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21
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2
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Feb
r
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2
1
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.
9
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4
7
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Feb
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ar
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56
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u
n
ctio
n
s
b
ased
o
n
a
s
i
n
g
le
L
E
O
s
atellite
i
s
an
u
r
g
e
n
t p
r
o
b
le
m
.
T
o
im
p
le
m
e
n
t
r
ad
io
m
o
n
ito
r
in
g
s
y
s
te
m
s
b
ased
o
n
s
m
all
s
p
ac
ec
r
af
t,
it
is
n
ec
ess
ar
y
to
co
n
d
u
ct
a
n
u
m
b
er
o
f
s
t
u
d
ies
r
elate
d
to
th
e
ev
al
u
atio
n
an
d
a
n
al
y
s
is
o
f
s
i
g
n
al
s
r
ec
eiv
ed
b
y
a
n
o
n
-
b
o
ar
d
m
ea
s
u
r
i
n
g
r
ec
eiv
er
,
s
u
b
s
tan
tiatio
n
o
f
m
eth
o
d
s
f
o
r
d
eter
m
i
n
in
g
t
h
e
l
o
ca
tio
n
o
f
g
r
o
u
n
d
-
b
ased
r
ad
i
o
e
m
is
s
io
n
s
o
u
r
ce
s
(
R
E
S),
th
e
ch
o
ice
o
f
s
tr
u
c
tu
r
e
s
an
d
o
r
b
its
o
f
s
p
ac
e
s
p
ac
ec
r
af
t,
etc.
T
h
is
p
ap
er
d
is
cu
s
s
e
s
t
h
e
is
s
u
es o
f
a
s
s
es
s
i
n
g
th
e
en
er
g
y
b
u
d
g
e
t
o
f
th
e
r
ad
io
lin
es
"
Gr
o
u
n
d
R
E
S
–
On
-
b
o
ar
d
m
ea
s
u
r
in
g
r
ec
eiv
er
"
,
an
d
also
alg
o
r
ith
m
s
f
o
r
d
eter
m
in
i
n
g
t
h
e
co
o
r
d
in
ates
o
f
R
E
S
f
o
r
th
e
g
o
n
io
m
etr
ic
m
et
h
o
d
b
ased
o
n
t
h
e
u
s
e
o
f
o
n
e
lo
w
-
o
r
b
it
s
m
a
ll
s
p
ac
ec
r
af
t
(
SS
C
)
.
2.
RE
S
E
ARCH
M
E
T
H
O
D
2
.
1
.
T
he
ener
g
y
bu
dg
et
o
f
a
ra
di
o
lin
e
a
nd
t
he
m
et
ho
d f
o
r
det
er
m
i
nin
g
RE
S c
o
o
rdina
t
es
W
h
en
cr
ea
tin
g
a
r
ad
io
m
o
n
ito
r
in
g
s
y
s
te
m
w
it
h
th
e
u
s
e
o
f
a
s
m
al
l
s
p
ac
ec
r
af
t,
it
is
n
ec
es
s
ar
y
to
ass
e
s
s
th
e
s
ig
n
al
lev
e
ls
a
t
t
h
e
i
n
p
u
t
o
f
t
h
e
o
n
-
b
o
ar
d
m
ea
s
u
r
i
n
g
r
ec
eiv
er
ca
u
s
ed
b
y
v
ar
io
u
s
g
r
o
u
n
d
-
b
ased
r
ad
iatio
n
e
m
is
s
io
n
s
o
u
r
ce
s
.
S
u
ch
an
as
s
ess
m
en
t
ca
n
b
e
ca
r
r
ied
o
u
t b
as
ed
o
n
th
e
m
eth
o
d
o
lo
g
y
f
o
r
ca
l
cu
lati
n
g
t
h
e
e
n
er
g
y
b
u
d
g
et
o
f
v
ar
io
u
s
r
ad
io
co
m
m
u
n
icatio
n
c
h
an
n
el
s
in
a
cc
o
r
d
an
ce
w
it
h
t
h
e
r
ec
o
m
m
en
d
atio
n
s
o
f
t
h
e
I
n
ter
n
atio
n
al
T
elec
o
m
m
u
n
icat
io
n
Un
io
n
[
1
2
-
1
7
]
.
A
n
an
al
y
s
i
s
w
a
s
m
ad
e
in
a
n
u
m
b
er
o
f
w
o
r
k
s
o
n
ca
lcu
lati
n
g
th
e
en
er
g
y
b
u
d
g
et
o
f
r
ad
io
ch
an
n
el
s
to
i
m
p
r
o
v
e
th
e
e
f
f
ici
en
c
y
o
f
co
m
m
u
n
icatio
n
s
y
s
te
m
s
b
ased
o
n
s
m
all
telec
o
m
m
u
n
icatio
n
s
atell
ite
s
[
1
8
-
2
1
]
.
I
n
th
i
s
w
o
r
k
,
th
e
p
ar
a
m
eter
s
o
f
th
e
r
ea
l
g
r
o
u
n
d
-
b
ased
r
ad
io
elec
tr
o
n
ic
eq
u
ip
m
en
t
o
p
er
atin
g
i
n
t
h
e
ter
r
ito
r
y
o
f
t
h
e
R
ep
u
b
lic
o
f
K
az
ak
h
s
ta
n
w
it
h
i
n
t
h
e
f
r
eq
u
e
n
c
y
r
an
g
e
f
r
o
m
9
4
MH
z
to
1
4
GHz
ar
e
s
elec
ted
f
o
r
th
e
an
al
y
s
i
s
o
f
th
e
en
er
g
y
b
u
d
g
et
o
f
th
e
r
ad
io
lin
e
o
f
th
e
r
ad
io
m
o
n
ito
r
in
g
s
y
s
te
m
b
ased
o
n
SS
C
.
T
h
e
r
esu
lt
s
o
f
th
e
ca
lc
u
latio
n
s
f
o
r
a
n
u
m
b
er
o
f
g
r
o
u
n
d
-
b
ased
R
E
S
s
ar
e
s
h
o
w
n
i
n
T
ab
le
1
.
W
h
en
s
o
l
v
i
n
g
t
h
e
p
r
o
b
le
m
o
f
d
eter
m
in
i
n
g
th
e
lo
ca
tio
n
o
f
a
R
E
S,
it
is
n
ec
es
s
ar
y
to
c
h
o
o
s
e
a
m
eth
o
d
f
o
r
d
eter
m
in
in
g
it
s
co
o
r
d
in
ate
s
.
I
n
[
2
2
-
2
5
]
,
m
et
h
o
d
s
f
o
r
d
eter
m
in
i
n
g
t
h
e
co
o
r
d
in
ates
o
f
r
ad
io
em
is
s
io
n
s
o
u
r
ce
s
u
s
in
g
a
lo
w
-
o
r
b
it
co
n
s
tellatio
n
o
f
s
atel
lites
ar
e
co
n
s
id
er
ed
an
d
p
r
o
p
o
s
ed
.
Ho
w
e
v
e
r
,
it
is
ad
v
is
ab
le
to
co
n
s
id
er
th
e
u
s
e
o
f
o
n
e
SS
C
at
th
e
f
ir
s
t
s
ta
g
e
o
f
cr
ea
tin
g
a
r
ad
io
m
o
n
it
o
r
in
g
s
y
s
te
m
;
th
i
s
w
il
l
s
i
m
p
l
if
y
a
n
d
r
ed
u
ce
th
e
co
s
t
o
f
t
h
e
r
ad
io
m
o
n
ito
r
in
g
s
y
s
te
m
.
T
o
d
eter
m
i
n
e
th
e
co
o
r
d
in
ate
s
(
latitu
d
e
a
n
d
lo
n
g
itu
d
e)
o
f
t
h
e
R
E
S
b
ased
o
n
o
n
e
SS
C
,
w
h
i
ch
i
s
i
n
a
cir
c
u
lar
p
o
lar
o
r
b
it
(
w
i
th
in
cl
in
at
io
n
o
f
i
=
9
0
0
)
,
it
is
p
r
o
p
o
s
ed
to
co
n
s
id
er
th
e
m
eth
o
d
,
th
e
p
r
in
c
ip
le
o
f
w
h
ic
h
is
e
x
p
lain
ed
i
n
F
ig
u
r
e
1.
O
r
b
i
t
a
l
p
l
a
n
e
o
f
S
S
C
B
–
S
S
C
c
u
r
r
e
n
t
p
o
s
i
t
i
o
n
S
S
C
g
r
o
u
n
d
t
r
a
c
k
D
–
R
E
S
l
o
c
a
t
i
o
n
D
С
A
B
O
Y
X
Z
θ
γ
α
β
η
μ
k
ϕ
S
S
S
C
–
s
m
a
l
l
s
p
a
c
e
c
r
a
f
t
G
r
e
e
n
w
i
c
h
m
e
r
i
d
i
a
n
E
q
u
a
t
o
r
Fig
u
r
e
1
.
Dete
r
m
in
a
tio
n
o
f
t
h
e
R
E
S c
o
o
r
d
in
ates o
n
th
e
b
as
is
o
f
o
n
e
SS
C
Evaluation Warning : The document was created with Spire.PDF for Python.
I
n
d
o
n
esia
n
J
E
lec
E
n
g
&
C
o
m
p
Sci
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N:
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-
4752
E
n
erg
y
B
u
d
g
et
a
n
d
Meth
o
d
s
f
o
r
Dete
r
min
in
g
C
o
o
r
d
in
a
tes fo
r
a
R
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o
n
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r
in
g
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A
lta
y
A
itma
g
a
mb
eto
v
)
947
T
h
e
f
ig
u
r
e
u
s
es
t
h
e
f
o
llo
w
i
n
g
d
esig
n
atio
n
s
:
O
-
th
e
ce
n
tr
e
o
f
E
ar
th
m
as
s
;
D
-
th
e
R
E
S
lo
c
atio
n
;
B
-
SS
C
p
o
s
itio
n
.
T
h
e
d
eter
m
i
n
at
io
n
o
f
th
e
R
E
S
lo
ca
tio
n
la
tit
u
d
e
w
as
ca
r
r
ied
o
u
t
b
ased
o
n
th
e
an
al
y
s
is
o
f
t
h
e
p
ar
am
eter
s
o
f
th
e
A
OB
tr
ian
g
le
b
u
ilt
i
n
an
ellip
s
e
(
s
ec
tio
n
o
f
th
e
s
p
h
er
o
id
b
y
th
e
Z
O
Y
p
lan
e)
.
Po
in
t
A
is
lo
ca
te
d
o
n
th
e
s
u
r
f
ac
e
o
f
t
h
e
SS
C
tr
ac
k
at
th
e
p
o
in
t
o
f
its
i
n
ter
s
ec
tio
n
w
it
h
th
e
p
ar
allel
o
n
w
h
ic
h
t
h
e
R
E
S
i
s
lo
ca
ted
(
th
at
is
,
at
th
e
s
a
m
e
l
atitu
d
e)
;
s
id
e
O
A
=
R
e
(
E
ar
th
r
ad
iu
s
)
d
ep
en
d
in
g
o
n
la
tit
u
d
e
φ;
s
id
e
OB
=
R
o
(
r
ad
iu
s
o
f
t
h
e
o
r
b
it o
f
t
h
e
s
m
al
l sp
ac
ec
r
af
t
)
; φ
is
th
e
R
E
S
lati
tu
d
e
(
th
e
an
g
le
b
et
w
ee
n
t
h
e
O
A
d
ir
ec
tio
n
a
n
d
th
e
eq
u
ato
r
ial
p
lan
e)
;
α
i
s
t
h
e
lati
tu
d
e
o
f
th
e
s
p
ac
ec
r
af
t
(
th
e
a
n
g
le
b
et
w
ee
n
t
h
e
OB
d
ir
ec
tio
n
an
d
t
h
e
eq
u
ato
r
ia
l
p
lan
e)
.
An
g
les
i
n
tr
ia
n
g
le
AOB
ar
e
th
e
f
o
llo
w
in
g
:
(
γ
)
-
la
titu
d
e
d
i
f
f
er
en
ce
;
th
e
a
n
g
le
is
o
p
p
o
s
ite
t
o
A
B
s
id
e;
β
is
t
h
e
a
n
g
le
at
w
h
ic
h
p
o
in
t
A
is
v
i
s
ib
le
f
r
o
m
th
e
s
m
all
s
p
ac
ec
r
af
t
r
elati
v
e
to
th
e
d
ir
ec
tio
n
OB
;
it
is
o
p
p
o
s
ite
to
th
e
s
id
e
O
A;
k
is
t
h
e
3
r
d
an
g
le
in
tr
ian
g
le,
o
p
p
o
s
ite
to
OB
s
id
e.
W
ith
t
h
e
k
n
o
w
n
3
p
ar
am
eter
s
o
f
t
h
e
tr
ia
n
g
le,
it
is
ea
s
y
to
f
i
n
d
it
s
o
th
er
p
ar
a
m
eter
s
.
I
n
t
h
is
c
ase,
th
e
OB
s
id
e
an
d
t
h
e
a
n
g
le
β
ar
e
k
n
o
w
n
(
d
eter
m
i
n
ed
d
u
r
i
n
g
s
ca
n
n
in
g
)
,
th
e
r
e
m
ain
i
n
g
p
ar
a
m
eter
s
d
ep
en
d
o
n
th
e
φ
t
h
at
n
ee
d
s
to
b
e
d
eter
m
i
n
ed
.
T
h
er
ef
o
r
e,
w
e
w
i
ll n
ee
d
to
ap
p
l
y
th
e
i
ter
atio
n
m
eth
o
d
.
In
p
ap
er
s
[
2
6
-
2
7
]
,
a
m
et
h
o
d
f
o
r
d
eter
m
i
n
i
n
g
th
e
R
E
S
co
o
r
d
in
ates
u
s
in
g
o
n
e
s
m
all
s
p
ac
ec
r
af
t
w
as
co
n
s
id
er
ed
to
d
eter
m
i
n
e
t
h
e
R
E
S
lo
ca
tio
n
.
Ho
w
e
v
er
,
th
e
d
is
tan
ce
O
A
(
E
ar
th
'
s
r
ad
iu
s
)
w
a
s
tak
e
n
as
a
co
n
s
ta
n
t
p
ar
am
eter
in
th
i
s
m
et
h
o
d
,
w
h
i
ch
lead
s
to
er
r
o
r
s
in
d
ete
r
m
in
i
n
g
th
e
R
E
S
co
o
r
d
in
ates.
Si
n
ce
th
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(
1
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[
2
8
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RE
SU
L
T
S AN
D
D
I
SCU
SS
I
O
N
3
.
1
.
Ana
ly
s
is
o
f
t
he
m
et
ho
d f
o
r
det
er
m
i
nin
g
t
he
RE
S c
o
o
rdin
a
t
es
T
o
d
eter
m
in
e
t
h
e
R
E
S
co
o
r
d
i
n
ates,
a
s
tr
u
c
tu
r
al
d
iag
r
a
m
f
o
r
th
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n
-
b
o
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d
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m
e
n
t
o
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th
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p
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s
eg
m
e
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o
f
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h
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b
a
s
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o
n
o
n
e
lo
w
-
o
r
b
it
s
m
a
ll
s
p
ac
ec
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af
t
i
s
p
r
o
p
o
s
ed
(
Fig
u
r
e
2
)
.
T
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i
m
p
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m
en
t
th
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s
s
y
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te
m
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t
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ce
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s
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te
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s
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t
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ased
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r
a
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A
P
AA
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t
y
p
e
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b
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s
m
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ll sp
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f
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e
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m
u
s
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av
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n
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e
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o
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t
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S.
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h
e
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ted
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ter
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tain
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o
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ith
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u
r
e
2
.
Stru
ct
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r
al
d
iag
r
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m
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e
s
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ac
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m
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n
t o
f
t
h
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o
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b
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d
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q
u
ip
m
en
t
3
.
2
.
P
ro
po
s
ed
a
lg
o
rit
h
m
f
o
r
det
er
m
ini
ng
t
he
la
t
it
ud
e
o
f
t
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RE
S lo
ca
t
io
n
An
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n
n
a
s
o
n
t
h
e
s
m
al
l sp
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af
t
s
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io
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h
e
b
ea
m
o
f
o
n
e
o
f
th
e
m
s
ca
n
s
in
th
e
m
er
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ian
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ir
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tio
n
(
in
t
h
e
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ir
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n
o
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m
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v
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m
e
n
t
o
f
t
h
e
s
m
a
ll
s
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r
af
t)
an
d
s
er
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es
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eter
m
in
e
t
h
e
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u
d
e
o
f
th
e
R
E
S
lo
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tio
n
at
t
h
e
m
o
m
en
t
o
f
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ig
n
al
r
ec
o
r
d
in
g
u
s
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t
h
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eq
u
i
s
ig
n
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to
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m
et
h
o
d
[
3
0
]
.
T
h
e
b
ea
m
o
f
th
e
s
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o
n
d
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ten
n
a
s
ca
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tio
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m
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e
m
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n
t
o
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p
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d
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m
in
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t
h
e
lo
n
g
it
u
d
e
o
f
th
e
R
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ca
tio
n
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As
s
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n
f
r
o
m
Fi
g
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r
e
1
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if
th
e
OB
s
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e
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d
th
e
an
g
le
β
ar
e
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n
o
w
n
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d
eter
m
i
n
ed
b
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s
ca
n
n
i
n
g
)
,
th
e
r
e
m
ain
in
g
p
ar
a
m
eter
s
d
ep
en
d
o
n
φ
to
b
e
d
eter
m
i
n
ed
.
Sin
ce
o
n
l
y
t
w
o
p
ar
a
m
eter
s
o
f
t
h
e
tr
ian
g
le
ar
e
k
n
o
w
n
,
it
w
il
l
b
e
n
ec
es
s
ar
y
to
ap
p
l
y
t
h
e
iter
atio
n
m
et
h
o
d
.
I
t
i
s
al
s
o
n
ec
es
s
ar
y
to
o
b
tain
a
n
a
n
s
w
e
r
to
th
e
q
u
est
i
o
n
o
f
w
h
at
r
an
g
e
o
f
R
E
S
lo
ca
tio
n
p
o
in
t
latit
u
d
es
is
“v
i
s
ib
le”
f
r
o
m
t
h
e
o
r
b
it
o
f
th
e
s
m
all
s
p
ac
ec
r
af
t.
T
o
d
o
th
is
,
w
e
n
ee
d
to
s
o
lv
e
th
e
s
y
s
te
m
o
f
eq
u
atio
n
s
:
Evaluation Warning : The document was created with Spire.PDF for Python.
I
n
d
o
n
esia
n
J
E
lec
E
n
g
&
C
o
m
p
Sci
I
SS
N:
2502
-
4752
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n
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h
e
ca
n
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n
ical
eq
u
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o
f
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e:
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6
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T
h
e
eq
u
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n
o
f
th
e
ta
n
g
en
t to
th
e
ellip
s
e
f
r
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m
t
h
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t
w
h
e
r
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th
e
SS
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is
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ca
ted
[
3
1
]
:
(
7
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I
t
is
co
n
v
e
n
ie
n
t
to
s
elec
t
th
e
S
SC
co
o
r
d
in
ates
at
t
h
e
eq
u
ato
r
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Y
b
=7
0
1
6
2
9
9
m
;
Z
b
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.
F
ir
s
t,
f
o
r
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w
e
f
i
n
d
,
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d
th
en
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e
f
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d
Z
k
:
[
(
)
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8
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C
o
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r
d
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ates o
f
t
h
e
p
o
in
t o
f
co
n
tact
Z
k
=2
6
4
8
8
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6
m
; Y
k
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7
9
8
0
1
6
m
.
T
h
e
latitu
d
e
o
f
t
h
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o
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t
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is
(
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.
T
h
u
s
,
th
e
R
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v
i
s
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le
f
r
o
m
t
h
e
s
m
al
l
s
p
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af
t
lo
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ted
at
th
e
eq
u
at
o
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ar
e
w
it
h
i
n
t
h
e
la
tit
u
d
e
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g
e
f
r
o
m
0
0
to
2
4
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5
5
0
,
th
at
is
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o
u
ts
id
e
th
e
ter
r
ito
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y
o
f
Kaz
a
k
h
s
tan
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W
h
en
th
e
s
p
ac
ec
r
a
f
t
m
o
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e
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a
la
tit
u
d
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f
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0
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ap
p
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i
m
atel
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th
e
s
a
m
e
r
a
n
g
e
o
f
v
is
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le
lat
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d
es o
f
th
e
R
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tio
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s
w
il
l r
e
m
ai
n
(
f
r
o
m
4
0
0
to
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4
.
5
5
0
).
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is
also
i
m
p
o
r
tan
t
to
an
s
w
er
t
h
e
q
u
esti
o
n
o
f
w
h
ich
s
ec
tio
n
o
f
th
e
φ(
β)
d
ep
en
d
en
ce
w
ill
r
ed
u
ce
th
e
φ
d
eter
m
in
i
n
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er
r
o
r
d
u
e
to
t
h
e
i
n
ac
cu
r
ac
y
o
f
t
h
e
β
esti
m
ate.
T
h
e
a
n
s
w
er
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n
b
e
o
b
tain
ed
b
y
s
o
lv
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n
g
t
h
e
i
n
v
er
s
e
p
r
o
b
lem
(
w
e
d
eter
m
i
n
e
β
f
r
o
m
k
n
o
w
n
φ)
.
W
e
ca
n
p
er
f
o
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m
th
e
ca
lc
u
latio
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u
s
in
g
t
h
e
f
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ll
o
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i
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g
f
o
r
m
u
la
(
t
h
e
ca
lcu
latio
n
r
esu
l
ts
ar
e
s
h
o
w
n
i
n
T
ab
le
2
.
)
:
*
+
(
9
)
T
ab
le
2
.
s
h
o
w
s
th
a
t
p
r
ef
er
en
ce
s
h
o
u
ld
b
e
g
iv
e
n
to
th
e
in
itial
s
ec
tio
n
o
f
t
h
e
β(φ)
d
ep
en
d
en
ce
.
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m
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lar
l
y
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n
e
ca
n
d
eter
m
i
n
e
th
e
d
ep
en
d
en
ce
s
o
f
β
o
n
φ
at
α
=
4
4
0
,
4
8
0
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an
d
5
2
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et
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eter
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h
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f
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h
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f
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t
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t.
T
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r
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eter
m
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la
tit
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d
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o
f
th
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eg
i
n
s
w
h
e
n
t
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e
s
p
ac
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af
t
is
at
a
latitu
d
e
o
f
α
=
4
0
0
(
h
ig
h
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itio
n
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n
g
ac
cu
r
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n
b
e
p
r
o
v
id
ed
u
s
in
g
GP
S/G
L
ON
AS
S
m
o
n
i
to
r
in
g
)
.
T
h
e
n
ar
r
o
w
d
ir
ec
ted
b
ea
m
o
f
th
e
a
n
ten
n
a
s
tar
ts
s
ca
n
n
in
g
in
t
h
e
m
er
id
ian
d
ir
ec
tio
n
to
th
e
n
o
r
th
,
s
tar
ti
n
g
f
r
o
m
t
h
e
s
u
b
-
s
atell
ite
p
o
in
t
(
β
=
0
0
)
to
β
=
3
3
.
7
8
0
4
0
.
T
h
is
co
r
r
esp
o
n
d
s
to
a
c
h
an
g
e
i
n
(
γ
)
f
r
o
m
0
to
4
d
eg
r
ee
s
.
A
t
s
o
m
e
p
o
in
t,
w
h
e
n
β
=
β
1
,
t
h
e
R
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S
s
i
g
n
al
is
r
ec
o
r
d
ed
,
th
en
d
is
ap
p
e
ar
s
.
W
h
en
th
e
b
ea
m
m
o
v
es
b
a
ck
to
t
h
e
s
o
u
t
h
,
t
h
e
s
ig
n
al
at
β
2
is
r
ec
o
r
d
ed
ag
ai
n
.
As
a
r
es
u
lt
o
f
u
s
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g
t
h
e
r
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s
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n
al
zo
n
e
m
et
h
o
d
,
w
e
o
b
tain
,
f
o
r
e
x
a
m
p
le
,
.
W
e
co
m
p
ar
e
th
i
s
v
al
u
e
w
it
h
th
e
av
er
a
g
e
β
o
f
T
ab
le
2
.
(
1
8
.
8
3
3
2
0
)
an
d
s
ee
,
it
is
les
s
.
W
e
co
m
p
ar
e
w
it
h
th
e
n
e
x
t
v
al
u
e
(
9
.
7
2
7
9
8
0
)
an
d
f
in
all
y
f
i
n
d
th
at
1
2
.
0
8
3
2
0
i
s
g
r
ea
ter
th
an
9
.
7
2
8
0
.
T
h
is
m
ea
n
s
th
a
t
th
e
R
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S lo
ca
tio
n
is
at
t
h
e
latit
u
d
e
b
et
w
ee
n
4
1
0
an
d
4
2
0
.
T
ab
le
2
.
Dep
en
d
en
ce
o
f
β o
n
th
e
latit
u
d
e
o
f
th
e
R
E
S lo
ca
tio
n
φ
at
α
=
4
0
0
.
φ
[
0
]
[
0
]
R
e
(
φ
)
[
m
]
A
B
(
)
[
m
]
β(
)
[
0
]
40
0
6
3
6
9
2
7
4
6
4
7
0
2
4
.
9
0
41
1
6
3
6
8
9
0
5
6
5
7
8
2
2
.
6
9
.
7
2
7
9
8
42
2
6
3
6
8
5
3
5
6
8
8
5
0
4
.
6
1
8
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8
3
3
2
43
3
6
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6
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1
6
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7
3
6
5
7
8
.
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2
6
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9
0
2
6
44
4
6
3
6
7
7
9
0
7
9
8
8
9
4
.
6
3
3
.
7
8
0
4
W
e
d
iv
id
e
t
h
is
in
ter
v
al
in
h
al
f
a
n
d
ca
lc
u
late
β
at
φ
=
4
1
.
5
0
;
it
i
s
m
o
r
e
a
g
ain
.
W
e
d
iv
id
e
th
e
lo
w
er
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ter
v
a
l
(
af
ter
th
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d
ec
i
m
al
p
o
i
n
t)
i
n
h
alf
an
d
ca
lc
u
late
β
at
φ
=
4
1
.
2
5
0
.
W
e
g
et
a
v
al
u
e
e
q
u
al
to
(
o
r
clo
s
e
to
)
th
e
m
ea
s
u
r
ed
v
alu
e.
T
h
is
m
ea
n
s
t
h
e
lo
ca
tio
n
o
f
R
E
S
i
s
at
la
titu
d
e
o
f
4
1
.
2
5
0
.
I
f
th
er
e
is
n
o
m
atc
h
an
d
a
h
i
g
h
er
ac
cu
r
ac
y
i
s
r
eq
u
ir
ed
,
t
h
en
,
d
ep
en
d
in
g
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n
t
h
e
co
m
p
ar
is
o
n
(
m
o
r
e
o
r
less
)
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w
e
d
i
v
id
e
t
h
e
lo
w
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o
r
u
p
p
er
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ter
v
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ls
a
f
ter
th
e
d
ec
i
m
al
p
o
in
t in
h
al
f
,
ca
lcu
late
β,
an
d
m
a
k
e
a
co
m
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is
o
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,
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d
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o
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n
.
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et
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n
s
id
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e
p
o
s
s
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le
er
r
o
r
s
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d
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m
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t
h
e
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o
f
th
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R
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co
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d
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g
to
th
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ab
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alg
o
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ith
m
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h
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d
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e
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th
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in
ac
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g
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th
e
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n
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n
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d
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th
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ce
n
tr
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o
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m
ass
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f
t
h
e
E
ar
th
(
p
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in
t O
)
(
o
th
er
h
ar
d
w
a
r
e
er
r
o
r
s
ca
n
also
b
e
in
clu
d
ed
h
er
e)
ca
n
b
e
d
eter
m
in
ed
b
y
t
h
e
f
o
r
m
u
la:
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
5
0
2
-
4752
I
n
d
o
n
esia
n
J
E
lec
E
n
g
&
C
o
m
p
Sci,
Vo
l.
21
,
No
.
2
,
Feb
r
u
ar
y
2
0
2
1
:
9
45
-
9
56
950
(
)
(
1
0
)
T
ab
le
3
s
h
o
w
s
t
h
e
a
v
er
ag
e
v
al
u
es
o
f
th
e
d
ep
en
d
e
n
ce
w
i
th
th
e
i
n
it
ial
d
ata
;
(
d
ata
f
r
o
m
T
ab
le
2
).
T
ab
le
3
.
Dep
en
d
en
cy
.
Δφ
o
[
0
]
0
.
1
0
2
8
0
.
0
9
2
5
2
0
.
0
8
2
2
4
0
.
0
7
1
9
6
0
.
0
6
1
6
8
0
.
0
5
1
4
0
.
0
4
1
1
2
0
.
0
3
0
8
4
0
.
0
2
0
5
6
0
.
0
1
0
2
8
Δβo
[
0
]
1
0
.
9
0
.
8
0
.
7
0
.
6
0
.
5
0
.
4
0
.
3
0
.
2
0
.
1
T
h
is
er
r
o
r
ca
n
b
e
r
ec
alcu
lated
in
to
lin
ea
r
d
i
m
en
s
io
n
s
u
s
i
n
g
t
h
e
ex
p
r
ess
io
n
[
3
2
]
as sh
o
w
n
i
n
T
ab
le
4
:
(
1
1
)
T
ab
le
4
.
Dep
en
d
en
cy
,
(
Δ
φ
o
is
ex
p
r
ess
ed
i
n
m
)
.
Δl
o
[
m]
1
1
4
2
7
.
4
1
0
2
8
4
7
9
1
4
1
.
9
6
7
9
9
9
.
2
2
6
8
5
6
.
4
7
5
7
1
3
.
7
3
4
5
7
0
.
9
8
3
4
2
8
.
2
4
2
2
5
5
.
5
0
1
1
4
2
.
7
5
5
7
1
.
3
7
4
Δ βo
[
0
]
1
0
.
9
0
.
8
0
.
7
0
.
6
0
.
5
0
.
4
0
.
3
0
.
2
0
.
1
0
.
0
5
I
n
th
e
s
ec
o
n
d
v
ar
ia
n
t
o
f
f
i
n
d
in
g
th
e
latit
u
d
e
o
f
t
h
e
R
E
S
(
φ)
,
β
an
d
α
(
latit
u
d
e
o
f
t
h
e
SS
C
)
ar
e
d
eter
m
in
ed
s
i
m
u
lta
n
eo
u
s
l
y
at
th
e
m
o
m
e
n
t
o
f
r
ec
o
r
d
in
g
t
h
e
R
E
S
s
ig
n
al.
T
h
e
s
ca
n
n
i
n
g
r
a
n
g
e
i
s
s
m
a
ller
,
b
u
t
s
u
c
h
th
at
it
w
a
s
p
o
s
s
ib
le
to
u
s
e
an
eq
u
is
i
g
n
a
l
s
ec
to
r
(
d
ep
en
d
in
g
o
n
th
e
w
id
t
h
o
f
th
e
an
ten
n
a
p
atter
n
)
.
I
t
ca
n
b
e
ass
u
m
ed
t
h
at
t
h
e
n
u
m
b
er
o
f
i
t
er
atio
n
s
to
o
b
tain
t
h
e
clo
s
e
s
t r
esu
lt
w
ill b
e
le
s
s
t
h
a
n
i
n
th
e
f
i
r
s
t o
p
tio
n
.
I
ter
atio
n
s
s
tar
t f
r
o
m
t
h
e
v
a
lu
e
φ
=
α
.
L
et
u
s
tak
e
t
h
e
s
ca
n
n
in
g
r
an
g
e
f
r
o
m
t
h
e
s
u
b
-
s
ate
llit
e
p
o
in
t
(
β
=
0
0
)
to
β
=
1
8
.
8
3
3
2
0
,
w
h
ic
h
co
r
r
esp
o
n
d
s
to
a
ch
an
g
e
(
γ
)
f
r
o
m
0
to
2
d
eg
r
ee
s
.
E
x
a
m
p
le:
at
th
e
m
o
m
en
t
o
f
s
ig
n
al
r
ec
o
r
d
in
g
,
α
=
4
0
.
8
0
an
d
β
=
7
.
8
1
0
7
0
ar
e
d
eter
m
i
n
ed
.
I
ter
atio
n
1
:
w
e
d
iv
id
e
th
e
s
ca
n
n
in
g
ar
ea
in
φ
f
r
o
m
4
0
.
8
0
to
4
2
.
8
0
in
h
alf
an
d
d
eter
m
in
e
β
at
φ
=
4
1
.
8
0
an
d
γ
=
1
0
.
R
esu
lt
β =
9
.
7
2
3
0
>
7
.
8
1
0
7
0
.
I
ter
atio
n
2
:
w
e
d
i
v
id
e
th
e
v
al
u
e
af
ter
th
e
d
ec
i
m
al
p
o
in
t
a
n
d
ch
o
o
s
e
th
e
lo
w
er
v
alu
e
φ
=
4
1
.
4
0
w
h
ile
γ
=
0
.
6
0
an
d
β =
5
.
8
7
7
0
<
7
.
8
1
0
7
0
.
I
ter
atio
n
3
:
w
e
d
iv
id
e
th
e
v
al
u
e
af
ter
t
h
e
d
ec
i
m
al
p
o
in
t
an
d
s
elec
t th
e
u
p
p
er
v
al
u
e
φ
=
4
1
.
6
0
w
h
ile
γ
=
0
.
8
0
an
d
β =
7
.
8
1
0
7
0
is
eq
u
al
to
th
e
m
e
asu
r
ed
v
al
u
e.
A
n
s
w
er
: φ
=
4
1
.
6
0
.
Fo
r
th
e
e
x
a
m
p
le
ab
o
v
e,
Δ
φ
/Δ
β
=
0
.
1
0
2
4
0
,
th
at
is
,
p
r
ac
ticall
y
d
id
n
o
t
c
h
a
n
g
e
r
elati
v
e
to
0
.
1
0
2
8
0
(
at
th
e
in
itial
s
ec
t
io
n
o
f
t
h
e
ch
ar
a
cter
is
tic)
,
th
er
ef
o
r
e,
th
e
er
r
o
r
s
co
r
r
esp
o
n
d
to
th
e
v
alu
es
i
n
T
ab
les
3
.
an
d
4
.
A
t
th
e
s
a
m
e
ti
m
e,
in
t
h
e
f
ir
s
t
v
er
s
io
n
,
th
e
R
E
S
ca
n
b
e
lo
ca
ted
o
n
th
e
f
in
al
p
ar
t
o
f
th
e
ch
ar
ac
ter
is
tic,
w
h
er
e
Δ
φ/Δ
β
=
0
.
1
4
5
4
0
(
th
e
er
r
o
r
s
w
ill
b
e
g
r
ea
ter
)
.
C
o
n
clu
s
io
n
:
th
e
s
ec
o
n
d
o
p
tio
n
f
o
r
s
o
lv
in
g
t
h
e
p
r
o
b
lem
o
f
d
eter
m
in
i
n
g
t
h
e
R
E
S
latit
u
d
e
i
s
b
etter
d
u
e
to
s
m
aller
er
r
o
r
s
a
n
d
a
s
m
aller
n
u
m
b
er
o
f
iter
ati
o
n
s
.
I
n
co
n
clu
s
io
n
,
u
s
i
n
g
th
e
last
e
x
a
m
p
le,
w
e
w
il
l
ev
a
lu
ate
th
e
e
f
f
ec
t
o
f
th
e
ter
r
ain
alt
it
u
d
e
ab
o
v
e
s
ea
l
ev
el
o
n
t
h
e
er
r
o
r
in
d
eter
m
in
i
n
g
th
e
R
E
S lo
ca
tio
n
latitu
d
e
(
let
h
=
1
0
0
0
m
)
.
T
h
en
R
e
(
4
1
.
6
0
)
+
1
0
0
0
=
6
3
6
9
6
8
3
m
;
n
e
w
v
al
u
e
A
B
=
6
5
3
3
1
8
.
4
2
7
m
,
n
e
w
v
alu
e
β
=
7
.
8
2
3
8
0
,
ch
an
g
e
Δ
β
=
0
.
0
1
3
0
,
an
d
er
r
o
r
Δ
φ
=
0
.
1
0
2
4
0
×
0
.
0
1
3
0
=
0
.
0
0
1
0
.
I
n
lin
ea
r
d
i
m
en
s
io
n
s
,
it
is
ap
p
r
o
x
i
m
atel
y
eq
u
al
to
1
1
1
m
.
T
h
e
alg
o
r
ith
m
f
o
r
d
eter
m
i
n
i
n
g
th
e
R
E
S
latit
u
d
e
is
s
h
o
w
n
i
n
Fi
g
u
r
e
3
.
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d
th
e
s
o
f
t
w
ar
e
ap
p
licatio
n
w
i
n
d
o
w
is
s
h
o
w
n
i
n
Fi
g
u
r
e
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n
d
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u
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R
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i
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atio
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Fig
u
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r
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r
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eter
m
i
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i
n
g
th
e
R
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S latit
u
d
e
3
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3
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po
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lg
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h
m
f
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ud
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t
he
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t
io
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Af
ter
d
eter
m
i
n
i
n
g
t
h
e
R
E
S
l
atitu
d
e
φ
(
ac
co
r
d
in
g
to
th
e
m
et
h
o
d
d
escr
ib
ed
in
s
u
b
s
ec
ti
o
n
3
.
2
)
,
w
e
p
r
o
ce
ed
to
d
eter
m
i
n
i
n
g
t
h
e
lo
n
g
i
tu
d
e.
L
et
u
s
co
n
s
id
er
th
e
f
e
atu
r
es
o
f
d
eter
m
i
n
i
n
g
t
h
e
R
E
S
lo
n
g
it
u
d
e
b
ased
o
n
th
e
an
al
y
s
is
o
f
t
h
e
p
ar
a
m
eter
s
o
f
th
e
tr
ian
g
le
s
A
B
D,
AC
D,
B
C
D
s
h
o
w
n
in
Fig
u
r
e
1
.
Scan
n
in
g
w
it
h
t
h
e
b
ea
m
r
elativ
e
to
p
o
in
t
A
i
s
ca
r
r
ied
o
u
t
alo
n
g
th
e
p
ar
allel
co
r
r
esp
o
n
d
in
g
to
lati
tu
d
e
φ
in
th
e
w
est
an
d
ea
s
t
d
ir
ec
tio
n
.
W
h
en
a
s
i
g
n
al
ap
p
ea
r
s
,
th
e
d
ir
ec
tio
n
to
th
e
S
R
S
is
r
e
g
is
ter
ed
u
s
in
g
t
h
e
an
g
le
μ
(
μ
is
th
e
an
g
le
b
et
w
ee
n
t
h
e
d
ir
ec
tio
n
s
f
r
o
m
t
h
e
SS
C
(
p
o
in
t
B
)
to
th
e
R
E
S
(
p
o
in
t
D)
an
d
to
th
e
p
o
in
t
A
)
,
a
s
w
ell
as
th
e
s
i
g
n
o
f
t
h
e
c
o
r
r
ec
tio
n
f
o
r
lo
n
g
it
u
d
e
η
r
elativ
e
to
th
e
S
SC
p
o
s
itio
n
lo
n
g
it
u
d
e
(
θ)
-
w
es
ter
l
y
d
i
r
ec
tio
n
(
-
)
,
ea
s
ter
l
y
Evaluation Warning : The document was created with Spire.PDF for Python.
I
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u
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s
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t
h
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E
S
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o
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p
o
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t
D)
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s
i
m
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p
o
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t
D
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n
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e
at
th
e
s
a
m
e
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g
le
μ
i
n
th
e
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s
ter
l
y
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ir
ec
tio
n
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o
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t
A
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s
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e
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o
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t o
f
i
n
ter
s
ec
tio
n
o
f
t
h
e
ab
o
v
e
p
ar
allel
w
it
h
th
e
g
r
o
u
n
d
tr
ac
k
o
f
th
e
s
m
all
s
p
ac
ec
r
af
t
o
r
b
it
o
n
th
e
ea
r
th
's
s
u
r
f
ac
e.
P
o
in
t
C
i
s
lo
ca
ted
o
n
t
h
e
O
Z
ax
i
s
at
t
h
e
in
ter
s
ec
tio
n
o
f
its
p
la
n
e
alo
n
g
t
h
e
p
ar
allel
o
n
w
h
ic
h
t
h
e
R
E
S
i
s
lo
ca
ted
(
th
at
is
,
at
t
h
e
s
a
m
e
lat
itu
d
e)
.
T
h
is
s
ec
tio
n
i
s
a
cir
cle
o
n
w
h
ich
p
o
in
ts
A
a
n
d
D
ar
e
lo
ca
ted
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an
d
p
o
in
t C is
t
h
e
ce
n
tr
e
o
f
th
is
cir
cle.
C
ir
cle
r
ad
iu
s
R
=
A
C
=
D
C
=
R
e
(
φ)
×
co
s
φ.
Sid
e
B
C
is
a
d
is
tan
ce
b
et
w
ee
n
th
e
SS
C
an
d
p
o
in
t
C
,
s
id
e
B
D
is
a
d
is
tan
ce
b
et
w
ee
n
th
e
S
SC
an
d
t
h
e
R
E
S,
s
id
e
B
A
i
s
a
d
is
tan
ce
b
e
t
w
ee
n
t
h
e
SS
C
an
d
p
o
in
t
A
;
t
h
e
k
n
o
w
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