Geography Reference
In-Depth Information
Fig. 21.6. Polynomial diagram, the polynomial representation of the conformal coordinate Easting X in a global
frame of reference of type Gauss-Krueger or UTM, the solid dots illustrate non-zero monomials, the open circles
zero monomials, according to Cox et al. ( 1996 , pp. 433-443)
21-412 The Second Step: Curvilinear Datum Transformation
With reference to Grafarend and Syffus ( 1995 , pp. 344-348), let us introduce the curvilinear
datum transformation from a local datum (regional, National, European) to a global datum
close to the identity reviewed in Box 21.12 .Notethat l and b refer to surface normal ellipsoidal
longitude/ellipsoidal latitude of an ellipsoid-of-revolution
in a local frame of reference (semi-
major axis a 1 , semi-minor axis a 2 , relative eccentricity squared e 2 := ( a 1
E
a 1 ,a 2
a 2 ) /a 1 ). The datum
transformation close to the identity is expressed as a linear function of the datum transformation
parameters, three parameters of translation
and
one scale parameter s . Note that the datum transformation in longitude close to the identity is
independent of the translation parameter t z and of the scale parameter s . In contrast, the datum
transformation in latitude close to the identity does not depend on the rotation parameter γ ( z
axis rotation). The coecients
{
t x ,t y ,t z }
, three parameters of rotation
{
α,β,γ
}
are given in Box 21.13 . The synthesis matrix S of a
datum transformation close to the identity depends on the ellipsoidal height h in a local frame of
reference. Only in a few cases local ellipsoidal height information is available. Within the matrix
decomposition S( h )=S 0 + h S 1 +O( h 2 ), we study the influence of local ellipsoidal height h .
{
s 10 , ..., s 27 }
Box 21.12 (Curvilinear datum transformation, synthesis close to the identity).
L =
= l + s 10 + s 11 t x + s 12 t y + s 13 t z + s 14 α + s 15 β + s 16 γ + s 17 s = l + δL,
δL ;=
= s 10 + s 11 t x + s 12 t y + s 13 t z + s 14 α + s 15 β + s 16 γ + s 17 s,
(21.67)
B =
= b + s 20 + s 21 t x + s 22 t y + s 23 t z + s 24 α + s 25 β + s 26 γ + s 27 s = b + δB,
δB :=
= s 20 + s 21 t x + s 22 t y + s 23 t z + s 24 α + s 25 β + s 26 γ + s 27 s.
 
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