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x − x
0
=
s
s
0
y − y
0
=
s
s
0
cos
α
(
s
)
ds,
sin
α
(
s
)
ds
(23.138)
1
1
6
cos α
0
(
κ
0
+
κ
0
tan
α
0
)
Δs
3
+
Δx
:=
x
−
x
0
=
cos α
0
Δs
−
2
κ
0
sin α
0
Δs
2
−
120
cosα
0
κ
0
+6
κ
0
κ
3
κ
0
Δs
5
1
3
κ
0
)
Δs
4
+
1
24
κ
0
cosα
0
(
κ
0
tan
α
0
−
0
tan
α
0
−
−
(23.139)
720
κ
0
cosα
0
κ
0
tan
α
0
−
15
κ
0
tan
α
0
Δs
6
+
O
(
Δs
7
)
1
10
κ
0
κ
0
−
1
2
κ
0
cos α
0
Δs
2
1
6
cos α
0
(
κ
0
tan
α
0
−
κ
0
)
Δs
3
Δy
:=
y
−
y
0
=
sin α
0
Δs
−
−
−
120
cosα
0
κ
0
tan
3
κ
0
tan
α
0
Δs
5
+
24
κ
0
cosα
0
(
κ
0
+3
κ
0
tan
α
0
)
Δs
4
+
1
1
6
κ
0
κ
0
−
−
(23.140)
720
κ
0
cosα
0
κ
0
+10
κ
0
κ
0
tan
α
0
15
κ
0
Δs
6
+
O
(
Δs
7
)
1
−
accurate up to order seven in
Δs
:=
s
−
s
0
. The initial curvatures
k
0
=
k
(
s
0
) are classified as
1
)
(ii)
κ
0
=1
/r
0
(
r
0
radius of circle
(i)
κ
0
= 0 (straight line
L
1
r
0
)
(iii)
κ
0
=
s
0
/a
2
(
a
2
positive parameter of clothoid
S
C
a
2
)
End of Lemma.
For the proof we depart from the integrals
x
0
=
s
s
0
x
−
cos α
(
s
)
ds
cos
α
0
+
κ
0
(
s
s
0
)
2
d
(
s
=
s
s
0
s
0
)+
1
2
κ
0
(
s
−
−
−
s
0
)
(23.141)
y − y
0
=
s
s
0
sin α
(
s
)
ds
=
s
s
0
sin
α
0
+
κ
0
(
s
s
0
)
2
d
(
s
s
0
)+
1
2
κ
0
(
s
−
−
−
s
0
)
,
(23.142)
subject to
s
0
)+
1
s
0
)
2
2
κ
0
(
s
α
(
s
)=
α
0
+
Δα, Δα
:=
κ
0
(
s
−
−
(23.143)
Table 23.1
Power series of (cos(
α
0
+
Δα
)
,
sin(
α
0
+
Δα
))
cos(
α
0
+
Δα
)=
cos
α
0
−
1!
−
2!
cos
α
0
Δα
2
+
3!
sin
α
0
Δα
3
+
sin
α
0
Δα
sin
α
0
Δα
5
+
O
c
Δα
6
sin(
α
0
+
Δα
)=sin
α
0
−
1!
+
4!
cos
α
0
Δα
4
−
5!
−
2!
sin
α
0
Δα
2
−
3!
cos
α
0
Δα
3
cos
α
0
Δα
cos
α
0
Δα
5
+
O
c
Δα
6
+
4!
sin
α
0
Δα
4
+
5!
+
By means of the
uniformly convergent power series
of type cos(
α
0
+
Δα
)andsin(
α
0
+
Δα
)
given in Table
23.1
and
the powers Δα
n
=(
α
0
+
Δα
)
n
given in
Table
23.2
up to
n
=5 we are
able to compute the fundamental integrals of Fresnel type outlined in Table
23.3
. Indeed due to
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