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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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