Dupin cyclides osculating surfaces (slajdy wykładu na seminarium w
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Dupin cyclides osculating surfaces (slajdy wykładu na seminarium w
Dupin cyclides osculating surfaces Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Colaborators: Remi Langevin (UdeB), Adam Bartoszek, Szymon Walczak (UŁ) Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces What is extrinsic conformal geometry? Conformal transformations = transformations preserving angles. Conformal group = group of conformal transformations; in R3 (S 3 or H 3 ) = Möbius group Möb3 = the group generated by all isometries and inversions Conformal geometry= theory of invariants of the Möbius group Extrinsic geometry (of surfaces) = theory of invariants of the second fundamental form (principal curvatures, principal directions and foliations, lines of curvature) etc. =⇒ extrinsic conformal geometry T = (extrinsic geometry) (conformal geometry) Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Conformal change of the metric 1 If two surfaces S ans S̃ are conformally equivalent, then their first fundamental forms g and g̃ are related by: g̃ = exp(2φ) · g for some function φ. If so, (1) their second fundamental forms b and b̃ satisfy b̃ = exp(φ) · b + ψ · g , (2) their shape (Weingarten) operators A and à satisfy à = exp(−φ) · A + ψ · I , Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Conformal change of the metric 2 (3) their principal directions are the same while unit principal vectors Xi and X̃i (i = 1, 2) satisfy X̃i = exp(−φ) · Xi , (4) their principal curvatures ki and k̃i satisfy k̃i = exp(−φ) · ki + ψ, therefore k̃1 − k̃2 = exp(−φ) · (k1 − k2 ). Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces First conformal invariants Consequently, the vector fields ξi = Xi /µ, i = 1, 2, where µ = (k1 − k2 )/2 are conformally invariant. Conformally invariant is also their Lie bracket: 1 1 [ξ1 , ξ2 ] = − θ2 · ξ1 − θ1 · ξ2 2 2 and the coefficients θ1 , θ2 (called principal conformal curvatures) in the above (Darboux, Tresse, 189*). Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Canonical position Problem Are the invariants we described above sufficient to determine a surface up to a Möbius transformation? Answer: NO. Proof. Any surface (at a non-umbilical point) can be mapped by a unique Möbius transformation to the one given locally by z = + 1 2 1 (x − y 2 ) + (θ1 x 3 + θ2 y 3 ) 2 6 1 (ax 4 + bx 3 y + Ψx 2 y 2 + cx 3 y + dy 4 ) + H.O.T . 24 Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Canal surfaces Canal surfaces = envelopes of 1-parameter families of spheres. Proposition (A. B., R. L., P. W.,20**) Canal surfaces can be characterized by vanishing of one of their conformal principal curvatures: θi = 0 for some i ∈ {1, 2}. The invariant Ψ is constant along the characteristic circles. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Special canals A canal surface is special if its nontrivial conformal principal curvature is constant along its characteristic circles. Proposition (A. B., R. L., P. W., 20**) Special canal surfaces are conformal images of surfaces of revolution, cylinders and cones over planar (spherical) curves. These three classes are characterized, respectively, by |Ψ| < 2, |Ψ| = 2, Ψ| > 2. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Dupin cyclides Dupin cyclides = canal surfaces in two ways (there are two 1-parameter families of spheres enveloped by such a surface). =⇒ On Dupin cyclides θ1 = θ2 = 0. =⇒ Dupin cyclides are special canals. =⇒ Dupin cyclides are conformal images of tori, cylinders and cones of revolution. =⇒ On Dupin cyclides Ψ = const. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Integrability condition Given a surface S, one has the unique map g : S → Möb3 such that g (p), p ∈ S, maps S to the canonical position (at p). Let ω = g −1 dg . ω is the 1-form on S with values in the Lie algebra of the Möbius group Möb3 . Using a matrix representation of Möb3 , one can write ω = A1 (θ1 , θ2 , Ψ) · ω1 + A2 (θ1 , θ2 , Ψ) · ω2 , where (ω1 , ω2 ) is the frame of 1-forms dual to (ξ1 , ξ2 ). Integrability condition: 1 d ω + [ω, ω] = 0. 2 Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Fialkov Theorem Theorem (Fialkov, 194*) Given 1-forms ω1 , ω2 and functions θ1 , θ2 , Ψ defined on a simply-connected domain U ⊂ R2 and satisfying the above integrability condition there, there exists – unique up to a Möbius transformation – immersion F : U → R3 , S 3 , H 3 such that the above data appear us the local conformal invariants of the surface S = F (U). Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Dupin necklace Theorem (A. B., R. L., P. W.) The osculating spheres Σ2 (t) for the principal curvature k2 along a characteristic circle C (which is a parameterized by t line of principal curvature for k1 ) of a canal surface K have an envelope which is a Dupin cyclide D. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces A problem The above privides motivation for the following Problem Given a generic point p of a surface S, find a Dupin cyclide D osculating S at p and determine the direction of highest order of tangency of D and S at p. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Osculating cyclide 1 Recall the equation of S in the canonical form: S :z = + 1 2 1 (x − y 2 ) + (θ1 x 3 + θ2 y 3 ) 2 6 1 4 3 (ax + bx y + Ψx 2 y 2 + cx 3 y + dy 4 ) + H.O.T . 24 Put a cyclide D in the canonical position. Its equation reads as D:z = + 1 2 (x − y 2 ) + 2 1 (3x 4 + ΨD x 2 y 2 − 3y 4 ) + H.O.T . 24 Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Osculating cyclide 2 =⇒ S and D are tangent of order 3 in the direction y = tx, where q t = − 3 θ1 /θ2 . For a suitable (unique) value of ΨD , S and D are tangent of order 4 in this direction. In this case, D is called the osculating cyclide of S at p. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Dupin foliation Here, we will use the following terminology: (1) the direction in Tp S making the angle α such that p tg α = − 3 θ1 /θ2 = Dupin direction, (2) the distribution (line field) on S built of straight lines in Dupin directions = Dupin line field, (3) the foliation determined by the Dupin line field = Dupin foliation, (4) leaves of the Dupin foliation = Dupin lines (and, perhaps, so on). Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces An example Example On canal surfaces (different from Dupin cyclides), the Dupin foliation coincides with one of the foliations by lines of curvature. Problem Do there exist surfaces for which the Dupin direction is constant (6= 0, 6= π/2)? Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Main Theorem (of today) Theorem (A. B., P. W., Sz. W., 201*) Given a foliation F on a convex planar domain U making non-zero angle with the direction of one of the coordinate lines, there exist surfaces S on which the coordinate lines correspond to the lines of curvature while the leaves of F correspond to the Dupin lines; the family of such surfaces is parametrized (up to Möbius transformations) by pairs of two functions: one of two variables and another one of one variable. Proof. ... Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Helcats 1 Example There exists a natural 1-parameter family of minimal surfaces connecting the helicoid to the catenoid. They are called helcats Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces A helcat Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Helcats 2 and are given by the equations x1 = cosα · sinh s · sin t + sin α · cosh s cos t, x2 = − cos α · sinh s · cos t + sin α · cosh s · sin t, x3 = sin α · s + cos α · t, For them, we have: θ1 = q 2(1 − sin α) · sinh s, θ2 = q 2(1 + sin α) · sinh s, cos α = const . 1 + sin α In particular, κ = 1 on the helicoid and κ = 0 on the catenoid. κ := θ1 /θ2 = Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Bibliography 1 A. Bartoszek, R. Langevin, P. Walczak, Special canal surfaces of S 3 , Bull. Braz. Math. Soc. 42 (2011), 301–320. A. Bartoszek, P. Walczak, Foliations by surfaces of a peculiar class, Ann. Polon. Math., 94 (2008), 89 – 95. A. Bartoszek, P. Walczak, Sz. Walczak, Dupin cyclides osculating surfaces, in preparation. G. Cairns, R. W. Sharpe and L. Webb. Conformal invariants for curves in three dimensional space forms, Rocky Mountain J. Math. 24 (1994), 933 – 959. G. Darboux, Leçons sur la théorie générale des surfaces, Guthier-Villars, Paris 1897. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces Bibliography 2 A. Fialkov, Conformal differential geometry of a subspace, Trans. Amer. Math. Soc. 56 (1944), 309 – 433. R. Garcia, R. Langevin, P. Walczak, Dynamical behaviour of Darboux curves, preprint, arXiv.0912.3749. (2009). R. Langevin, P. Walczak, Conformal geometry of foliations, Geom. Dedicata 132 (2008), 135 – 178. A. Tresse, Sur les invariants différentiels d’une surface par rapport aux transformations conformes de l’espace, C.R. Acad. Sci. Paris 114 (1892), 948 – 950. Paweł Walczak, Uniwersytet Łódzki, Dijon, 25 stycznia 2012 Dupin cyclides osculating surfaces