po
wer
tra
nsm
ission
and
m
ult
iphas
e
rec
t
ifi
er
s
y
stems
,
the
nu
m
ber
of
phase
c
an
be
design
ed
a
nd
deve
lop
ed
in
m
ult
ipl
es
o
f
thre
e
.
Th
ere
for
e
,
the
v
ari
ab
le
sp
ee
d
m
ult
iph
ase
drive
s
y
st
em
co
nsidere
d
in
the
liter
at
ure
ar
e
m
ostl
y
of
f
iv
e,
seve
n
,
nin
e,
el
ev
en,
tw
el
ve
,
and
fiftee
n
phase
.
So,
the
r
e
is
a
n
ee
d
to
d
e
sign
and
dev
el
o
p
spec
i
al
t
ran
sfo
rm
er
which
conve
rts
from
3
to
7
phase
for
diffe
ren
t
arr
ang
e
m
ent
of
input
and
output.
Thus,
with
the
proposed
te
chn
i
que,
a
pure
sev
en
-
phase
sin
e
-
wave
of
f
ixed
volt
ag
e/
cur
r
ent
a
nd
fre
quen
c
y
is
obta
in
ed,
whi
ch ca
n
b
e
used
for
RL
loa
d
and
m
otor
te
sting
purposes.
Com
pl
et
e
design
and
sim
ula
ti
on
of
the
proposed
soluti
on
is
pre
s
ent
ed
.
Anal
y
t
ica
l
ca
l
culati
on
an
d
sim
ula
ti
on
res
ult
s
for
RL
loa
d
is
pre
sen
ted
in
the
pape
r
.
Thi
s
m
odel
ca
n
be
sim
ula
t
ed
b
y
using
Orca
d
sim
ula
ti
on
so
ftwa
re
and
“
Sim
Po
werS
y
stem”
bloc
k
sets
of
MA
TL
AB/S
IM
ULINK
software
.
Ke
yw
or
d
s
:
Har
m
on
ic
r
e
du
ct
ion
Mult
iph
ase
po
wer t
ransf
or
m
er
Seve
n
-
phase
Sp
eci
al
tra
ns
f
orm
er
Thr
ee
-
ph
ase
W
i
ndin
g
c
onne
ct
ion
s
Copyright
©
201
9
Instit
ut
e
o
f Ad
vanc
ed
Engi
n
ee
r
ing
and
S
cienc
e
.
Al
l
rights re
serv
ed
.
Corres
pond
in
g
Aut
h
or
:
Me
hrdad A
hma
di K
am
arposht
i,
Dep
a
rt
m
ent o
f
Ele
ct
rical
En
gi
neer
i
ng,
Jo
uy
bar Bra
nc
h,
Islam
ic
A
zad
Un
i
ver
sit
y,
Jo
uy
bar,
Ir
a
n.
Em
a
il
s:
m
.ah
m
adi@
j
ouyba
ria
u.
ac.i
r,
m
ehr
da
d.
a
hm
adi.k
@
gm
ai
l.co
m
1.
INTROD
U
CTION
Mult
i
-
ph
a
se
(
m
or
e
than
thre
e
-
phase
)
syst
em
s
hav
e
recei
ve
d
m
uch
at
te
ntion
of
researc
he
rs
in
recen
t
tim
es
du
e
to
their
in
her
e
nt
ad
van
ta
ges
wh
e
n
c
om
par
e
d
with
the
co
nv
e
n
ti
onal
th
r
ee
-
phase
c
ount
erp
art.
The
a
pp
li
cabil
i
ty
of
m
ulti
-
ph
a
se
syst
e
m
s
is
i
nv
e
sti
gated
in
el
ect
ric
power
gen
e
rati
on
[
1
-
2],
tra
ns
m
issi
o
n
[
3
-
4]
and
util
iz
at
ion
[5
-
7].
T
he
rese
arch
on
six
-
ph
ase
transm
issio
n
syst
em
was
init
ia
te
d
du
e
to
risin
g
cost
of
rig
ht
of
way
for
tra
ns
m
issi
on
co
rri
dors,
e
nvir
onm
ental
issues
and
va
rio
us
st
rin
gen
t
li
censi
ng
la
ws.
Six
-
ph
a
se
transm
issi
on
li
nes
ca
n
pr
ov
i
de
the
sam
e
powe
r
ca
pacit
y
with
a
lo
we
r
phase
to
phase
vo
lt
age
an
d
s
m
al
le
r,
m
or
e
com
pact
towe
rs
as
c
om
par
ed
to
a
s
ta
nd
a
rd
do
ub
l
e
ci
rcu
it
t
hr
ee
-
phase
li
ne.
T
he
ge
om
et
ry
of
the
six
-
ph
a
se
com
pact
towe
rs
m
ay
al
so
ai
d
in
the
re
duct
ion
of
m
agn
et
ic
fiel
ds
an
d
thu
s
el
ect
r
oma
gn
et
ic
interfe
ren
ce
iss
ues
as
w
el
l
[3
]
.
The
re
searc
h
on
m
ulti
-
ph
ase
gen
e
rato
rs
have
sta
rted
rece
nt
ly
[1
-
2].
M
ulti
-
phase
syst
em
s
are
m
os
tl
y
the
s
ubj
ect
of
interest
in
va
ri
able
s
peed
m
oto
r
dr
i
ve
a
ppli
cat
ion
s.
Re
sea
rch
on
m
ulti
ph
ase
dr
i
ve
is
m
o
stl
y
fo
c
us
e
d
on
fi
ve
-
phase
a
nd
si
x
-
phase
syst
e
m
s
with
the
obj
ect
iv
e
of
de
velo
ping
highl
y
reli
able
an
d
eff
ic
ie
nt
Evaluation Warning : The document was created with Spire.PDF for Python.
In
t J
Elec
&
C
om
p
En
g
IS
S
N:
20
88
-
8708
Mo
difi
ed
ap
proa
c
h
f
or
harm
on
ic
red
uctio
n i
n
t
hr
ee
-
ph
as
e
to
seve
n
…
(
M
ehr
dad
A
hma
di
Kamar
po
s
hti
)
1497
dr
i
ve
syst
em
.
The
researc
h
r
esults
on
m
ulti
-
phase
dri
ves
are
s
umm
arized
in
[
7
-
8].
It
is
to
be
note
d
t
hat
the
m
ul
ti
-
ph
ase
m
otors
a
re
in
va
r
ia
bly
s
upplied
by
po
wer
el
ect
ronic
c
onve
rters
si
nce
var
ia
bl
e
sp
ee
d
a
pp
li
c
at
ion
s
are
sought.
Th
us
the
em
ph
asi
s
of
the
resea
r
ch
on
m
ult
i
-
phase
el
ect
ric
dr
ive
is
lim
it
ed
t
o
the
m
od
el
li
ng
an
d
con
t
ro
l
of
t
he
powe
r
el
ect
ronic
co
nverters
su
c
h
as
in
ve
r
te
rs
an
d
m
at
ri
x
c
on
ver
te
rs
[
7
-
17]
.
I
niti
al
ly,
only
two
-
le
vel
c
onve
rters
wer
e
us
e
d
[
6],
a
nd
la
te
r
on
m
ulti
-
le
vel
m
ult
i
-
ph
ase
c
onve
rters
is
i
nvest
igate
d
[
18
]
.
W
a
rd
and H
a
rer [
19
]
p
r
opos
e
d
m
ultip
ha
se m
oto
r dri
ves,
but t
he re
search
on it
wa
s slo
w
in
it
s r
el
ease.
The
resea
rch
on
m
ult
iph
ase
dri
ve
syst
e
m
s
has
been
sig
nifi
cantl
y
dev
el
op
ed
since
the
be
ginnin
g
of
this
centur
y
due
to
ad
van
ce
m
ent
in
se
m
i
condu
ct
or
de
vices
an
d
dig
i
ta
l
sign
al
pr
oc
esso
rs
te
chno
log
ie
s
.
Detai
le
d
re
views
on
sta
te
-
of
-
the
-
art
m
ulti
ph
ase
dr
i
ve
resea
rch
a
re
avail
ab
le
in
[15]
-
[
18]
and
[
20
]
.
It
is
to
be
e
m
ph
asi
zed
he
re
that
ac/
dc/a
c
co
nverters
ge
ner
al
l
y
s
uppl
y
the
m
ulti
ph
ase
m
oto
rs.
Th
us
,
the
f
ocu
s
of
the
current
resea
r
ch
on
m
ulti
ph
ase
el
ect
ric
dr
ives
is
li
m
i
te
d
to
t
he
m
od
el
ing
a
nd
c
ontr
olli
ng
of
t
he
powe
r
conve
rter
s
[
21
]
-
[
26
]
,
[
27
]
,
[
28
]
,
[
29
]
-
[
31
]
.
Li
tt
le
eff
or
t
is
be
ing
m
ade
to
de
velo
p
sta
ti
c
transfor
m
at
ion
syst
e
m
to
cha
nge
the
ph
a
se
nu
m
ber
from
three
-
to
-
n
-
phase
(where
n>
3
a
nd
od
d).
An
ex
cepti
on
is
[
32
]
,
wh
e
r
e
a
ne
w
ty
pe
of
tra
nsfo
rm
er
is
pr
e
sent
ed,
w
hich
is
th
ree
-
to
-
fi
ve
-
pha
se
syst
em
.
In
[
33
]
a
nd
[
34
]
,
t
he
a
u
t
hors
pre
sented
an
intere
sti
ng
s
olu
ti
on
f
or
th
re
e
-
to
-
five
-
phase
co
nv
e
rsion.
A
t
the
en
d
of
[
33
]
,
the
a
uthor
s
br
ie
fly
m
ention
the
seve
n
-
ph
a
se sy
stem
; ho
we
ver,
no s
t
ud
y
or an
al
ysi
s w
as
done
on three
-
to
-
s
even
-
pha
se
tra
ns
f
or
m
er.
Accor
dingly
,
this
pap
e
r
is
ba
sed
on
the
sa
m
e
pr
inci
ple
a
s
that
of
[
32
]
.
The
analy
sis
and
de
sig
n,
howe
ver,
ar
e
c
om
plete
ly
diff
eren
t.
I
n
our
a
ppr
oac
h,
i
n
c
on
t
rast
to
the
syst
e
m
of
[
32
]
,
t
he
phase
a
ngle
bet
ween
two
co
ns
ec
utive
phases
is
not
a
n
i
nteger
num
ber
.
Mult
ip
hase,
es
pecial
ly
6
-
a
nd
12
-
ph
ase,
syst
em
s
ar
e
fou
nd
to
pr
oduce
le
s
s
am
plit
ud
e
of
rip
ples
with
hi
gh
e
r
f
re
qu
e
nc
y
in
ac
dc
recti
fier
syst
em
[
35
]
.
T
hu
s
,
6
-
a
nd
12
-
ph
a
se
trans
for
m
ers
are
design
e
d
to
fee
d
a
m
ulti
-
pu
lse
recti
fier
syst
em
an
d
the
te
chnolo
gy
is
m
at
ur
e
d.
Re
centl
y,
24
-
an
d
36
-
phas
e
trans
f
or
m
er
syst
e
m
s
were
pro
posed
f
or
s
upplyi
ng
a
m
ult
i
-
pu
lse
r
ect
ifie
r
syst
e
m
[
3
6
-
3
9]
.
The
reason o
f
ad
opti
ng
a 6
-
, 1
2
-
, o
r
24
-
phas
e
syst
e
m
is
that
these
num
ber
s
are
m
ulti
ples
of
t
hr
ee
a
nd
desig
ning
su
c
h
syst
e
m
is
si
m
ple
and
strai
ghtf
orward.
H
oweve
r,
inc
reas
ing
the
num
ber
of
phases
ce
rtai
nly
aff
ect
s
the
c
om
plexit
y
of
th
e
syst
e
m
.
No
s
uch
desig
n
is
avail
able
f
or
odd
num
ber
of
ph
a
ses,
s
uch
a
s
7,
11,
et
c.,
as
far
as
is
known
to
th
e
auth
or
s
.
The
us
ual
pract
ic
e
fo
r
a
naly
sis
is
to
te
st
the
design
e
d
m
oto
r
fo
r
a
nu
m
ber
of
ope
rati
ng
co
ndit
ion
s
with
pure
sinu
s
oi
dal
sup
ply
[
40
]
.
Norm
ally,
no
-
loa
d
te
st
,
bl
ock
e
d
r
otor
,
a
nd
load
te
sts
are
pe
rfor
m
ed
on
a
m
oto
r
to
determ
ine
it
s
par
a
m
et
ers.
Alth
ough
supp
ly
us
e
d
for
m
ult
iph
ase
m
oto
r
dr
i
ves
obta
ine
d
f
ro
m
m
ulti
ph
a
se
inv
e
rter
s
cou
l
d
ha
ve
m
or
e
cur
re
nt
rip
ples,
the
re
are
co
ntr
ol
m
et
hods
avail
able to
lo
wer t
he
c
urre
nt d
ist
ort
ion bel
ow
1%,
base
d o
n
a
pp
li
cat
io
n
a
nd r
e
quirem
ent [
25
]
.
The
m
achine
par
am
et
ers
ob
ta
ined
us
i
ng
a
P
W
M
in
ver
t
er
m
ay
no
t
p
rovide
the
c
or
rect
val
ue.
Th
us
,
a
pu
re
s
inu
s
oid
al
s
uppl
y
syst
e
m
is
r
equ
i
red
to
fee
d
the
m
oto
r
f
or
bette
r
a
naly
sis.
Accor
dingly
,
this
pap
e
r
pr
opos
e
s
a
sp
eci
al
transfor
m
er
co
nnect
ion
schem
e
to
ob
ta
in
a
ba
la
nced
th
ree
-
to
-
se
ve
n
-
phase
su
pply
with sin
usoidal
w
ave
form
s.
The
ex
pected a
ppli
cat
ion
areas
of
the
pro
pose
d
tran
sf
or
m
er ar
e the
el
ect
ric p
owe
r
transm
issi
on
syst
e
m
,
po
wer
e
le
ct
ro
nic
co
nv
erters
(ac
-
dc
a
nd
ac
-
ac),
a
nd
the
m
ulti
ph
ase
el
ect
ric
dr
ive
syst
e
m
.
The
fi
xe
d
three
-
phase vo
lt
a
ge
and
f
ixe
d
fr
e
quency
avail
able in
gri
d
powe
r
s
upply
can b
e
tr
ansfo
rm
ed
to
fixe
d
vo
lt
age
an
d
fixed
fr
e
que
ncy
seve
n
-
ph
a
se
ou
t
pu
t
s
upply.
Furtherm
or
e,
the
outp
ut
m
a
gn
it
ude
m
ay
be
m
ade
var
ia
ble
by
in
serti
ng
a
th
ree
-
phase
a
uto
tra
ns
f
or
m
er
at
th
e
input
side
.
I
n
t
his
pa
per
,
the
in
put
an
d
ou
t
put
su
pply
ca
n be
arr
a
ng
e
d
i
n
th
e
foll
ow
i
ng m
ann
ers:
a.
Inp
ut star,
outp
ut star.
b.
Inp
ut star,
outp
ut h
e
ptag
on.
c.
Inp
ut d
el
ta
, o
utp
ut
sta
r.
d.
Inp
ut d
el
ta
, o
utp
ut
he
ptag
on.
Since
input
is
a
three
-
phase
syst
em
the
winding
s
are
c
onnecte
d
in
us
ua
l
m
ann
er
.
The
outp
ut/se
conda
ry
side
sta
r
connecti
on
is
discuss
e
d
in
the
fo
ll
ow
ing
sect
io
ns
.
The
he
ptag
on
ou
tp
ut
connecti
on
m
a
y
be
der
ive
d
f
ollow
i
ng
a
sim
il
ar
app
r
oac
h.
Th
us
,
only
sta
r
ou
t
pu
t
co
nne
ct
ion
is
discusse
d
in
the foll
owin
g
s
ect
ion
a
nd o
t
he
r
c
onnecti
ons a
re
om
i
tt
ed.
2.
WIN
DI
NG A
RRA
NGEME
NT SE
VEN
-
P
HAS
E
STA
R OUTP
UT
Thr
ee
se
pa
rate
iron
c
ores
are
desig
ned
with
each
of
them
carryin
g
one
pri
m
ary
and
fou
r
seco
ndary
coils,
exce
pt
in
one
c
or
e
w
he
re
fiv
e
seco
ndary
c
oils
are
wou
nd.
Six
te
r
m
inals
of
pr
i
m
aries
are
c
onne
ct
ed
in
an
ap
propriat
e
m
ann
er
res
ulti
ng
in
sta
r
an
d/or
delta
connecti
ons,
an
d
the
26
te
rm
inals
of
seco
nd
a
ry
are
connecte
d
in
a
diff
e
re
nt
fas
hi
on
res
ulti
ng
i
n
a
sta
r
or
hep
ta
gon
ou
t
pu
t
.
Th
e
connecti
on
s
chem
e
o
f
seco
nd
a
ry
windin
gs
to
obta
in
sta
r
outp
ut
is
il
lustrated
in
F
ig
ure
s
.
1
an
d
2
a
nd
t
he
co
rr
es
pond
i
ng
ph
a
sor
dia
gr
am
is
il
lustrate
d
in
Fig
ure
3.
T
he
con
st
ru
ct
io
n
of
ou
t
pu
t
phas
es
with
re
quisi
te
ph
ase
a
ng
l
es
of
360/
7
=
51.43
◦
be
twee
n
each
ph
a
se
is
ob
ta
in
ed
us
i
ng
a
ppr
opriat
e
tur
n
rati
os
an
d
the
gove
rn
i
ng
ph
a
sor
equ
at
io
n
is
i
ll
us
trat
ed
in
(1
c
).
T
he
tu
r
n
ra
ti
os
a
re
dif
fer
e
nt
in
each
ph
a
se
as
sho
w
n
in
Fig
ure
1.
The
ch
oice
of
tur
n
rati
o
is
the
key
in
creati
ng
the
r
e
qu
isi
te
phase
di
sp
la
cem
ent
in
the
ou
tp
ut
ph
ases.
The
tu
rn
rati
os
betwee
n
diff
e
ren
t
phas
es
are
Evaluation Warning : The document was created with Spire.PDF for Python.
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8708
In
t J
Elec
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C
om
p
En
g,
V
ol.
9
, N
o.
3
,
June
201
9
:
1496
-
1505
1498
giv
e
n
in
Ta
ble
1
.
T
he
in
pu
t
ph
a
ses
a
re
de
sign
at
e
d
with
le
tt
ers
“X
,”
“Y,
”
a
nd
“Z”
an
d
th
e
ou
t
put
are
desig
nated
wit
h
le
tt
ers
“a,”
“
b,
”
“c
,”
“
d,
”
“
e
,”
“f
,”
a
nd
“g
.”
The
m
at
he
m
a
t
ic
al
basis
f
or
this
c
onnecti
on
is
t
he
basic
a
dd
it
io
n
of
real
a
nd
im
agina
ry
pa
rts
of
t
he
vecto
rs.
For
e
xam
ple,
the
so
l
utio
n
f
or
(
1a)
gi
ves
t
he
tur
n
rati
o of
phase “
b,
”
(
Vb take
n
a
s unit
y)
1
21
s
i
n
21
c
o
s
7
2
s
i
n
7
2
c
o
s
Vx
j
Vz
j
(1)
Fig
ure
1.
Pro
pose
d
tra
ns
f
orm
er
windin
g
c
onnecti
on (
sta
r)
Fig
ure
2.
Pro
pose
d
tra
ns
f
orm
er
w
in
ding arra
ng
em
ents (
sta
r
-
sta
r)
Evaluation Warning : The document was created with Spire.PDF for Python.
In
t J
Elec
&
C
om
p
En
g
IS
S
N:
20
88
-
8708
Mo
difi
ed
ap
proa
c
h
f
or
harm
on
ic
red
uctio
n i
n
t
hr
ee
-
ph
as
e
to
seve
n
…
(
M
ehr
dad
A
hma
di
Kamar
po
s
hti
)
1499
Fig
ure
3.
P
has
or d
ia
gr
am
o
f
t
he pr
opos
e
d
t
r
an
sf
orm
er co
nnect
ion (sta
r
-
st
ar)
T
a
b
l
e
1
.
T
u
r
n
R
a
t
i
o
S
e
c
o
n
d
a
r
y
T
u
r
n
s
(N
2
)
t
o
P
r
i
m
a
r
y
(A
1
A
2
)
T
u
r
n
s
(N
1
)
Turn
s ratio N2
/N1
Na
m
e
of
the win
d
in
g
Turn
s
ratio N2
/N1
Na
m
e
of
the win
d
in
g
Turn
s ratio N2
/N1
Na
m
e
of
the win
d
in
g
0
.50
1
0
c1
c2
0
.78
5
4
b1b2
0
.17
2
1
a1
a2
0
.78
5
4
c3
c4
0
.50
1
0
b3b4
1
.00
0
0
a3
a4
0
.34
0
4
c5
c6
0
.90
2
8
b5b6
0
.17
2
1
a5
a6
0
.90
2
8
c7
c8
0
.34
0
4
b7b8
0
.65
0
5
a7
a8
Eq
uating real
a
nd im
aginar
y p
arts
an
d sol
ving
for
V
x
a
nd
V
z
we get
:
s
i
n
/
2
1
0
.
1
7
2
1
s
i
n
/
3
Vx
(2)
s
i
n
2
/
7
0
.
9
0
2
8
s
i
n
/
3
Vz
(3)
The
(1
c
)
is
th
e
res
ult
of
so
l
utions
of
e
qua
ti
on
s
li
ke
(
1a)
for
oth
e
r
ph
a
ses.
T
her
e
fore,
by
sim
ply
su
m
m
ing
the
vo
lt
age
s
of
tw
o
dif
fer
e
nt
coils,
on
e
outp
ut
ph
a
se
is
create
d.
It
is
i
m
po
rtant
to
no
te
th
at
the
ph
a
se “a” ou
t
put i
s g
ene
rated
from
o
nly on
e coil nam
ely “a
3a4
”
in c
ontras
t t
o
oth
er phas
es w
hic
h
util
iz
es two
coils.
T
hu
s
,
th
e
volt
age
rati
ng
of
“a
3a
4”
co
il
sh
ould
be
ke
pt
to
that
of
rat
ed
ph
ase
volt
age
to
obta
in
ba
la
nce
d
and eq
ual
vo
lt
a
ges
.
Vz
Vy
Vx
Ve
Vd
Vc
Vb
Va
0
)
7
2
s
i
n
(
)
21
s
i
n
(
)
21
5
s
i
n
(
)
21
2
s
i
n
(
0
)
7
s
i
n
(
0
)
21
4
s
i
n
(
0
)
7
s
i
n
(
)
21
4
s
i
n
(
)
21
2
s
i
n
(
)
21
5
s
i
n
(
0
)
7
2
s
i
n
(
0
)
21
s
i
n
(
0
0
)
3
s
i
n
(
*
)
3
s
i
n
(
1
(4)
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8708
In
t J
Elec
&
C
om
p
En
g,
V
ol.
9
, N
o.
3
,
June
201
9
:
1496
-
1505
1500
Wh
e
re t
he
th
re
e
-
phase
volt
ag
es (
li
ne
-
to
-
ne
ut
ral) a
re
def
i
ned as
:
m
a
x
sin
3
,
,
,
0
,
2
,
4
j
V
V
t
n
j
x
y
z
n
(5)
m
a
x
s
in
,
,
,
,
,
,
,
7
0
,
2
,
4
,
6
,
8
,
1
0
,
1
2
k
V
V
t
n
k
a
b
c
d
e
f
g
a
n
d
n
(6)
Using
(1
c
),
a
seve
n
-
phase
ou
t
pu
t
can
be
create
d
f
r
om
a
th
ree
-
phase
input
s
upply.
A
ge
ner
a
l
expressi
on
for
an
“n”
phase
syst
e
m
is
der
ived
a
nd
sho
w
n
in
(
6
)
.
Si
nce
a
transfo
rm
er
works
as
a
two
-
po
rt
netw
ork,
the
re
ver
se
co
nnect
ion
is
al
so
poss
ible,
i.e.,
if
a
s
even
-
ph
ase
s
upply
is
giv
e
n
a
t
the
in
pu
t
t
he
ou
t
pu
t
can
be
th
ree
phase.
T
his
is
especial
ly
i
m
po
rtant
if
el
ect
ric
power
is
ge
ne
rated
usi
ng
a
seven
-
ph
ase
al
t
ern
at
or
and
t
he
s
upply
to
the
gr
i
d
is
giv
e
n
as
th
ree
ph
a
se.
T
o
ob
ta
in
three
-
ph
ase
ou
t
pu
ts
from
a
seve
n
-
ph
a
se
in
pu
t
su
pply
,
fo
ll
owi
ng r
el
at
io
ns
hold go
od
.
Ve
Vd
Vc
Vb
Va
Vz
Vy
Vx
t
0
0
0
)
21
4
s
i
n
(
0
0
)
21
2
s
i
n
(
0
0
0
)
21
2
s
i
n
(
0
0
)
21
4
s
i
n
(
0
0
0
0
0
0
)
7
2
s
i
n
(
*
)
7
2
s
i
n
(
1
(7)
3.
WIN
DI
NG A
RRA
NGEME
NT SE
VEN
-
P
HAS
E
DELT
A
O
UTP
UT
Thr
ee
se
pa
rate
iron
c
ores
are
desig
ned
with
each
of
them
carryin
g
one
pri
m
ary
and
fou
r
seco
ndary
coils,
exce
pt
in
one
c
or
e
w
he
re
fiv
e
seco
ndary
c
oils
are
wou
nd.
Six
te
r
m
inals
of
pr
i
m
aries
are
c
onne
ct
ed
in
an
ap
pro
pr
ia
te
m
ann
er
resu
lt
i
ng
i
n
delta
co
nnect
ions,
an
d
t
he
26
te
rm
inals
of
sec
onda
ries
are
co
nn
ect
e
d
in
a
diff
e
re
nt
fas
hi
on
res
ulti
ng
in
a
sta
r
ou
t
put.
The
c
onnecti
on
schem
e
of
seco
nd
a
ry
wi
ndin
gs
to
obta
in
sta
r
ou
t
pu
t i
s
il
lustr
a
te
d
in
Fig
ure
4
.
Figure
4.
Pro
pose
d
tra
ns
f
orm
er
wi
ndin
g
ar
ra
ng
em
ents (delt
a
-
sta
r)
Evaluation Warning : The document was created with Spire.PDF for Python.
In
t J
Elec
&
C
om
p
En
g
IS
S
N:
20
88
-
8708
Mo
difi
ed
ap
proa
c
h
f
or
harm
on
ic
red
uctio
n i
n
t
hr
ee
-
ph
as
e
to
seve
n
…
(
M
ehr
dad
A
hma
di
Kamar
po
s
hti
)
1501
T
he
co
rr
es
pondin
g
phaso
r
di
agr
am
is
il
lustrate
d
in
Fig
ure
5
.
The
c
on
st
ruct
ion
of
ou
t
pu
t
ph
ases
wit
h
requisi
te
phase
angles
of
360/
7=
51.
43
◦
betw
een
eac
h phase
is
obta
ine
d using ap
pro
pr
ia
te
tur
n
rati
os
.
Figure
5.
P
has
or d
ia
gr
am
o
f
t
he pr
opos
e
d
t
r
an
sf
orm
er co
nnect
ion (
delta
-
sta
r)
4.
WIN
DI
NG A
RRA
NGEME
NT SE
VEN
-
P
HAS
E
HEPT
AGON
OUTP
UT
The
c
onstr
uction
of
ou
t
pu
t
phases
with
requisi
te
phase
a
ngle
s
of
360/
8=
45◦
bet
ween
e
ach
ph
as
e
is
ob
ta
ine
d
us
i
ng
ap
pro
pr
ia
te
tu
rn
rati
os.
T
hre
e
sepa
rate
ir
on
co
res
a
re
desi
gn
e
d
with
each
of
them
carryi
ng
one
pr
im
ary
and
f
our
sec
onda
ry
c
oils,
exce
pt
in
on
e
c
ore
w
here
five
sec
onda
r
y
coils
are
w
ound.
Six
te
rm
i
nals
of
pr
im
aries
ar
e
connecte
d
i
n
an
appr
opriat
e
m
ann
e
r
re
su
lt
in
g
in
delta
or
sta
r
co
nnect
ion
s
,
and
t
he
28
te
r
m
inals
of
s
eco
ndarie
s
are
c
onnect
ed
in
a
he
pt
agon
outp
ut.
Figure
6
s
how
p
r
opos
e
d
t
ran
s
f
or
m
er
wind
i
ng
arr
a
ng
em
ents
(
sta
r
-
hep
ta
gon)
.
T
a
b
l
e
2
s
h
o
w
t
urn
r
a
t
i
o
s
e
c
o
n
d
a
r
y
t
u
r
n
s
(N
2
)
t
o
p
r
i
m
a
r
y
(A
1
A
2
)
t
u
r
n
s
(
N
1
)
s
t
a
r
-
h
e
p
t
a
g
o
n
a
n
d
d
e
l
t
a
-
h
e
p
t
a
go
n
[
4
1
]
.
Fig
ure
6.
Pro
pose
d
tra
ns
f
orm
er
windin
g
ar
ra
ng
em
ents (
sta
r
-
hep
ta
gon)
Evaluation Warning : The document was created with Spire.PDF for Python.
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S
N
:
2088
-
8708
In
t J
Elec
&
C
om
p
En
g,
V
ol.
9
, N
o.
3
,
June
201
9
:
1496
-
1505
1502
T
a
b
l
e
2
.
T
u
r
n
R
a
t
i
o
S
e
c
o
n
d
a
r
y
T
u
r
n
s
(N
2
)
to
P
r
i
m
a
r
y
(A
1
A
2
)
T
u
r
n
s
(N
1
)
S
t
a
r
-
H
e
p
t
a
g
o
n
a
n
d
D
e
l
t
a
H
e
p
t
a
g
o
n
[
4
1
]
Turn
s ratio
N2
/N1
Na
m
e
of
the win
d
in
g
Turn
s ratio
N2
/N1
Na
m
e
of
the win
d
in
g
Turn
s ratio
N2
/N1
Na
m
e
of
the
win
d
in
g
0
.81
6
5
c
1
c2
0
.57
7
3
b
1b2
1
.00
0
0
a
1
a2
0
.57
7
3
c
3
c4
0
.81
6
5
b
3b4
0
.29
8
8
a
3
a4
0
.81
6
5
c
5
c6
0
.57
7
3
b
5b6
0
.29
8
8
a
5
a6
0
.57
7
3
c
7
c8
0
.81
6
5
b
7b8
1
.00
0
0
a
7
a8
0
.29
8
8
a9
a1
0
0
.29
8
8
a1
1
a1
2
5.
SIMULATI
O
N RESULTS
The
desi
gn
e
d
transfor
m
er
is
at
first
si
m
ula
te
d
us
in
g
“Si
m
Po
wer
S
yst
e
m
”
blo
ck
set
s
of
the
MATLAB/Si
m
ulink
s
of
t
war
e
.
T
he
i
nbuilt
trans
f
or
m
er
bloc
ks
a
re
us
e
d
t
o
sim
ulate
the
co
nce
ptu
al
de
sig
n.
The
a
pprop
riat
e
tur
n
rati
os
a
re
set
in
the
di
al
og
bo
x
an
d
the
sim
ulatio
n
i
s
r
un.
Tu
r
n
rati
os
are
s
ho
wn
i
n
Table
s
1
a
nd
2
.
The
re
su
lt
in
g
input
and
outpu
t
vo
lt
age
wa
vefor
m
s
are
il
l
us
trat
ed
i
n
Fig
ure
7.
It
is
see
n
that
the outp
ut is a
balance
d
se
ve
n
-
phase
sup
ply f
or a
balance
d
t
hr
ee
-
phase
in
put.
Va=Vx
(a)
Vb
=
0.1
721Vx
-
0.902
8V
z
(b)
Vc
=
0.785
4V
y
-
0.3
404Vz
(c)
Vd =
-
0.6
505Vx+0.5
010Vy
(d)
Ve=
-
0.6
505 V
x+0.50
20Vz
(e)
Vf
=
-
0.3
404V
x+0.78
54Vz
(f)
Fig
ure
7
.
(
a
)
V
a outp
ut volt
ag
e an
d
in
puts
V
x
, (
b
)
V
b ou
t
put v
oltage
an
d i
nputs
Vx and
–
Vz
,
(
c
)
Vc o
utput v
oltage a
nd in
puts Vy
an
d
–
Vz
, (
d
)
V
d o
utpu
t vo
lt
age
a
nd inputs
–
Vx
an
d Vy
,
(
e
)
Ve o
utput v
oltage a
nd in
puts
-
V
x
a
nd V
z
, (
f
)
Vf
ou
t
pu
t
vo
lt
age
and i
nputs
-
Vx and
V
z
,
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Va
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Vb
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Vc
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Vd
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Ve
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Vf
Evaluation Warning : The document was created with Spire.PDF for Python.
In
t J
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om
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g
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S
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20
88
-
8708
Mo
difi
ed
ap
proa
c
h
f
or
harm
on
ic
red
uctio
n i
n
t
hr
ee
-
ph
as
e
to
seve
n
…
(
M
ehr
dad
A
hma
di
Kamar
po
s
hti
)
1503
Vg =0
.17
21V
x
-
0.9
028Vy
(g)
(h)
(i)
Figure
7.
(
g
)
V
g ou
t
pu
t
volt
ag
e an
d
in
puts
V
x
a
nd
–
Vy
, (
h)
input v
oltage
Vx and
Vy a
nd V
z
,
(i)
T
he
outp
ut
vo
lt
age
V
a
, Vb
, V
c
, Vd
, Ve,
Vf
an
d Vg
The
outp
ut
will
be
unbalance
d
if
the
input
is
unbalance
d.
The
un
balanci
ng
stu
dy
is
ou
t
of
the
sco
pe
of
this
pap
e
r
a
nd
will
be
deal
t
separ
at
el
y
and
re
ported
in
t
he
f
uture.
I
ndivid
ual
outp
ut
ph
a
ses
are
al
so
sh
ow
n
al
ong
with
t
heir
res
pecti
ve
in
pu
t
vo
lt
age
s.
T
he
phase
Va
is
no
t
s
how
n
bec
ause
Va
=V
x
,
i.
e.,
the
in
put
an
d
th
e
ou
t
pu
t
phases
are
sa
m
e.
Fig
ure
7
s
hows
the
reconstr
uc
ti
on
of
seve
n
-
phase
outp
ut
wav
ef
or
m
fr
om
a
three
-
phase
i
nput
wav
e
f
or
m
.
The
t
hr
ee
-
phas
e
outp
ut
f
ro
m
a
seve
n
-
phase
input
sup
ply
c
an
al
s
o
be
ob
ta
ined
i
n
si
m
il
ar f
ashio
n.
6.
FFT A
NA
L
Y
SIS
Four
ie
r
a
naly
s
is
is
the
proce
ss
of
re
pr
ese
nt
ing
a
functi
on
in
te
rm
s
of
sinu
s
oi
dal
com
po
ne
nts.
It
is
widely
em
plo
ye
d
in
m
any
areas
of
e
ng
i
neer
i
ng,
sci
e
nce,
a
nd
a
pp
li
ed
m
at
h
e
m
at
ic
s.
It
pro
vid
es
i
nfo
rm
ati
on
as
to
w
hat
fr
e
que
ncy
com
po
ne
nt
s
rep
r
esent
a
f
un
ct
io
n.
The
F
FT
analy
sis
gi
ves
the
T
H
D
of
the
syst
em
to
that
of
a fun
dam
ental
value.
Rat
e
of
har
m
on
ic
g
e
ne
rati
on
i
n
Star
-
S
ta
r
m
od
e v
ery
high and the ra
te
o
f
the
har
m
on
ic
in
novel c
onnecti
on d
el
ta
-
sta
r
r
e
aches t
o
zer
o.
Fi
gure
8a
a
nd
8b is T
HD m
ea
su
re
d
at
t
he posi
ti
on
s
how
n.
Fig
ure
8a. T
he
outp
ut volt
age
fu
ndam
ental
h
arm
on
ic
s in
t
he
star
–
sta
rs
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
Vg
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
V
i
n
0
0
.
0
0
5
0
.
0
1
0
.
0
1
5
0
.
0
2
0
.
0
2
5
-
4
0
0
-
2
0
0
0
200
400
T
i
m
e
V
o
u
t
Evaluation Warning : The document was created with Spire.PDF for Python.
IS
S
N
:
2088
-
8708
In
t J
Elec
&
C
om
p
En
g,
V
ol.
9
, N
o.
3
,
June
201
9
:
1496
-
1505
1504
Fig
ure
8b. Th
e outp
ut volt
ag
e f
unda
m
ental
h
arm
on
ic
s in
t
he delt
a
–
sta
rs
7.
CONCL
US
I
O
N
This
pap
e
r
give
s
a
new
m
et
h
od
to
c
onve
rt
3
ph
a
se
to
7
phase
us
in
g
sp
e
ci
al
transfor
m
er
c
onnecti
on
.
The
wi
nd
i
ng
arr
a
ng
em
ent
and
the
vecto
r
diagr
am
,
al
on
g
with
the
tur
n
rati
os,
are
giv
en
in
the
ta
ble.
The
s
uccess
fu
l
i
m
ple
m
entat
i
on
of
t
he
pr
opos
e
d
co
nnect
io
n
s
chem
e
is
elab
orat
ed
upon
us
in
g
sim
ulatio
n
of
m
at
la
b
so
ftwa
r
e
us
in
g
sim
po
wer
syst
em
blo
ck
s.
T
he
pr
opos
e
d
co
nnect
io
n
sc
hem
e
can
be
use
d
i
n
dri
ve
s
an
d
oth
e
r
m
ulti
ph
ase ap
plica
ti
on
s
. By usi
ng the
sam
e
m
et
ho
d we ca
n
al
s
o get the
hep
ta
gon o
utput.
REFERE
NCE
S
[1]
D.
Basic,
J.G
.
Z
hu
and
G.
Board
m
an,
“
Tra
nsien
t
per
form
anc
e
stu
d
y
of
brushless
doubl
y
fed
twin
stat
or
g
ene
ra
tor
,
”
IEE
E
Tr
ans.
On
Ene
rgy
Con
ve
rs
i
on
,
vol
.
18
,
issue
3,
pp.
400
-
408,
2003.
[2]
L.
A.
Periera
and
V.M.
Cana
ll
i
,
“
Five
-
phase
per
m
ane
nt
m
agne
t
s
ynchr
onous
m
a
chi
ne
oper
a
ti
ng
as
gene
ra
tor
design
,
par
amete
r
d
et
er
m
ina
ti
on
b
y
FE
M
and
per
form
anc
e
,
”
Proc.
37th
IEE
E
Ind.
Appl.
Annual
Soci
ety
mee
ti
ng
IAS
,
vol
.
1,
pp
.
398
-
405
,
13
-
18
,
Octo
ber
2
002.
[3]
J.R.
Stewar
t
an
d
D.D.
W
il
son,
“
High
phase
orde
r
tra
nsm
ission
-
A
fea
sibil
ity
an
aly
sis
Part
-
I
-
Stea
d
y
sta
t
e
conside
ra
ti
ons
,
”
IEE
E
Tr
ans.
On
PA
S
,
vol
.
PA
S
-
97,
issue
6,
pp
23
00
-
2307,
Nov.
1
978.
[4]
J.R.
Stewar
t
an
d
D.D.
W
il
son,
“
High
phase
or
der
tra
nsm
ission
-
A
fea
sibil
ity
a
naly
s
is
Part
-
II
-
Over
volt
age
s
a
nd
insula
ti
on
req
u
ir
ements
,
”
IE
E
E
T
rans
.
On P
AS
,
v
ol.
PA
S
-
97,
issue
6,
pp
2308
-
231
7,
Nov.
1978.
[5]
K.N.
Pavit
hr
an,
R.
Parimel
al
ag
a
n
and
M.R
.
Krs
ihna
m
urth
y
,
‘St
udie
s
on
inve
rt
e
r
fed
f
ive
-
ph
ase
induc
t
ion
m
oto
r
drive
,
”
I
EE
E
Tr
ans.
Powe
r
Elec
t
.
vol
.
3
,
no
.
2
,
pp
.
224
-
235
.
[6]
A.
Iqba
l
,
S.
P
y
a
m
i,
R
.
K.
Behr
a,
and
A.
Anad
,
“
Fiel
d
Ori
ent
ed
c
ontrol
le
d
Five
-
p
hase
Induc
ti
on
m
otor
drive
wi
t
h
ac
t
ive
f
ront end rec
t
ifi
er
,
”
IE
EE
PE
CON
, 2
-
5
De
c.
,
Mal
a
y
s
ia,
CD
-
ROM
,
pp.
328
-
332.
[7]
E.
L
evi
,
“
Multi
p
hase
Elec
tr
ic
Ma
chi
nes
for
Vari
a
ble
-
Speed
Appl
i
ca
t
ions”
IEEE
T
ran
s on
Ind.
Elec
t.
,
vo
l.
55
,
No.
5,
pp.
1893
-
1909
.
[8]
J.R.
Stewar
t
an
dD.D.Wilson,
“
High
phase
orde
r
tra
nsm
ission
-
Afea
sibil
ity
anal
y
sis
—
Part
-
II
:
Over
volt
age
s
a
nd
insula
ti
on
req
u
ir
ements,
”
IEEE
T
rans
.
Powe
r
App
.
S
y
s
t.,
vol
.
PA
S
-
97,
no
.
6
,
pp
.
2
308
–
2317,
Nov.
1978.
[9]
J
.
R.
Stewar
t,
E.
Kall
aur
,
and
J.
S.
Grant
,
“
E
con
om
ic
s
of
EHV
high
phase
ord
er
t
ran
sm
ission,”
IE
EE
Tr
ans.
Power
App.
S
yst
.
,
vo
l.
-
PA
S 103,
no.
11
,
pp
.
3386
–
3392
,
Nov.
1984
.
[10]
S.
N.
T
ewa
ri
,
G.
K.
Singh,
and
A.
B.
Sa
roor,
“
Multi
phase
Pow
er
tr
ansm
ission
rese
arc
h
—
A
surv
e
y
,
”
E
le
c
tr.
Pow
er
Syst.
Re
s
.
,
vo
l. 2
4,
pp
.
207
–
215
,
1992.
[11]
C.
M.
Portel
a
a
ndM.C.
Ta
var
es
,
“
Six
-
phase
tra
nsm
ission
li
ne
-
p
ropa
gation
cha
r
ac
t
eri
sti
cs
and
new
thre
e
-
phase
rep
rese
nt
at
ion
,
”
IEE
E
Tr
ans.
Po
wer
Delive
ry
,
vo
l.
18
,
no
.
3
,
pp
.
1
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