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Gruber P. Convex and Discrete Geometry

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64 <strong>Convex</strong> Bodies<br />

in contradiction to the minimality of A. Hence the first case cannot hold. Second<br />

case: x ∈ relbd cl conv R(A). Then we may choose u ∈ S d−1 such that x ∈<br />

H(u)∩cl conv R(A) but cl conv R(A) �⊆ H(u).By(5),x −µ(A + ) ∈ cl conv R(A 0 ).<br />

The set A 0 ∈ M is minimal such that x − µ(A + ) ∈ cl conv R(A 0 ). Otherwise<br />

A ∈ M would not be minimal such that x ∈ cl conv R(A). Since cl conv R(A) �⊆<br />

H(u), Proposition (5) shows that the dimension of cl conv R(A 0 ) is smaller than<br />

the dimension of cl conv R(A). IfR(A 0 ) ={o} we have x = µ(A + ) <strong>and</strong> we are<br />

done. If not, we may repeat the above argument with x − µ(A + ) <strong>and</strong> A 0 instead of<br />

x <strong>and</strong> A to show that x − µ(A + ) − µ(A 0+ ) ∈ cl conv R(A 00 ), where the dimension<br />

of cl conv R(A 00 ) is smaller than the dimension of cl conv R(A 0 ), etc. In any case,<br />

after finitely many repetitions we arrive at (6).<br />

Propositions (2) <strong>and</strong> (6) finally yield (1), concluding the proof of the theorem.<br />

⊓⊔<br />

Remark. The range of a finite non-atomic vector-valued signed measure is actually<br />

a zonoid <strong>and</strong> vice versa, as shown by Rickert [835]. See also Bolker [141]. Zonoids<br />

are particular convex bodies. See Sect. 7.3 for a definition.<br />

4.4 Pontryagin’s Minimum Principle<br />

The minimum principle, sometimes also called maximum principle, of Pontryagin<br />

<strong>and</strong> his collaborators Boltyanskiĭ, Gamkrelidze <strong>and</strong> Mishchenko [813] is a central<br />

result of control theory. It yields information on optimal controls.<br />

In the following we present a version which makes essential use of support<br />

hyperplanes <strong>and</strong> which rests on convexity arguments, both finite <strong>and</strong> infinite<br />

dimensional.<br />

For more information on control theory see, e.g. Pontryagin, Boltyanskiĭ,<br />

Gamkrelidze, Mishchenko [813] <strong>and</strong> Agrachev <strong>and</strong> Sachkov [2].<br />

The Time Optimal Control Problem<br />

Consider a system of linear differential equations with given initial value:<br />

(1) ˙x = Ax + Bu, x(0) = a,<br />

where A <strong>and</strong> B are real d × d, respectively, d × c matrices <strong>and</strong> a ∈ E d .Acontrol<br />

u :[0, +∞) → C is the parametrization of a curve which is contained in a given<br />

convex body C in E c . We suppose that each of its c components is measurable (with<br />

respect to Lebesgue measure on R). Given a control u,byasolution of (1), we mean<br />

a continuous parametrization x :[0, +∞) → E d of a curve, such that the components<br />

of x are almost everywhere differentiable <strong>and</strong> (1) holds almost everywhere on<br />

[0, +∞). A control u is said to transfer the initial state a to a state b ∈ E d \{a} in<br />

time t if x(t) = b holds for the corresponding solution x of (1).<br />

The time optimal control problem is to find a control u which transfers a to b in<br />

minimum time.

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