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cos
A
=
cos
Φ
cos
B
cos(
Λ
−
Ω
)
.
(3.76)
(ii) The third identity:
sin
B
=
−
cos
Φ
sin
I
sin(
Λ − Ω
)+sin
Φ
cos
I.
(3.77)
Box 3.14 (From the meta-equatorial (oblique) frame of reference
{
E
1
,
E
2
,
E
3
|O}
to the
equatorial frame of reference
{
E
1
,
E
2
,
E
3
|O}
: the inverse transformation).
(i) The first identity:
X
R
cos
Φ
,
X
=
R
cos
Φ
cos
Λ
⇒
cos
Λ
=
(3.78)
1
cos
Φ
(cos
B
cos
A
cos
Ω
cos
Λ
=
−
cos
B
sin
A
sin
Ω
cos
I
+sin
B
sin
Ω
sin
I
)
.
(ii) The second identity:
Y
R
cos
Φ
,
Y
=
R
cos
Φ
sin
Λ
⇒
sin
Λ
=
(3.79)
1
sin
Λ
=
cos
Φ
(cos
B
cos
A
sin
Ω
+cos
B
sin
A
cos
Ω
cos
I −
sin
B
cos
Ω
sin
I
)
.
(iii) The third identity:
sin
Φ
=
Z
R
,
sin
Φ
=cos
B
sin
A
sin
I
+sin
B
cos
I.
Z
=
R
sin
Φ
⇒
(3.80)
Box 3.15 (The backward problem of transforming spherical frames of reference. Input vari-
ables:
A, B, Ω, I
. Output variables:
Λ, Φ
).
(i) The first and second identities:
tan
Λ
=
cos
B
cos
A
sin
Ω
+cos
B
sin
A
cos
Ω
cos
I
−
sin
B
cos
Ω
sin
I
cos
B
sin
A
sin
Ω
cos
I
+sin
B
sin
Ω
sin
I
.
(3.81)
cos
B
cos
A
cos
Ω
−
(ii) The third identity:
sin
Φ
=cos
B
sin
A
sin
I
+sin
B
cos
I.
(3.82)
3-33 The Transverse Frame of Reference of the Sphere: Part One
In the framework of the
transverse aspect
, we are aiming at establishing a special oblique frame of
reference by the inclination
I
=90
◦
. We have to deal with two problems depending on the input
data.
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