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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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