International Journal of Mathematical Archive-3(2), 2012, Page: Available online through ISSN

Size: px
Start display at page:

Download "International Journal of Mathematical Archive-3(2), 2012, Page: Available online through ISSN"

Transcription

1 Inernaional Jornal o Mahemaical Archive- age: Available online hrogh wwwijmaino ISSN A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS OR A OURH ORDER SEUDOHYEROI EQUAION Azizbayov EI* an Y Mehraliyev Mechanics-mahemaics acly a Sae Universiy a Azerbaijan azel_azerbaijan@mailr Receive on: 6-- Accepe on: 4-- ASRA In he paper he classic solion o one-imensional bonary vale problem or a pseohyperbolic eaion wih non-classic bonary coniions is invesigae or ha he sae problem is rece o he no-sel-ajoin bonary vale problem wih eivalen bonary coniion hen sing he meho o separaion o variables by means o he nown specral problem he given no sel-ajoin bonary vale problem is rece o an inegral eaion he eisence an nieness o he inegral eaion is prove by means o he conracion mappings principle an i is shown ha his solion is a nie solion or a no-ajoin bonary vale problem inally sing he eivalence he heorem on he eisence an nieness o a non-local bonary vale problem wih inegral coniion is prove Mahemaics Sbjec lassiicaion: G Keywors an hrases: mie problem conrace mappings ie poin eisence nieness classic solion pseohyperbolic eaion INRODUION: onemporary problems o naral sciences mae necessary o sae an invesigae aliaive new problems he sriing eample o which is he class o non-local problems or parial ierenial eaions Among non-local problems we can isingish a class o problems wih inegral coniions Sch coniions appear by mahemaical simlaion o phenomena relae o physical plasma [ isribion o he hea [ process o moisre ranser in capillary-simple environmens [ wih he problems o emography an mahemaical biology HE ROEM SAEMEN AND IS REDUION O HE EQUIVAEN ROEM: onsier he eaion [4 in he omain { : } an sae or i a problem wih iniial coniions D an non-local coniions 4 ± is a given nmber are he given ncions is a sogh ncion Earlier he bonary vale problems wih non-local inegral eaions were consiere in he papers [ [ an [8 Here or we have an Ionin ype bonary coniion [ *orresponing ahor: Azizbayov EI** azel_azerbaijan@mailr Inernaional Jornal o Mahemaical Archive- eb 59

2 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: Deiniion: Uner he classic solion o problem -4 we nersan he ncion coninos in a close omain D ogeher wih all is erivaives conaine in eaion an saisying all coniions -4 in he orinary sense he ollowing lemma is prove similarly [7 emma : e [ D [ an he ollowing agreemen coniions be lille: 5 hen he problem on ining he classic solion o problem -4 is eivalen o he problem on eining o he ncion rom - an 6 roo: e be he solion o problem -4 Inegraing eaion wih respec o rom o we have: 7 Assming ha an allowing or we in: Hence we arrive a lillmen o 6 Now assme ha is he solion o problem - 6 hen allowing or 6 rom 8 we in: 8 rom an i is obvios ha 9 Since problem 8 9 has only a rivial solion hen ie coniion 4 is saisie he lemma is prove AUIIARY AS: Now in orer o invesigae problem - 6 we cie some nown acs onsier he ollowing specral problem [ an [5: ± IJMA All Righs Reserve 5

3 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: onary vale problem is no sel-ajoin he problem will be a conjgae problem Y Y Y Y Y Y We enoe he sysem o eigen an ajoin ncions o problem in he ollowing way [5: a b a bcos sin 4 π a / b / 5 We choose he sysem o eigen an ajoin ncions o he conjgae problem as ollows [5: Y Y 4cos Y 4 b asin 6 I is irecly veriie ha he biorhogonaliy coniions are lille Here δ ij is Kronecer s symbol he ollowing heorem is vali i Yj i Yj δij heorem [7: he sysem o ncions 4 orms a Riesz basis in he space an he esimaes r g g R g g g Y g Y r a b b a b c[ 4 R 8 b a [ are vali or any ncion g 7 Uner he assmpions i g [ g i s s s s g g g g s i i we esablish he valiiy o he esimaes: i i g g 8 i i i g g b a aig 9 IJMA All Righs Reserve 5

4 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: rher ner he assmpions i g [ g i s s s s g g g g i s i we prove he valiiy o he esimaes: i i g g i i i g g b a ai g Now enoe by α [6 an aggregae o all he ncions o he orm onsiere in D each o he ncions rom is coninos on [ an J [ α he norm in his se is eine as ollows: I is nown ha α J α is a anach space α α < [ [ EISENE AND UNIQUENESS O HE SOIION O HE OUNDARY VAUE ROEM: Since he sysem 4 orms a Riesz basis in an sysems 4 6 orm a sysem o ncions biorhogonal in each solion o problem - 6 has he orm: Y Moreover an Y are eine by relaions 4 an 6 respecively Applying he meho o separaion o variables or eermining he sogh ncions rom we have: 4 5 a 6 7 Y Y Y IJMA All Righs Reserve 5

5 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: Solving problem -4 we have: 8 cos sin sin 9 cos sin sin a sin sin cos a ξ sin ξ ξ sin a sin Aer sbsiion o epressions o 8 9 respecively in we have: cos sin cos sin sin a a sin sin cos sin ξ sin ξ ξsin a sin Now proceeing rom einiion o he solion o problem - 6 similar o [6 he ollowing lemma is prove emma : I is any solion o problem - 6 he ncions saisy sysem 8- heorem : e [ ± [ [ 4 D D IJMA All Righs Reserve 5

6 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: IJMA All Righs Reserve 54 hen problem - 6 ner small vales o has a nie classic solion roo: Denoing eal he righ han sies o 8 9 respecively an we wrie eaion in he orm: We ll sy eaion in he space I is easy o see ha / < < < < aing ino accon hese relaions we have: [ [ [ [ [ [ [ [ [ a a a a [ [ a a Here allowing or 8- we have: [ [ D a a a

7 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: [ [ 4 D 4 8 b a a 8 b a a [ Now consier he operaor in he sphere 8 b a a 8a D a 8 a a 5 8 D [ K K R A rom a a a 4 a D A a 4 4 a D 8 b a a 8 b a a 8 b a a 6 I is seen rom -5 ha or any K he esimaes : R A D 7 are vali 8 9 a [ hen i ollows rom esimaes 7 8 ha ner sicienly small vales o he operaor acs in he sphere K K R rom an i is conracive hereore in he sphere K K R he operaor has a nie ie poin{ } ha is a solion o eaion he ncion as an elemen o he space is coninos an has coninos erivaives on D Now prove ha an are coninos in D rom 4-6 we have: 4 [ [ [ [ 5 [ [ [ IJMA All Righs Reserve [ a 4 [

8 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: IJMA All Righs Reserve 56 I ollows rom esimaes 4-4 ha an are coninos in D rher i ollows rom 7 ha since by he given heorem < < < < an he more so < < hs coniions are lille I is obvios ha coniions is lille or he ncion I is easy o see ha [ [ a 4 Now i we se sysems 5-7 ealiy 4 aes he orm: 44 Where he ncions are eermine by relaion 4 an Uner he coniions o he heorem i is obvios ha < 45 hen i ollows rom 45 ha or any ie [ : [ 46 hs relaions 44 an 46 yiel

9 Azizbayov EI* / A NON-OA OUNDARY VAUE ROEM WIH INEGRA ONDIIONS / IJMA- eb- age: onseenly he ncion saisies eaion every in D So is a solion o problem - 6 an by lemma i is nie he heorem is prove y means o lemma we prove he ollowing heorem : e all he coniions o heorem an agreemen coniions 5 be lille hen or sicienly small vales o problem - has a nie classic solion 4 ONUSION: he ollowing resls have been obaine: he eisence o he solion o a no sel-ajoin bonary vale problem or a orh orer pseohyperbolic eaion has been prove he nieness o he solion o a no sel-ajoin bonary vale problem or a orh orer pseohyperbolic eaion has been shown he eisence o he classic solion o a non-classic bonary vale problem wih inegral bonary or a orh orer pseohyperbolic eaion has been prove 4 he nieness o he classic solion o a non-classic bonary vale problem wih inegral bonary or a orh orer pseohyperbolic eaion has been shown REERENES: [ eilin S Eisence o solions or one-imensional wave eaions wih non-local coniion Elecronic J o Dier Ea 76-8 [ oziani A Solion ore n probleme mie avec coniions non locales por ne classe eaions hyperbolies llein e la lasse es Sciences Acaemie Royale e elgie [ Ionin N I Solions o bonary vale problem in hea concions heory wih non-local bonary coniions Dierens Uravn [4 Gabov SA Orazov he eaion [ an several problems associae wih i USSR ompaional Mahemaics an Mahemaical hysics [5 Kasmov Mirzoyev VS On one generalizaion o Ionin s eample he absracs o scieniic conerence evoe o h anniversary o he honore scienis aca AIHseynov [6 Khaveriyev KI Azizbeov EI Invesigaion o classical solion o an one-imensional no sel-ajoin mie problem or a class o semi-linear pseopseohyperbolic eaions o orh orer roc a Sae Universiy phys-mahser 4- [7 Mehraliyev Y Ysiov MR he solion o a bonary vale problem or a secon orer parabolic eaion wih inegral coniions roceeings o IMM NAS o Azerb [8 lina S Non local problem wih inegral coniions or a pseohyperbolic eaion Di Uravnen ************************ IJMA All Righs Reserve 57

Journal of Quality Measurement and Analysis JQMA 7(1) 2011, Jurnal Pengukuran Kualiti dan Analisis

Journal of Quality Measurement and Analysis JQMA 7(1) 2011, Jurnal Pengukuran Kualiti dan Analisis Jornl o Qliy Mesremen n Anlysis JQMA 7 7- Jrnl Pengrn Klii n Anlisis A NON-OA BOUNDARY VAUE PROBEM WIH INEGRA ONDIIONS OR A SEOND ORDER HYPERBOI EQUAION S Mslh Nili Sempn -Seemp engn Syr Kmirn bgi S Persmn

More information

Suyash Narayan Mishra, Piyush Kumar Tripathi & Alok Agrawal

Suyash Narayan Mishra, Piyush Kumar Tripathi & Alok Agrawal IOSR Journal o Mahemaics IOSR-JM e-issn: 78-578 -ISSN: 39-765X. Volume Issue Ver. VI Mar - Ar. 5 PP 43-5 www.iosrjournals.org A auberian heorem or C α β- Convergence o Cesaro Means o Orer o Funcions Suash

More information

Integral representations and new generating functions of Chebyshev polynomials

Integral representations and new generating functions of Chebyshev polynomials Inegral represenaions an new generaing funcions of Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 186 Roma, Ialy email:

More information

SOLVING AN OPTIMAL CONTROL PROBLEM WITH MATLAB

SOLVING AN OPTIMAL CONTROL PROBLEM WITH MATLAB SOLVING AN OPIMAL CONROL PROBLEM WIH MALAB RGeeharamani, SSviha Assisan Proessor, Researh Sholar KG College O Ars and Siene Absra: In his paper, we presens a Ponryagin Priniple or Bolza problem he proedre

More information

Positive continuous solution of a quadratic integral equation of fractional orders

Positive continuous solution of a quadratic integral equation of fractional orders Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.

More information

Theory of! Partial Differential Equations!

Theory of! Partial Differential Equations! hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

The Fundamental Theorems of Calculus

The Fundamental Theorems of Calculus FunamenalTheorems.nb 1 The Funamenal Theorems of Calculus You have now been inrouce o he wo main branches of calculus: ifferenial calculus (which we inrouce wih he angen line problem) an inegral calculus

More information

A Limit Symmetry of Modified KdV Equation and Its Applications

A Limit Symmetry of Modified KdV Equation and Its Applications Commun. Theor. Phys. 55 011 960 964 Vol. 55 No. 6 June 15 011 A Limi Symmery o Modiied KdV Equaion and Is Applicaions ZHANG Jian-Bing Ï 1 JI Jie SHEN Qing ã 3 and ZHANG Da-Jun 3 1 School o Mahemaical Sciences

More information

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information

Chapter Three Systems of Linear Differential Equations

Chapter Three Systems of Linear Differential Equations Chaper Three Sysems of Linear Differenial Equaions In his chaper we are going o consier sysems of firs orer orinary ifferenial equaions. These are sysems of he form x a x a x a n x n x a x a x a n x n

More information

Theory of! Partial Differential Equations-I!

Theory of! Partial Differential Equations-I! hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL HE PUBLISHING HOUSE PROCEEDINGS OF HE ROMANIAN ACADEMY, Series A, OF HE ROMANIAN ACADEMY Volume, Number 4/200, pp 287 293 SUFFICIEN CONDIIONS FOR EXISENCE SOLUION OF LINEAR WO-POIN BOUNDARY PROBLEM IN

More information

Surfaces in the space E

Surfaces in the space E 3 Srfaces in he sace E Le ecor fncion in wo ariables be efine on region R = x y y whose scalar coorinae fncions x y y are a leas once iffereniable on region. Hoograh of ecor fncion is a iece-wise smooh

More information

On Gronwall s Type Integral Inequalities with Singular Kernels

On Gronwall s Type Integral Inequalities with Singular Kernels Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies

More information

Existence Theory of Second Order Random Differential Equations

Existence Theory of Second Order Random Differential Equations Global Journal of Mahemaical Sciences: Theory and Pracical. ISSN 974-32 Volume 4, Number 3 (22), pp. 33-3 Inernaional Research Publicaion House hp://www.irphouse.com Exisence Theory of Second Order Random

More information

MIXED BOUNDARY VALUE PROBLEM FOR A QUARTER-PLANE WITH A ROBIN CONDITION

MIXED BOUNDARY VALUE PROBLEM FOR A QUARTER-PLANE WITH A ROBIN CONDITION Jornal o Science, Ilamic Repblic o Iran 3: 65-69 Naional Cener For Scieniic Reearch, ISSN 6-4 MIXED OUNDRY VLUE PROLEM FOR QURTER-PLNE WITH ROIN CONDITION ghili * Deparmen o Mahemaic, Facl o Science, Gilan

More information

Optimal Control. Lecture 5. Prof. Daniela Iacoviello

Optimal Control. Lecture 5. Prof. Daniela Iacoviello Opimal Conrol ecre 5 Pro. Daniela Iacoviello THESE SIDES ARE NOT SUFFICIENT FOR THE EXAM: YOU MUST STUDY ON THE BOOKS Par o he slides has been aken rom he Reerences indicaed below Pro. D.Iacoviello - Opimal

More information

arxiv: v1 [physics.data-an] 14 Dec 2015

arxiv: v1 [physics.data-an] 14 Dec 2015 1/ noise rom he nonlinear ransormaions o he variables Bronislovas Kaulakys, Miglius Alaburda, and Julius Ruseckas Insiue o Theoreical Physics and Asronomy, Vilnius Universiy, A. Gošauo 1, 118 Vilnius,

More information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick

More information

A NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University

A NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University A NOTE ON THE STRUCTURE OF BILATTICES A. Avron School of Mahemaical Sciences Sacler Faculy of Exac Sciences Tel Aviv Universiy Tel Aviv 69978, Israel The noion of a bilaice was rs inroduced by Ginsburg

More information

Generalized Chebyshev polynomials

Generalized Chebyshev polynomials Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT

More information

Scientific Research of the Institute of Mathematics and Computer Science DIFFERENT VARIANTS OF THE BOUNDARY ELEMENT METHOD FOR PARABOLIC EQUATIONS

Scientific Research of the Institute of Mathematics and Computer Science DIFFERENT VARIANTS OF THE BOUNDARY ELEMENT METHOD FOR PARABOLIC EQUATIONS Scieniic Research o he Insiue o Mahemaics and Compuer Science DIERENT VARIANTS O THE BOUNDARY ELEMENT METHOD OR PARABOLIC EQUATIONS Ewa Majchrzak,, Ewa Ładyga Jerzy Mendakiewicz, Alicja Piasecka Belkhaya

More information

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as Proceedings of he rd IMT-GT Regional Conference on Mahemaics Saisics and Applicaions Universii Sains Malaysia ANALYSIS ON () + () () = G( ( ) ()) Jessada Tanhanch School of Mahemaics Insie of Science Sranaree

More information

Chapter 10. Optimization: More than One Choice Variable

Chapter 10. Optimization: More than One Choice Variable Chaper Opimiaion: More han One Choice Variable William Sanle Jevons 85-88 Carl Menger 8 9. Opimiaion Problems Chaper 9: ma u one choice variable: consumpion Chaper : ma u o choice variables: leisure Chaper

More information

Homework 2 Solutions

Homework 2 Solutions Mah 308 Differenial Equaions Fall 2002 & 2. See he las page. Hoework 2 Soluions 3a). Newon s secon law of oion says ha a = F, an we know a =, so we have = F. One par of he force is graviy, g. However,

More information

The Bloch Space of Analytic functions

The Bloch Space of Analytic functions Inernaional OPEN ACCESS Jornal O Modern Engineering Research (IJMER) The Bloch Space o Analyic ncions S Nagendra, Pro E Keshava Reddy Deparmen o Mahemaics, Governmen Degree College, Pormamilla Deparmen

More information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow 1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering

More information

A Review of Gradient Algorithms for Numerical Computation of Optimal Trajectories

A Review of Gradient Algorithms for Numerical Computation of Optimal Trajectories doi:.58/jam..45 A Review o Gradien Algorihms or Nmerical Compaion o Opimal rajecories Wander Almodovar Goleo,*, Sandro da Silva Fernandes² Deparameno de Ciência e ecnologia Aeroespacial São José dos Campos/SP

More information

Section 2.6 Derivatives of products and quotients

Section 2.6 Derivatives of products and quotients Secion 2.6 Derivaives of proucs an quoiens (3/19/08) Overview: In his secion, we erive formulas for erivaives of funcions ha are consruce by aking proucs an quoiens of oher funcions, an we use hese formulas

More information

EXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN DIFFERENCE-DIFFERENTIAL EQUATIONS

EXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN DIFFERENCE-DIFFERENTIAL EQUATIONS Elecronic Journal of Differenial Equaions, Vol. 29(29), No. 49, pp. 2. ISSN: 72-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN

More information

When to Sell an Asset Where Its Drift Drops from a High Value to a Smaller One

When to Sell an Asset Where Its Drift Drops from a High Value to a Smaller One American Journal of Operaions Research, 5, 5, 54-55 Publishe Online November 5 in SciRes. hp://www.scirp.org/journal/ajor hp://x.oi.org/.436/ajor.5.564 When o Sell an Asse Where Is Drif Drops from a High

More information

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b) Applied Mahemaics E-Noes, 15(215), 14-21 c ISSN 167-251 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Mapping Properies Of The General Inegral Operaor On The Classes R k (ρ, b) And V k

More information

Solution of Integro-Differential Equations by Using ELzaki Transform

Solution of Integro-Differential Equations by Using ELzaki Transform Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform

More information

Lecture 9: Advanced DFT concepts: The Exchange-correlation functional and time-dependent DFT

Lecture 9: Advanced DFT concepts: The Exchange-correlation functional and time-dependent DFT Lecure 9: Advanced DFT conceps: The Exchange-correlaion funcional and ime-dependen DFT Marie Curie Tuorial Series: Modeling Biomolecules December 6-11, 2004 Mark Tuckerman Dep. of Chemisry and Couran Insiue

More information

4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be

4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be 4 COVARIANCE ROAGAION 41 Inrodcion Now ha we have compleed or review of linear sysems and random processes, we wan o eamine he performance of linear sysems ecied by random processes he sandard approach

More information

Scalar Conservation Laws

Scalar Conservation Laws MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )

More information

Boundary Control of the Viscous Generalized Camassa-Holm Equation

Boundary Control of the Viscous Generalized Camassa-Holm Equation ISSN 1749-3889 prin, 1749-3897 online Inernaional Journal of Nonlinear Science Vol89 No,pp173-181 Bounary Conrol of he Viscous Generalize Camassa-Holm Equaion Yiping Meng 1,, Lixin Tian 1 School of Mahemaics

More information

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations Applied Mahemaics Leers 5 (0) 058 065 Conens liss available a SciVerse ScienceDirec Applied Mahemaics Leers jornal homepage: www.elsevier.com/locae/aml Oscillaion resls for forh-order nonlinear dynamic

More information

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method Available a hp://pva.ed/aa Appl. Appl. Mah. ISSN: 93-9466 Special Isse No. (Ags ) pp. 8 93 Applicaions Applied Maheaics: An Inernaional Jornal (AAM) Eac soliary-wave Special Solions for he Nonlinear Dispersive

More information

Riemann Function and Methods of Group Analysis

Riemann Function and Methods of Group Analysis American Research Jornal of Mahemaics Original Aricle ISSN 378-74X Volme Isse 3 5 Riemann Fncion and Mehods of Grop Analsis Akimov Andre Chernov Igor Abdllina Rfina 3 4533 Serliamak Rssia Lenina sree 47A

More information

Characteristics of Linear System

Characteristics of Linear System Characerisics o Linear Sysem h g h : Impulse response F G : Frequency ranser uncion Represenaion o Sysem in ime an requency. Low-pass iler g h G F he requency ranser uncion is he Fourier ransorm o he impulse

More information

On the probabilistic stability of the monomial functional equation

On the probabilistic stability of the monomial functional equation Available online a www.jnsa.com J. Nonlinear Sci. Appl. 6 (013), 51 59 Research Aricle On he probabilisic sabiliy of he monomial funcional equaion Claudia Zaharia Wes Universiy of Timişoara, Deparmen of

More information

Asymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice

Asymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice Asympoic Solion of he Ani-Plane Problem for a Two-Dimensional Laice N.I. Aleksandrova N.A. Chinakal Insie of Mining, Siberian Branch, Rssian Academy of Sciences, Krasnyi pr. 91, Novosibirsk, 6391 Rssia,

More information

Classical Thermodynamics as a Consequence of Spacetime Geometry

Classical Thermodynamics as a Consequence of Spacetime Geometry Classical Thermoynamics as a Consequence of Spaceime Geomery Jay R. Yablon 9 Norhumberlan Drive Schenecay, New York 239-284 jyablon@nycap.rr.com January 6, 25 Absrac: Jus as Maxwell s magneic equaions

More information

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier

More information

-e x ( 0!x+1! ) -e x 0!x 2 +1!x+2! e t dt, the following expressions hold. t

-e x ( 0!x+1! ) -e x 0!x 2 +1!x+2! e t dt, the following expressions hold. t 4 Higher and Super Calculus of Logarihmic Inegral ec. 4. Higher Inegral of Eponenial Inegral Eponenial Inegral is defined as follows. Ei( ) - e d (.0) Inegraing boh sides of (.0) wih respec o repeaedly

More information

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations A Sharp Exisence and Uniqueness Theorem for Linear Fuchsian Parial Differenial Equaions Jose Ernie C. LOPE Absrac This paper considers he equaion Pu = f, where P is he linear Fuchsian parial differenial

More information

Operators related to the Jacobi setting, for all admissible parameter values

Operators related to the Jacobi setting, for all admissible parameter values Operaors relaed o he Jacobi seing, for all admissible parameer values Peer Sjögren Universiy of Gohenburg Join work wih A. Nowak and T. Szarek Alba, June 2013 () 1 / 18 Le Pn α,β be he classical Jacobi

More information

ON JENSEN S INEQUALITY FOR g-expectation

ON JENSEN S INEQUALITY FOR g-expectation Chin. Ann. Mah. 25B:3(2004),401 412. ON JENSEN S INEQUALITY FOR g-expectation JIANG Long CHEN Zengjing Absrac Briand e al. gave a conerexample showing ha given g, Jensen s ineqaliy for g-expecaion sally

More information

Derivatives of Inverse Trig Functions

Derivatives of Inverse Trig Functions Derivaives of Inverse Trig Fncions Ne we will look a he erivaives of he inverse rig fncions. The formlas may look complicae, b I hink yo will fin ha hey are no oo har o se. Yo will js have o be carefl

More information

Convergence of the Neumann series in higher norms

Convergence of the Neumann series in higher norms Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann

More information

POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE

POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE Urainian Mahemaical Journal, Vol. 55, No. 2, 2003 POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE A. G. Mazo UDC 517.983.27 We invesigae properies of posiive and monoone differenial sysems wih

More information

On Two Integrability Methods of Improper Integrals

On Two Integrability Methods of Improper Integrals Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169

More information

The Miki-type identity for the Apostol-Bernoulli numbers

The Miki-type identity for the Apostol-Bernoulli numbers Annales Mahemaicae e Informaicae 46 6 pp. 97 4 hp://ami.ef.hu The Mii-ype ideniy for he Aposol-Bernoulli numbers Orli Herscovici, Toufi Mansour Deparmen of Mahemaics, Universiy of Haifa, 3498838 Haifa,

More information

The law of conservation of mass: Mass can be neither created nor destroyed. It can only be transported or stored.

The law of conservation of mass: Mass can be neither created nor destroyed. It can only be transported or stored. UDMETL COCEPTS OR LOW LYSIS We covere mehos of analysis of nonflowing fluis in he previous chaper. In his chaper, we evelop he funamenal conceps of flow analysis, incluing he way o escribe flui flow, naural

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

An Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation

An Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation Commun Theor Phys Beijing, China 43 2005 pp 591 596 c Inernaional Academic Publishers Vol 43, No 4, April 15, 2005 An Invariance for 2+1-Eension of Burgers Equaion Formulae o Obain Soluions of KP Equaion

More information

Proca equation for laser pulses interaction with matter

Proca equation for laser pulses interaction with matter Proca euaion or laser pulses ineracion wi maer Janina Marciak- Kozłowska Mirosław Kozłowski* Insiue o Elecron Tecnology Al. Loników 3/46-668 Warsaw Polan *Corresponing auor Absrac In is paper e ineracion

More information

1. Introduction. Rawid Banchuin

1. Introduction. Rawid Banchuin 011 Inernaional Conerence on Inormaion and Elecronics Engineering IPCSIT vol.6 (011 (011 IACSIT Press, Singapore Process Induced Random Variaion Models o Nanoscale MOS Perormance: Eicien ool or he nanoscale

More information

New Oscillation Criteria For Second Order Nonlinear Differential Equations

New Oscillation Criteria For Second Order Nonlinear Differential Equations Researh Inveny: Inernaional Journal Of Engineering And Siene Issn: 78-47, Vol, Issue 4 (Feruary 03), Pp 36-4 WwwResearhinvenyCom New Osillaion Crieria For Seond Order Nonlinear Differenial Equaions Xhevair

More information

Classical Thermodynamics Entropy Laws as a Consequence of Spacetime Geometry

Classical Thermodynamics Entropy Laws as a Consequence of Spacetime Geometry Classical Thermoynamics Enropy Laws as a Consequence of Spaceime Geomery Jay R. Yablon 9 Norhumberlan Drive Schenecay, New York 239-284 jyablon@nycap.rr.com January 7, 25 Absrac: Jus as Maxwell s magneic

More information

The Successive Backward Sweep Method for Optimal Control of Nonlinear Systems with Constraints

The Successive Backward Sweep Method for Optimal Control of Nonlinear Systems with Constraints AAS -6 he Sccessive Backward Sweep Mehod or Opimal Conrol o Nonlinear Sysems wih Consrains D. H. Cho * and Srinivas R. Vadali his paper presens variaions o he Sccessive Backward Sweep (SBS mehod or solving

More information

Computers and Mathematics with Applications

Computers and Mathematics with Applications Compers and Mahemaics wih Applicaions 59 (00) 80 809 Conens liss available a ScienceDirec Compers and Mahemaics wih Applicaions jornal homepage: www.elsevier.com/locae/camwa Solving fracional bondary vale

More information

Dirac s hole theory and the Pauli principle: clearing up the confusion.

Dirac s hole theory and the Pauli principle: clearing up the confusion. Dirac s hole heory and he Pauli rincile: clearing u he conusion. Dan Solomon Rauland-Borg Cororaion 8 W. Cenral Road Moun Prosec IL 656 USA Email: dan.solomon@rauland.com Absrac. In Dirac s hole heory

More information

Some Ramsey results for the n-cube

Some Ramsey results for the n-cube Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain

More information

Lecture 10: The Poincaré Inequality in Euclidean space

Lecture 10: The Poincaré Inequality in Euclidean space Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?

More information

4 Sequences of measurable functions

4 Sequences of measurable functions 4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences

More information

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics

More information

Solving a System of Nonlinear Functional Equations Using Revised New Iterative Method

Solving a System of Nonlinear Functional Equations Using Revised New Iterative Method Solving a Sysem of Nonlinear Funcional Equaions Using Revised New Ieraive Mehod Sachin Bhalekar and Varsha Dafardar-Gejji Absrac In he presen paper, we presen a modificaion of he New Ieraive Mehod (NIM

More information

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity ANNALES POLONICI MATHEMATICI LIV.2 99) L p -L q -Time decay esimae for soluion of he Cauchy problem for hyperbolic parial differenial equaions of linear hermoelasiciy by Jerzy Gawinecki Warszawa) Absrac.

More information

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions Proceedings of he World Congress on Engineering and Compuer Science 23 Vol I WCECS 23, 23-25 Ocober, 23, San Francisco, USA Homoopy Perurbaion Mehod for Solving Some Iniial Boundary Value Problems wih

More information

Differential Harnack Estimates for Parabolic Equations

Differential Harnack Estimates for Parabolic Equations Differenial Harnack Esimaes for Parabolic Equaions Xiaodong Cao and Zhou Zhang Absrac Le M,g be a soluion o he Ricci flow on a closed Riemannian manifold In his paper, we prove differenial Harnack inequaliies

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

arxiv:math/ v1 [math.nt] 3 Nov 2005

arxiv:math/ v1 [math.nt] 3 Nov 2005 arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming

More information

DESIGN OF TENSION MEMBERS

DESIGN OF TENSION MEMBERS CHAPTER Srcral Seel Design LRFD Mehod DESIGN OF TENSION MEMBERS Third Ediion A. J. Clark School of Engineering Deparmen of Civil and Environmenal Engineering Par II Srcral Seel Design and Analysis 4 FALL

More information

SOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC CONVEX FUNCTIONS MUHAMMAD ASLAM NOOR, KHALIDA INAYAT NOOR, SABAH IFTIKHAR AND FARHAT SAFDAR

SOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC CONVEX FUNCTIONS MUHAMMAD ASLAM NOOR, KHALIDA INAYAT NOOR, SABAH IFTIKHAR AND FARHAT SAFDAR Inernaional Journal o Analysis and Applicaions Volume 16, Number 3 2018, 427-436 URL: hps://doi.org/10.28924/2291-8639 DOI: 10.28924/2291-8639-16-2018-427 SOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC

More information

GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256

GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256 Tile Auhor(s) GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION Zhao, Liang Ciaion Osaka Journal of Mahemaics. 51(1) P.45-P.56 Issue Dae 014-01 Tex Version publisher URL hps://doi.org/10.18910/9195

More information

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen

More information

KEY. Math 334 Midterm III Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm III Fall 2008 sections 001 and 003 Instructor: Scott Glasgow KEY Mah 334 Miderm III Fall 28 secions and 3 Insrucor: Sco Glasgow Please do NOT wrie on his exam. No credi will be given for such work. Raher wrie in a blue book, or on your own paper, preferably engineering

More information

Model Reduction for Dynamical Systems Lecture 6

Model Reduction for Dynamical Systems Lecture 6 Oo-von-Guericke Universiä Magdeburg Faculy of Mahemaics Summer erm 07 Model Reducion for Dynamical Sysems ecure 6 v eer enner and ihong Feng Max lanck Insiue for Dynamics of Complex echnical Sysems Compuaional

More information

On the Regularity of the Primitive Equations of the Ocean

On the Regularity of the Primitive Equations of the Ocean On he Regulariy of he Primiive Equaions of he Ocean Igor Kukavica Mohamme Ziane Ocober 9, 007 Deparmen of Mahemaics Universiy of Souhern alifornia Los Angeles, A 90089 e-mails: kukavica@usc.eu, ziane@usc.eu

More information

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien

More information

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z.

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z. Ma 67 Engineering Calcls III Updaed on 04/0/0 r. Firoz Tes solion:. a) Find he cener and radis of he sphere 4 4 4z 8 6 0 z ( ) ( ) z / 4 The cener is a (, -, 0), and radis b) Find he cener and radis of

More information

1 First Order Partial Differential Equations

1 First Order Partial Differential Equations Firs Order Parial Differenial Eqaions The profond sdy of nare is he mos ferile sorce of mahemaical discoveries. - Joseph Forier (768-830). Inrodcion We begin or sdy of parial differenial eqaions wih firs

More information

Existence of positive solution for a third-order three-point BVP with sign-changing Green s function

Existence of positive solution for a third-order three-point BVP with sign-changing Green s function Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion

More information

PH2130 Mathematical Methods Lab 3. z x

PH2130 Mathematical Methods Lab 3. z x PH130 Mahemaical Mehods Lab 3 This scrip shold keep yo bsy for he ne wo weeks. Yo shold aim o creae a idy and well-srcred Mahemaica Noebook. Do inclde plenifl annoaions o show ha yo know wha yo are doing,

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

On the Stability of the n-dimensional Quadratic and Additive Functional Equation in Random Normed Spaces via Fixed Point Method

On the Stability of the n-dimensional Quadratic and Additive Functional Equation in Random Normed Spaces via Fixed Point Method In. Journal of Mah. Analysis, Vol. 7, 013, no. 49, 413-48 HIKARI Ld, www.m-hikari.com hp://d.doi.org/10.1988/ijma.013.36165 On he Sabiliy of he n-dimensional Quadraic and Addiive Funcional Equaion in Random

More information

Haar Wavelet Operational Matrix Method for Solving Fractional Partial Differential Equations

Haar Wavelet Operational Matrix Method for Solving Fractional Partial Differential Equations Copyrigh 22 Tech Science Press CMES, vol.88, no.3, pp.229-243, 22 Haar Wavele Operaional Mari Mehod for Solving Fracional Parial Differenial Equaions Mingu Yi and Yiming Chen Absrac: In his paper, Haar

More information

Convolution. Lecture #6 2CT.3 8. BME 333 Biomedical Signals and Systems - J.Schesser

Convolution. Lecture #6 2CT.3 8. BME 333 Biomedical Signals and Systems - J.Schesser Convoluion Lecure #6 C.3 8 Deiniion When we compue he ollowing inegral or τ and τ we say ha he we are convoluing wih g d his says: ae τ, lip i convolve in ime -τ, hen displace i in ime by seconds -τ, and

More information

Math 334 Fall 2011 Homework 11 Solutions

Math 334 Fall 2011 Homework 11 Solutions Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then

More information

y h h y

y h h y Porland Communiy College MTH 51 Lab Manual Limis and Coninuiy Aciviy 4 While working problem 3.6 you compleed Table 4.1 (ormerly Table 3.1). In he cone o ha problem he dierence quoien being evaluaed reurned

More information

Nonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique

Nonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique Filoma 29:5 (2015), 1067 1080 DOI 10.2298/FI1505067W Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Nonlinear Fuzzy Sabiliy of a Funcional

More information

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS MICHAEL DORFF AND J. SZYNAL Absrac. Differen mehods have been used in sudying he univalence of he inegral ) α ) f) ) J α, f)z) = f ) d, α,

More information

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT Inerna J Mah & Mah Sci Vol 4, No 7 000) 48 49 S0670000970 Hindawi Publishing Corp GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT RUMEN L MISHKOV Received

More information

Transcendence of solutions of q-airy equation.

Transcendence of solutions of q-airy equation. Josai Mahemaical Monographs vol. 0 (207), pp. 29 37 Transcendence of soluions of q-airy equaion. Seiji NISHIOKA Absrac. In his paper, we prove ranscendence of soluions of he ieraed Riccai equaions associaed

More information

Differential Equations

Differential Equations Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding

More information

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations Annals of Pure and Applied Mahemaics Vol. 6, No. 2, 28, 345-352 ISSN: 2279-87X (P), 2279-888(online) Published on 22 February 28 www.researchmahsci.org DOI: hp://dx.doi.org/.22457/apam.v6n2a Annals of

More information

Symmetry Reduction for a System of Nonlinear Evolution Equations

Symmetry Reduction for a System of Nonlinear Evolution Equations Nonlinear Mahemaical Physics 1996, V.3, N 3 4, 447 452. Symmery Reducion for a Sysem of Nonlinear Evoluion Equaions Lyudmila BARANNYK Insiue of Mahemaics of he Naional Ukrainian Academy of Sciences, 3

More information