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L 02 ) 2 cos B 0 sin B 0 (1
E 2 sin 2 B 0 ) 5 / 2
t 20 = ( L 01
A 1 (1
E 2 ) 2
E 2 sin 2 B 0 ) 1 / 2 5
L 02 ) 4 tan B 0 (1
E 2
28 sin 2 B 0
( L 01
16 E 2 sin 2 B 0 +24sin 4 B 0 +
+86 E 2 sin 4 B 0 +26 E 4 sin 4 B 0
72 E 2 sin 6 B 0
100 E 4 sin 6 B 0
12 E 6 sin 6 B 0 +
+77 E 4 sin 8 B 0 +39 E 6 sin 8 B 0
28 E 6 sin 10 B 0 [48 A 1 (1
E 2 ) 3 ] 1 ,
t 11 = ( L 01 L 02 )cos B 0 (1 E 2 sin 2 B 0 ) 3 / 2
A 1 (1
+
E 2 )
+( L 01 − L 02 ) 3 cos B 0 (1 − E 2 sin 2 B 0 ) 3 / 2 5 − E 2
18 sin 2 B 0 18 E 2 sin 2 B 0
+45 E 2 sin 4 B 0 +
+15 E 4 sin 4 B 0
28 E 4 sin 6 B 0 [6 A 1 (1
E 2 ) 3 ] 1 ,
E 2 sin 2 B 0 ) 5 / 2
L 02 ) 2 cos B 0 sin B 0 (1
( L 01
t 02 =
A 1 (1
E 2 ) 2
E 2 sin 2 B 0 ) 1 / 2 5
L 02 ) 4 E 2 cos B 0 sin B 0 (1
E 2
28 sin 2 B 0
( L 01
16 E 2 sin 2 B 0 +24sin 4 B 0 +
+86 E 2 sin 4 B 0 +26 E 4 sin 4 B 0 72 E 2 sin 6 B 0 100 E 4 sin 6 B 0
12 E 6 sin 6 B 0 +
+77 E 4 sin 8 B 0 +39 E 6 sin 8 B 0
28 E 6 sin 10 B 0 [16 A 1 (1
E 2 ) 4 ] 1 .
15-62 Two Examples of Strip Transformations
Let us consider two examples of a strip transformation of conformal coordinates of Gauss-
Krueger type with a dilatation factor ρ =1( Schoedlbauer 1981a , b , 1982a , b) and a strip trans-
formation of conformal coordinates of UTM type with p =0 . 999578. Due to Example 15.8 ,
we start from the coordinates ellipsoidal longitude/latitude of TP I.O. Bonstetten (
=
{ 10 42 59 . 3215 , 48 26 45 . 4355 } ) on the Bessel ellipsoid of semi-major axis A = 377,397.155m and
reciprocal flattening f 1 = 299 . 15281285. The first and second strip has been fixed with L 01 =9
and L 02 =12 , respectively. The ellipsoidal latitude of the reference point was chosen to B 0 =48 .
In addition, we compared the direct transformation {L, B}→{x 1 ,y 1 } and {L, B}→{x 2 ,y 2 } as
illustrated by the commutative diagram of Fig. 15.17 , leading to differences in the submillimeter
range. By contrast, Example 15.9 gives the strip transformation of a point
{
L, B
}
12 . 01 , 49 }
on the ellipsoid referring to WGS84 ( A =6 , 378 , 137 m ,f 1 = 298 . 257223563) with a first refer-
ence meridian of L 01 =9 and a second of L 01 =15 . The differences again in the comparison of
both ways of calculating the UTM coordinates have been in the submillimeter range the closer
B 0 is chosen to the point
{
L, B
}
=
{
{
L, B
}
.
 
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