Fractional Fourier Series with Applications

Similar documents
Suggested Solution for Pure Mathematics 2011 By Y.K. Ng (last update: 8/4/2011) Paper I. (b) (c)

On Absolute Indexed Riesz Summability of Orthogonal Series

Extension of Hardy Inequality on Weighted Sequence Spaces

EE757 Numerical Techniques in Electromagnetics Lecture 9

Existence Of Solutions For Nonlinear Fractional Differential Equation With Integral Boundary Conditions

ON PRODUCT SUMMABILITY OF FOURIER SERIES USING MATRIX EULER METHOD

A new approach to Kudryashov s method for solving some nonlinear physical models

Fourier Series and Applications

Desigualdades integrales fraccionales y sus q-análogos

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1)

ONE RANDOM VARIABLE F ( ) [ ] x P X x x x 3

SLOW INCREASING FUNCTIONS AND THEIR APPLICATIONS TO SOME PROBLEMS IN NUMBER THEORY

An arithmetic interpretation of generalized Li s criterion

Week 8 Lecture 3: Problems 49, 50 Fourier analysis Courseware pp (don t look at French very confusing look in the Courseware instead)

EXTERNALLY AND INTERNALLY POSITIVE TIME- VARYING LINEAR SYSTEMS

ON BILATERAL GENERATING FUNCTIONS INVOLVING MODIFIED JACOBI POLYNOMIALS

VISCOSITY APPROXIMATION TO COMMON FIXED POINTS OF kn- LIPSCHITZIAN NONEXPANSIVE MAPPINGS IN BANACH SPACES

Boundary Value Problems of Conformable. Fractional Differential Equation with Impulses

). So the estimators mainly considered here are linear

Solution of Laplace s Differential Equation and Fractional Differential Equation of That Type

Coefficient Inequalities for Certain Subclasses. of Analytic Functions

SUMMATION OF INFINITE SERIES REVISITED

Supplement: Gauss-Jordan Reduction

K3 p K2 p Kp 0 p 2 p 3 p

NATURAL TRANSFORM AND SOLUTION OF INTEGRAL EQUATIONS FOR DISTRIBUTION SPACES

On a New Subclass of Multivalant Functions Defined by Al-Oboudi Differential Operator

Forced Oscillation of Nonlinear Impulsive Hyperbolic Partial Differential Equation with Several Delays

Meromorphic Functions Sharing Three Values *

Summer MA Lesson 4 Section P.3. such that =, denoted by =, is the principal square root

Transient Solution of the M/M/C 1 Queue with Additional C 2 Servers for Longer Queues and Balking

Fractional Order EOQ Model with Linear Trend of Time-Dependent Demand

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type

Common Fixed Point Theorem in Intuitionistic Fuzzy Metric Space via Compatible Mappings of Type (K)

ERROR ESTIMATES FOR APPROXIMATING THE FOURIER TRANSFORM OF FUNCTIONS OF BOUNDED VARIATION

Comparison between Fourier and Corrected Fourier Series Methods

Institute of Actuaries of India

Local Fractional Kernel Transform in Fractal Space and Its Applications

Degree of Approximation of Conjugate of Signals (Functions) by Lower Triangular Matrix Operator

EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D. S. Palimkar

Department of Mathematical and Statistical Sciences University of Alberta

An Extension of Hermite Polynomials

In an algebraic expression of the form (1), like terms are terms with the same power of the variables (in this case

NEIGHBOURHOODS OF A CERTAIN SUBCLASS OF STARLIKE FUNCTIONS. P. Thirupathi Reddy. E. mail:

On computing two special cases of Gauss hypergeometric function

MATRIX ALGEBRA, Systems Linear Equations

Online Supplement to Reactive Tabu Search in a Team-Learning Problem

ON SOME FRACTIONAL PARABOLIC EQUATIONS DRIVEN BY FRACTIONAL GAUSSIAN NOISE

BE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion

Application of Fixed Point Theorem of Convex-power Operators to Nonlinear Volterra Type Integral Equations

The analysis of the method on the one variable function s limit Ke Wu

BIBECHANA A Multidisciplinary Journal of Science, Technology and Mathematics

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws.

Elzaki transform and the decomposition method for nonlinear fractional partial differential equations

Numerical methods for ordinary differential equations

HOMEWORK 6 - INTEGRATION. READING: Read the following parts from the Calculus Biographies that I have given (online supplement of our textbook):

BINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =

DERIVING THE DEMAND CURVE ASSUMING THAT THE MARGINAL UTILITY FUNCTIONS ARE LINEAR

Some Properties of Semi-E-Convex Function and Semi-E-Convex Programming*

MATH 118 HW 7 KELLY DOUGAN, ANDREW KOMAR, MARIA SIMBIRSKY, BRANDEN LASKE

Generalization of Quasi-Differentiable Maps

Dynamic response under moving concentrated loads of non uniform rayleigh beam resting on pasternak foundation

Special Functions. Leon M. Hall. Professor of Mathematics University of Missouri-Rolla. Copyright c 1995 by Leon M. Hall. All rights reserved.

Integration and Differentiation

Reinforcement Learning

Journal of Quality Measurement and Analysis JQMA 12(1-2) 2016, Jurnal Pengukuran Kualiti dan Analisis

Extended Laguerre Polynomials

Improvement Over General And Wider Class of Estimators Using Ranked Set Sampling

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T.

LIPSCHITZ ESTIMATES FOR MULTILINEAR COMMUTATOR OF MARCINKIEWICZ OPERATOR

5.1-The Initial-Value Problems For Ordinary Differential Equations

Physics 232 Exam I Feb. 14, 2005

Functions, Limit, And Continuity

Integral Operator Defined by k th Hadamard Product

Taylor Polynomials. The Tangent Line. (a, f (a)) and has the same slope as the curve y = f (x) at that point. It is the best

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION

7. Discrete Fourier Transform (DFT)

LOCUS 1. Definite Integration CONCEPT NOTES. 01. Basic Properties. 02. More Properties. 03. Integration as Limit of a Sum

CHAPTER 5: FOURIER SERIES PROPERTIES OF EVEN & ODD FUNCTION PLOT PERIODIC GRAPH

r = cos θ + 1. dt ) dt. (1)

A Note on a Characterization of J-Shaped Distribution. by Truncated Moment

CSE 5311 Notes 12: Matrices

Classifications of Ordered Semigroups in Terms of Bipolar Fuzzy Bi-Ideals

An Introduction to Trigonometry

Chapter 7 Infinite Series

STK4080/9080 Survival and event history analysis

Fourier series. (sine and cosine)( ) ... : w h ere 2 (1 1)

8.3 THE TRIGONOMETRIC FUNCTIONS. skipped 8.4 THE ALGEBRAIC COMPLETENESS OF THE COMPLEX FIELD. skipped 8.5 FOURIER SERIES

UNIVERSITY OF BRISTOL. Examination for the Degrees of B.Sc. and M.Sci. (Level C/4) ANALYSIS 1B, SOLUTIONS MATH (Paper Code MATH-10006)

APPLICATION OF DIFFERENCE EQUATIONS TO CERTAIN TRIDIAGONAL MATRICES

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k.

Extremal graph theory II: K t and K t,t

Basic Results in Functional Analysis

A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY

RESEARCH PAPERS FACULTY OF MATERIALS SCIENCE AND TECHNOLOGY IN TRNAVA SLOVAK UNIVERSITY OF TECHNOLOGY IN BRATISLAVA

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation.

1. Six acceleration vectors are shown for the car whose velocity vector is directed forward. For each acceleration vector describe in words the

MA 131 Lecture Notes Calculus Sections 1.5 and 1.6 (and other material)

GENERALIZED OSTROWSKI TYPE INEQUALITIES FOR FUNCTIONS WHOSE LOCAL FRACTIONAL DERIVATIVES ARE GENERALIZED s-convex IN THE SECOND SENSE

Transcription:

Aeric Jourl o Couiol d Alied Mheics 4, 4(6): 87-9 DOI: 593/jjc446 Frciol Fourier Series wih Alicios Abu Hd I, Khlil R * Uiversiy o Jord, Jord Absrc I his er, we iroduce coorble rciol Fourier series We use such series o solve ceri ril rciol diereil equios Keywords Frciol ourier series, Coorble rciol derivive Iroducio Fourier series is oe o he os ior ools i lied scieces For exle oe c solve ril diereil equios usi Fourier series Furher oe c id he su o ceri uericl series usi Fourier series Frciol ril diereil equios ered o hve y licios i hysics d eieeri There re y deiiios o rciol derivive Oe o he os rece oes is he coorl rciol derivive [5] Recely [], rciol Tylor ower series ws iroduced, d beuiul heory ws lyed here However, o work is doe o rciol Fourier series, houh here is soe work o rciol ourier rsor The i o his er is o iroduce coorble rciol Fourier series As licio we solve soe rciol ril diereil equios usi rciol Fourier series Foe ore licios o coorble rciol derivive we reeree o [-4] Bsics o Coorble Frciol Derivive The subjec o rciol derivive is s old s clculus I 5 d 695, L Hoil sked i he exressio hs y 5 dx ei Sice he, y reserchers hve bee ryi o eerlize he coce o he usul derivive o rciol derivives These dys, y deiiios or hec rciol derivive re vilble Mos o hese deiiios use ierl or The os oulr deiiios re: (i) Rie - Liouville Deiiio: I is osiive * Corresodi uhor: roshdi@juedujo (Khlil R) Published olie h://jourlsubor/jc Coyrih 4 Scieiic & Acdeic Publishi All Rihs Reserved ieer d [, ) ive by, he h derivive o is d ( x) Γ( ) d ( x) (ii) Cuo Deiiio For [, ) D dx derivive o is +, he ( ) ( x) D ( ) dx Γ( ) x + Now, ll deiiios re eed o sisy he usul roeries o he sdrd derivive The oly roery iheried by ll deiiios o rciol derivive is he lieriy roery However, he ollowi re he se- bcks o oe deiiio or oher: (i) The Rie-Liouville derivive does o sisy D ( D or he Cuo derivive), i is o url uber (ii) All rciol derivives do o sisy he kow roduc rule: D ( ) D ( ) + D ( ) (iii) All rciol derivives do o sisy he kow quoie rule: D D D / (iv) All rciol derivives do o sisy he chi rule: ( D ) ο (v) All rciol derivives do o sisy:

88 Abu Hd I e l: Frciol Fourier Series wih Alicios + i eerl D D D (vi) Cuo deiiio ssues h he ucio is diereible T λ, or ll cos ucios (vii) λ I ew deiiio clled coorble rciol derivive ws iroduced Deiiio I > he we deie T [ ] ([ ] ) [ ] ( + ε ) ( ) li, ε ε where [ ] is he ceili o We cll T he rciol derivive o o order We shll wrie ( ) T ( ) The ew deiiio sisies: T ( b ) T bt ( ) T ( λ ), or ll cos ucios or + +, or ll b, λ Furher, or (,] d, be -diereible oi, wih The 3 T ( ) T ( ) + T ( ) T ( ) T ( ) 4 T We lis here he rciol derivives o ceri ucios, or he urose o cori he resuls o he ew deiiio wih he usul deiiio o he derivive: T ( ) 3 4 T si cos T cos si T e e O lei i hese derivives, we e he corresodi ordiry derivives Oe should oice h ucio could be -diereible oi bu o diereible, or exle, ke T The Hece T Bu T ( ) does o exis This is o he cse or he kow clssicl rciol derivives 3 Frciol Fourier Series Le <, d ϕ :[, ) R be deied by d [ [ ϕ :, ) R be y ucio Le :, ) R be deied by ϕ is clled -eriodicl For exle, i cos, he cos Deiiio 3 A ucio wih eriod i or ll [, ) ( ϕ ) ϕ + As exle, cos eriod is -eriodic wih Deiiio 3 Two ucios, h re clled -orhool o [,b ] i b hd Exles 3 cos d cos, Proo Pu x d The dx d -orhool o Furher, whe, x, d whe Hece ( ) re, x coscos cos( x)cos( x) dx d

Aeric Jourl o Couiol d Alied Mheics 4, 4(6): 87-9 89 I eerl, usi he ide i exle??? oe c esily rove: Theore 3, ) (i) cos d cos, or ll, ) (ii) si d si, or ll, ) (iii) si d cos, or ll, re orhool o re orhool o re orhool o Now le us deies he Fourier coeicies o -eriodic ucio wih eriod Deiiio 33 Le : [, ) R be ive eicewise coiuous -eriodic wih eriod : The we deie: (i) The cosie -Fourier coeicies o s d ()cos( ),,,3 (ii) The sie -Fourier coeicies o s d b ()si( ),,,3 For exle, he cosie -Fourier coeicies o he ucio cos is:, d or ll, where, Now, we ive he deiiio o he rciol Fourier series: Deiiio 34 Le : [, ) R be ive eicewise coiuous ucio which is -eriodicl wih eriod : The he -rciol Fourier series o ssocied wih he iervl [, ] is S + cos( ) + si( ) where d b re s i???? Le us hve soe exles Exle 3 Le i () i < wih o he iervl [, ]: The, d cos( ) d cos( ) d cos( ), d d + ( )cos( ), d Usi che o vribles: θ, we e dθ, θ i,, θ i, d θ i () Hece, he ierl becoes θcos( θ) dθ + ( θ )cos θdθ Siilrly b θsi( θ) dθ + ( θ )si θdθ So, 4 + + S 4 ( )( ) ( )si +

9 Abu Hd I e l: Frciol Fourier Series wih Alicios d i Exle 33 Le () i < < i The b ( ) d cos ( ) d si Hece S( ) si ( ) Oe c esily rove he ollowi clssicl resul Theore 3 The rciol Fourier series o iece wise coiuous - eriodicl ucio coveres oiwise o he vere lii o he ucio ech oi o discoiuiy, d o he ucio ech oi o coiuiy 4 Alicios I his secio we will use rciol Fourier series o solve soe rciol ril diereil equios Nely, we will solve he equio (, ) u( x, ) u x (4) <, < (4) u o, u L,, u x,, u x, x, < x< L (43) d Soluio We will use serio o vribles echique u x, P x Q Subsiue i he equio So le o e Fro which we e ( ) ( ) P x Q P x Q ( ) P( x) ( ) Q P x Q Sice x d re ideede vribles, he we e ( ) P( x) ( ) Q P x Q λ, cos o be deeried Hece d ( ) λ P x P x (44) ( ) λ Q Q (45) Codiios (43) suess h we work wih equio (44) irs There re hree ossibiliies or λ: (i) λ The equio (44) becoes P ( ) ( x), d ro he roery () o coorble rciol P x c Codiio (43) shows derivive, we e h c : (ii) λ > The equio (44) becoes P x λp x, d ro orul (4) o he coorble rciol derivive, we e λ P x ce Codiio (43) shows h c : (iii) λ < The equio (44) becoes µ P x + P x Usi oruls () d (3) we e x x P( x) ccos µ csi µ + (46) Codiio (43) ilies h c So si x c P x Aoher use o codiio (43) µ L ives si µ Hece So µ, wih, L (47) si x P x c L (48) Now, we o bck o equio (45) o e µ Q Q Usi orul (4) we e

Aeric Jourl o Couiol d Alied Mheics 4, 4(6): 87-9 9 µ µ + Q x e e Codiio (43) ilies h - Hece Q x Cobii (48) d (4) o e (49) sih µ (4) x u( x, ) b si sih (4) L L Now, usi he codiio u( x ),, o e x x x b si sih L L Usi he - Fourier series o - x, we id b REFERENCES [] Abdeljwd, T O coorble rciol clculus To er [] Abu-Hd, M, d Khlil, R Coorble Frciol He Diereil Equio Ieriol Jourl o Pure d Alied Mheics, 94 (4) 5-7 [3] Abu-Hd, M, d Khlil, R Abel S Forul Ad Wroski For Coorble Frciol Diereil Equios IJ Diereil Equios d Alicios, 3 (4) 77-83 [4] Abu-Hd, M, d Khlil, R Leedre rciol diereil equio d Leeder rciol olyoils IJ o Alied Mheicl Reserch, 3 (3) (4) 4-9 [5] Khlil, R, Al Hori, M, Youse A d Sbbheh, M, A ew Deiio o Frciol Derivive, J Cou Al Mh 64 657, 4