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Edita Vranková<br />

(intM∩intN=∅). The overlapping of two arbitrary polygons M(x) and N or<br />

its dense placements can be expressed geometrically by the following sets<br />

O(M,N)={x∈E 2 ; M(x) overlaps N, i.e. intM(x)∩intN ≠ ∅},<br />

D(M,N)={x∈E 2 ; M(x), N are densely placed,<br />

i.e. ∂M(x)∩∂N ≠ ∅ and intM(x)∩intN = ∅},<br />

where M(x) is the translated position of polygon M=M(o) to the (reference)<br />

point x and the point o (origin) is a fixed point in the plane E 2 [7]. Some<br />

constructions of the set D(M,N) are described e.g. in [3], [6], [7]. We<br />

suppose that the origin o is an interior point of the polygon M.<br />

2 Two-periodical placement of rectangular<br />

polygons along a line<br />

Among the simplest tasks of the periodical placements belong placements<br />

of mutually congruent polygons (M=N). In this case is the set D(M,M)<br />

symmetrical by origin o [7]. If every two neighboring translated polygons<br />

M i and M i+1 (i∈Z) are dense placed in strip, then we obtain dense periodical<br />

placement of polygon M along a line [9].<br />

Definition 1. A periodical placement of union U=M∪M'(x) nonoverlapping<br />

polygons M and M'(x) along a line given by vector u, where<br />

M′=s o (M) is the image of M by the central symmetry s o (with symmetry<br />

center o) and M'(x) is the translated position of M' to the point x [7] we call<br />

two-periodical placement of polygon M along a line with basis u (Fig. 1)<br />

and we denote it by Uu or MM'u.<br />

M′ −1<br />

u<br />

M′(x) x<br />

M′ 1 M′ 2<br />

o<br />

M<br />

u<br />

M 1 M 2<br />

M′<br />

M −1<br />

w<br />

Fig. 1: Two-periodical placement Uu of polygon M with along a line<br />

Analogically by [9], [10], two-periodical placement of a polygon M is<br />

the system<br />

Uu=MM'u={U i =U+iu; i∈Z}.<br />

of non-overlapping figures U i which are copies of the figure<br />

U=M∪M'(x) under translations given by the vectors iu for all integers i∈Z<br />

(see Fig. 1). The polygons M, M'(x) are called the generators of the twoperiodical<br />

placement MM'u. The basis u defines for plane strip (with width<br />

w) a translation in strip. It is obvious that M=M(o)=M 0 and U i =M i ∪M' i (x).<br />

294

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