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Conformal Geometric Algebra in Stochastic Optimization Problems ...

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6 CHAPTER 1. INTRODUCTION<br />

Spherical Reflection<br />

This example demonstrates that a spherical reflection is possible, yet its ma<strong>in</strong> message<br />

is the simplicity of reason<strong>in</strong>g; some elementary calculations and assumptions<br />

lead to a profound result.<br />

Consider a circle C <strong>in</strong> 3D - it can clearly be thought of as an <strong>in</strong>tersection of two<br />

spheres. Given one sphere, which co<strong>in</strong>cides with the circle, the set of suitable<br />

spheres to reconstruct the circle is endlessly big. The set also comprises a plane,<br />

that is a special sphere with <strong>in</strong>f<strong>in</strong>ite radius, which actually is the circle’s plane PC.<br />

Let S denote a different set that conta<strong>in</strong>s pairs of spheres such that the <strong>in</strong>tersection<br />

between the respective spheres of each pair yields the circle. Each pair <strong>in</strong> S for<br />

which the constitut<strong>in</strong>g spheres locally <strong>in</strong>tersect at right angles can now be taken to<br />

build the (<strong>in</strong>f<strong>in</strong>itely big) subset S⊥ ⊂ S. There are at least two special cases <strong>in</strong> S⊥.<br />

• One sphere is of m<strong>in</strong>imal size the other one is of maximum size: the circle<br />

plane PC <strong>in</strong>tersected with the sphere SC whose center lies on PC yields C,<br />

see figure 1.1. The radius of SC equals the circle’s radius.<br />

• Symmetrical case: both spheres, SI and SJ, have equal radius, see figure 1.2.<br />

Fig. 1.1: Construction of the circle C from sphere and plane.<br />

Because both cases fulfill the requirement of perpendicularity, the results of section<br />

1.1.3 can be used and the circle C can be built <strong>in</strong> two ways<br />

CSP = SCPC and CSS = SISJ .<br />

Note that, <strong>in</strong> the symmetrical case, each sphere can be replaced by the reflection of<br />

the opposite sphere <strong>in</strong> the circle’s plane, for example SJ ≡ PCSIPC. The follow<strong>in</strong>g<br />

calculation makes use of this fact. It starts from C ≡ [CSP ∝ CSS].<br />

SCPC ∝ SISJ employ SJ ∝ PCSIPC<br />

SCPC ∝ SI(PCSIPC) multiply by PC<br />

SCP 2 C ∝ SIPCSIP 2 C<br />

SC ∝ SIPCSI s<strong>in</strong>ce P 2 C ∈ � by axiom<br />

(1.2)<br />

Besides, with S 2 I ∈ �, PC ∝ SISCSI is implied. The feasibility of a spherical<br />

reflection has hereby been shown, though solely for the special setup <strong>in</strong> which the<br />

center of SI is located on SC.

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