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		<title>Bending Circle Limits - Versionsgeschichte</title>
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		<title>Gbachelier: Die Seite wurde neu angelegt: „  == Reference == Vladimir Bulatov: Bending Circle Limits. In: Bridges 2013. Pages 167–174   == DOI ==  == Abstract == M.C.Escher’s hyperbolic tess…“</title>
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				<updated>2015-01-28T11:20:12Z</updated>
		
		<summary type="html">&lt;p&gt;Die Seite wurde neu angelegt: „  == Reference == Vladimir Bulatov: &lt;a href=&quot;/index.php?title=Bending_Circle_Limits&quot; title=&quot;Bending Circle Limits&quot;&gt;Bending Circle Limits&lt;/a&gt;. In: &lt;a href=&quot;/index.php?title=Bridges_2013&quot; title=&quot;Bridges 2013&quot;&gt;Bridges 2013&lt;/a&gt;. Pages 167–174   == DOI ==  == Abstract == M.C.Escher’s hyperbolic tess…“&lt;/p&gt;
&lt;p&gt;&lt;b&gt;Neue Seite&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
== Reference ==&lt;br /&gt;
Vladimir Bulatov: [[Bending Circle Limits]]. In: [[Bridges 2013]]. Pages 167–174 &lt;br /&gt;
&lt;br /&gt;
== DOI ==&lt;br /&gt;
&lt;br /&gt;
== Abstract ==&lt;br /&gt;
M.C.Escher’s hyperbolic tessellations “Circle Limit I-IV” are based on a tiling of hyperbolic plane by identical&lt;br /&gt;
triangles. These tilings are rigid because hyperbolic triangles are unambiguously defined by their vertex angles.&lt;br /&gt;
However, if one reduce the symmetry of the tiling by joining several triangles into a single polygonal tile, such tiling&lt;br /&gt;
can be deformed. Hyperbolic tilings allow a deformation which is called bending. One can extend tiling of the&lt;br /&gt;
hyperbolic plane by identical polygons into tiling of the hyperbolic space by identical infinite prisms (chimneys).&lt;br /&gt;
The original polygon being the chimney’s cross section. The shape of these 3D prisms can be carefully changed by&lt;br /&gt;
rotating some of its sides in space and preserving all dihedral angles.&lt;br /&gt;
&lt;br /&gt;
The resulting tiling of 3D hyperbolic space creates 2D tiling at the infinity of hyperbolic space, which can be thought&lt;br /&gt;
of as the sphere at infinity. This sphere can be projected back into the plane using stereographic projection. After&lt;br /&gt;
small bending the original circle at infinity of the 2D tiling becomes fractal curve. Further bending results in thinning&lt;br /&gt;
the fractal features which eventually form a fractal set of circular holes which in the end disappear.&lt;br /&gt;
&lt;br /&gt;
== Extended Abstract ==&lt;br /&gt;
&lt;br /&gt;
== Bibtex == &lt;br /&gt;
&lt;br /&gt;
== Used References ==&lt;br /&gt;
[1] M.C. Escher. M.C. Escher, His Life and Complete Graphic Work. 1992.&lt;br /&gt;
&lt;br /&gt;
[2] M. von Gagern and J. Richter-Gebert. Hyperbolization of euclidean ornaments. The Electronic Journal&lt;br /&gt;
of Combinatorics, 16R2, 2009.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Links ==&lt;br /&gt;
=== Full Text === &lt;br /&gt;
http://archive.bridgesmathart.org/2013/bridges2013-167.pdf&lt;br /&gt;
&lt;br /&gt;
[[intern file]]&lt;br /&gt;
&lt;br /&gt;
=== Sonstige Links ===&lt;br /&gt;
http://archive.bridgesmathart.org/2013/bridges2013-167.html&lt;/div&gt;</summary>
		<author><name>Gbachelier</name></author>	</entry>

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