GEOMETRICAL DESCRIPTION OF ONE SURFACE IN ECONOMY

Similar documents
Visualisations of Gussian and Mean Curvatures by Using Mathematica and webmathematica

Lecture 9: 3.4 The Geometry of Linear Systems

THE DIFFERENTIAL GEOMETRY OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE

Vectors in Rn un. This definition of norm is an extension of the Pythagorean Theorem. Consider the vector u = (5, 8) in R 2

Lecture 3. (2) Last time: 3D space. The dot product. Dan Nichols January 30, 2018

OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIELD OF A POLYHEDRAL BODY WITH LINEARLY INCREASING DENSITY 1

Differential Geometry. Peter Petersen

Classify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled.

Invariant surfaces in H 2 R with constant (mean or Gauss) curvature

CS 450: COMPUTER GRAPHICS VECTORS SPRING 2016 DR. MICHAEL J. REALE

When Closed Graph Manifolds are Finitely Covered by Surface Bundles Over S 1

arxiv: v1 [math.co] 25 Sep 2016

Spring, 2008 CIS 610. Advanced Geometric Methods in Computer Science Jean Gallier Homework 1, Corrected Version

The Cross Product of Two Vectors in Space DEFINITION. Cross Product. u * v = s ƒ u ƒƒv ƒ sin ud n

The Real Stabilizability Radius of the Multi-Link Inverted Pendulum

Effects of Soil Spatial Variability on Bearing Capacity of Shallow Foundations

MATH2715: Statistical Methods

The Brauer Manin obstruction

Numerical Model for Studying Cloud Formation Processes in the Tropics

Convex Hypersurfaces of Constant Curvature in Hyperbolic Space

Research Article Uniqueness of Solutions to a Nonlinear Elliptic Hessian Equation

Existence of HCMU metrics on higher genus Riemann surfaces

Study of the diffusion operator by the SPH method

Linear Strain Triangle and other types of 2D elements. By S. Ziaei Rad

Study on the Mathematic Model of Product Modular System Orienting the Modular Design

Reduction of over-determined systems of differential equations

Change of Variables. f(x, y) da = (1) If the transformation T hasn t already been given, come up with the transformation to use.

The SISTEM method. LOS ascending

Geometry of Span (continued) The Plane Spanned by u and v

Graphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007

Math 144 Activity #10 Applications of Vectors

6.4 VECTORS AND DOT PRODUCTS

u P(t) = P(x,y) r v t=0 4/4/2006 Motion ( F.Robilliard) 1

ON THE PERFORMANCE OF LOW

A GAP PROGRAM FOR COMPUTING THE HOSOYA POLYNOMIAL AND WIENER INDEX OF NANO STRUCTURES

Exercise 4. An optional time which is not a stopping time

On the uniqueness of Lp-Minkowski problems: The constant p-curvature case in R^3

Complexity of the Cover Polynomial

L 1 -smoothing for the Ornstein-Uhlenbeck semigroup

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING

1 Differential Equations for Solid Mechanics

We automate the bivariate change-of-variables technique for bivariate continuous random variables with

ANOVA INTERPRETING. It might be tempting to just look at the data and wing it

Exercise 1 (Formula for connection 1-forms) Using the first structure equation, show that

Trace-class Monte Carlo Markov Chains for Bayesian Multivariate Linear Regression with Non-Gaussian Errors

CALCULUS ON MANIFOLDS. 1. Riemannian manifolds Recall that for any smooth manifold M, dim M = n, the union T M =

Solving the Lienard equation by differential transform method

Affine Invariant Total Variation Models

Sources of Non Stationarity in the Semivariogram

Suyeon Shin* and Woonjae Hwang**

Section 7.4: Integration of Rational Functions by Partial Fractions

CRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE. Jingbo Xia

G. Mahadevan 1 Selvam Avadayappan 2 V. G. Bhagavathi Ammal 3 T. Subramanian 4

Modelling, Simulation and Control of Quadruple Tank Process

Applying Fuzzy Set Approach into Achieving Quality Improvement for Qualitative Quality Response

On Theory of logarithmic Poisson Cohomology

Lesson 81: The Cross Product of Vectors

Restricted Three-Body Problem in Different Coordinate Systems

IN this paper we consider simple, finite, connected and

Euler Characteristic of Two-Dimensional Manifolds

CONSIDER an array of N sensors (residing in threedimensional. Investigating Hyperhelical Array Manifold Curves Using the Complex Cartan Matrix

FEA Solution Procedure

Complementing the Lagrangian Density of the E. M. Field and the Surface Integral of the p-v Vector Product

EE2 Mathematics : Functions of Multiple Variables

Notes on Cartan s Method of Moving Frames

Review of Matrices and Vectors 1/45

Approximate Solution for the System of Non-linear Volterra Integral Equations of the Second Kind by using Block-by-block Method

CONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4

Restricted cycle factors and arc-decompositions of digraphs. J. Bang-Jensen and C. J. Casselgren

Mean Value Formulae for Laplace and Heat Equation

Discussion Papers Department of Economics University of Copenhagen

The Replenishment Policy for an Inventory System with a Fixed Ordering Cost and a Proportional Penalty Cost under Poisson Arrival Demands

1. Geometry of the unit tangent bundle

A Characterization of Interventional Distributions in Semi-Markovian Causal Models

Elements of Coordinate System Transformations

Available online at ScienceDirect. Procedia Engineering 150 (2016 )

The Open Civil Engineering Journal

Digital Image Processing. Lecture 8 (Enhancement in the Frequency domain) Bu-Ali Sina University Computer Engineering Dep.

The Heat Equation and the Li-Yau Harnack Inequality

The spreading residue harmonic balance method for nonlinear vibration of an electrostatically actuated microbeam

1 The space of linear transformations from R n to R m :

3.3 Operations With Vectors, Linear Combinations

Application of Fractional Fourier Transform in Non-stationary Signal Time Frequency Analysis

The Faraday Induction Law and Field Transformations in Special Relativity

A Computational Study with Finite Element Method and Finite Difference Method for 2D Elliptic Partial Differential Equations

Concept of Stress at a Point

Geometry of the Legendre transformation

Differential Geometry of Surfaces

On a class of topological groups. Key Words: topological groups, linearly topologized groups. Contents. 1 Introduction 25

Bäcklund transformation, multiple wave solutions and lump solutions to a (3 + 1)-dimensional nonlinear evolution equation

Solving a Class of PDEs by a Local Reproducing Kernel Method with An Adaptive Residual Subsampling Technique

VIBRATION MEASUREMENT UNCERTAINTY AND RELIABILITY DIAGNOSTICS RESULTS IN ROTATING SYSTEMS

The New (2+1)-Dimensional Integrable Coupling of the KdV Equation: Auto-Bäcklund Transformation and Non-Travelling Wave Profiles

INTERIOR CURVATURE ESTIMATES AND THE ASYMPTOTIC PLATEAU PROBLEM IN HYPERBOLIC SPACE

A New Method for Calculating of Electric Fields Around or Inside Any Arbitrary Shape Electrode Configuration

Krauskopf, B., Lee, CM., & Osinga, HM. (2008). Codimension-one tangency bifurcations of global Poincaré maps of four-dimensional vector fields.

Discussion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli

PHASE PLANE DIAGRAMS OF DIFFERENCE EQUATIONS. 1. Introduction

Subcritical bifurcation to innitely many rotating waves. Arnd Scheel. Freie Universitat Berlin. Arnimallee Berlin, Germany

is constant [3]. In a recent work, T. IKAWA proved the following theorem for helices on a Lorentzian submanifold [1].

Transcription:

GOMTRICAL DSCRIPTION OF ON SURFAC IN CONOMY a Kaňkoá Abstract The principal object of this paper is the reglar parametric srface M in R defined by the formla The geometrical description methods we are going to se are based on Cartan s moing frame method and on Weingarten map The stdied map is reglar Let : U R R M U R where U is an open neighborhood of the point q= and p= V M R open neighborhood in R of the point where V is an Key words: Cartan s moing frame method Weingarten map Gassian cratre Main cratre moing frame JL Code: C00 Introdction Let U R is an open neighborhood of a point U and means that the rank of Jacobian matri J A sbset dimensional srface in R and the map : U R is gien by the formla R if for each M : U R is a reglar map which M R is called reglar two there eist an open neighborhood V of V of an open sbset U R onto M V The map Now we hae to constrct the moing frame and orthonormal moing frame which is the base for Cartan method The net method is based on Weingarten mapping Cartan s method The moing frame has the form 554

555 0 0 n Symbols and are sed instead of etc Vectors and form the basis of the tangent space T M On T M we can constrct moing frame As the ectors and are tangent ectors of M the n is a normal ector Vector N is the nit normal ector Orthonormal moing frame has the form 0 8 Differential d eqals d d 0 8 0 8 d Differential form is:

55 d d d 8 8 d d d d We hae

557 The differential form is d d d Frther we try to constrct differential form Differential form is d d Now we will constrct forms and d d d d d d d

d d d d d The eterior prodct of forms and is d d d d from which follows d d For control we hae d 8 0 8 0 d d 8 d d 558

d d d The reslt is d d The differential of the form d is essential for calclation of the Gass cratre Let s stdy the following eqations: d ω ω ω d d d d d d d d d d d K θ θ d 55

50 where K is the Gassian cratre We hae K Weingarten method qation j i ij j i gies j i d which means M T M T We hae We hae system of two eqations for Thanks to Cramer s rle we obtain 8 8 Frther we hae

5 8 8 8 8 8 4 We hae 8 4 4 Analogically we obtain

5 8 8 D

5 Weingarten map can be represented by the matri W W As W and W we obtain: W

54 det W As was gien before the Gassian cratre is K Frther we obtain

4 4 4 4 4 8 7 H t r W 7 So the trace of the matri W is 4 4 4 54 8 7 5 H trw 54 8 4 7 5 Conclsion By the method of moing frame we reached that the reslt of Gassian cratre is K By the method of Weingarten mapping we reached that the reslt of Main cratre is H tr W References Bochner S A new iewpoint in differential geometry Canadian Jornal of mathematics Jornal Canadian de Mathematiqes 5: 40 470 Breš J Kaňka M Some Conditions for a Srface in Mathematica Bohemica 4 4 s 7 7 4 to be a Part of the Sphere Cartan É Oeres complètes-partie I Vol Paris: Gathier-Villars 5 Cartan É Oeres complètes-partie II Vol Paris: Gathier-Villars 5 Cartan É Oeres complètes-partie II Vol Paris: Gathier-Villars 5 Cartan É Oeres complètes-partie III Vol Paris: Gathier-Villars 55 S 55

Cartan É Oeres complètes-partie III Vol Paris: Gathier-Villars 55 Kaňka M ample of Basic Strctre qations of Riemannian Manifolds Mnds Symbolics 5 s 57 Chern SS Some new Viewpoints in Differential geometry in the large Blletin of the American mathematical Society 4: 0 Kobayashi S Nomiz K Fondations of Differential Geometry New York: Wiley Interscience Kostant B On differential geometry and homogeneos space Proceedings of the national Academy of sciences of the United States of America 5: 58 Kostant B On differential geometry and homogeneos space Proceedings of the national Academy of sciences of the United States of America 5: 54 57 Nomiz K Lie Grops and Differential Geometry Tokyo: The Mathematical Society of Japan 5 Rach H A contribtion to differential geometry in the large Annals of Mathematics :8 55 Sternberg S Lectres on Differential Geometry nglewood Cliffs NJ: Prentice-Hall 4 Contact a Kaňkoá Uniersity of conomics Prage W Chrchill Sq 4 0 7 Prage Czech Repblic kankoa@secz 5