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SUMMARY:Hermann Karcher (University of Bonn)
DTSTART:20201215T180000Z
DTEND:20201215T190000Z
DTSTAMP:20260423T035019Z
UID:OSGA/41
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/OSGA/41/">Nu
 merical experiments with closed constant curvature space curves</a>\nby He
 rmann Karcher (University of Bonn) as part of Online Seminar "Geometric An
 alysis"\n\n\nAbstract\nThe discovery story will be told with pictures illu
 strating all steps\, including the <em>observation</em>\nbelow which we us
 ed but could not prove. Since the shape of space curves is difficult to be
 \ncorrectly deduced from planar images\, most images will be  red-green an
 aglyphs. They\ncan be looked at without red-green glasses\, but without gi
 ving the 3D impression.\n\n<strong>Dec 15\,2020: H. Karcher: Closed consta
 nt curvature space curves</strong>\n\nThe only closed constant curvature s
 pace curves which I knew in 2004\nwere made from pieces of circles and hel
 ices.\nThe Frenet equations allow to construct space curves of constant cu
 rvature $\\kappa$\nby prescribing a torsion function $\\tau(s)$. For close
 d curves one needs periodic\ntorsion functions\, for example Fourier polyn
 omials. If one chooses these\nfunctions so that they are skew symmetric wi
 th respect to their zeros\, $\\tau(a-s)=-\\tau(a+s)$\, then\nthe resulting
  curves have the normal planes at these points as planes of\nmirror symmet
 ry. If adjacent symmetry planes have angles such as $\\pi/3$\,\nthen the c
 urves are forced by their symmetries to be closed. This gives the \nfirst 
 collection of new examples.\n\nIf the torsion functions are even with resp
 ect to their extremal points\, i.e.\n$\\tau(a-s) = \\tau(a+s)$\, then the 
 resulting curves have their principal normals\nat these points as symmetry
  axes for $180^\\circ$ rotations. If two such adjacent\nsymmetry normals a
 re coplanar and intersect under rational angles <br> ($\\pi p/q$)\,\nthen 
 the curves are again forced by their symmetries to close up. Therefore\non
 e can hope to get examples by solving a 2-parameter problem.\n\nThis is ma
 de simple by an <em>observation</em> which I cannot prove: The distance of
 \nadjacent symmetry normals depends in a surprisingly monotone way on the 
 constant\nterm in the Fourier polynomial  $\\tau(s) = b_0 + b_1\\\,\\sin(s
 ) + b_3\\\, \\sin(3s)$. This\nallows to consider $b_0 = b_0(\\kappa\, b_1\
 , b_3)$\, such that the symmetry normals of the\nresulting curves are copl
 anar and hence intersect all in one point. Therefore we\nhave again to sol
 ve a 1-parameter problem by choosing $\\kappa\, b_1\, b_3$ in such a way\n
 that adjacent symmetry normals intersect with a rational angle. This gives
  a wealth\nof new examples.\n\nThe evolutes of such curves have also const
 ant curvature $\\kappa$\, but they have \nsingularities at the zeros of $\
 \tau(s)$. This led to a search for closed examples with $\\tau(s) > 0$.\nA
  (2-11)-torus knot showed up and suggested to look for examples on tori. E
 asy ones\nare again found by symmetries and more complicated ones as solut
 ions of intermediate\nvalue problems. The formulas work also on cylinders 
 and revealed easier examples than\nall the previous ones!\n\nThen E. Tjade
 n suggested to look for examples which are <strong>congruent</strong> to t
 heir evolutes.\nThey were found by modifying the Frenet equations. The $(2
 \, 2n+1)$- torus knots among\nthem are in fact their own evolutes.\n
LOCATION:https://researchseminars.org/talk/OSGA/41/
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