Calculus of Variations: Minimal Surface of Revolution
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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. -
Embedded Minimal Surfaces, Exotic Spheres, and Manifolds with Positive Ricci Curvature
Annals of Mathematics Embedded Minimal Surfaces, Exotic Spheres, and Manifolds with Positive Ricci Curvature Author(s): William Meeks III, Leon Simon and Shing-Tung Yau Source: Annals of Mathematics, Second Series, Vol. 116, No. 3 (Nov., 1982), pp. 621-659 Published by: Annals of Mathematics Stable URL: http://www.jstor.org/stable/2007026 Accessed: 06-02-2018 14:54 UTC JSTOR is a not-for-profit service that helps scholars, researchers, and students discover, use, and build upon a wide range of content in a trusted digital archive. We use information technology and tools to increase productivity and facilitate new forms of scholarship. For more information about JSTOR, please contact [email protected]. Your use of the JSTOR archive indicates your acceptance of the Terms & Conditions of Use, available at http://about.jstor.org/terms Annals of Mathematics is collaborating with JSTOR to digitize, preserve and extend access to Annals of Mathematics This content downloaded from 129.93.180.106 on Tue, 06 Feb 2018 14:54:09 UTC All use subject to http://about.jstor.org/terms Annals of Mathematics, 116 (1982), 621-659 Embedded minimal surfaces, exotic spheres, and manifolds with positive Ricci curvature By WILLIAM MEEKS III, LEON SIMON and SHING-TUNG YAU Let N be a three dimensional Riemannian manifold. Let E be a closed embedded surface in N. Then it is a question of basic interest to see whether one can deform : in its isotopy class to some "canonical" embedded surface. From the point of view of geometry, a natural "canonical" surface will be the extremal surface of some functional defined on the space of embedded surfaces. -
Surfaces Minimales : Theorie´ Variationnelle Et Applications
SURFACES MINIMALES : THEORIE´ VARIATIONNELLE ET APPLICATIONS FERNANDO CODA´ MARQUES - IMPA (NOTES BY RAFAEL MONTEZUMA) Contents 1. Introduction 1 2. First variation formula 1 3. Examples 4 4. Maximum principle 5 5. Calibration: area-minimizing surfaces 6 6. Second Variation Formula 8 7. Monotonicity Formula 12 8. Bernstein Theorem 16 9. The Stability Condition 18 10. Simons' Equation 29 11. Schoen-Simon-Yau Theorem 33 12. Pointwise curvature estimates 38 13. Plateau problem 43 14. Harmonic maps 51 15. Positive Mass Theorem 52 16. Harmonic Maps - Part 2 59 17. Ricci Flow and Poincar´eConjecture 60 18. The proof of Willmore Conjecture 65 1. Introduction 2. First variation formula Let (M n; g) be a Riemannian manifold and Σk ⊂ M be a submanifold. We use the notation jΣj for the volume of Σ. Consider (x1; : : : ; xk) local coordinates on Σ and let @ @ gij(x) = g ; ; for 1 ≤ i; j ≤ k; @xi @xj 1 2 FERNANDO CODA´ MARQUES - IMPA (NOTES BY RAFAEL MONTEZUMA) be the components of gjΣ. The volume element of Σ is defined to be the p differential k-form dΣ = det gij(x). The volume of Σ is given by Z Vol(Σ) = dΣ: Σ Consider the variation of Σ given by a smooth map F :Σ × (−"; ") ! M. Use Ft(x) = F (x; t) and Σt = Ft(Σ). In this section we are interested in the first derivative of Vol(Σt). Definition 2.1 (Divergence). Let X be a arbitrary vector field on Σk ⊂ M. We define its divergence as k X (1) divΣX(p) = hrei X; eii; i=1 where fe1; : : : ; ekg ⊂ TpΣ is an orthonormal basis and r is the Levi-Civita connection with respect to the Riemannian metric g. -
Calculus Terminology
AP Calculus BC Calculus Terminology Absolute Convergence Asymptote Continued Sum Absolute Maximum Average Rate of Change Continuous Function Absolute Minimum Average Value of a Function Continuously Differentiable Function Absolutely Convergent Axis of Rotation Converge Acceleration Boundary Value Problem Converge Absolutely Alternating Series Bounded Function Converge Conditionally Alternating Series Remainder Bounded Sequence Convergence Tests Alternating Series Test Bounds of Integration Convergent Sequence Analytic Methods Calculus Convergent Series Annulus Cartesian Form Critical Number Antiderivative of a Function Cavalieri’s Principle Critical Point Approximation by Differentials Center of Mass Formula Critical Value Arc Length of a Curve Centroid Curly d Area below a Curve Chain Rule Curve Area between Curves Comparison Test Curve Sketching Area of an Ellipse Concave Cusp Area of a Parabolic Segment Concave Down Cylindrical Shell Method Area under a Curve Concave Up Decreasing Function Area Using Parametric Equations Conditional Convergence Definite Integral Area Using Polar Coordinates Constant Term Definite Integral Rules Degenerate Divergent Series Function Operations Del Operator e Fundamental Theorem of Calculus Deleted Neighborhood Ellipsoid GLB Derivative End Behavior Global Maximum Derivative of a Power Series Essential Discontinuity Global Minimum Derivative Rules Explicit Differentiation Golden Spiral Difference Quotient Explicit Function Graphic Methods Differentiable Exponential Decay Greatest Lower Bound Differential -
Generating Carbon Schwarzites Via Zeolite-Templating
Generating carbon schwarzites via zeolite-templating Efrem Brauna, Yongjin Leeb,c, Seyed Mohamad Moosavib, Senja Barthelb, Rocio Mercadod, Igor A. Baburine, Davide M. Proserpiof,g, and Berend Smita,b,1 aDepartment of Chemical and Biomolecular Engineering, University of California, Berkeley, CA 94720; bInstitut des Sciences et Ingenierie´ Chimiques (ISIC), Valais, Ecole´ Polytechnique Fed´ erale´ de Lausanne (EPFL), CH-1951 Sion, Switzerland; cSchool of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China; dDepartment of Chemistry, University of California, Berkeley, CA 94720; eTheoretische Chemie, Technische Universitat¨ Dresden, 01062 Dresden, Germany; fDipartimento di Chimica, Universita` degli Studi di Milano, 20133 Milan, Italy; and gSamara Center for Theoretical Materials Science (SCTMS), Samara State Technical University, Samara 443100, Russia Edited by Monica Olvera de la Cruz, Northwestern University, Evanston, IL, and approved July 9, 2018 (received for review March 25, 2018) Zeolite-templated carbons (ZTCs) comprise a relatively recent ZTC can be seen as a schwarzite (24–28). Indeed, the experi- material class synthesized via the chemical vapor deposition of mental properties of ZTCs are exactly those which have been a carbon-containing precursor on a zeolite template, followed predicted for schwarzites, and hence ZTCs are considered as by the removal of the template. We have developed a theoret- promising materials for the same applications (21, 22). As we ical framework to generate a ZTC model from any given zeolite will show, the similarity between ZTCs and schwarzites is strik- structure, which we show can successfully predict the structure ing, and we explore this similarity to establish that the theory of known ZTCs. We use our method to generate a library of of schwarzites/TPMSs is a useful concept to understand ZTCs. -
Minimal Surfaces Saint Michael’S College
MINIMAL SURFACES SAINT MICHAEL’S COLLEGE Maria Leuci Eric Parziale Mike Thompson Overview What is a minimal surface? Surface Area & Curvature History Mathematics Examples & Applications http://www.bugman123.com/MinimalSurfaces/Chen-Gackstatter-large.jpg What is a Minimal Surface? A surface with mean curvature of zero at all points Bounded VS Infinite A plane is the most trivial minimal http://commons.wikimedia.org/wiki/File:Costa's_Minimal_Surface.png surface Minimal Surface Area Cube side length 2 Volume enclosed= 8 Surface Area = 24 Sphere Volume enclosed = 8 r=1.24 Surface Area = 19.32 http://1.bp.blogspot.com/- fHajrxa3gE4/TdFRVtNB5XI/AAAAAAAAAAo/AAdIrxWhG7Y/s160 0/sphere+copy.jpg Curvature ~ rate of change More Curvature dT κ = ds Less Curvature History Joseph-Louis Lagrange first brought forward the idea in 1768 Monge (1776) discovered mean curvature must equal zero Leonhard Euler in 1774 and Jean Baptiste Meusiner in 1776 used Lagrange’s equation to find the first non- trivial minimal surface, the catenoid Jean Baptiste Meusiner in 1776 discovered the helicoid Later surfaces were discovered by mathematicians in the mid nineteenth century Soap Bubbles and Minimal Surfaces Principle of Least Energy A minimal surface is formed between the two boundaries. The sphere is not a minimal surface. http://arxiv.org/pdf/0711.3256.pdf Principal Curvatures Measures the amount that surfaces bend at a certain point Principal curvatures give the direction of the plane with the maximal and minimal curvatures http://upload.wikimedia.org/wi -
Schwarz' P and D Surfaces Are Stable
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Differential Geometry and its Applications 2 (1992) 179-195 179 North-Holland Schwarz’ P and D surfaces are stable Marty Ross Department of Mathematics, Rice University, Houston, TX 77251, U.S.A. Communicated by F. J. Almgren, Jr. Received 30 July 1991 Ross, M., Schwarz’ P and D surfaces are stable, Diff. Geom. Appl. 2 (1992) 179-195. Abstract: The triply-periodic minimal P surface of Schwarz is investigated. It is shown that this surface is stable under periodic volume-preserving variations. As a consequence, the conjugate D surface is also stable. Other notions of stability are discussed. Keywords: Minimal surface, stable, triply-periodic, superfluous. MS classijication: 53A. 1. Introduction The existence of naturally occuring periodic phenomena is of course well known, Recently there have been suggestions that certain periodic behavior, including surface interfaces, might be suitably modelled by triply-periodic minimal and constant mean curvature surfaces (see [18, p. 2401, [l], [2] and th e references cited there). This is not unreasonable as such surfaces are critical points for a simple functional, the area functional. However, a naturally occuring surface ipso facto exhibits some form of stability, and thus we are led to consider as well the second variation of any candidate surface. Given an oriented immersed surface M = z(S) 5 Iw3, we can consider a smooth variation Mt = z(S,t) of M, and the resulting effect upon the area, A(t). M = MO is minimal if A’(0) = 0 for every compactly supported variation which leaves dM fixed. -
MINIMAL SURFACES THAT GENERALIZE the ENNEPER's SURFACE 1. Introduction
Novi Sad J. Math. Vol. 40, No. 2, 2010, 17-22 MINIMAL SURFACES THAT GENERALIZE THE ENNEPER'S SURFACE Dan Dumitru1 Abstract. In this article we give the construction of some minimal surfaces in the Euclidean spaces starting from the Enneper's surface. AMS Mathematics Subject Classi¯cation (2000): 53A05 Key words and phrases: Enneper's surface, minimal surface, curvature 1. Introduction We start with the well-known Enneper's surface which is de¯ned in the 2 3 u3 3-dimensional Cartesian by the application x : R ! R ; x(u; v) = (u ¡ 3 + 2 v3 2 2 2 uv ; v¡ 3 +vu ; u ¡v ): The point (u; v) is mapped to (f(u; v); g(u; v); h(u; v)), which is a point on Enneper's surface [2]. This surface has self-intersections and it is one of the ¯rst examples of minimal surface. The fact that Enneper's surface is minimal is a consequence of the following theorem: u3 2 Theorem 1.1. [1] Consider the Enneper's surface x(u; v) = (u ¡ 3 + uv ; v ¡ v3 2 2 2 3 + vu ; u ¡ v ): Then: a) The coe±cients of the ¯rst fundamental form are (1.1) E = G = (1 + u2 + v2)2;F = 0: b) The coe±cients of the second fundamental form are (1.2) e = 2; g = ¡2; f = 0: c) The principal curvatures are 2 2 (1.3) k = ; k = ¡ : 1 (1 + u2 + v2)2 2 (1 + u2 + v2)2 Eg+eG¡2F f It follows that the mean curvature H = EG¡F 2 is zero, which means the Enneper's surface is minimal. -
Bour's Theorem in 4-Dimensional Euclidean
Bull. Korean Math. Soc. 54 (2017), No. 6, pp. 2081{2089 https://doi.org/10.4134/BKMS.b160766 pISSN: 1015-8634 / eISSN: 2234-3016 BOUR'S THEOREM IN 4-DIMENSIONAL EUCLIDEAN SPACE Doan The Hieu and Nguyen Ngoc Thang Abstract. In this paper we generalize 3-dimensional Bour's Theorem 4 to the case of 4-dimension. We proved that a helicoidal surface in R 4 is isometric to a family of surfaces of revolution in R in such a way that helices on the helicoidal surface correspond to parallel circles on the surfaces of revolution. Moreover, if the surfaces are required further to have the same Gauss map, then they are hyperplanar and minimal. Parametrizations for such minimal surfaces are given explicitly. 1. Introduction Consider the deformation determined by a family of parametric surfaces given by Xθ(u; v) = (xθ(u; v); yθ(u; v); zθ(u; v)); xθ(u; v) = cos θ sinh v sin u + sin θ cosh v cos u; yθ(u; v) = − cos θ sinh v cos u + sin θ cosh v sin u; zθ(u; v) = u cos θ + v sin θ; where −π < u ≤ π; −∞ < v < 1 and the deformation parameter −π < θ ≤ π: A direct computation shows that all surfaces Xθ are minimal, have the same first fundamental form and normal vector field. We can see that X0 is the helicoid and Xπ=2 is the catenoid. Thus, locally the helicoid and catenoid are isometric and have the same Gauss map. Moreover, helices on the helicoid correspond to parallel circles on the catenoid. -
Minimal Surfaces, a Study
Alma Mater Studiorum · Università di Bologna SCUOLA DI SCIENZE Corso di Laurea in Matematica MINIMAL SURFACES, A STUDY Tesi di Laurea in Geometria Differenziale Relatore: Presentata da: Dott.ssa CLAUDIA MAGNAPERA ALESSIA CATTABRIGA VI Sessione Anno Accademico 2016/17 Abstract Minimal surfaces are of great interest in various fields of mathematics, and yet have lots of application in architecture and biology, for instance. It is possible to list different equivalent definitions for such surfaces, which correspond to different approaches. In the following thesis we will go through some of them, concerning: having mean cur- vature zero, being the solution of Lagrange’s partial differential equation, having the harmonicity property, being the critical points of the area functional, being locally the least-area surface with a given boundary and proving the existence of a solution of the Plateau’s problem. Le superfici minime, sono di grande interesse in vari campi della matematica, e parec- chie sono le applicazioni in architettura e in biologia, ad esempio. È possibile elencare diverse definizioni equivalenti per tali superfici, che corrispondono ad altrettanti approcci. Nella seguente tesi ne affronteremo alcuni, riguardanti: la curvatura media, l’equazione differenziale parziale di Lagrange, la proprietà di una funzione di essere armonica, i punti critici del funzionale di area, le superfici di area minima con bordo fissato e la soluzione del problema di Plateau. 2 Introduction The aim of this thesis is to go through the classical minimal surface theory, in this specific case to state six equivalent definitions of minimal surface and to prove the equiv- alence between them. -
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. -
Surface Area of a Sphere in This Example We Will Complete the Calculation of the Area of a Surface of Rotation
Surface Area of a Sphere In this example we will complete the calculation of the area of a surface of rotation. If we’re going to go to the effort to complete the integral, the answer should be a nice one; one we can remember. It turns out that calculating the surface area of a sphere gives us just such an answer. We’ll think of our sphere as a surface of revolution formed by revolving a half circle of radius a about the x-axis. We’ll be integrating with respect to x, and we’ll let the bounds on our integral be x1 and x2 with −a ≤ x1 ≤ x2 ≤ a as sketched in Figure 1. x1 x2 Figure 1: Part of the surface of a sphere. Remember that in an earlier example we computed the length of an infinites imal segment of a circular arc of radius 1: r 1 ds = dx 1 − x2 In this example we let the radius equal a so that we can see how the surface area depends on the radius. Hence: p y = a2 − x2 −x y0 = p a2 − x2 r x2 ds = 1 + dx a2 − x2 r a2 − x2 + x2 = dx a2 − x2 r a2 = dx: 2 2 a − x The formula for the surface area indicated in Figure 1 is: Z x2 Area = 2πy ds x1 1 ds y z }| { x r Z 2 z }| { a2 p 2 2 = 2π a − x dx 2 2 x1 a − x Z x2 a p 2 2 = 2π a − x p dx 2 2 x1 a − x Z x2 = 2πa dx x1 = 2πa(x2 − x1): Special Cases When possible, we should test our results by plugging in values to see if our answer is reasonable.