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Gruber P. Convex and Discrete Geometry

Gruber P. Convex and Discrete Geometry

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150 <strong>Convex</strong> Bodies<br />

Integration implies that<br />

n=1<br />

x ′ (s) 2 + y ′ (s) 2 = 1for0≤ s ≤ 2π.<br />

�2π<br />

0<br />

x ′ (t) 2 dt +<br />

�<br />

0<br />

2π<br />

y ′ (t) 2 dt = 2π.<br />

Consider the Fourier series for x(·) <strong>and</strong> y(·),<br />

x(s) = a0<br />

2 +<br />

∞�<br />

(an cos ns + bn sin ns), y(s) = c0<br />

2 +<br />

∞�<br />

(cn cos ns + dn sin ns).<br />

Then<br />

x ′ ∞�<br />

(s) = (nbn cos ns − nan sin ns), y ′ ∞�<br />

(s) = (ndn cos ns − ncn sin ns).<br />

n=1<br />

The formula of Leibniz to calculate the area of a planar set bounded by a closed<br />

Jordan curve of class C 1 <strong>and</strong> a version of Parseval’s theorem then yield the following.<br />

<strong>and</strong><br />

L 2 = 4π 2 ⎛<br />

�<br />

= 2π ⎝<br />

Thus<br />

L 2 − 4π A = 2π 2<br />

A =<br />

0<br />

= 2π 2<br />

2π<br />

�2π<br />

0<br />

x(t)y ′ (t)dt = π<br />

x ′ (t) 2 dt +<br />

�<br />

0<br />

2π<br />

y ′ (t) 2 dt<br />

n=1<br />

n=1<br />

∞�<br />

n(<strong>and</strong>n − bncn)<br />

n=1<br />

⎞<br />

⎠ = 2π 2<br />

∞�<br />

n 2 (a 2 n + b2 n + c2 n + d2 n ).<br />

n=1<br />

∞� � 2 2<br />

n (an + b 2 n + c2 n + d2 n ) − 2n(<strong>and</strong>n − bncn) �<br />

n=1<br />

∞� �<br />

(nan − dn) 2 + (nbn + cn) 2 + (n 2 − 1)(c 2 n + d2 n )� ≥ 0,<br />

n=1<br />

where equality holds if <strong>and</strong> only if<br />

In this case<br />

cn = dn = an = bn = 0forn ≥ 2, a1 = d1, b1 =−c1.<br />

x(s) = a0<br />

2 + a1 cos s + b1 sin s,<br />

y(s) = c0<br />

2 − b1 cos s + a1 sin s.<br />

This is the parametrization of a circle – note that<br />

�<br />

x(s) − a0<br />

2<br />

� 2<br />

�<br />

+ y(s) − c0<br />

2<br />

� 2<br />

= a 2 1 + b2 1 . ⊓⊔

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