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Box 21.8 (Decomposition of the synthesis matrix B = B 0 + h B 1 +O 2 ( h 2 ).).
B=
=
e 2 ) n + h ]sin b cos l
( n + h )cos b
e 2 ) n + h ]sin b sin l
( n + h )cos b
[(1
[(1
sin l
( n + h )cos b
cos l
( n + h )cos b
0
···
(21.43)
[ n 2 (1 e 2 )+ mh ]sin l
m ( m + h )
[ n 2 (1 e 2 )+ mh ]cos l
m ( m + h )
sin b cos l
m + h
sin b sin l
m + h
cos b
m + h
1
0
0
0
2 × 9 ,
···
R
[ e 2 m sin 2 b +2(1 e 2 ) n ]sin b cos b
2( m + h )(1 −e 2 )
0 e 2 n sin b cos b
m + h
e 2 n sin b cos b
a 1 ( m + h )
B 0 :=
=
sin l
n cos b
cos l
n cos b
e 2 )tan b cos l
e 2 )tan b sin l
0
(1
(1
···
(21.44)
[ n 2 (1
e 2 )] sin l
m 2
[ n 2 (1
e 2 )] cos l
m 2
sin b cos l
m
sin b sin l
m
cos b
m
,
1
0
0
0
···
e 2 m sin 3 b cos b +2(1 e 2 ) n sin b cos b
2 m (1
0 e 2 n sin b cos b
e 2 n sin b cos b
a 1 m
m
e 2 )
B 1 :=
=
e n tan b cos l
e n tan b sin l
sin l
n 2 cos b
cos l
n 2 cos b
0
···
(21.45)
[ m 2 n 2 (1 e 2 )] sin l
m 3
[ n 2 (1 e 2 ) m 2 ]cos l
m 3
sin b cos l
m 2
sin b sin l
m 2
cos b
m 2
.
0
0
0
0
···
[ e 2 m sin 2 b +2(1 e 2 ) n ]sin b cos b
2 m 2 (1 −e 2 )
e 2 n sin b cos b
m 2
e 2 n sin b cos b
a 1 m 2
0
Example 21.1 numerically illustrates that for the computation of global
{
L, B
}
from local
{
l,b
}
and from datum parameters
{
t x ,t y ,t z ,α,β,γ,s,δa, δe 2
}
we can neglect h B 1 . Accordingly, the
synthesis of
{
L, B
}
is performed by [ L, B ] T =[ l,b ] T +B 0 [ t x ,t y ,t z ,α,β,γ,s,δa,δe 2 ] T .
Example 21.1 (Synthesis
of
{
L, B
}
from
{
l,b
}
and
from
datum
parameters
t x ,t y ,t z ,α,β,γ,s,δA,δE 2
{
}
, simulation of impact of local height h ).
a 1 := 6 , 377 , 397 . 155 [m] , e 2 := 0 . 006674372 , A 1 := 6 , 378 , 137 [m] ,
E 2 := 0 . 0066943800229 .
l =14 ,b =40 ,h = 1000m (assumed)
t x ,t y ,t z ,α,β,γ,s,δA,δE 2
{
}
from first section .
L 0 = L ( l,b )
13 59 54 . 2696
B 0 = B ( l,b )
40 00 00 . 06944
L = L ( l,b,h )
13 59 54 . 2704
B = B ( l,b,h )
40 00 00 . 06942
End of Example.
 
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