Manprit Kaur and Arun Kumar

Similar documents
One Class of Splitting Iterative Schemes

Unbounded solutions of second order discrete BVPs on infinite intervals

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL

Bogoliubov Transformation in Classical Mechanics

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem

arxiv: v1 [math.mg] 25 Aug 2011

Chapter 4. The Laplace Transform Method

Research Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation

Singular perturbation theory

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value

General System of Nonconvex Variational Inequalities and Parallel Projection Method

Robustness analysis for the boundary control of the string equation

ON ASYMPTOTIC FORMULA OF THE PARTITION FUNCTION p A (n)

Notes on Phase Space Fall 2007, Physics 233B, Hitoshi Murayama

Asymptotic behavior of solutions of mixed problem for linear thermo-elastic systems with microtemperatures

A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY

A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho

Approximate Analytical Solution for Quadratic Riccati Differential Equation

Online Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations

The Hassenpflug Matrix Tensor Notation

A Full-Newton Step Primal-Dual Interior Point Algorithm for Linear Complementarity Problems *

A note on the bounds of the error of Gauss Turán-type quadratures

arxiv:math/ v2 [math.ca] 2 May 2006

Introduction to Laplace Transform Techniques in Circuit Analysis

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order


REVERSE HÖLDER INEQUALITIES AND INTERPOLATION

INITIAL-VALUE PROBLEMS FOR HYBRID HADAMARD FRACTIONAL DIFFERENTIAL EQUATIONS

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004

Weber Schafheitlin-type integrals with exponent 1

where F (x) (called the Similarity Factor (SF)) denotes the function

Domain Optimization Analysis in Linear Elastic Problems * (Approach Using Traction Method)

Lecture 10 Filtering: Applied Concepts

Nonlinear Single-Particle Dynamics in High Energy Accelerators

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems

Preemptive scheduling on a small number of hierarchical machines

Hyperbolic Partial Differential Equations

STOCHASTIC EVOLUTION EQUATIONS WITH RANDOM GENERATORS. By Jorge A. León 1 and David Nualart 2 CINVESTAV-IPN and Universitat de Barcelona

c n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova

Problem Set 8 Solutions

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

New bounds for Morse clusters

STOCHASTIC DIFFERENTIAL GAMES:THE LINEAR QUADRATIC ZERO SUM CASE

SOME RESULTS ON INFINITE POWER TOWERS

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle

Dragomir and Gosa type inequalities on b-metric spaces

MATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.:

Chapter 13. Root Locus Introduction

k-connectivity of uniform s-intersection graphs

STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS

Primitive Digraphs with the Largest Scrambling Index

UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE

HELICAL TUBES TOUCHING ONE ANOTHER OR THEMSELVES

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1

Finite Difference Formulae for Unequal Sub- Intervals Using Lagrange s Interpolation Formula

L 2 -transforms for boundary value problems

Digital Control System

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS

III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SUBSTANCES

SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document.

AMS 212B Perturbation Methods Lecture 20 Part 1 Copyright by Hongyun Wang, UCSC. is the kinematic viscosity and ˆp = p ρ 0

The fractional stochastic heat equation on the circle: Time regularity and potential theory

List coloring hypergraphs

On Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces

Reliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay

SOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR

arxiv: v2 [math.nt] 30 Apr 2015

arxiv: v1 [math.nt] 18 Jan 2016

On mild solutions of a semilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach spaces

Multi-dimensional Fuzzy Euler Approximation

Question 1 Equivalent Circuits

Avoiding Forbidden Submatrices by Row Deletions

V = 4 3 πr3. d dt V = d ( 4 dv dt. = 4 3 π d dt r3 dv π 3r2 dv. dt = 4πr 2 dr

arxiv: v1 [math.ca] 23 Sep 2017

INITIAL VALUE PROBLEMS OF FRACTIONAL ORDER HADAMARD-TYPE FUNCTIONAL DIFFERENTIAL EQUATIONS

Research Article Existence for Nonoscillatory Solutions of Higher-Order Nonlinear Differential Equations

Electronic Theses and Dissertations

ON TESTING THE DIVISIBILITY OF LACUNARY POLYNOMIALS BY CYCLOTOMIC POLYNOMIALS Michael Filaseta* and Andrzej Schinzel 1. Introduction and the Main Theo

arxiv: v4 [math.co] 21 Sep 2014

Riemann s Functional Equation is Not Valid and its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS

arxiv:math/ v4 [math.ag] 1 Aug 2007

Lecture 7: Testing Distributions

Laplace Transformation

Factor Analysis with Poisson Output

Coordinate independence of quantum-mechanical q, qq. path integrals. H. Kleinert ), A. Chervyakov Introduction

Laplace Adomian Decomposition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernels

Jump condition at the boundary between a porous catalyst and a homogeneous fluid

Long-term returns in stochastic interest rate models

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES

Transcription:

CUBIC X-SPLINE INTERPOLATORY FUNCTIONS Manprit Kaur and Arun Kumar manpreet2410@gmail.com, arun04@rediffmail.com Department of Mathematic and Computer Science, R. D. Univerity, Jabalpur, INDIA. Abtract: Cubic X-pline function wa introduced to generalize cubic pline function. Here we tudy exitence and error of approximation of cubic pline interpolation having interpolatory condition area matching in each ub-interval. Keyword: Cubic X-pline function, Cubic pline function, Interpolation. AMS Claification: MCS2010 41A15-1. DEFINITIONS AND NOTATIONS : Let : 0 = x 0 < x 1 < x 2 <...< x n = 1, be a knot equence in the interval [0,1]. We denote the ub-interval of the partition by I i = [, ], i = 1,2,...,n. Let α = {α i } n 1 i=1 be a parameter of n-1 real number. A cubic polynomial function C 1 [0,1] i termed a a Cubic X- Spline on the interval [0,1] with knot equence, parameter α = {α i } n 1 i=1, if it atifie the following three condition: i i a Cubic polynomial on each ub-interval [, ], i=1,2,...,n and it i denoted by i. ii C 1 [0,1], that i, for i = 1,2,...,n, i = i+1, i = i+1. and iii i+1 - i = α i [ i+1 - i ], i = 1,2,...,n. We denote uch cla of pline function by 4,,α. 1 139

The X-Spline wa conidered to generalize the conventional pline. Here the econd derivative i allowed to poe dicontinuitie at the knot. The magnitude of thee dicontinuitie are related to thoe of the dicontinuitie in the third derivative by mean of a imple relationhip which introduce one free parameter to each ub-interval. Thi give a choice of the parameter for meeting certain requirement, for example to chooe it to adjut error. The importance of pline function have been conidered in e.g. [1],[3] and [4]. An error analyi of finding the optimal etimate for the uniform norm of approximation of continuou function by interpolating cubic and quadratic X-pline with arbitrary paced knot reult wa obtained in [2] and [5]. It i intereting to have a reult on Cubic X-pline, o that it include the correponding reult of Cubic Spline a a particular cae. Subequently, the reult concerning X-Spline wa obtained by Da [4]. The error of approximation wa alo tudied. In thi paper we conider X-Spline the ame a conidered by Da [4] and replacing the condition of point interpolation by Area Matching. We firt prove the following theorem and it error of approximation i obtained ubequently. THEOREM : Let f be a 1- periodic bounded continuou function and let { } n i=0 be knot point of the partition with - = h for all i. For a given α = {α i } n 1 i=1 the et of non-negative real number, there exit a unique 1-periodic Cubic X-Spline atifying the interpolating condition : 1 xi xdx = fxdx, 2 if h 4α i α i 1 δ6δ + δ 2 + 6 12α i 1 1 + δ + α i 1 δ 2 + 12α i 1 + 2δ + α i δ 2 13 + δ. Proof of the theorem : We write = M i, i = 0,1,...,n-1, and let i = y i, i = 1,2,...,n value of the pline defined at on the i-th interval i.e., in [, ]. It can be een that uch pline can be written on the interval [, ], i = 1,2,...,n a 2 140

3 h 3 x = M i 1 hx x 2 M i hx 2 x +y i 1 x 2 [2x + h] +y i x 2 [2 x + h]. We have 4 h 3 x = M i 1 h[ x 2 2 xx ] M i h[2x x x 2 ] +2y i 1 [ x 2 x{2x + h}] +2y i [ x 2 + x {2 x + h}]. We find that i = i+1 = M i, i = 0, 1,..., n 1. Thi how that continuou at the knot,i.e., x C 1. Further, we ee that 5 h 3 i x = 6M i 1h + 6M i h + 12y i 1 12y i. Thu pline conidered here are X-pline. i.e., we have i+1 i = α i [ i+1 i ], for i = 1, 2,..., n. On ubtitution in the above X-pline equation we find that 6 2hM i+1 h + 3α i 8h 2 M i 2hM i 1 h 3α i = 6[h + 2α i y i+1 y i + h 2α i y i y i 1 ]. Now applying area matching interpolatory condition 1, we have xi fxdx = M i 1 h 2 x x 2 dx M i h 2 x 2 xdx +y i 1 h 3 { x 2 [2x + h]}dx 3 141

i.e., 7 ay. Thi yield, +y i h 3 {x 2 [2 x + h]}dx, xi h 2 fxdx = M i 1 12 M h 2 i 12 + h 2 y i 1 + h 2 y i = F i, 8 F i+1 F i = h2 6 M i h2 12 M i+1 h2 12 M i 1 + h 2 y i+1 y i + h 2 y i y i 1. After eliminating y i in the above equation from 6 and 7, we have 9 W i = pm i 2 + qm i 1 + rm i + M i+1, i = 1, 2,..., n, where W i = 12h 2 [α i 1 h + 2α i F i+1 F i + α i h 2α i 1 F i F i 1 ], p = hα i 4α i α i 1, q = hα i 1 12α i α i 1 + 10hα i, r = 10hα i 1 + 12α i α i 1 + hα i, = hα i 1 + 4α i α i 1. The ytem of equation have unique olution if the coefficient matrix of the above ytem of equation i non-ingular. In order to etablih it non-ingularity, we decompoe the matrix a the following : B = 1 0... 0 0 0 1... 0 0 0 0 1.. 0 0........................ 0 0 0.. 0 1, C = p λ 0 0... 0 0 0 p λ 0... 0 0 0 0 p λ 0.. 0 0.............................. λ 0 0.... 0 p, 4 142

where and λ are determined by the et of the following equation : and λ + p = q + λ = r. Subtituting the value of λ, and r we ee that + λ r = 0. The value of are given by the equation αi 1 + 10α i α i 2 + α i 1 10α i 1 + α i h 12α i α i 1 + 4α i α i 1 + 12α i α i 1 + 4α i α i 1 2 = 0. Let u conider = 1 + δ, for mall poitive δ, i.e., δ < 1 2. The value of the above expreion i 12α i 1 1 δ + α i 1 δ 2 + 12α i 1 2δ + α i δ 2 13 δh +24α i α i 1 δ1 δ + 4α i α i 1 δ, which i poitive. And at = 1 δ, it become 12αi 1 1 + δ + α i 1 δ 2 + 12α i 1 + 2δ + α i δ 2 13 + δ h 4α i α i 1 δ6δ + δ 2 + 6, which i negative if 4α i α i 1 δ6δ + δ 2 + 6 10 h 12α i 1 1 + δ + α i 1 δ 2 + 12α i 1 + 2δ + α i δ 2 13 + δ. on δ. Thu, one of the root of lie in [ 1 δ, 1+δ] under the condition Now we how that the matri diagonally dominant with the diagonal element λ. We have λ = α i 1 + 10α i α i h + 4α i α i 1 3 and thi i negative if h 4α iα i 1 3 α i 1 + 10α i α i. 5 143

Thi i true for [ 1 δ, 1 + δ] if 11 h 12α iα i 1 4α i α i 1 1 + δ α i 1 + 10α i α i 1 δ. therefore Next we ee that from the hypothei 2 p i alo negative. Obviouly i poitive. We have λ p λ p 1 + δ 12 D = 2α i 1 + α i 1 δ 10α i + 11α i δ α i δ 2 h 1 + δ Thi i poitive if 13 h < 8α iα i 1 16α i α i 1 δ + 4α i α i 1 δ 2. 1 + δ 4α i α i 1 2 4δ + δ 2 α i 10 + δ 2 11δ + 2 δα i 1. We ee that the expreion on the right hand ide of the inequality 10 i maller than the expreion on the right hand ide of the inequalitie 11 and 13. Hence the reult i true if h 4α i α i 1 δ6δ + δ 2 + 6 12α i 1 1 + δ + α i 1 δ 2 + 12α i 1 + 2δ + α i δ 2 13 + δ. To viualize the above condition we take, for example, δ = 0.1 in thi cae the above condition become h 2.644α i α i 1 13.21α i 1 + 14.531α i. ERROR OF APPROXIMATION : We write ex = x fx. Since = M i, i = 1,2,...,n, we get e i = M i f i. 6 144

From 9 we find 14 pe i 2 + qe i 1 + re i + e i+1 = W i pf i 2 qf i 1 rf i f i+1, i = 1,2,...,n. We denote the right hand ide of the above expreion by U i, ay. We have U i = 12h 2 [α i 1 h + 2α i F i+1 F i +α i h 2α i 1 F i F i 1 ] hα i 4α i α i 1 f i 2 hα i 1 12α i α i 1 + 10hα i f i 1 10hα i 1 + 12α i α i 1 + hα i f i hα i 1 + 4α i α i 1 f i+1. By Taylor erie expanion, we ee that F i+1 F i = +1 x Hence f ξ i+1 x f i+1 + x f η i x f i dx + h2 U i =h12h 2 +1 x + x f η i x f i dx 2 f i+1 + h2 2 f i. dx f ξ i+1 x f i+1 dxα i 1 + x f ξ i x f i dx + 2 x f η i 1 x f i 1 dxα i +5α i 1 f i+1 4α i 1f i + 5α if i 4α if i 1 α if i 2 α i 1f i 1 +24h 2 α i α i 1 +1 x f ξ i+1 x f i+1 dx + x f η i x f i dx x f ξ i x f i dx 2 x f η i 1 x f i 1 dx +12α i α i 1 f i+1 f i + 4α i α i 1 f i 2 f i+1. 7 145

U i h 12α i 1ω f ; h +4α i f i f i 1 + 72α i α i 1 ω f ; h, + 12α i ω + α i 1 f i+1 f i 1 18α i 1 + α i h + 4α i α i 1 ω f ; h. f ; h + 4α i 1 f i+1 f i + α i f i f i 2 If we take α = max{α i } then Hence We have U i 36α h + 2α ω f ; h. e i = up e i A 1 U i e i 18α i 1 + α i h + 4α i α i 1 D 1 ω f ; h where D i defined in 12. From the condition 1 there i at leat one point x i 1 in [, ] uch that ex i 1 = 0. Thi give that ex = x x e xdx. i 1 Therefore ex h 18α i 1 + α i h + 4α i α i 1 D 1 ω f ; h. Reference : 1. Ahlberg, J.H. Nilon, E.N and Walh, J.L., 1967. The theory of pline and their application, London, Academic Pre. 2. Bujalka A. and Smarzewki R., Quadratic X-Spline, IMA, J.Numer. Analyi, 1982, 2, 37-47. 3. Clenhaw C.W.; Negu B., The Cubic X-pline and it application to interpolation, J. Int. Math. Appl., 221978, 109-119. 4. Da, V.B., Spline interpolation by lower degree polynomial uing area matching condition, Ph.D. Thei, Rani Durgawati Uni. 2004, Jabalpur. 5. Smarzewki R. and Bujalka A.,Uniform Convergence of Cubic and Quadratic X-pline interpolant, IMA, J. Numer. Analyi, 1983 3, 353-372. 8 146