A Survey on Classical Minimal Surface Theory
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Brief Information on the Surfaces Not Included in the Basic Content of the Encyclopedia
Brief Information on the Surfaces Not Included in the Basic Content of the Encyclopedia Brief information on some classes of the surfaces which cylinders, cones and ortoid ruled surfaces with a constant were not picked out into the special section in the encyclo- distribution parameter possess this property. Other properties pedia is presented at the part “Surfaces”, where rather known of these surfaces are considered as well. groups of the surfaces are given. It is known, that the Plücker conoid carries two-para- At this section, the less known surfaces are noted. For metrical family of ellipses. The straight lines, perpendicular some reason or other, the authors could not look through to the planes of these ellipses and passing through their some primary sources and that is why these surfaces were centers, form the right congruence which is an algebraic not included in the basic contents of the encyclopedia. In the congruence of the4th order of the 2nd class. This congru- basis contents of the book, the authors did not include the ence attracted attention of D. Palman [8] who studied its surfaces that are very interesting with mathematical point of properties. Taking into account, that on the Plücker conoid, view but having pure cognitive interest and imagined with ∞2 of conic cross-sections are disposed, O. Bottema [9] difficultly in real engineering and architectural structures. examined the congruence of the normals to the planes of Non-orientable surfaces may be represented as kinematics these conic cross-sections passed through their centers and surfaces with ruled or curvilinear generatrixes and may be prescribed a number of the properties of a congruence of given on a picture. -
Quintic Parametric Polynomial Minimal Surfaces and Their Properties
Differential Geometry and its Applications 28 (2010) 697–704 Contents lists available at ScienceDirect Differential Geometry and its Applications www.elsevier.com/locate/difgeo Quintic parametric polynomial minimal surfaces and their properties ∗ Gang Xu a,c, ,Guo-zhaoWangb a Hangzhou Dianzi University, Hangzhou 310018, PR China b Department of Mathematics, Zhejiang University, Hangzhou 310027, PR China c Galaad, INRIA Sophia-Antipolis, 2004 Route des Lucioles, 06902 Sophia-Antipolis Cedex, France article info abstract Article history: In this paper, quintic parametric polynomial minimal surface and their properties are Received 28 November 2009 discussed. We first propose the sufficient condition of quintic harmonic polynomial Received in revised form 14 April 2010 parametric surface being a minimal surface. Then several new models of minimal surfaces Available online 31 July 2010 with shape parameters are derived from this condition. We also study the properties Communicated by Z. Shen of new minimal surfaces, such as symmetry, self-intersection on symmetric planes and MSC: containing straight lines. Two one-parameter families of isometric minimal surfaces are 53A10 also constructed by specifying some proper shape parameters. 49Q05 © 2010 Elsevier B.V. All rights reserved. 49Q10 Keywords: Minimal surface Harmonic surfaces Isothermal parametric surface Isometric minimal surfaces 1. Introduction Since Lagrange derived the minimal surface equation in R3 in 1762, minimal surfaces have a long history of over 200 years. A minimal surface is a surface with vanishing mean curvature. As the mean curvature is the variation of area functional, minimal surfaces include the surfaces minimizing the area with a fixed boundary. Because of their attractive properties, minimal surfaces have been extensively employed in many areas such as architecture, material science, aviation, ship manufacture, biology and so on. -
Deformations of the Gyroid and Lidinoid Minimal Surfaces
DEFORMATIONS OF THE GYROID AND LIDINOID MINIMAL SURFACES ADAM G. WEYHAUPT Abstract. The gyroid and Lidinoid are triply periodic minimal surfaces of genus 3 embed- ded in R3 that contain no straight lines or planar symmetry curves. They are the unique embedded members of the associate families of the Schwarz P and H surfaces. In this paper, we prove the existence of two 1-parameter families of embedded triply periodic minimal surfaces of genus 3 that contain the gyroid and a single 1-parameter family that contains the Lidinoid. We accomplish this by using the flat structures induced by the holomorphic 1 1-forms Gdh, G dh, and dh. An explicit parametrization of the gyroid using theta functions enables us to find a curve of solutions in a two-dimensional moduli space of flat structures by means of an intermediate value argument. Contents 1. Introduction 2 2. Preliminaries 3 2.1. Parametrizing minimal surfaces 3 2.2. Cone metrics 5 2.3. Conformal quotients of triply periodic minimal surfaces 5 3. Parametrization of the gyroid and description of the periods 7 3.1. The P Surface and tP deformation 7 3.2. The period problem for the P surface 11 3.3. The gyroid 14 4. Proof of main theorem 16 4.1. Sketch of the proof 16 4.2. Horizontal and vertical moduli spaces for the tG family 17 4.3. Proof of the tG family 20 5. The rG and rL families 25 5.1. Description of the Lidinoid 25 5.2. Moduli spaces for the rL family 29 5.3. -
MINIMAL TWIN SURFACES 1. Introduction in Material Science, A
MINIMAL TWIN SURFACES HAO CHEN Abstract. We report some minimal surfaces that can be seen as copies of a triply periodic minimal surface related by reflections in parallel planes. We call them minimal twin surfaces for the resemblance with crystal twinning. Twinning of Schwarz' Diamond and Gyroid surfaces have been observed in experiment by material scientists. In this paper, we investigate twinnings of rPD surfaces, a family of rhombohedral deformations of Schwarz' Primitive (P) and Diamond (D) surfaces, and twinnings of the Gyroid (G) surface. Small examples of rPD twins have been constructed in Fijomori and Weber (2009), where we observe non-examples near the helicoid limit. Examples of rPD twins near the catenoid limit follow from Traizet (2008). Large examples of rPD and G twins are numerically constructed in Surface Evolver. A structural study of the G twins leads to new description of the G surface in the framework of Traizet. 1. Introduction In material science, a crystal twinning refers to a symmetric coexistence of two or more crystals related by Euclidean motions. The simplest situation, namely the reflection twin, consists of two crystals related by a reflection in the boundary plane. Triply periodic minimal surfaces (TPMS) are minimal surfaces with the symmetries of crystals. They are used to model lyotropic liquid crystals and many other structures in nature. Recently, [Han et al., 2011] synthesized mesoporous crystal spheres with polyhedral hollows. A crystallographic study shows a structure of Schwarz' D (diamond) surface. Most interestingly, twin structures are observed at the boundaries of the domains; see Figure 1. In the language of crystallography, the twin boundaries are f111g planes. -
Complete Minimal Surfaces in R3
Publicacions Matem`atiques, Vol 43 (1999), 341–449. COMPLETE MINIMAL SURFACES IN R3 Francisco J. Lopez´ ∗ and Francisco Mart´ın∗ Abstract In this paper we review some topics on the theory of complete minimal surfaces in three dimensional Euclidean space. Contents 1. Introduction 344 1.1. Preliminaries .......................................... 346 1.1.1. Weierstrass representation .......................346 1.1.2. Minimal surfaces and symmetries ................349 1.1.3. Maximum principle for minimal surfaces .........349 1.1.4. Nonorientable minimal surfaces ..................350 1.1.5. Classical examples ...............................351 2. Construction of minimal surfaces with polygonal boundary 353 3. Gauss map of minimal surfaces 358 4. Complete minimal surfaces with bounded coordinate functions 364 5. Complete minimal surfaces with finite total curvature 367 5.1. Existence of minimal surfaces of least total curvature ...370 5.1.1. Chen and Gackstatter’s surface of genus one .....371 5.1.2. Chen and Gackstatter’s surface of genus two .....373 5.1.3. The surfaces of Espirito-Santo, Thayer and Sato..378 ∗Research partially supported by DGICYT grant number PB97-0785. 342 F. J. Lopez,´ F. Mart´ın 5.2. New families of examples...............................382 5.3. Nonorientable examples ................................388 5.3.1. Nonorientable minimal surfaces of least total curvature .......................................391 5.3.2. Highly symmetric nonorientable examples ........396 5.4. Uniqueness results for minimal surfaces of least total curvature ..............................................398 6. Properly embedded minimal surfaces 407 6.1. Examples with finite topology and more than one end ..408 6.1.1. Properly embedded minimal surfaces with three ends: Costa-Hoffman-Meeks and Hoffman-Meeks families..........................................409 6.1.2. -
Experimental Form-Finding for Möbius Strip and Ennerper Minimal
ISSN: 2319-5967 ISO 9001:2008 Certified International Journal of Engineering Science and Innovative Technology (IJESIT) Volume 2, Issue 5, September 2013 Experimental Form-Finding for Möbius Strip and Ennerper Minimal Surfaces Using Soap Film Models Hooi Min YEE1, Kok Keong CHOONHG2, Jae-Yeol KIM3 1Faculty of Civil Engineering, University Technology MARA Penang, Malaysia 2Academic staff , School of Civil Engineering, University Sains Malaysia, Penang, Malaysia 3Corresponding Author, Associate Professor, Hyupsung University, Hwasung, Korea Abstract—This paper describes an effort to produce soap film models with boundaries corresponding to those defined by Möbius strip and Enneper minimal surfaces. Soap film models with surfaces deviating from mathematically defined minimal surfaces of Möbius strip and Enneper are shown. Index Terms— Form-finding, Soap film model, Möbius strip, Enneper. I. INTRODUCTION Soap film model is used to find the surface form that minimizes area subject to appreciate constraints. Ireland [1] has presented some puzzling measurements of the tension between soap film and a solid surface. Moulton and Pelesko[2] have investigated Catenoid soap film model subjected to an axially symmetric electric field. The experimental and theoretical analysis for this Field Driven Mean Curvature Surface (FDMC) surface provides a step in understanding how electric fields interact with surfaces driven by surface tension. Such interactions may be of great benefit in micro scale systems such as micro electro mechanical systems (MEMS) and self-assembly. Brakke[3] has treated the area minimization problem with boundary constraints. Koiso and Palmer[4] have studied a variational problem whose solutions are a geometric model for thin films with gravity which is partially supported by a given contour. -
Minimal Surfaces
Minimal Surfaces December 13, 2012 Alex Verzea 260324472 MATH 580: Partial Dierential Equations 1 Professor: Gantumur Tsogtgerel 1 Intuitively, a Minimal Surface is a surface that has minimal area, locally. First, we will give a mathematical denition of the minimal surface. Then, we shall give some examples of Minimal Surfaces to gain a mathematical under- standing of what they are and nally move on to a generalization of minimal surfaces, called Willmore Surfaces. The reason for this is that Willmore Surfaces are an active and important eld of study in Dierential Geometry. We will end with a presentation of the Willmore Conjecture, which has recently been proved and with some recent work done in this area. Until we get to Willmore Surfaces, we assume that we are in R3. Denition 1: The two Principal Curvatures, k1 & k2 at a point p 2 S, 3 S⊂ R are the eigenvalues of the shape operator at that point. In classical Dierential Geometry, k1 & k2 are the maximum and minimum of the Second Fundamental Form. The principal curvatures measure how the surface bends by dierent amounts in dierent directions at that point. Below is a saddle surface together with normal planes in the directions of principal curvatures. Denition 2: The Mean Curvature of a surface S is an extrinsic measure of curvature; it is the average of it's two principal curvatures: 1 . H ≡ 2 (k1 + k2) Denition 3: The Gaussian Curvature of a point on a surface S is an intrinsic measure of curvature; it is the product of the principal curvatures: of the given point. -
A Chiral Family of Triply-Periodic Minimal Surfaces from the Quartz Network
A chiral family of triply-periodic minimal surfaces from the quartz network Shashank G. Markande 1, Matthias Saba2, G. E. Schroder-Turk¨ 3 and Elisabetta A. Matsumoto 1∗ 1School of Physics, Georgia Tech, Atlanta, GA 30318, USA 2 Department of Physics, Imperial College, London, UK 3School of Engineering and IT, Mathematics and Statistics, Murdoch University, Murdoch, Australia ∗ Author for correspondence: [email protected] May 21, 2018 Abstract We describe a new family of triply-periodic minimal surfaces with hexagonal symmetry, related to the quartz (qtz) and its dual (the qzd net). We provide a solution to the period problem and provide a parametrisation of these surfaces, that are not in the regular class, by the Weierstrass-Enneper formalism. We identified this analytical description of the surface by generating an area-minimising mesh interface from a pair of dual graphs (qtz & qzd) using the generalised Voronoi construction of De Campo, Hyde and colleagues, followed by numerical identification of the flat point structure. This mechanism is not restricted to the specific pair of dual graphs, and should be applicable to a broader set of possible dual graph topologies and their corresponding minimal surfaces, if existent. 1 Introduction The discovery of cubic structures with vivid photonic properties in a wide range of biological systems, such as those responsible for the structural colouring seen in the wing scales of butterflies [1, 2, 3, 4] and in beetle cuticles [5, 6], has driven a renewed interest in mathematics of minimal surfaces – surfaces which, every- where, have zero mean curvature. The optical properties in these structures comes from the periodic nature of their bulk structure. -
Blackfolds, Plane Waves and Minimal Surfaces
Blackfolds, Plane Waves and Minimal Surfaces Jay Armas1;2 and Matthias Blau2 1 Physique Th´eoriqueet Math´ematique Universit´eLibre de Bruxelles and International Solvay Institutes ULB-Campus Plaine CP231, B-1050 Brussels, Belgium 2 Albert Einstein Center for Fundamental Physics, University of Bern, Sidlerstrasse 5, 3012 Bern, Switzerland [email protected], [email protected] Abstract Minimal surfaces in Euclidean space provide examples of possible non-compact horizon ge- ometries and topologies in asymptotically flat space-time. On the other hand, the existence of limiting surfaces in the space-time provides a simple mechanism for making these configura- tions compact. Limiting surfaces appear naturally in a given space-time by making minimal surfaces rotate but they are also inherent to plane wave or de Sitter space-times in which case minimal surfaces can be static and compact. We use the blackfold approach in order to scan for possible black hole horizon geometries and topologies in asymptotically flat, plane wave and de Sitter space-times. In the process we uncover several new configurations, such as black arXiv:1503.08834v2 [hep-th] 6 Aug 2015 helicoids and catenoids, some of which have an asymptotically flat counterpart. In particular, we find that the ultraspinning regime of singly-spinning Myers-Perry black holes, described in terms of the simplest minimal surface (the plane), can be obtained as a limit of a black helicoid, suggesting that these two families of black holes are connected. We also show that minimal surfaces embedded in spheres rather than Euclidean space can be used to construct static compact horizons in asymptotically de Sitter space-times. -
Computation of Minimal Surfaces H
COMPUTATION OF MINIMAL SURFACES H. Terrones To cite this version: H. Terrones. COMPUTATION OF MINIMAL SURFACES. Journal de Physique Colloques, 1990, 51 (C7), pp.C7-345-C7-362. 10.1051/jphyscol:1990735. jpa-00231134 HAL Id: jpa-00231134 https://hal.archives-ouvertes.fr/jpa-00231134 Submitted on 1 Jan 1990 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. COLLOQUE DE PHYSIQUE Colloque C7, supplkment au no23, Tome 51, ler dkcembre 1990 COMPUTATION OF MINIMAL SURFACES H. TERRONES Department of Crystallography, Birkbeck College, University of London, Malet Street, GB- ond don WC~E~HX, Great-Britain Abstract The study of minimal surfaces is related to different areas of science like Mathemat- ics, Physics, Chemistry and Biology. Therefore, it is important to make more accessi- ble concepts which in the past were used only by mathematicians. These concepts are analysed here in order to compute some minimal surfaces by solving the Weierstrass equations. A collected list of Weierstrass functions is given. Knowing these functions we can get important characteristics of a minimal surface like the metric, the unit normal vectors and the Gaussian curvature. 1 Introduction The study of Minimal Surfaces (MS) is not a new field. -
Classical Minimal Surfaces in Euclidean Space by Examples
Classical Minimal Surfaces in Euclidean Space by Examples Geometric and Computational Aspects of the Weierstra¼ representation September 25, 2001 Matthias Weber 2 Contents 1 Introduction 6 2 Basic Di®erential Geometry Of Surfaces 7 2.1 Local Surface Parameterizations . 7 2.2 The Stereographic Projection . 8 2.3 The Normal Vector or Gau¼ Map . 9 3 The Weierstrass Representation 11 3.1 The Gau¼ map . 11 3.2 Harmonic coordinate functions . 12 3.3 Weierstrass data . 13 3.4 The ¯rst examples . 15 3.5 Local analysis at regular points . 17 3.6 The associate family . 19 3.7 The conjugate surface and symmetries . 20 4 Minimal surfaces on Punctured Spheres 22 4.1 Period conditions . 22 4.2 A surface with a planar end and an Enneper end . 23 4.3 A sphere with one planar and two catenoid ends . 24 4.4 The k-Noids of Jorge and Meeks . 25 5 The Scherk Surfaces 28 5.1 The singly periodic Scherk surface . 28 3 5.2 The period conditions . 28 5.3 Changing the angle between the ends . 30 5.4 The doubly periodic Scherk surface . 32 5.5 Singly periodic Scherk surfaces with higher dihedral symmetry 34 5.6 The twist deformation of Scherk's singly periodic surface . 35 5.7 The Schwarz-Christo®el formula . 39 6 Minimal Surfaces De¯ned On Punctured Tori 41 6.1 Complex tori . 41 6.2 Algebraic equations . 42 6.3 Theta functions . 43 6.4 Elliptic functions via Schwarz-Christo®el maps . 44 6.5 The Chen-Gackstatter surface . -
What Are Minimal Surfaces?
What are Minimal surfaces? RUKMINI DEY International Center for Theoretical Sciences (ICTS-TIFR), Bangalore ICTS-TIFR, Bangalore May, 2018 Topology of compact oriented surfaces – genus Sphere, torus, double torus are usual names you may have heard. Sphere and ellipsoids are abundant in nature – for example a ball and an egg. They are topologically “same” – in the sense if they were made out of plasticine, you could have deformed one to the other. Figure 1: Sphere and a glass ball Rukmini Dey µ¶ ToC ·¸ Minimal Surfaces page 2 of 46 Figure 2: Ellipsoids and an egg Figure 3: Tori and donut Rukmini Dey µ¶ ToC ·¸ Minimal Surfaces page 3 of 46 Figure 4: Triple torus and surface of a pretzel Rukmini Dey µ¶ ToC ·¸ Minimal Surfaces page 4 of 46 Handle addition to the sphere –genus Figure 5: Triple torus In fact as the above figure suggests one can construct more and more complicated sur- faces by adding handles to a sphere – the number of handles added is the genus. Rukmini Dey µ¶ ToC ·¸ Minimal Surfaces page 5 of 46 Genus classifies compact oriented surfaces topologically Sphere (genus g =0) is not topologically equivalent to torus (genus g =1) and none of them are topologically equivalent to double torus (genus g =2) and so on. One cannot continuously deform one into the other if the genus-es are different. F Euler’s formula: Divide the surface up into faces (without holes) with a certain number of vertices and edges. Let no. of vertices = V , no. of faces = F , no. of edges = E, no.