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Lemma 1.
For any
r
and
s
,
r<s<r
+
ˀ
,
in the domain of
ʳ
,
y
2sin
s−r
2
|
ʳ
(
s
)
−
ʳ
(
r
)
|≥
.
ʳ
(
s
)=(
x
(
s
)
,y
(
s
))
Proof.
Assume, without loss of generality,
that
r
= 0 and that
ʳ
(
r
) is at the origin
O
(i.e.
ʳ
(0) = (0
,
0)); the lemma is then equiva-
lent to
ʷ
=(
y
(
s
)
, −x
(
s
))
ʳ
(
˄
)
ʳ
(
˄
)
2sin
2
(Fig.
2
). We prove this
by lower-bounding the derivative of
|
ʳ
(
s
)
|≥
x
O
2
:
|
ʳ
(
s
)
|
ʳ
(0)
Fig. 2.
|Oʳ
(
s
)
|≥
2sin
s
2
, the slope
of
Oʳ
(
s
)isatmosttan
s
2
.
(
|ʳ
(
s
)
|
2
)
=2
ʳ
(
s
)
· ʳ
(
s
)=2
s
0
ʳ
(
˄
)
· ʳ
(
s
)
d˄
=2
s
0
≥
2
s
0
cos
∠
s˄ d˄
cos(
s − ˄
)
d˄
=2sin
s
cos
s
)=4sin
2
2
.
Hence
|
ʳ
(
s
)
|
2
≥
2(1
−
sin(
ʸ/
2)
ʸ/
2
Corollary 1.
For al l
i
,
1
≤
i<n
,
|
ʳ
(
t
i
+1
)
−
ʳ
(
t
i
)
|≥|
t
i
+1
−
t
i
|
.
sin((
t
i
+1
−
t
i
)
/
2)
(
t
i
+1
−t
i
)
/
2
Proof.
It suces to observe that, since 0
≤
t
i
+1
−
t
i
≤
ʸ
,
≥
sin(
ʸ/
2)
ʸ/
2
.
Lemma 2.
For any
r
and
s
,
r<s<r
+
ˀ
, in the domain of
ʳ
, the angle
between
ʳ
(
r
)
and the ray
ʳ
(
r
)
ʳ
(
s
)
is at most
s−r
2
.
Proof.
Assume again that
r
= 0 and that
ʳ
(0) =
O
; also assume w.l.o.g.
that
ʳ
(0) is horizontal (
ʳ
(0) = (1
,
0)). Let
ʳ
(
s
)=(
x
(
s
)
,y
(
s
)), and let
k
(
s
)=
y
(
s
)
/x
(
s
) be the slope of the ray
Oʳ
(
s
) (Fig.
2
, left). Then the lemma is
equivalent to
k
(
s
)
tan
2
, which we will prove by showing that
k
≤
1
cos
s
sin
2
s
−
≤
=
2cos
2
(
s/
2)
= (tan
2
)
.
By definition, for any
˄<s
the angle between
ʳ
(
˄
)and
ʳ
(
s
) is at most
1
˄
; in particular
ʳ
(
s
)
s
. It follows that
x
(
s
)=(
x
(
s
)
,y
(
s
))
(1
,
0) =
ʳ
(
s
)
s
−
≤
·
·
ʳ
(0) = cos
∠
s
0
≥
cos
s
, and thus
x
(
s
)
≥
sin
s
. Next, consider the unit vector
ʷ
=(
y
(
s
)
,
x
(
s
)), orthogonal to
ʳ
(
s
) (Fig.
2
). Since the angle between
ʳ
(
˄
)
and
ʷ
is at least
ˀ/
2
−
˄
), it follows that (
x
(
˄
)
,y
(
˄
))
−
(
s
−
·
ʷ
≤
cos(
ˀ/
2
−
(
s
−
˄
)),
or
x
(
˄
)
y
(
s
)
y
(
˄
)
x
(
s
)
−
≤
sin(
s
−
˄
). Integrating over
˄
from0to
s
,weget
x
(
s
)
y
(
s
)
y
(
s
)
x
(
s
)
−
≤
1
−
cos
s
. Combining this with
x
(
s
)
≥
sin
s
, we obtain
what we need:
k
=(
y/x
)
=
y
x
−
x
y
x
2
1
−
cos
s
sin
2
s
≤
.
Corollary 2.
The angle between the ray
ʳ
(
t
i−
1
)
ʳ
(
t
i
)
and
ʳ
(
t
i
)
is at most
sin
−
1
(
min
{
d
θ
,
|
ʳ
(
t
i−
1
)
ʳ
(
t
i
)
|}
2
)
Proof.
By the lemma, the angle between the ray
ʳ
(
t
i−
1
)
ʳ
(
t
i
)and
ʳ
(
t
i
)isatmost
t
i
−
t
i−
2
, which is always at most
ʸ/
2=sin
−
1
(
d
2
). So, it suces to consider the
case where
t
i
−t
i−
1
2
sin
−
1
(
|ʳ
(
t
i−
1
)
ʳ
(
t
i
)
|
2
|
ʳ
(
t
i−
1
)
ʳ
(
t
i
)
|
<d
ʸ
. But in this case,
≤
),
by Lemma
1
.
In summary, we have shown the following:
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