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.
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test
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ig
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ar
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en
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n
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h
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t
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er
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J
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,
th
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s
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t
(
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,
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r
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ici
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t
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,
th
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ttle
co
m
m
a
n
d
r
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n
(
)
an
d
m
o
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m
e
co
n
s
ta
n
t.
T
w
o
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s
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m
test
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s
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er
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t
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m
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d
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ased
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th
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r
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cip
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o
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t
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r
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s
t
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icien
t.
T
h
e
p
ar
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m
eter
f
o
u
n
d
i
n
t
h
is
p
ap
er
w
i
ll
b
e
u
s
ed
to
r
ep
r
esen
t
a
q
u
ad
r
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to
r
s
y
s
te
m
w
i
th
an
“
X
”
co
n
f
ig
u
r
atio
n
.
T
h
e
p
ar
a
m
e
t
er
id
en
ti
f
icatio
n
p
r
o
ce
s
s
w
a
s
co
n
d
u
cted
b
y
tak
i
n
g
th
e
r
ea
l
q
u
ad
r
o
to
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p
ar
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m
ea
s
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r
e
m
e
n
t
i
n
th
e
lab
.
T
h
e
q
u
ad
r
o
to
r
m
o
d
el
u
s
ed
in
th
is
p
ap
er
w
ill
b
e
ex
p
lain
ed
i
n
Sectio
n
2
an
d
p
ar
a
m
eter
id
en
ti
f
icat
io
n
p
r
o
ce
s
s
w
il
l b
e
d
escr
ib
ed
in
d
etail
in
S
ec
tio
n
3
.
2.
Q
UAD
RO
T
O
R
M
O
DE
L
I
n
t
h
is
p
ap
er
,
th
e
co
n
f
ig
u
r
ati
o
n
ch
o
s
en
f
o
r
th
e
q
u
ad
r
o
to
r
is
th
e
“
X”
co
n
f
ig
u
r
atio
n
.
B
y
u
s
in
g
th
e
v
ec
to
r
co
o
r
d
in
ate
n
o
tatio
n
,
t
h
e
tr
an
s
la
tio
n
al
p
o
s
itio
n
a
n
d
a
n
g
u
lar
p
o
s
itio
n
o
f
th
e
q
u
ad
r
o
to
r
w
it
h
r
e
s
p
ec
t to
t
h
e
E
ar
th
f
r
a
m
e
ca
n
b
e
d
ef
i
n
ed
in
E
q
u
atio
n
1
an
d
2
r
esp
ec
tiv
el
y
.
ῃ
= [
]
T
(
1
)
ᵹ
= [
]
T
(
2
)
T
h
e
ac
ce
ler
atio
n
o
f
th
e
ce
n
ter
o
f
m
as
s
o
f
t
h
e
r
ig
id
b
o
d
y
q
u
ad
r
o
to
r
is
b
ased
o
n
th
e
f
o
r
ce
s
an
d
ac
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ler
atio
n
s
ac
tin
g
o
n
t
h
e
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o
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y
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e
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eter
m
i
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h
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cit
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s
tate
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q
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atio
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a
s
d
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ib
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in
E
q
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a
tio
n
3
.
W
h
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e,
is
lin
ea
r
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ler
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o
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th
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ce
n
t
er
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f
m
a
s
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y
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,
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tal
m
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s
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q
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ad
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it
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,
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th
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E
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ler
A
n
g
le
s
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atr
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x
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ir
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tr
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s
late
th
e
g
r
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t
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ac
t
in
t
h
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o
d
y
f
r
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m
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t
h
e
cr
o
s
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-
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r
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d
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atr
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o
r
r
o
tatio
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cit
y
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eq
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ir
ed
to
m
ap
r
o
tat
io
n
al
v
e
lo
cit
y
to
th
e
ti
m
e
d
er
iv
ati
v
e
o
f
t
h
e
an
g
l
es.
(
3
)
W
h
en
co
n
s
id
er
i
n
g
t
h
e
m
o
tio
n
o
f
t
h
e
q
u
ad
r
o
to
r
,
an
o
th
er
s
tate
eq
u
atio
n
th
a
t
n
ee
d
to
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e
co
n
s
id
er
ed
i
s
t
h
e
an
g
u
lar
v
elo
cit
y
s
tate
eq
u
atio
n
as
i
n
E
q
u
at
io
n
4
.
T
h
is
eq
u
a
tio
n
is
b
ased
o
n
E
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ler
`
s
eq
u
a
tio
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r
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ig
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o
d
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d
y
n
a
m
ics.
T
h
i
s
eq
u
atio
n
d
esc
r
ib
es
th
e
c
h
a
n
g
e
in
r
o
ll
(
P
)
,
p
itch
(
Q)
a
n
d
y
a
w
(
R
)
r
ates
ca
u
s
ed
b
y
th
e
in
er
tia
,
an
g
u
lar
v
elo
cit
y
,
an
d
th
e
m
o
m
en
ts
ap
p
lied
b
y
th
e
m
o
to
r
-
p
r
o
p
eller
s
y
s
te
m
.
W
h
er
e
is
th
e
cr
o
s
s
-
p
r
o
d
u
ct
m
atr
i
x
f
o
r
r
o
tatio
n
al
v
elo
cit
y
a
n
d
is
th
e
r
o
tatio
n
al
v
elo
cit
y
o
f
th
e
q
u
ad
r
o
to
r
b
o
d
y
w
it
h
i
n
th
e
b
o
d
y
f
r
a
m
e.
(
4
)
T
h
r
u
s
t a
n
d
ae
r
o
d
y
n
a
m
ics ap
p
l
ies f
o
r
ce
o
n
th
e
q
u
ad
r
o
to
r
o
n
th
e
p
o
s
iti
v
e
z
-
a
x
is
a
s
g
i
v
e
n
b
y
E
q
u
atio
n
5
.
(
5
)
T
h
e
r
elatio
n
s
h
ip
m
atr
i
x
b
et
w
ee
n
th
e
th
r
u
s
t
a
n
d
to
r
q
u
e
w
it
h
m
o
to
r
R
P
M
ca
n
b
e
co
n
s
tr
u
cted
in
E
q
u
atio
n
6
,
w
h
er
e
d
is
th
e
le
n
g
th
o
f
th
e
ar
m
.
Evaluation Warning : The document was created with Spire.PDF for Python.
I
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d
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3
3
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r
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ar
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f
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n
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a
s
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ed
.
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d
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e
t
h
e
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M
AX
1
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4
7
p
r
o
p
eller
,
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MA
X
X
A
2
2
1
2
m
o
to
r
w
as
u
s
ed
.
Fo
r
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S
C
,
Ho
b
b
y
s
k
y
m
o
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el
w
a
s
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m
s
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f
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DJ
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b
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as a
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e
m
o
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co
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tr
o
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d
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MA
X
b
atter
y
w
as
u
s
ed
.
3.
P
ARAM
E
T
E
R
I
DE
N
T
I
F
I
C
AT
I
O
N
I
n
th
i
s
s
ec
tio
n
,
th
e
eq
u
atio
n
s
r
elate
d
to
th
e
d
y
n
a
m
ic
m
o
d
el
o
f
th
e
q
u
ad
r
o
to
r
w
er
e
d
is
cu
s
s
ed
an
d
o
f
w
h
ic
h
th
e
p
ar
a
m
eter
s
to
b
e
id
en
ti
f
ied
f
r
o
m
ac
t
u
al
p
h
y
s
ica
l
co
m
p
o
n
en
t
s
ar
e
,
,
,
,
b
an
d
tc
.
T
h
ese
p
ar
am
eter
s
n
ee
d
to
b
e
d
eter
m
i
n
ed
e
m
p
i
r
icall
y
an
d
w
ill b
e
d
is
cu
s
s
ed
in
d
etail
t
h
r
o
u
g
h
o
u
t th
is
s
ec
tio
n
.
3
.
1
.
M
a
s
s
M
o
m
e
nt
o
f
I
nert
ia
,
J
T
o
d
eter
m
i
n
e
th
e
m
o
m
en
t
o
f
i
n
er
tia,
th
e
q
u
ad
r
o
to
r
v
eh
icle
w
a
s
s
ep
ar
ated
in
to
d
if
f
er
en
t
c
o
m
p
o
n
en
t
s
.
T
h
e
m
o
d
el
o
f
ea
ch
co
m
p
o
n
e
n
t
s
w
a
s
r
ep
r
esen
ted
b
y
a
s
i
m
p
l
i
f
ied
g
eo
m
etr
ic
s
h
ap
e
o
f
co
n
s
ta
n
t
in
ter
n
al
d
en
s
it
y
.
T
h
en
,
th
e
w
ei
g
h
t o
f
ea
c
h
co
m
p
o
n
en
t
w
as
m
ea
s
u
r
ed
.
T
h
e
m
o
m
en
t o
f
i
n
er
tia
o
f
ea
c
h
co
m
p
o
n
en
t a
b
o
u
t th
e
,
,
an
d
ax
es
o
f
th
e
v
e
h
icle
is
d
eter
m
in
ed
b
y
u
s
in
g
th
e
p
ar
allel
-
ax
is
t
h
eo
r
e
m
.
T
h
e
to
tal
m
o
m
e
n
t
o
f
i
n
er
tia
m
a
tr
i
x
o
f
t
h
e
v
eh
ic
le,
is
t
h
e
s
u
m
t
h
e
in
er
tias
f
o
r
e
v
er
y
co
m
p
o
n
e
n
t
ab
o
u
t
ea
ch
ax
i
s
.
T
h
e
co
m
p
o
n
en
t
t
h
at
n
ee
d
s
to
b
e
m
o
d
elled
ar
e
th
e
m
o
to
r
,
t
h
e
E
SC
,
ar
m
s
a
n
d
t
h
e
ce
n
tr
al
h
u
b
.
T
h
e
p
ar
allel
ax
i
s
t
h
eo
r
e
m
is
d
ef
in
ed
i
n
E
q
u
atio
n
7.
(
7
)
W
h
er
e,
is
th
e
m
o
m
e
n
t
o
f
i
n
er
tia
o
f
an
i
n
d
iv
id
u
al
co
m
p
o
n
e
n
t
alo
n
g
it
s
o
w
n
a
x
is
p
ar
allel
t
o
th
e
ax
is
it
i
s
to
b
e
m
o
v
ed
,
is
t
h
e
m
as
s
o
f
i
n
d
iv
id
u
al
co
m
p
o
n
en
t
an
d
is
t
h
e
p
er
p
en
d
icu
lar
d
is
tan
ce
b
etw
ee
n
t
h
e
p
ar
alle
l
ax
es.
T
h
e
m
o
d
eli
n
g
o
f
ea
c
h
in
d
iv
id
u
al
co
m
p
o
n
e
n
t
o
f
q
u
a
d
r
o
to
r
an
d
th
eir
m
as
s
m
o
m
e
n
t
o
f
i
n
er
tia
alo
n
g
co
r
r
esp
o
n
d
in
g
ax
i
s
is
ca
lc
u
lat
ed
in
th
e
n
e
x
t
s
ec
tio
n
.
3
.
1
.
1.
M
o
t
o
rs:
So
lid
Cy
lin
ders
T
h
e
m
o
to
r
s
w
er
e
m
o
d
elled
as
a
s
o
lid
c
y
lin
d
er
to
d
eter
m
in
e
th
e
m
a
s
s
m
o
m
en
t
o
f
i
n
er
tia
f
o
r
all
f
o
u
r
m
o
to
r
s
.
Fi
g
u
r
e
1
s
h
o
w
s
th
e
q
u
ad
r
o
to
r
s
tr
u
ct
u
r
e
t
h
at
i
n
d
icat
es
t
h
e
d
i
m
en
s
io
n
s
t
h
at
n
ee
d
t
o
b
e
co
n
s
id
er
ed
to
esti
m
ate
t
h
e
m
a
s
s
m
o
m
e
n
t o
f
i
n
er
tia
f
o
r
m
o
to
r
s
.
E
q
u
atio
n
8
s
h
o
w
s
t
h
e
eq
u
atio
n
o
f
t
h
e
m
as
s
m
o
m
e
n
t o
f
in
er
tia
f
o
r
an
d
ax
es a
n
d
E
q
u
atio
n
9
f
o
r
ax
es r
esp
ec
ti
v
el
y
.
Fig
u
r
e
1
.
Di
m
e
n
s
io
n
s
to
b
e
co
n
s
id
er
ed
f
o
r
m
as
s
m
o
m
e
n
t o
f
i
n
er
tia
ca
lcu
la
tio
n
o
f
t
h
e
m
o
to
r
s
(
8
)
(
9
)
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
0
8
8
-
8
694
I
n
t J
P
o
w
E
lec
&
Dr
i
S
y
s
t
,
Vo
l.
9
,
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.
2
,
J
u
n
e
2
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1
8
:
865
–
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868
B
ased
o
n
th
e
s
p
ec
if
icatio
n
s
th
at
ar
e
u
s
ed
f
o
r
th
e
m
o
to
r
s
in
t
h
is
ex
p
er
i
m
e
n
t,
th
e
m
a
s
s
,
d
i
m
en
s
io
n
s
,
h
eig
h
t
an
d
r
ad
iu
s
w
a
s
f
o
u
n
d
as
=
5
7
g
,
=
2
6
.
0
3
5
cm
,
=
3
.
0
cm
an
d
=
1
.
3
5
cm
.
Usi
n
g
th
e
d
i
m
en
s
io
n
s
m
ea
s
u
r
ed
,
th
e
m
o
m
e
n
t
o
f
in
er
tia
o
f
m
o
to
r
co
r
r
esp
o
n
d
in
g
to
ea
ch
a
x
i
s
is
an
d
.
3
.
1
.
2.
E
SC’
s
T
hi
n F
la
t
P
la
t
e
s
T
h
e
E
SC
’
s
w
er
e
m
o
d
eled
as
th
i
n
f
lat
p
lates
a
n
d
th
e
m
a
s
s
m
o
m
e
n
t
o
f
i
n
er
tia
f
o
r
all
f
o
u
r
m
o
to
r
s
is
f
o
u
n
d
b
ased
o
n
Fig
u
r
e
2
,
E
q
u
atio
n
1
0
an
d
1
1
.
B
ased
o
n
th
e
E
SC
s
u
s
ed
in
th
is
p
r
o
j
ec
t,
th
e
m
as
s
an
d
th
e
d
i
m
en
s
io
n
s
o
f
th
e
E
SC
s
w
er
e
m
ea
s
u
r
ed
to
b
e
as
m
=
2
2
g
,
a
=
4
.
5
cm
,
b
=
2
.
6
cm
,
=
1
1
.
0
5
cm
.
Usi
n
g
th
e
d
i
m
en
s
io
n
s
m
ea
s
u
r
ed
,
th
e
m
o
m
e
n
t
o
f
in
er
tia
o
f
E
S
C
s
co
r
r
esp
o
n
d
in
g
to
ea
ch
ax
is
is
an
d
.
Fig
u
r
e
2
.
Di
m
en
s
io
n
s
to
b
e
co
n
s
id
er
ed
f
o
r
m
as
s
m
o
m
en
t o
f
in
er
tia
ca
lcu
l
a
tio
n
o
f
t
h
e
E
S
C
s
.
(
1
0
)
(
1
1
)
3
.
1
.
3.
Cent
ra
l H
UB
:
So
lid
Cy
lin
der
T
h
e
ce
n
tr
al
h
u
b
w
as
m
o
d
eled
as a
s
o
lid
c
y
li
n
d
er
an
d
th
e
m
as
s
m
o
m
en
t o
f
in
er
tia
f
o
r
th
e
ce
n
tr
al
h
u
b
w
a
s
f
o
u
n
d
b
ased
o
n
Fi
g
u
r
e
3
,
E
q
u
atio
n
s
1
2
an
d
1
3
.
Fig
u
r
e
3
.
Di
m
en
s
io
n
s
to
b
e
co
n
s
id
er
ed
f
o
r
m
as
s
m
o
m
en
t o
f
in
er
tia
ca
lcu
la
tio
n
o
f
t
h
e
C
e
n
t
r
al
HUB
.
(
1
2
)
(
1
3
)
Evaluation Warning : The document was created with Spire.PDF for Python.
I
n
t J
P
o
w
E
lec
&
Dr
i
S
y
s
t
I
SS
N:
2
0
8
8
-
8
694
Mo
d
ellin
g
a
n
d
P
a
r
a
mete
r
s
I
d
en
tifi
ca
tio
n
o
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a
d
r
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r
…
(
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h
a
mma
d
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h
a
fiq
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h
a
mm
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d
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h
r
a
f
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869
B
ased
o
n
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h
e
q
u
ad
r
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to
r
,
th
e
m
as
s
a
n
d
t
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i
m
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o
f
t
h
e
C
e
n
tr
al
H
UB
w
er
e
m
ea
s
u
r
e
d
to
b
e
as
m
=
3
3
5
g
,
r
=
6
.
2
cm
,
H
=
8
.
0
cm
.
U
s
in
g
t
h
e
d
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m
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n
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io
n
s
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ea
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r
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,
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e
m
o
m
e
n
t
o
f
i
n
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tia
o
f
th
e
C
e
n
tr
al
HUB
co
r
r
esp
o
n
d
in
g
to
ea
ch
ax
is
is
as
an
d
.
3
.
1
.
4.
Ar
m
s
:
L
o
ng
Cy
lin
dric
a
l R
o
ds
T
o
m
ea
s
u
r
e
t
h
e
m
o
m
e
n
t
o
f
i
n
er
tia
f
o
r
th
e
ar
m
s
,
a
c
y
li
n
d
r
ic
al
r
o
d
s
co
n
f
ig
u
r
atio
n
w
a
s
s
ele
cted
.
T
h
e
m
as
s
m
o
m
en
t o
f
i
n
er
tia
f
o
r
th
e
ar
m
s
w
er
e
f
o
u
n
d
b
ased
o
n
Fi
g
u
r
e
4
,
E
q
u
atio
n
s
1
4
an
d
1
5
.
Fig
u
r
e
4
.
Di
m
e
n
s
io
n
s
to
b
e
co
n
s
id
er
ed
f
o
r
m
as
s
m
o
m
e
n
t o
f
i
n
er
tia
ca
lcu
la
tio
n
o
f
t
h
e
A
r
m
s
(
1
4
)
(
1
5
)
B
ased
o
n
th
e
Fra
m
e,
t
h
e
m
as
s
an
d
t
h
e
d
i
m
en
s
io
n
s
o
f
t
h
e
A
r
m
s
w
er
e
m
ea
s
u
r
ed
to
b
e
as
m
=
5
7
g
,
r
=
0
.
5
c
m
,
L
=
2
2
c
m
,
=
3
.
5
cm
.
Usi
n
g
t
h
e
d
i
m
e
n
s
io
n
s
m
ea
s
u
r
ed
,
th
e
m
o
m
e
n
t o
f
in
er
tia
o
f
th
e
A
r
m
s
co
r
r
esp
o
n
d
in
g
to
ea
ch
ax
is
i
s
=
=
an
d
.
Fin
all
y
,
b
y
s
u
m
m
i
n
g
o
f
all
in
d
iv
id
u
a
l
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m
p
o
n
e
n
t
s
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o
f
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in
d
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id
u
a
l
co
m
p
o
n
e
n
t
s
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d
th
e
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f
all
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d
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al
co
m
p
o
n
e
n
ts
,
t
h
e
m
o
m
en
t
o
f
in
er
tia
m
atr
i
x
is
p
o
p
u
lated
in
E
q
u
atio
n
1
6
.
(
1
6
)
3
.
2
.
T
he
T
hrus
t
Co
ef
f
icient
,
T
h
e
th
r
u
s
t
co
e
f
f
icie
n
t
ca
n
b
e
f
o
u
n
d
b
y
d
eter
m
in
i
n
g
t
h
e
g
r
ad
ien
t
o
f
th
e
t
h
r
u
s
t
v
er
s
u
s
(
R
P
M)
2
g
r
ap
h
.
T
h
e
p
r
in
cip
le
o
f
m
ea
s
u
r
e
m
en
t
o
f
th
r
u
s
t
ca
n
b
e
s
ee
n
as
i
n
Fi
g
u
r
e
5
.
T
h
e
m
ec
h
an
i
s
m
is
p
i
v
o
ted
at
p
o
in
t
A
a
n
d
as th
e
t
h
r
u
s
t is
g
en
er
ated
b
y
t
h
e
m
o
to
r
,
it c
an
b
e
m
ea
s
u
r
ed
at
p
o
in
t B
.
Fig
u
r
e
5
.
P
r
in
cip
le
o
f
th
r
u
s
t
m
ea
s
u
r
e
m
en
t
A
test
r
i
g
w
a
s
b
u
ilt
to
v
i
s
u
al
ize
th
e
p
r
i
n
cip
le
o
f
m
ea
s
u
r
em
en
t
i
n
Fi
g
u
r
e
5
.
T
o
m
ea
s
u
r
e
th
e
t
h
r
u
s
t
co
ef
f
icie
n
t,
a
tes
t
r
ig
s
h
o
w
n
i
n
Fi
g
u
r
e
6
(
a)
w
a
s
b
u
ilt.
T
o
ca
p
tu
r
e
th
e
R
P
M
v
a
lu
e,
a
n
ele
ctr
o
n
ics
s
y
s
te
m
w
a
s
d
esig
n
ed
as
s
h
o
w
n
i
n
Fi
g
u
r
e
6
(
b
)
.
T
h
e
R
P
M
v
alu
e
w
as
s
i
m
p
l
y
ca
p
t
u
r
ed
b
y
u
s
in
g
p
h
o
to
tr
an
s
is
to
r
,
w
h
ic
h
d
etec
ts
th
e
b
lad
e
cr
o
s
s
in
g
,
a
n
d
R
P
M
v
alu
e
w
a
s
d
eter
m
i
n
ed
b
y
m
ea
s
u
r
in
g
th
e
ti
m
e
b
et
w
e
en
th
e
co
n
s
ec
u
t
iv
e
b
lad
e
cr
o
s
s
in
g
s
.
T
h
is
d
ata
w
a
s
th
e
n
f
ed
in
to
an
A
r
d
u
i
n
o
b
ased
m
icr
o
co
n
tr
o
ller
an
d
th
en
i
m
p
o
r
ted
to
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
0
8
8
-
8
694
I
n
t J
P
o
w
E
lec
&
Dr
i
S
y
s
t
,
Vo
l.
9
,
No
.
2
,
J
u
n
e
2
0
1
8
:
865
–
872
870
Mic
r
o
s
o
f
t
E
x
ce
l
to
b
e
p
lo
tted
in
to
a
g
r
ap
h
o
f
th
r
u
s
t
v
er
s
u
s
(
R
P
M)
2
.
T
o
ca
p
tu
r
e
th
e
th
r
u
s
t,
a
s
i
m
p
le
h
o
u
s
e
h
o
ld
d
ig
ital
w
ei
g
h
t
w
as
u
s
ed
.
(
a)
(
b
)
Fig
u
r
e
6
.
(
a)
T
est r
ig
to
m
ea
s
u
r
e
T
h
r
u
s
t
C
o
ef
f
icie
n
t.
(
b
)
E
lectr
o
n
ics s
y
s
te
m
to
m
ea
s
u
r
e
R
P
M
T
o
f
in
d
th
e
t
h
r
u
s
t
co
ef
f
icie
n
t,
th
e
T
h
r
u
s
t
v
alu
e
v
s
g
r
ap
h
w
a
s
d
r
a
w
n
a
n
d
th
e
b
est
-
f
it
g
r
ad
i
en
t
w
as
t
h
e
n
d
eter
m
in
ed
.
Fi
g
u
r
e
7
s
h
o
w
s
th
e
d
ata
ca
p
tu
r
ed
o
n
t
h
e
g
r
ap
h
o
f
t
h
r
u
s
t
v
s
(
R
P
M)
2
.
T
h
en
,
a
li
n
ea
r
ap
p
r
o
x
im
a
tio
n
w
a
s
m
ad
e
an
d
f
in
a
ll
y
t
h
e
t
h
r
u
s
t c
o
ef
f
icie
n
t
w
a
s
f
o
u
n
d
to
b
e
2
-
7
.
Fig
u
r
e
7
.
Gr
ap
h
o
f
Ne
w
to
n
v
s
(
R
P
M)
2
to
d
eter
m
i
n
e
t
h
e
th
r
u
s
t c
o
ef
f
icie
n
t.
3
.
3
.
T
he
T
o
rque
Co
ef
f
icient
,
T
h
e
p
r
in
cip
le
o
f
m
ea
s
u
r
e
m
e
n
t
o
f
T
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[1
]
B.
T
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M
.
L
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[2
]
K.
P
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J.
Ba
rv
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,
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M
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.
[3
]
Z.
R.
M
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[4
]
J.
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a
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to
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]
N.
M
.
Ra
h
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rja,
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F
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a
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h
,
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h
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to
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.
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sc
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,
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sis
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De
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rtme
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f
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0
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J.
Ba
z
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in
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A
At
mo
s
p
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1
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.
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in
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0
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/R
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ter
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telli
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2
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S
.
Bo
u
a
b
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t
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l.
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sig
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4
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.
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ter
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5
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.
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(a
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K.
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m
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h
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e
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p
p
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s,
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in
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p
.
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2
0
1
6
.
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7
]
M
.
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in
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Kro
u
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o
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in
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trica
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mp
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n
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in
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(
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)
2
3
rd
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o
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p
p
.
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-
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0
1
0
.
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8
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N.
M
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t
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p
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ti
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s,
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AS
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T
ra
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sa
c
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s
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ics
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v
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.
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9
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G
.
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.
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a
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c
o
p
ter
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li
g
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t
Dy
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a
m
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a
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Co
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p
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in
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d
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p
.
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-
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0
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.
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0
]
N.
F
a
u
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e
t.
a
l.
,
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Diff
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t
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Driv
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in
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ti
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n
d
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ter
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ts,
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in
32
nd
Dig
it
a
l
Avio
n
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s
S
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ste
ms
Co
n
fer
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c
e
,
p
p
.
1
-
1
5
,
2
0
1
3
.
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