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h
e
s
t
a
t
o
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f
th
e
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d
u
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m
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o
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its
w
h
ile
th
e
r
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t
o
r
b
a
r
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o
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m
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cir
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its
.
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h
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el
ec
t
r
i
ca
l
ci
r
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ar
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m
u
tu
all
y
co
u
p
lin
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et
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m
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th
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tan
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h
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m
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u
s
in
g
s
im
p
le
m
ath
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o
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m
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las.
W
F
A
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ap
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late
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ac
h
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p
a
r
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eter
s
,
s
t
at
o
r
w
in
d
in
g
tu
r
n
s
,
r
o
to
r
b
a
r
an
d
ai
r
-
g
a
p
e
cc
en
tr
i
c
ities
.
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cc
o
r
d
in
g
t
o
p
r
in
ci
p
l
e
o
f
th
is
th
eo
r
y
,
th
e
m
u
tu
al
an
d
s
elf
-
in
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u
ct
an
ce
s
b
etw
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s
tat
o
r
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d
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d
r
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t
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r
b
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(
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d
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)
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tat
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r
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cu
its
ca
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ed
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h
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r
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ati
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etw
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n
th
ese
w
in
d
in
g
is
tim
e
v
ar
y
in
g
b
e
ca
u
s
e
it
d
e
p
en
d
s
o
f
th
e
r
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t
o
r
p
o
s
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ti
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w
ith
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esp
ec
t
e
ac
h
o
th
e
r
an
d
w
ith
s
tato
r
w
in
d
in
g
.
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e
le
ak
ag
e
in
d
u
ct
an
ce
o
f
b
o
th
s
ta
to
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in
d
in
g
an
d
r
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to
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b
ar
s
a
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c
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id
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s
tan
ts
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o
m
p
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s
in
g
s
p
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d
esig
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f
o
r
m
u
las.
I
n
cu
r
r
en
t
w
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r
k
t
w
o
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r
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ce
d
u
r
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o
f
W
FA
h
av
e
b
ee
n
co
n
s
id
er
e
d
.
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h
e
s
l
o
t
ef
f
ec
t
is
n
o
t
in
c
lu
d
e
d
in
th
e
f
ir
s
t
ty
p
e
w
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er
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th
e
c
o
u
p
l
in
g
m
m
f
s
h
av
e
a
s
in
u
s
o
id
al
s
h
a
p
e
.
W
h
il
e
in
s
ec
o
n
d
a
p
p
r
o
ac
h
a
r
ea
l
w
in
d
in
g
d
is
t
r
i
b
u
ti
o
n
in
th
e
s
lo
ts
is
ass
u
m
ed
an
d
m
m
f
s
h
a
v
e
a
n
o
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s
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co
m
p
lete
m
o
d
el
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f
3
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ca
g
e
in
d
u
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m
o
to
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w
h
ich
h
as
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m
-
s
tato
r
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ct
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ci
r
cu
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ts
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d
n
-
r
o
to
r
b
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r
s
is
i
m
p
lem
en
ted
u
s
in
g
m
atlab
s
o
f
t
w
ar
e
[
1
3
]
.
A
n
ep
ic
s
tr
ateg
y
to
d
is
p
la
y
elec
tr
ica
l
m
ac
h
in
e
s
d
ep
en
d
en
t o
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W
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A
is
p
r
o
p
o
s
ed
.
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n
tr
ad
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al
W
F
A
,
it i
s
ac
ce
p
ted
t
h
at
tr
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in
air
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g
ap
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o
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t
s
p
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h
ea
d
in
g
.
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im
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s
id
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s
o
f
t
h
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s
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v
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t
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y
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w
h
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c
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p
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n
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w
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d
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t
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f
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m
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d
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m
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p
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m
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latio
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lt
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p
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d
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w
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p
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f
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m
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p
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m
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n
t
a
l
r
e
s
u
l
t
s
[
1
4
-
1
6
]
.
2.
CO
NST
R
UCT
I
O
N
O
F
T
H
R
E
E
P
H
AS
E
I
N
DUCT
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O
N
M
O
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R
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DE
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N
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WF
A
As
s
tated
p
r
ev
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s
l
y
t
h
e
m
o
d
el
o
f
3
-
Ф
in
d
u
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m
o
to
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s
in
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a
w
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d
in
g
f
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t
h
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as
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co
n
s
tr
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cted
.
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t
'
s
co
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s
id
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t
h
at
th
e
m
o
d
el
o
f
s
tato
r
an
d
r
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to
r
to
b
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f
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m
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lated
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s
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v
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ctr
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cir
cu
its
w
h
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h
ar
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co
u
p
led
to
g
eth
er
.
A
ls
o
it
's
ass
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m
ed
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cu
r
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en
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f
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t
h
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cir
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h
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llo
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m
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s
:
-
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s
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s
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ted
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tr
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tio
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f
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v
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th
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s
tato
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s
lo
ts
h
a
v
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b
ee
n
tak
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to
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.
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f
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it
y
ir
o
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p
er
m
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(
μ
ir
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=
∞)
to
in
tr
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d
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ce
th
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co
r
r
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t
b
eh
av
io
r
o
f
ac
tu
al
m
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to
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.
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Un
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f
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m
a
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g
ap
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ter
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b
ar
cu
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en
t
s
h
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v
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a
s
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m
ed
,
w
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e
ea
ch
ad
j
ac
en
t
b
ar
f
o
r
m
a
s
ep
ar
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cir
cu
it.
-
T
h
e
r
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to
r
b
ar
s
an
d
th
e
m
o
to
r
w
i
n
d
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g
s
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a
v
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b
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s
u
g
g
e
s
t
ed
to
h
av
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a
s
y
m
m
etr
ic
d
is
tr
ib
u
ti
o
n
.
-
T
h
e
ef
f
ec
t o
f
s
atu
r
atio
n
at
s
tar
tin
g
an
d
h
ea
v
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lo
ad
in
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ar
e
n
e
g
lecte
d
.
-
No
n
-
s
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s
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id
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tr
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ted
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u
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to
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lo
ts
e
f
f
ec
t a
ls
o
h
as b
ee
n
i
n
tr
o
d
u
ce
d
.
2
.
1
.
M
o
delin
g
o
f
v
o
lt
a
g
e
equa
t
io
ns
T
h
e
s
tato
r
o
f
th
e
in
d
u
cti
o
n
m
o
to
r
m
o
d
el
u
s
ed
in
cu
r
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n
t
w
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k
h
a
v
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a
3
-
Ф
w
i
n
d
in
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s
,
th
er
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f
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r
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a
th
r
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v
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ltag
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eq
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ar
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m
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T
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r
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s
s
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m
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as sh
o
w
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Fi
g
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r
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1
[
1
7
]
.
Fig
u
r
e
1
.
R
o
to
r
lo
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p
s
cu
r
r
en
t d
is
tr
ib
u
tio
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I
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(
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1107
w
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Fig
u
r
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1
d
is
p
lay
t
h
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cu
r
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is
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tio
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o
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e
r
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to
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lo
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p
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y
:
[
]
=
[
]
[
]
+
[
]
/
(
1
)
[
0
]
=
[
]
[
]
+
[
]
/
(
2
)
[
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=
[
]
[
]
+
[
]
[
]
(
3
)
[
]
=
[
]
[
]
+
[
]
[
]
(
4)
w
h
er
e,
Vs
i
s
t
h
e
v
ec
to
r
o
f
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h
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s
tato
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r
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r
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to
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,
R
s
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m
atr
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x
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s
tato
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,
R
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h
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m
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x
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t
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r
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to
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r
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tan
ce
s
,
L
s
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e
m
atr
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f
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d
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L
r
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e
m
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r
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to
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in
d
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s
,
L
s
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r
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g
s
lin
k
a
g
e
f
l
u
x
r
esp
ec
ti
v
el
y
[
1
2
,
1
8
,
1
9
]
.
Fro
m
(
1
)
an
d
(
3
)
,
th
e
v
o
ltag
e
eq
u
atio
n
s
o
f
th
e
s
tato
r
p
er
p
h
ase
m
a
y
b
e
w
r
itte
n
as
:
V
a
=
R
s
I
a
+
(
L
a
+
L
1s
)
+
L
ab
+
L
ac
(
5
)
V
b
=
R
s
I
b
+
(
L
b
+
L
1s
)
+
L
ba
+
L
bc
(
6)
V
c
=
R
s
I
c
+
(
L
c
+
L
1s
)
+
L
ca
+
L
cb
(
7
)
w
h
er
e
V
a
,
V
b
an
d
V
c
ar
e
t
h
e
p
er
p
h
ase
s
tato
r
v
o
lta
g
es
ia,
ib
an
d
ic
ar
e
th
e
p
er
p
h
ase
s
tato
r
cu
r
r
en
ts
L
a,
L
b
a
n
d
L
c
ar
e
t
h
e
p
er
p
h
ase
s
ta
to
r
s
elf
-
i
n
d
u
cta
n
ce
s
,
L
ab
,
L
bc
an
d
L
ca
ar
e
th
e
p
er
p
h
ase
s
ta
to
r
m
u
tu
a
l
in
d
u
c
tan
ce
s
L
ls
i
s
th
e
lea
k
a
g
e
i
n
d
u
cta
n
ce
o
f
th
e
s
tato
r
p
er
p
h
ase
.
T
h
ese
eq
u
ati
o
n
s
ar
e
r
e
w
r
it
ten
in
s
u
itab
le
w
a
y
t
o
s
u
it
th
e
b
asic
m
.
f
i
l
e
.
F
o
r
e
x
a
m
p
l
e
r
e
f
e
r
t
o
p
h
a
s
e
"
a
"
t
h
e
s
o
l
v
e
o
n
e
p
h
a
s
e
c
u
r
r
e
n
t
i
a
(
t
)
r
e
w
r
i
t
t
e
n
o
f
e
q
u
a
t
i
o
n
i
n
t
h
e
f
o
l
l
o
w
i
n
g
f
r
o
m
:
=
1
L
a
(
(
v
a
−
R
s
∗
)
−
(
L
ab
+
L
ac
+
L
)
)
(
8
)
w
h
er
e
,
L
ab
L
ac
,
L
ar
ar
e
in
d
u
cta
n
ce
s
an
d
t
h
eir
v
a
lu
e
ca
n
b
e
co
m
p
u
ted
b
ased
o
n
t
h
e
p
o
s
itio
n
o
f
r
o
to
r
.
Si
m
i
lar
l
y
th
e
ab
o
v
e
eq
u
atio
n
s
ca
n
b
e
a
r
r
an
g
ed
f
o
r
th
e
o
t
h
er
t
w
o
p
h
a
s
es
(
d
ib
/d
t
an
d
d
ic/d
t)
c
u
r
r
en
t
s
a
n
d
t
w
o
d
a
m
p
er
w
i
n
d
i
n
g
s
cu
r
r
en
t
s
.
T
h
e
co
m
p
lete
m
.
f
ile
f
o
r
th
r
ee
p
h
a
s
e
d
y
n
a
m
ic
m
o
d
el
o
f
in
d
u
ctio
n
m
ac
h
in
e.
T
h
e
r
o
to
r
lo
o
p
s
cu
r
r
en
ts
(
ir
1
,
ir
2
,
…,
ir
n
)
,
(
L
ar
1
,
L
ar
2
,
…,
L
ar
n
)
ar
e
m
u
tu
a
l i
n
d
u
cta
n
ce
s
o
f
s
ta
to
r
ph
ase
A
to
r
o
to
r
lo
o
p
s
,
(
L
b
r
1
,
L
b
r
2
,
…,
L
b
r
n
)
ar
e
m
u
t
u
al
i
n
d
u
cta
n
ce
s
o
f
s
tato
r
p
h
as
e
B
to
r
o
to
r
lo
o
p
s
,
an
d
(
L
cr
1
,
L
cr
2
,
…,
L
cr
n
)
ar
e
m
u
tu
al
in
d
u
cta
n
ce
s
o
f
s
tato
r
p
h
ase
C
to
r
o
to
r
lo
o
p
s
.
A
ll
r
o
to
r
cir
cu
its
ar
e
m
u
tu
al
l
y
co
u
p
led
w
it
h
ea
c
h
o
t
h
er
an
d
w
it
h
s
tato
r
p
h
ase
’
s
w
i
n
d
in
g
s
.
B
ased
o
n
2
an
d
4
an
d
w
ith
d
ep
en
d
o
n
Fig
u
r
e
1
,
th
e
r
o
to
r
l
o
o
p
v
o
lt
ag
e
eq
u
a
ti
o
n
k
m
ay
b
e
g
iv
en
as
:
0
=
2
(
R
b
)
I
rk
−
R
b
(
I
r
(
k
−
1
)
+
I
r
(
k
+
1
)
)
+
2
(
L
b
+
L
e
)
dI
rk
d
t
⁄
−
L
b
(
dI
r
(
k
−
1
)
d
t
⁄
+
dI
r
(
k
+
1
)
d
t
⁄
)
+
(
L
k1
dI
r1
d
t
⁄
+
L
k2
dI
r2
d
t
⁄
+
⋯
+
L
kk
dI
rk
d
t
⁄
+
⋯
+
L
kn
dI
rn
d
t
⁄
)
−
d
d
t
⁄
(
L
ak
I
a
+
L
bk
I
b
+
L
ck
I
c
(
9
)
w
h
er
e,
R
e,
r
b
,
L
b
,
L
e,
a
r
e
th
e
r
esis
t
an
ce
an
d
in
d
u
ct
an
ce
o
f
ea
ch
r
o
t
o
r
b
a
r
.
L
k
k
is
th
e
s
elf
in
d
u
ctan
c
e
o
f
ea
ch
r
o
to
r
l
o
o
p
(
L
k
1
,
L
k
2
,
…,
L
k
(
k
-
1
)
,
L
k
(
k
+
1
)
..
.
,
L
k
n
)
ar
e
th
e
m
u
tu
al
i
n
d
u
c
t
a
n
c
e
s
l
o
o
p
k
t
o
t
h
e
o
t
h
e
r
r
o
t
o
r
l
o
o
p
s
(
L
a
k
,
L
b
k
,
a
n
d
L
c
k
)
a
r
e
t
h
e
s
t
a
t
o
r
m
u
t
u
a
l
i
n
d
u
c
t
a
n
c
e
s
w
i
t
h
r
o
t
o
r
l
o
o
p
k
.
2
.
2
.
E
qu
a
t
io
n o
f
elec
t
ro
m
a
g
net
ic
t
o
rque
T
h
e
e
q
u
ati
o
n
o
f
th
e
el
ec
t
r
o
m
ag
n
etic
t
o
r
q
u
e
c
an
b
e
d
et
er
m
in
ed
b
ase
d
o
n
th
e
en
e
r
g
y
co
n
v
er
s
i
o
n
th
eo
r
y
,
th
e
e
lec
tr
o
m
ag
n
etic
to
r
q
u
e
e
q
u
ati
o
n
p
r
o
d
u
c
e
d
b
y
a
3
-
p
h
a
s
e
in
d
u
cti
o
n
m
o
to
r
ca
n
b
e
c
o
m
p
u
ted
u
s
in
g
th
e
f
o
ll
o
w
in
g
eq
u
ati
o
n
[
12
]:
T
e
=
[
]
[
]
[
r
]
(
1
0
)
w
h
er
e,
θ
r
is
th
e
an
g
u
lar
p
o
s
iti
o
n
of
r
o
t
o
r
,
T
e
is
th
e
d
ev
el
o
p
e
d
t
o
r
q
u
e
p
r
o
d
u
ce
d
b
y
th
e
m
o
to
r
.
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
0
8
8
-
8708
I
n
t J
E
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&
C
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m
p
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n
g
,
Vo
l.
11
,
No
.
2
,
A
p
r
il 2
0
2
1
:
1
1
0
5
-
1113
1108
2
.
3
.
E
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ro
m
ec
ha
nica
l
equa
t
io
n
T
h
e
m
ec
h
an
ic
al
e
q
u
ati
o
n
o
f
r
o
to
r
m
ay
b
e
w
r
itten
as
[
1
2
,
1
8
]
:
T
e
=
j
dw
r
d
t
⁄
+
w
r
+
TL
(
1
1
)
=
1
Ѳ
r
w
h
er
e,
J
is
m
o
m
en
t o
f
in
e
r
ti
a
o
f
r
o
t
o
r
,
w
r
is
r
o
to
r
an
g
u
la
r
s
p
e
ed
,
B
is
th
e
f
r
i
cti
o
n
c
o
ef
f
ici
en
t
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L
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th
e
l
o
a
d
t
o
r
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e
,
Ѳ
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e
an
g
u
la
r
p
o
s
it
io
n
o
f
th
e
r
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t
o
r
.
3.
NO
N
-
SI
NUSO
I
DA
L
SH
AP
E
S S
E
L
F
AN
D
M
UT
UAL I
NDUC
T
ANCE F
O
RM
UL
A
USI
N
G
WF
A
T
h
e
im
p
o
r
tan
t
k
e
y
o
f
W
F
A
o
f
th
e
in
d
u
ctio
n
m
o
to
r
is
to
co
m
p
u
te
th
e
v
alu
e
s
o
f
i
n
d
u
cta
n
ce
s
eq
u
atio
n
s
ac
cu
r
atel
y
,
i
n
[
2
,
3
]
th
e
w
i
n
d
i
n
g
f
u
n
ctio
n
m
et
h
o
d
h
ad
b
ee
n
ap
p
lied
in
o
r
d
er
ca
lcu
late
th
e
in
d
u
cta
n
ce
s
o
f
t
h
e
m
o
to
r
in
ter
m
s
a
n
g
u
lar
p
o
s
iti
o
n
o
f
r
o
to
r
θ
r
.
W
FA
is
an
an
al
y
tical
m
e
th
o
d
u
s
ed
to
ca
lcu
late
th
e
s
elf
a
n
d
m
u
tu
al
i
n
d
u
cta
n
ce
s
b
ased
o
n
t
h
e
d
is
tr
ib
u
tio
n
o
f
MM
F
in
th
e
air
-
g
ap
r
e
g
io
n
d
u
e
to
a
f
o
llo
w
a
cu
r
r
en
t
o
f
"
1
"
A
v
alu
e
p
ass
t
h
r
o
u
g
h
th
e
w
i
n
d
i
n
g
u
n
d
er
co
n
s
id
er
atio
n
.
Fro
m
t
h
e
p
r
in
cip
les
o
f
W
F
A
,
it
’
s
e
v
id
en
t
th
a
t
it
’
s
r
eq
u
ir
ed
to
ca
lcu
late
all
th
e
in
d
u
ctan
ce
s
o
f
t
h
e
m
ac
h
in
e
u
s
i
n
g
t
h
e
i
n
d
u
cta
n
ce
m
atr
ices.
T
h
ese
in
d
u
cta
n
ce
s
ar
e
n
o
r
m
all
y
d
eter
m
i
n
ed
u
s
i
n
g
W
F
A
.
T
h
e
g
en
er
al
f
o
r
m
u
la
t
h
at
w
ill
b
e
u
s
ed
to
ca
lcu
late
th
e
m
o
to
r
in
d
u
cta
n
ce
s
(
s
elf
a
n
d
m
u
tu
al)
is
d
e
f
i
n
ed
b
y
(
11
)
.
Usi
n
g
w
i
n
d
i
n
g
f
u
n
ctio
n
ap
p
r
o
ac
h
,
th
e
m
u
t
u
al
i
n
d
u
c
t
an
ce
b
et
w
ee
n
t
w
o
co
u
p
led
elec
tr
ic
cir
cu
it
s
(
s
tato
r
p
h
ases
o
r
r
o
to
r
b
ar
s
)
f
o
r
an
y
elec
tr
ical
m
ac
h
i
n
e
m
a
y
b
e
d
eter
m
i
n
ed
u
s
in
g
t
h
e
f
o
llo
w
in
g
eq
u
at
io
n
[
20
-
24]
:
L
ij
θ
)
=
µ
⁄
∫
2
0
(
,
)
(
,
)
(
1
2
)
w
h
er
e:
µ
is
t
h
e
p
er
m
ea
b
ili
t
y
o
f
air
an
d
=4
π.
1
0
-
7
H,
is
t
h
e
w
i
d
th
o
f
th
e
a
ir
g
ap
,
is
t
h
e
a
n
g
u
l
ar
p
o
s
itio
n
o
f
th
e
r
o
to
r
,
is
th
e
av
er
ag
e
r
ad
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s
o
f
th
e
air
g
ap
,
is
th
e
ef
f
ec
t
l
en
g
t
h
o
f
th
e
m
o
to
r
s
tack
,
is
a
ce
r
tain
p
o
in
t
alo
n
g
t
h
e
air
g
ap
,
(
,
)
is
ca
lled
th
e
w
i
n
d
in
g
f
u
n
ctio
n
a
n
d
r
ep
r
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ts
t
h
e
d
is
tr
ib
u
tio
n
o
f
t
h
e
m
ag
n
eto
m
o
ti
v
e
f
o
r
ce
alo
n
g
th
e
air
g
a
p
w
h
en
a
c
u
r
r
en
t
o
f
'
1
'
A
f
lo
w
in
th
e
w
i
n
d
in
g
.
I
n
cu
r
r
en
t
p
ap
er
a
th
r
ee
p
h
ase
in
d
u
ctio
n
m
o
to
r
,
3
6
s
tato
r
s
l
o
ts
an
d
s
y
m
m
etr
ical
co
n
ce
n
tr
ate
w
i
n
d
in
g
.
W
h
i
le
t
h
e
ca
g
e
r
o
to
r
o
f
th
e
m
o
to
r
co
m
p
r
o
m
is
e
a
2
8
-
eq
u
all
y
s
p
ac
ed
b
ar
s
.
T
h
e
g
eo
m
etr
ic
co
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[1
]
J
.
Ca
rre
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,
R
.
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ra
n
c
e
sc
h
i,
G
.
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o
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d
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8
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.
[2
]
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.
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tro
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n
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6
5
.
[3
]
M
.
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h
o
d
s,
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siri
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ri,
F
.
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.
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8
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2
.
[4
]
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sil
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l
.
2
,
p
p
.
41
-
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6
,
2
0
1
3
.
[5
]
R.
Kra
ll
,
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Kre
n
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d
A
.
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c
h
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id
,
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ra
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ter
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OPT
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2
0
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4
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.
4
3
7
-
4
4
4
.
[6
]
Ah
-
Ja
c
o
A
.
,
“
M
o
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e
Ly
o
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ll
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,
1
9
9
7
.
[7
]
J.
C.
M
o
re
ria
a
n
d
T
.
A
.
L
ip
o
,
“
M
o
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ted
A
C
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in
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g
a
p
f
lu
x
h
a
rm
o
n
ic
c
o
m
p
o
n
e
n
ts,”
in
IEE
E
T
ra
n
sa
c
ti
o
n
s
o
n
I
n
d
u
stry
Ap
p
li
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s
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l.
2
8
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n
o
.
2
,
p
p
.
3
4
3
-
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4
9
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.
Evaluation Warning : The document was created with Spire.PDF for Python.
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[8
]
K.
C.
De
e
k
sh
it
Ko
m
p
e
ll
a
,
M
.
V
e
n
u
G
o
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la
Ra
o
,
R.
S
rin
iv
a
sa
Ra
o
,
“
Ba
rin
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F
a
u
lt
Dia
g
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s
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o
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m
Tec
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e
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o
u
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n
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l
o
f
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e
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trica
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m
,
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1
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.
1
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1
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0
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7
[9
]
A
.
Do
u
latsh
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h
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d
P
.
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ri
,
“
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h
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we
r
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n
d
Dr
ive
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C)
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n
,
2
0
1
6
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p
.
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9
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4
.
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0
]
H.
A
.
T
o
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y
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t,
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.
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ian
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d
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.
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,
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3
rd
I
n
t.
Co
n
f.
El
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trica
l
R
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ti
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g
M
a
c
h
i
n
es
-
EL
ROM
A
,
2
0
0
6
.
[1
1
]
R.
A
li
p
o
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r
-
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a
ra
b
i,
Z
.
Na
siri
-
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h
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ri,
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.
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o
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h
ian
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u
n
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ti
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p
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ro
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h
,
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n
sa
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ti
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6
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p
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1
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4
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2
]
H.
A
.
T
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L
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o
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Tran
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ri
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f
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u
lt
s,”
in
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ra
n
s
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c
ti
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rg
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2
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p
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2
4
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4
7
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5
.
[1
3
]
S
.
M
.
R
a
z
iee
,
O.
M
isir
a
n
d
B.
P
o
n
ick
,
“
W
in
d
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F
u
n
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ti
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A
p
p
ro
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o
r
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in
d
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g
A
n
a
l
y
sis,”
in
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ra
n
sa
c
ti
o
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s
o
n
M
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g
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ti
c
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.
1
0
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p
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1
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9
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.
[1
4
]
M
.
No
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rm
o
h
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m
m
a
d
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r
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M
.
Kh
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li
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n
d
K.
A
b
b
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sz
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h
,
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ti
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,
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2
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2
n
d
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ra
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2
0
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4
,
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p
.
7
9
3
-
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9
7
.
[1
5
]
F
.
Bo
u
b
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k
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r,
A
.
A
issa
,
K.
A
b
d
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ll
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d
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im
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2
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ter
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o
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(
ICM
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A
lg
iers
,
2016
,
p
p
.
4
1
8
-
4
2
3
.
[1
6
]
F
.
Bo
u
b
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k
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r,
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A
b
d
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ll
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h
,
A
.
M
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.
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n
d
3
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F
i
n
it
e
El
e
m
e
n
t
M
e
th
o
d
s,”
2
0
1
5
4
t
h
In
ter
n
a
ti
o
n
a
l
Co
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fer
e
n
c
e
o
n
El
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c
trica
l
En
g
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rin
g
(
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)
,
Bo
u
m
e
rd
e
s,
2
0
1
5
,
p
p
.
1
-
5.
[1
7
]
S
.
Na
n
d
i,
S
.
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.
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.
[1
8
]
H.
A
.
T
o
li
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n
d
M
.
S
.
A
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,
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4
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p
.
9
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-
9
1
8
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9
9
6
.
[1
9
]
G
.
M
.
Jo
k
si
m
o
v
ic,
J.
P
e
n
m
a
n
,
a
n
d
N.
A
rth
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“
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u
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o
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p
p
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1
4
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0
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0
]
P
e
tar
M
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ć
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lek
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lo
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2
.
[2
1
]
T
o
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t
H.
A
.
,
L
ip
o
T
.
A
.
,
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it
e
J.
C.
,
“
A
n
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,
v
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l
.
6
,
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4
,
p
p
.
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-
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4
,
1991.
[2
2
]
L
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.
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.
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.
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3
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2
.
[2
4
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A
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d
.
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li
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2
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9
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-
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.
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5
]
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U
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ij
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.
[2
6
]
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.
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o
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n
d
H.
G
u
o
,
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In
teg
ra
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4
.
[2
7
]
K.
E.
Am
in
,
R.
M
.
Ha
m
o
u
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,
A
.
D.
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k
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