Australian Journal of Basic and Applied Sciences, 4(9): , 2010 ISSN

Size: px
Start display at page:

Download "Australian Journal of Basic and Applied Sciences, 4(9): , 2010 ISSN"

Transcription

1 Australia Joural of Basic ad Applid Scics, 4(9): 4-43, ISSN Th Caoical Product of th Diffrtial Equatio with O Turig Poit ad Sigular Poit A Dabbaghia, R Darzi, 3 ANaty ad 4 A Jodayr Akbarfa, Islaic Azad Uivrsity Nka Brach, Nka, Ira 3 Dpartt of Mathatics, Uivrsity of Mazadara, Babolsar, Ira 4 Dpartt of Mathatics, Uivrsity of Tabriz, Tabriz, Ira Abstract: W cosidr th diffrtial quatio y qy y for I ( ) ( ) : [,], (*) whr th wight fuctio f is ral ad has o zro i th op itrval (,), so calld turig poit, ad th assuptio that is odd ordr This turig poit is adittd to b pol of th fuctio q Usig th asyptotic solutio as wll as th distributio of positiv ad gativ igvalu, w driv th caoical product of a particular solutio of th Stur-Liouvill i o turig poit cas Ky words: Turig poit; Sigular poit; Eigvalus; Stur-Liouvill; Ifiit products INTRODUCTION W cosidr th diffrtial quatio y qy y ( ) ( ), () Hr = is th igvalu paratr W assu that th wight fuctio f is ral ad has o zro i th op itrval (,), so calld turig poit, ad th assuptio that is odd ordr This turig poit is adittd to b pol of th fuctio q Diffrtial quatios with turig poits hav various applicatios i athatics, lasticity, optics, gophysics ad othr brachs of atural scics (s (Ebrhard t al, 994; Goldvizr t al, 997) ad th rfrcs thri) Th iportac of asyptotic aalysis i obtaiig iforatio o th solutio of a Stur-Liouvill quatio with ultipl turig poits was ralizd by Lug (Lug, 977), Olvr (977a; 977b), Hadig (Hadig, 977), ad Ebrhard, Frilig ad Schidr i (Ebrhard t al, 994) Th rsults of Dorodicy (Dorodicy, 96), Kazarioff (Kazarioff, 958), Lagr, (93), Dyachko, (), Marasi ad Jodayr i (6) ad Naaty (999), Naaty ad Dabbaghia (7) brig iportat iovatios to th asyptotic approiatio of solutios of Stur-Liouvill quatios It is cssary to poit out that applyig asyptotic solutios for studyig ivrs probl i turig poits cass, is or coplicatd ad practically is ot covit to us Espcially i drivig th asyptotic forulas, o should apply Bssl fuctio typ I additio a or difficult ad challgig task is to shap th asyptotic bhavior of th solutios ad corrspodig igvalus So th ivrs probl of rcostructig th pottial fuctio fro th giv spctral iforatio ad corrspodig dual quatio caot b studid by usig th asyptotic fors I fact, i asyptotic thods o caot grally prss th act solutio i closd for Idd i thods coctd with dual quatios, th closd for of th solutio is dd Th rprstig solutio of th ifiit product for plays a iportat rol for ivstigatig th corrspodig dual quatios I th prvious articl (Khiri ad Jodayr, 3), authors cosidrd th followig Stur-Liouvill quatio () It is assud that q() is a ral fuctio that is Lbsgu itgrabl o th itrval [,], = is th spctral paratr ad ( ) ( ) ( ), 4 whr < <, N, > for [,], is a twic cotiuously diffrtiabl o [,], ad () Corrspodig Author: A Dabbaghia, Islaic Azad Uivrsity Nka Brach, Nka, Ira E-ail: adabbaghia@iaukaacir 4

2 Aust J Basic & Appl Sci, 4(9): 4-43, has o zro i [,], so calld turig poit Th solutio y(,) of such ad quatio with iitial coditios y(, ) =, y(, ) = was foud to hav th ifiit product for ( ) y (, ) ( ) () p ( ), k k zk ( ) y (, ) ( ) () p( ) f ( )cos ( rk( )) p ( ) ( uk( ) ) f ( ),, k k k k () (3) whr th squc {u k ()} rprsts th squc of positiv igvalus ad {r k ()} th squc of gativ igvalus of th Dirichlt probl associatd with () o [,], for ach i (, ] Th squc { k ()}, for ach fid, <, rprsts th squc of gativ igvalus of th Dirichlt probl for Eq() o th closd itrval [,], whr p ( ) ( t) dt for, f( ) ( t) dt for, k zk ( ) for k,,, p ( ),, k,,, Ad ad th positiv zros of J( ), J, rspctivly I this papr w obtai th k k ( ) 3 ifiit product rprstatio of solutio of () i a cas whr th wight fuctio has o zro that it is adittd to b pol of th fuctio q otatios ad Prliiary Rsults: Lt C(,) b th solutio of () corrspodig to th iitial coditios C(,)=, C(,)= I ordr to rprst th solutio C(,) as a ifiit product w us a suitabl fudatal syst of solutios (FSS) for Eq() as costructd i [4] Itroducig so triology at this poit w writ I [, ] [, ] [,], ), (,], : ( 4 A) l with arg (, ], ad []: = + O( - ) ) () is ral ad has i (,) o zro l, of ordr l whr l is odd I th triology of [4], l is of typ IV Th fuctios : I, R, ( ): ( ) ( ), ar o-vaishig ad ral-aalytic; dot k : ( ) 3) q has th for q ( ) A( ) B( ) C( ), ( I, ),, 43

3 Aust J Basic & Appl Sci, 4(9): 4-43, With costats A l, B ad a boudd ral-aalytic fuctio C 4) For [,] lt ( ): () (): a{, ()} R t dt with t t Accordig to th typ of l w kow fro [4, Thor,6] that i th sctor S { arg [,]}, 4 thr ist a fudatal syst of solutios of () { IV IV Z (, ), Z (, )}, ad such that t dt [],, Z (, ) si ( l 3) si ( l ) [] [], i i t dt i 4 t dt i si si, t dt [],, IV N i ( t) dti Z (, ) si 4 [],, si ( l 3) (5) W ( ) [] I th squl w also d { Z (, ), Z (, )} Fro [4] w hav i si ( l 3) si ( l ) IV N 4 4 Z (, ) k V V, si si whr ( ) i O() 4 ( ) V ( ) icsc ( ), ad O() V ( ) icsc ( ) ( ) i 4 ( ) Cosqutly Z ( ) IV N (, ) ( ) csc i si ( l 3) si ( l ) i [] si si i i (6) 44

4 Aust J Basic & Appl Sci, 4(9): 4-43, Siilarly i IV N Z (, ) ( ) [] si ( l ( ) 3) 3asyptotic For of th Solutio: W cosidr th diffrtial quatio () with th followig coditios C(,) =, C(,) = (7) Applyig th { (, ), (, )} Z Z for I,, whr l is of typ IV W hav C (, ) CZ(, ) CZ(, ) That usig of Crar's rul lads to th quatio C (, ) ( (, ) (, ) (, ) (, )) Z Z Z Z Takig (4)-(5) ito accout w driv C (, ) whr si ( l 3) ( t) dti 4 M( ) si ( t) dt ( t) dt () [] [], i () t dt i ( ) t dt [] ( ) M M [],, si ( l ) ( t) dti si t dti 4 4 M( ) i si si ( l 3) By virtu of (9) ad (), th followig stiats ar also valid: C (, ) si ( l 3) ( t) dti ( t) dti 4 () [[]],, si Siilarly, usig of (6), (7) ad (8) for = w fid that ( t) dt () [[]],, (8) (9) () () l ( t) dt i( ) C (, ) i () ( ) csc ( ) ( t) dt si () ( ) csc ( ) si ( l 3) 45

5 Aust J Basic & Appl Sci, 4(9): 4-43, l i( ) ( t) dt () ( ) csc i 4 ( ) 4distributio of th Eigvalu: W cosidr th boudary valu probl [[]] L L q b ( ( ), ( ), ) () for Eq() with boudary coditios y(, ), y(, ), y( b, ) Th boudary valu probl L for Fro (Taarki, 97) w hav ( b) O( ), b ( t) dt ad for = l siilarly fro () w hav ( ) 4 ( ) O( ) ( t) dt b(, ) has a coutabl st of gativ igvalus { ( b)} Th spctru {l } of boudary valu probl L for l < b, cosist of two squcs of gativ ad positiv igvalus: { ( b)} { ( b)} { ( b)}, N, 4 ( b) O( ), b ( tdt ) 4 ( b) O( ) ( tdt ) such that 5Mai rsults: Sic th solutio C(,r) of th Stur-Liouvill quatio dfid by a fid st of iitial coditios is a (3) (4) (5) (6) tir fuctio of r for ach fid [,], thus it follows fro th classical Hadaard's factorizatio thor that such solutio is prssibl as a ifiit product For fid b(, ) by Halvors's rsult (Halvors, 987), C(b, ) is a tir fuctio of ordr Thrfor w ca us Hadaard's thor to rprst th solutio i th for whr h(b) is a fuctio idpdt of l but ay dpd o b ad th ifiit ubr of gativ igvalus, { ( b)} zro st of C(b, l) for ach b Sic Cb (, ()) b for th, ths l (b) corrspod to igvalus of th boudary valu probl L o th closd itrval [,b], < b < W rwrit th ifiit product as ( b) Cb (, ) hb () ( ) h() b( ) ( b) with z (8) 46

6 Aust J Basic & Appl Sci, 4(9): 4-43, ( ): ( ) z h, b h b ( b) whr z R ( b) Now (3) iplis that z z O( ) ( ) b It follows fro th rsults of [6] that th ifiit product z is absolutly covrgt o ay copact subitrval of (, ) Th fuctio is cotiuous ( b) ( b) ad so th O-tr is uiforly boudd i b Thor Lt C(, ) b th solutio of () satisfyig th iitial coditios C(, ) =, C(, ) = Th for < <, (, ) () ( ) ( C R ) (9) z whr th squc ( ),, rprsts th squc of gativ igvalus of th boudary valu probl L o [,]proof Lt { ( b )} fid b =, < < th accordig to [] w hav b th igvalus of th boudary valu probl L o [,b], for ( ) sih R ( ) log ( ) O( ) () z R ( ) C (, ) Thus fro (), (8), w obtai h ( ) () R ( ) ( ) ( ) z Siilarly for b = agai by Hadaard's thor w that C (, ) A( ( ) ) () whr A is costat Lt, =,, b th squc of positiv zros of th Bssl fuctio of ordr h, th (s []) O( ), R ( ) ( ) So th ifiit product R ( ) ( ) ar absolutly covrgt Cosqutly w ay writ as bfor, ( ( )) R ( ) C (, ), A () 47

7 Aust J Basic & Appl Sci, 4(9): 4-43, whr A A R ( ) ( ) Thor For b =, l i( ) () V( ) R ( ) R c (, ) whr V t dt ( ) li ( ) ( ( )) ( ) proof Accordig to (Jodayr ad Migarlli, ) th ifiit product ( ( )) R ( ) is a tir fuctio of l, whos roots ar prcisly ( ), Morovr ( ( )) R ( ) log ( )[ i R( )] J ( i R ( ))( O( )) Uiforly o th Circls R ( ) Thus it follows fro (), l i( ) C (, ) () V ( ) R ( ) ( ( )) R ( ) A Siilarly for b =, < <, th boudary valu probl L o [,] has a ifiit ubr of positiv ad gativ igvalus which ar dotd by { ( )} { ( )} { ( )}, rspctivly By Hadaard's thor, th solutio o [,], < < is of th for C (, ) g ( ) ( )( ) ( ) ( ) (4) Lt,,,, b th positiv zros of J( z), drivativ of th Bssl fuctio of ordr o Th distributio of is of th for O(), (s []) Cosqutly, w hav O( ), R ( ) ( ) O( ) R ( ) ( ) (5) (6) 48

8 Aust J Basic & Appl Sci, 4(9): 4-43, Cosqutly, th ifiit products R ( ) ( ) ad R ( ) ( ) ar absolutly covrgt for ach (,) Thrfor w ay writ ( ( )) R ( ) ( ( ) ) R ( ) C (, ) g( ) with g ( ) g( ) R ( ) ( ) R ( ) ( ) Thor 3 For < <, C (, ) () ( R( R ) ( )) 8 si ( l 3) ( ( )) R( ) ( ( ) ) R( ) si (7) (8) (9) proof: Fro Las ad 3 of [] th ifiit products ( ( )) R( ) ( ( ) ) R( ) ar tir fuctios of l for fid, thos roots ar prcisly ( ) ad ( ), ³, rspctivly Morovr ( ( )) R( ) ( ( ) ) R( ) R ( ) 4 R O 4 ( ) ( ) cos( ( ) ) ( ), R R as Thus by usig of th asyptotic pasio of C(,l) i [] w gt g ( ) C (, ) ( ( )) R ( ) ( ( ) ) R ( ) si ( l 3) () ( ( ) ( )) R R 8 si REFERENCES Abraowitz, M, JA Stgu, 964 Hadbook of Mathatical Fuctios, Appl Math Sr 55, U S Govt Pritig Offic, Washigto, DC 49

9 Aust J Basic & Appl Sci, 4(9): 4-43, Dorodicy, AA96 Asyptotic laws of distributio of th charactristic valus for crtai spcial fors of diffrtial quatios of th scod ordr, Ar Math Soc Trasl Sr, (6): - Dyachko, AX Asyptotics of th igvalus of aidfiit Stur-Liouvill probl, Math Nots, 68(I): -4 Ebrhard, W, G Frilig, K Wilck, Idfiit igvalu probls with svral sigular poits ad turig poits, Math Nachr, 9: 5-7 Ebrhard, W, G Frilig, A Schidr, 994 Coctio forula for scod-ordr diffrtial quatios with a copl paratr ad havig a arbitrary ubr of turig poits, Math Nachr, 65: 5-9 Evs, HW, 979 Fuctios of a copl variabl, Pridl, Wbr ad Schidt, pp: Goldvizr, AL, VB Lidsky, PE Tovstik, 979 Fr vibratio of thi lastic shlls, Nauka, Moscow Halvors, SG, 987 A fuctio thortic proprty of solutios of th quatio ( q), Quart J Math Oford, (38): Hadig, J, 977 Global phas-itgral thods, Quart J Mch Appl Math, 3: 8-3 Jodayr, A, Akbarfa, AB Migarlli, Th caoical product of th solutio of th Stur- Liouvill quatio i o turig poit cas, Caad Appl Math Quart, 8(4): 35-3 Kazarioff, ND, 985 Asyptotic thory of scod ordr diffrtial quatios with two sipl turig poits, Arch Ratio Mch Aal, : 9-5 Khiri, H, A Jodayr Akbarfa, 3 O th ifiit product rprstatio of solutio ad dual quatios of Stur-Liouvill quatio with turig poit of ordr 4+, Bull Iraia Math Soc, 9(): 35-5 Lagr, RE, 93 O th asyptotic solutio of ordiary diffrtial quatios with a applicatio to Bssl fuctios of larg ordr, Tras Ar Math Soc, 33: 3-64 Lug, A, 977 Distributio of igvalus i th prsc of highr ordr turig poits, Tras Ar Math Soc, 9: -35 Marasi, HR, A Jodayr Akbarfa, 7 O th caoical solutio of idfiit probl with turig poits of v ordr, J Math aal Appl, doi: 6/aa 6 49 Naaty, A, A Dabbaghia, 7 Asyptotic for of th solutio of Stur-Liouvill probl with turig poits of odd-v ordr, Far East J Appl Math, 9(): 6-7 Naaty, A, 999 Th caoical product of th solutio of th Stur-Liouvill probls, Ira J Sci Tchol Tras A () Olvr, FWJ, 977 Coctio forulas for scod-ordr diffrtial quatios havig a arbitrary ubr of turig poits of arbitrary ultiplicitis, SIAM J Math Aal, 8: Olvr, FWJ, 977 Coctio forulas for scod-ordr diffrtial quatios with ultipl turig poits, SIAM J Math Aal, 8: 7-54 Taarki, JD, 97 So gral probls of th thory of ordiary liar diffrtial quatios ad pasios of a arbitrary fuctio i sris of fudatal fuctios, Math Z 7:

Digital Signal Processing, Fall 2006

Digital Signal Processing, Fall 2006 Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti

More information

PURE MATHEMATICS A-LEVEL PAPER 1

PURE MATHEMATICS A-LEVEL PAPER 1 -AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio

More information

The Asymptotic Form of Eigenvalues for a Class of Sturm-Liouville Problem with One Simple Turning Point. A. Jodayree Akbarfam * and H.

The Asymptotic Form of Eigenvalues for a Class of Sturm-Liouville Problem with One Simple Turning Point. A. Jodayree Akbarfam * and H. Joral of Scic Ilaic Rpblic of Ira 5(: -9 ( Uirity of Thra ISSN 6- Th Ayptotic For of Eigal for a Cla of Str-Lioill Probl with O Sipl Trig Poit A. Jodayr Abarfa * ad H. Khiri Faclty of Mathatical Scic Tabriz

More information

SOME IDENTITIES FOR THE GENERALIZED POLY-GENOCCHI POLYNOMIALS WITH THE PARAMETERS A, B AND C

SOME IDENTITIES FOR THE GENERALIZED POLY-GENOCCHI POLYNOMIALS WITH THE PARAMETERS A, B AND C Joural of Mathatical Aalysis ISSN: 2217-3412, URL: www.ilirias.co/ja Volu 8 Issu 1 2017, Pags 156-163 SOME IDENTITIES FOR THE GENERALIZED POLY-GENOCCHI POLYNOMIALS WITH THE PARAMETERS A, B AND C BURAK

More information

1985 AP Calculus BC: Section I

1985 AP Calculus BC: Section I 985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b

More information

DEPARTMENT OF MATHEMATICS BIT, MESRA, RANCHI MA2201 Advanced Engg. Mathematics Session: SP/ 2017

DEPARTMENT OF MATHEMATICS BIT, MESRA, RANCHI MA2201 Advanced Engg. Mathematics Session: SP/ 2017 DEARMEN OF MAEMAICS BI, MESRA, RANCI MA Advad Egg. Mathatis Sssio: S/ 7 MODULE I. Cosidr th two futios f utorial Sht No. -- ad g o th itrval [,] a Show that thir Wroskia W f, g vaishs idtially. b Show

More information

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris

More information

On the approximation of the constant of Napier

On the approximation of the constant of Napier Stud. Uiv. Babş-Bolyai Math. 560, No., 609 64 O th approximatio of th costat of Napir Adri Vrscu Abstract. Startig from som oldr idas of [] ad [6], w show w facts cocrig th approximatio of th costat of

More information

NET/JRF, GATE, IIT JAM, JEST, TIFR

NET/JRF, GATE, IIT JAM, JEST, TIFR Istitut for NET/JRF, GATE, IIT JAM, JEST, TIFR ad GRE i PHYSICAL SCIENCES Mathmatical Physics JEST-6 Q. Giv th coditio φ, th solutio of th quatio ψ φ φ is giv by k. kφ kφ lφ kφ lφ (a) ψ (b) ψ kφ (c) ψ

More information

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist

More information

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of

More information

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120 Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,

More information

Inverse Nodal Problems for Differential Equation on the Half-line

Inverse Nodal Problems for Differential Equation on the Half-line Australia Joural of Basic ad Applied Scieces, 3(4): 4498-4502, 2009 ISSN 1991-8178 Iverse Nodal Problems for Differetial Equatio o the Half-lie 1 2 3 A. Dabbaghia, A. Nematy ad Sh. Akbarpoor 1 Islamic

More information

NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES

NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES Digst Joural of Naomatrials ad Biostructurs Vol 4, No, March 009, p 67-76 NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES A IRANMANESH a*, O KHORMALI b, I NAJAFI KHALILSARAEE c, B SOLEIMANI

More information

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges. Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt

More information

Calculus & analytic geometry

Calculus & analytic geometry Calculus & aalytic gomtry B Sc MATHEMATICS Admissio owards IV SEMESTER CORE COURSE UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION CALICUT UNIVERSITYPO, MALAPPURAM, KERALA, INDIA 67 65 5 School of Distac

More information

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2 MATHEMATIS --RE Itgral alculus Marti Huard Witr 9 Rviw Erciss. Evaluat usig th dfiitio of th dfiit itgral as a Rima Sum. Dos th aswr rprst a ara? a ( d b ( d c ( ( d d ( d. Fid f ( usig th Fudamtal Thorm

More information

Iterative Methods of Order Four for Solving Nonlinear Equations

Iterative Methods of Order Four for Solving Nonlinear Equations Itrativ Mods of Ordr Four for Solvig Noliar Equatios V.B. Kumar,Vatti, Shouri Domii ad Mouia,V Dpartmt of Egirig Mamatis, Formr Studt of Chmial Egirig Adhra Uivrsity Collg of Egirig A, Adhra Uivrsity Visakhapatam

More information

+ x. x 2x. 12. dx. 24. dx + 1)

+ x. x 2x. 12. dx. 24. dx + 1) INTEGRATION of FUNCTION of ONE VARIABLE INDEFINITE INTEGRAL Fidig th idfiit itgrals Rductio to basic itgrals, usig th rul f ( ) f ( ) d =... ( ). ( )d. d. d ( ). d. d. d 7. d 8. d 9. d. d. d. d 9. d 9.

More information

STIRLING'S 1 FORMULA AND ITS APPLICATION

STIRLING'S 1 FORMULA AND ITS APPLICATION MAT-KOL (Baja Luka) XXIV ()(08) 57-64 http://wwwimviblorg/dmbl/dmblhtm DOI: 075/МК80057A ISSN 0354-6969 (o) ISSN 986-588 (o) STIRLING'S FORMULA AND ITS APPLICATION Šfkt Arslaagić Sarajvo B&H Abstract:

More information

15/03/1439. Lectures on Signals & systems Engineering

15/03/1439. Lectures on Signals & systems Engineering Lcturs o Sigals & syms Egirig Dsigd ad Prd by Dr. Ayma Elshawy Elsfy Dpt. of Syms & Computr Eg. Al-Azhar Uivrsity Email : aymalshawy@yahoo.com A sigal ca b rprd as a liar combiatio of basic sigals. Th

More information

Derivation of a Predictor of Combination #1 and the MSE for a Predictor of a Position in Two Stage Sampling with Response Error.

Derivation of a Predictor of Combination #1 and the MSE for a Predictor of a Position in Two Stage Sampling with Response Error. Drivatio of a Prdictor of Cobiatio # ad th SE for a Prdictor of a Positio i Two Stag Saplig with Rspos Error troductio Ed Stak W driv th prdictor ad its SE of a prdictor for a rado fuctio corrspodig to

More information

International Journal of Advanced and Applied Sciences

International Journal of Advanced and Applied Sciences Itratioal Joural of Advacd ad Applid Scics x(x) xxxx Pags: xx xx Cotts lists availabl at Scic Gat Itratioal Joural of Advacd ad Applid Scics Joural hompag: http://wwwscic gatcom/ijaashtml Symmtric Fuctios

More information

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms Math Sci Ltt Vol No 8-87 (0) adamard Exotial al Matrix, Its Eigvalus ad Som Norms İ ad M bula Mathmatical Scics Lttrs Itratioal Joural @ 0 NSP Natural Scics Publishig Cor Dartmt of Mathmatics, aculty of

More information

Ordinary Differential Equations

Ordinary Differential Equations Basi Nomlatur MAE 0 all 005 Egirig Aalsis Ltur Nots o: Ordiar Diffrtial Equatios Author: Profssor Albrt Y. Tog Tpist: Sakurako Takahashi Cosidr a gral O. D. E. with t as th idpdt variabl, ad th dpdt variabl.

More information

Restricted Factorial And A Remark On The Reduced Residue Classes

Restricted Factorial And A Remark On The Reduced Residue Classes Applid Mathmatics E-Nots, 162016, 244-250 c ISSN 1607-2510 Availabl fr at mirror sits of http://www.math.thu.du.tw/ am/ Rstrictd Factorial Ad A Rmark O Th Rducd Rsidu Classs Mhdi Hassai Rcivd 26 March

More information

Revised Variational Iteration Method for Solving Systems of Ordinary Differential Equations

Revised Variational Iteration Method for Solving Systems of Ordinary Differential Equations Availabl at http://pvau.du/aa Appl. Appl. Math. ISSN: 9-9 Spcial Iu No. Augut 00 pp. 0 Applicatio ad Applid Mathatic: A Itratioal Joural AAM Rvid Variatioal Itratio Mthod for Solvig St of Ordiar Diffrtial

More information

An Introduction to Asymptotic Expansions

An Introduction to Asymptotic Expansions A Itroductio to Asmptotic Expasios R. Shaar Subramaia Asmptotic xpasios ar usd i aalsis to dscrib th bhavior of a fuctio i a limitig situatio. Wh a fuctio ( x, dpds o a small paramtr, ad th solutio of

More information

COLLECTION OF SUPPLEMENTARY PROBLEMS CALCULUS II

COLLECTION OF SUPPLEMENTARY PROBLEMS CALCULUS II COLLECTION OF SUPPLEMENTARY PROBLEMS I. CHAPTER 6 --- Trscdtl Fuctios CALCULUS II A. FROM CALCULUS BY J. STEWART:. ( How is th umbr dfid? ( Wht is pproimt vlu for? (c ) Sktch th grph of th turl potil fuctios.

More information

Chapter Taylor Theorem Revisited

Chapter Taylor Theorem Revisited Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o

More information

DETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS.

DETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS. ICSV4 Cairs Australia 9- July 7 DTRMINATION OF MCHANICAL PROPRTIS OF A NON- UNIFORM BAM USING TH MASURMNT OF TH XCITD LONGITUDINAL LASTIC VIBRATIONS Pavel Aokhi ad Vladimir Gordo Departmet of the mathematics

More information

Analysis of a Finite Quantum Well

Analysis of a Finite Quantum Well alysis of a Fiit Quatu Wll Ira Ka Dpt. of lctrical ad lctroic girig Jssor Scic & Tcology Uivrsity (JSTU) Jssor-748, Baglads ika94@uottawa.ca Or ikr_c@yaoo.co Joural of lctrical girig T Istitutio of girs,

More information

Chapter At each point (x, y) on the curve, y satisfies the condition

Chapter At each point (x, y) on the curve, y satisfies the condition Chaptr 6. At ach poit (, y) o th curv, y satisfis th coditio d y 6; th li y = 5 is tagt to th curv at th poit whr =. I Erciss -6, valuat th itgral ivolvig si ad cosi.. cos si. si 5 cos 5. si cos 5. cos

More information

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1 DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT

More information

Chapter 3 Fourier Series Representation of Periodic Signals

Chapter 3 Fourier Series Representation of Periodic Signals Chptr Fourir Sris Rprsttio of Priodic Sigls If ritrry sigl x(t or x[] is xprssd s lir comitio of som sic sigls th rspos of LI systm coms th sum of th idividul rsposs of thos sic sigls Such sic sigl must:

More information

Lectures 9 IIR Systems: First Order System

Lectures 9 IIR Systems: First Order System EE3054 Sigals ad Systms Lcturs 9 IIR Systms: First Ordr Systm Yao Wag Polytchic Uivrsity Som slids icludd ar xtractd from lctur prstatios prpard by McCllla ad Schafr Lics Ifo for SPFirst Slids This work

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordiary Diffrtial Equatio Aftr radig thi chaptr, you hould b abl to:. dfi a ordiary diffrtial quatio,. diffrtiat btw a ordiary ad partial diffrtial quatio, ad. Solv liar ordiary diffrtial quatio with fid

More information

Problem Value Score Earned No/Wrong Rec -3 Total

Problem Value Score Earned No/Wrong Rec -3 Total GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING ECE6 Fall Quiz # Writt Eam Novmr, NAME: Solutio Kys GT Usram: LAST FIRST.g., gtiit Rcitatio Sctio: Circl t dat & tim w your Rcitatio

More information

Motivation. We talk today for a more flexible approach for modeling the conditional probabilities.

Motivation. We talk today for a more flexible approach for modeling the conditional probabilities. Baysia Ntworks Motivatio Th coditioal idpdc assuptio ad by aïv Bays classifirs ay s too rigid spcially for classificatio probls i which th attributs ar sowhat corrlatd. W talk today for a or flibl approach

More information

Discrete Fourier Transform (DFT)

Discrete Fourier Transform (DFT) Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial

More information

P.L. Chebyshev. The Theory of Probability

P.L. Chebyshev. The Theory of Probability P.L. Chbyshv Th Thory of Probability Traslatd by Oscar Shyi Lcturs dlivrd i 879 88 as tak dow by A.M. Liapuov Brli, 4 Oscar Shyi www.shyi.d.., 879 88.....!" 936 Cotts Itroductio by th Traslator Forword

More information

Thomas J. Osler. 1. INTRODUCTION. This paper gives another proof for the remarkable simple

Thomas J. Osler. 1. INTRODUCTION. This paper gives another proof for the remarkable simple 5/24/5 A PROOF OF THE CONTINUED FRACTION EXPANSION OF / Thomas J Oslr INTRODUCTION This ar givs aothr roof for th rmarkabl siml cotiud fractio = 3 5 / Hr is ay ositiv umbr W us th otatio x= [ a; a, a2,

More information

A Simple Proof that e is Irrational

A Simple Proof that e is Irrational Two of th most bautiful ad sigificat umbrs i mathmatics ar π ad. π (approximatly qual to 3.459) rprsts th ratio of th circumfrc of a circl to its diamtr. (approximatly qual to.788) is th bas of th atural

More information

SECTION 2.6 THE SECOND ALTERNATIVE

SECTION 2.6 THE SECOND ALTERNATIVE 54 SECTION 2.6 THE SECOND ALTERNATIVE We ow discuss the probles where the Secod Alterative holds. The suppositio is that there is a otrivial solutio for L(y) =, B (y) = B 2 (y) =. The Fredhol Theores assure

More information

7. Differentiation of Trigonometric Function

7. Differentiation of Trigonometric Function 7. Diffrtiatio of Trigootric Fctio RADIAN MEASURE. Lt s ot th lgth of arc AB itrcpt y th ctral agl AOB o a circl of rais r a lt S ot th ara of th sctor AOB. (If s is /60 of th circfrc, AOB = 0 ; if s =

More information

New Families of Fourth-Order Derivative-Free Methods for Solving Nonlinear Equations with Multiple Roots

New Families of Fourth-Order Derivative-Free Methods for Solving Nonlinear Equations with Multiple Roots Arica Joural o Coputatioal ad Applid Mathatics (4: 7- DOI:.59/j.ajca.4. Nw Failis o Fourth-Ordr Drivativ-Fr Mthods or Solvig Noliar Equatios with Multipl Roots R. Thukral Padé Rsarch Ctr 9 Daswood Hill

More information

Linear Algebra Existence of the determinant. Expansion according to a row.

Linear Algebra Existence of the determinant. Expansion according to a row. Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit

More information

07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n

07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n 07 - SEQUENCES AND SERIES Pag ( Aswrs at h d of all qustios ) ( ) If = a, y = b, z = c, whr a, b, c ar i A.P. ad = 0 = 0 = 0 l a l

More information

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions Solutios for HW 8 Captr 5 Cocptual Qustios 5.. θ dcrass. As t crystal is coprssd, t spacig d btw t plas of atos dcrass. For t first ordr diffractio =. T Bragg coditio is = d so as d dcrass, ust icras for

More information

The Interplay between l-max, l-min, p-max and p-min Stable Distributions

The Interplay between l-max, l-min, p-max and p-min Stable Distributions DOI: 0.545/mjis.05.4006 Th Itrplay btw lma lmi pma ad pmi Stabl Distributios S Ravi ad TS Mavitha Dpartmt of Studis i Statistics Uivrsity of Mysor Maasagagotri Mysuru 570006 Idia. Email:ravi@statistics.uimysor.ac.i

More information

Probability & Statistics,

Probability & Statistics, Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said

More information

Time regularity of solutions to linear equations with Lévy noise in infinite dimensions

Time regularity of solutions to linear equations with Lévy noise in infinite dimensions Tim rgularity of solutios to liar quatios with Lévy ois i ifiit dimsios S. Pszat Faculty of Applid Mathmatics, AG Uivrsity of Scic ad Tchology, Kraków, Polad, E-mail adrss: apszat@cyf-kr.du.pl. J. Zabczyk

More information

Legendre Wavelets for Systems of Fredholm Integral Equations of the Second Kind

Legendre Wavelets for Systems of Fredholm Integral Equations of the Second Kind World Applid Scincs Journal 9 (9): 8-, ISSN 88-495 IDOSI Publications, Lgndr Wavlts for Systs of Frdhol Intgral Equations of th Scond Kind a,b tb (t)= a, a,b a R, a. J. Biazar and H. Ebrahii Dpartnt of

More information

Problem. Consider the sequence a j for j N defined by the recurrence a j+1 = 2a j + j for j > 0

Problem. Consider the sequence a j for j N defined by the recurrence a j+1 = 2a j + j for j > 0 GENERATING FUNCTIONS Give a ifiite sequece a 0,a,a,, its ordiary geeratig fuctio is A : a Geeratig fuctios are ofte useful for fidig a closed forula for the eleets of a sequece, fidig a recurrece forula,

More information

Folding of Hyperbolic Manifolds

Folding of Hyperbolic Manifolds It. J. Cotmp. Math. Scics, Vol. 7, 0, o. 6, 79-799 Foldig of Hyprbolic Maifolds H. I. Attiya Basic Scic Dpartmt, Collg of Idustrial Educatio BANE - SUEF Uivrsity, Egypt hala_attiya005@yahoo.com Abstract

More information

Class #24 Monday, April 16, φ φ φ

Class #24 Monday, April 16, φ φ φ lass #4 Moday, April 6, 08 haptr 3: Partial Diffrtial Equatios (PDE s First of all, this sctio is vry, vry difficult. But it s also supr cool. PDE s thr is mor tha o idpdt variabl. Exampl: φ φ φ φ = 0

More information

On a problem of J. de Graaf connected with algebras of unbounded operators de Bruijn, N.G.

On a problem of J. de Graaf connected with algebras of unbounded operators de Bruijn, N.G. O a problm of J. d Graaf coctd with algbras of uboudd oprators d Bruij, N.G. Publishd: 01/01/1984 Documt Vrsio Publishr s PDF, also kow as Vrsio of Rcord (icluds fial pag, issu ad volum umbrs) Plas chck

More information

Chapter 4. Fourier Series

Chapter 4. Fourier Series Chapter 4. Fourier Series At this poit we are ready to ow cosider the caoical equatios. Cosider, for eample the heat equatio u t = u, < (4.) subject to u(, ) = si, u(, t) = u(, t) =. (4.) Here,

More information

UNIVERSALITY LIMITS INVOLVING ORTHOGONAL POLYNOMIALS ON AN ARC OF THE UNIT CIRCLE

UNIVERSALITY LIMITS INVOLVING ORTHOGONAL POLYNOMIALS ON AN ARC OF THE UNIT CIRCLE UNIVERSALITY LIMITS INVOLVING ORTHOGONAL POLYNOMIALS ON AN ARC OF THE UNIT CIRCLE DORON S. LUBINSKY AND VY NGUYEN A. W stablish uivrsality limits for masurs o a subarc of th uit circl. Assum that µ is

More information

Discrete Fourier Transform. Nuno Vasconcelos UCSD

Discrete Fourier Transform. Nuno Vasconcelos UCSD Discrt Fourir Trasform uo Vascoclos UCSD Liar Shift Ivariat (LSI) systms o of th most importat cocpts i liar systms thory is that of a LSI systm Dfiitio: a systm T that maps [ ito y[ is LSI if ad oly if

More information

CORRECTIONS TO THE WU-SPRUNG POTENTIAL FOR THE RIEMANN ZEROS AND A NEW HAMILTONIAN WHOSE ENERGIES ARE THE PRIME NUMBERS

CORRECTIONS TO THE WU-SPRUNG POTENTIAL FOR THE RIEMANN ZEROS AND A NEW HAMILTONIAN WHOSE ENERGIES ARE THE PRIME NUMBERS CORRECTIONS TO THE WU-SPRUNG POTENTIAL FOR THE RIEMANN ZEROS AND A NEW HAMILTONIAN WHOSE ENERGIES ARE THE PRIME NUMBERS Jos Javir Garcia Morta Graduat studt of Physics at th UPV/EHU (Uivrsity of Basqu

More information

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.

More information

10. Joint Moments and Joint Characteristic Functions

10. Joint Moments and Joint Characteristic Functions 0 Joit Momts ad Joit Charactristic Fctios Followig sctio 6 i this sctio w shall itrodc varios paramtrs to compactly rprst th iformatio cotaid i th joit pdf of two rvs Giv two rvs ad ad a fctio g x y dfi

More information

Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations

Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations Iteratioal Joural o Recet ad Iovatio Treds i Coputig ad Couicatio IN: 31-8169 Volue: 5 Issue: 5 16 Applicatio of Hootopy Aalysis Meod for olvig various types of Probles of Ordiary Differetial Equatios

More information

H2 Mathematics Arithmetic & Geometric Series ( )

H2 Mathematics Arithmetic & Geometric Series ( ) H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic

More information

Journal of Modern Applied Statistical Methods

Journal of Modern Applied Statistical Methods Joural of Modr Applid Statistical Mthods Volum Issu Articl 6 --03 O Som Proprtis of a Htrogous Trasfr Fuctio Ivolvig Symmtric Saturatd Liar (SATLINS) with Hyprbolic Tagt (TANH) Trasfr Fuctios Christophr

More information

Bertrand s postulate Chapter 2

Bertrand s postulate Chapter 2 Bertrad s postulate Chapter We have see that the sequece of prie ubers, 3, 5, 7,... is ifiite. To see that the size of its gaps is ot bouded, let N := 3 5 p deote the product of all prie ubers that are

More information

SOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3

SOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3 SOLVED EXAMPLES E. If f() E.,,, th f() f() h h LHL RHL, so / / Lim f() quls - (D) Dos ot ist [( h)+] [(+h) + ] f(). LHL E. RHL h h h / h / h / h / h / h / h As.[C] (D) Dos ot ist LHL RHL, so giv it dos

More information

APPENDIX: STATISTICAL TOOLS

APPENDIX: STATISTICAL TOOLS I. Nots o radom samplig Why do you d to sampl radomly? APPENDI: STATISTICAL TOOLS I ordr to masur som valu o a populatio of orgaisms, you usually caot masur all orgaisms, so you sampl a subst of th populatio.

More information

The Application of Eigenvectors for the Construction of Minimum-Energy Wavelet Frames Based on FMRA

The Application of Eigenvectors for the Construction of Minimum-Energy Wavelet Frames Based on FMRA Applid ad Coputatioal Mathatics 0; 7(3: 6-66 http://www.scicpublishiggroup.co/j/ac doi: 0.6/j.ac.00703. ISS: 3-5605 (Prit; ISS: 3-563 (Oli Th Applicatio of Eigvctors for th Costructio of Miiu-Ergy Wavlt

More information

ECE 901 Lecture 4: Estimation of Lipschitz smooth functions

ECE 901 Lecture 4: Estimation of Lipschitz smooth functions ECE 9 Lecture 4: Estiatio of Lipschitz sooth fuctios R. Nowak 5/7/29 Cosider the followig settig. Let Y f (X) + W, where X is a rado variable (r.v.) o X [, ], W is a r.v. o Y R, idepedet of X ad satisfyig

More information

Statistics 3858 : Likelihood Ratio for Exponential Distribution

Statistics 3858 : Likelihood Ratio for Exponential Distribution Statistics 3858 : Liklihood Ratio for Expotial Distributio I ths two xampl th rjctio rjctio rgio is of th form {x : 2 log (Λ(x)) > c} for a appropriat costat c. For a siz α tst, usig Thorm 9.5A w obtai

More information

Introduction to Quantum Information Processing. Overview. A classical randomised algorithm. q 3,3 00 0,0. p 0,0. Lecture 10.

Introduction to Quantum Information Processing. Overview. A classical randomised algorithm. q 3,3 00 0,0. p 0,0. Lecture 10. Itroductio to Quatum Iformatio Procssig Lctur Michl Mosca Ovrviw! Classical Radomizd vs. Quatum Computig! Dutsch-Jozsa ad Brsti- Vazirai algorithms! Th quatum Fourir trasform ad phas stimatio A classical

More information

Fooling Newton s Method a) Find a formula for the Newton sequence, and verify that it converges to a nonzero of f. A Stirling-like Inequality

Fooling Newton s Method a) Find a formula for the Newton sequence, and verify that it converges to a nonzero of f. A Stirling-like Inequality Foolig Nwto s Mthod a Fid a formla for th Nwto sqc, ad vrify that it covrgs to a ozro of f. ( si si + cos 4 4 3 4 8 8 bt f. b Fid a formla for f ( ad dtrmi its bhavior as. f ( cos si + as A Stirlig-li

More information

Assignment Number 3 Solutions

Assignment Number 3 Solutions Math 4354, Assigmet Number 3 Solutios 1. u t (x, t) = u xx (x, t), < x (1) u(, t) =, u(, t) = u(x, ) = x ( 1) +1 u(x, t) = e t si(x). () =1 Solutio: Look for simple solutios i the form u(x, t) =

More information

Combined effects of Hall current and rotation on free convection MHD flow in a porous channel

Combined effects of Hall current and rotation on free convection MHD flow in a porous channel Idia Joural of Pur & Applid Physics Vol. 47, Sptbr 009, pp. 67-63 Cobid ffcts of Hall currt ad rotatio o fr covctio MHD flow i a porous chal K D Sigh & Raksh Kuar Dpartt of Mathatics (ICDEOL, H P Uivrsy,

More information

Empirical Study in Finite Correlation Coefficient in Two Phase Estimation

Empirical Study in Finite Correlation Coefficient in Two Phase Estimation M. Khoshvisa Griffith Uivrsity Griffith Busiss School Australia F. Kaymarm Massachustts Istitut of Tchology Dpartmt of Mchaical girig USA H. P. Sigh R. Sigh Vikram Uivrsity Dpartmt of Mathmatics ad Statistics

More information

Sigma notation. 2.1 Introduction

Sigma notation. 2.1 Introduction Sigma otatio. Itroductio We use sigma otatio to idicate the summatio process whe we have several (or ifiitely may) terms to add up. You may have see sigma otatio i earlier courses. It is used to idicate

More information

PH4210 Statistical Mechanics

PH4210 Statistical Mechanics PH4 Statistical Mchaics Probl Sht Aswrs Dostrat that tropy, as giv by th Boltza xprssio S = l Ω, is a xtsiv proprty Th bst way to do this is to argu clarly that Ω is ultiplicativ W ust prov that if o syst

More information

Time Dependent Solutions: Propagators and Representations

Time Dependent Solutions: Propagators and Representations Tim Dpdt Solutios: Propagators ad Rprstatios Michal Fowlr, UVa 1/3/6 Itroductio W v spt most of th cours so far coctratig o th igstats of th amiltoia, stats whos tim dpdc is mrly a chagig phas W did mtio

More information

Chapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering

Chapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering haptr. Physical Problm for Fast Fourir Trasform ivil Egirig Itroductio I this chaptr, applicatios of FFT algorithms [-5] for solvig ral-lif problms such as computig th dyamical (displacmt rspos [6-7] of

More information

CDS 101: Lecture 5.1 Reachability and State Space Feedback

CDS 101: Lecture 5.1 Reachability and State Space Feedback CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray ad Hido Mabuchi 5 Octobr 4 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls

More information

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr

More information

Chapter 2. Asymptotic Notation

Chapter 2. Asymptotic Notation Asyptotic Notatio 3 Chapter Asyptotic Notatio Goal : To siplify the aalysis of ruig tie by gettig rid of details which ay be affected by specific ipleetatio ad hardware. [1] The Big Oh (O-Notatio) : It

More information

Электронный архив УГЛТУ ЭКО-ПОТЕНЦИАЛ 2 (14),

Электронный архив УГЛТУ ЭКО-ПОТЕНЦИАЛ 2 (14), УДК 004.93'; 004.93 Электронный архив УГЛТУ ЭКО-ПОТЕНЦИАЛ (4), 06 V. Labuts, I. Artmov, S. Martyugi & E. Osthimr Ural dral Uivrsity, Ykatriburg, Russia Capricat LLC, USA AST RACTIOAL OURIER TRASORMS BASED

More information

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 116C. Problem Set 4. Benjamin Stahl. November 6, 2014

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 116C. Problem Set 4. Benjamin Stahl. November 6, 2014 UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 6C Problem Set 4 Bejami Stahl November 6, 4 BOAS, P. 63, PROBLEM.-5 The Laguerre differetial equatio, x y + ( xy + py =, will be solved

More information

An Introduction to Asymptotic Expansions

An Introduction to Asymptotic Expansions A Itroductio to Asmptotic Expasios R. Shaar Subramaia Dpartmt o Chmical ad Biomolcular Egirig Clarso Uivrsit Asmptotic xpasios ar usd i aalsis to dscrib th bhavior o a uctio i a limitig situatio. Wh a

More information

2. Fourier Series, Fourier Integrals and Fourier Transforms

2. Fourier Series, Fourier Integrals and Fourier Transforms Mathematics IV -. Fourier Series, Fourier Itegrals ad Fourier Trasforms The Fourier series are used for the aalysis of the periodic pheomea, which ofte appear i physics ad egieerig. The Fourier itegrals

More information

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad

More information

Law of large numbers

Law of large numbers Law of larg umbrs Saya Mukhrj W rvisit th law of larg umbrs ad study i som dtail two typs of law of larg umbrs ( 0 = lim S ) p ε ε > 0, Wak law of larrg umbrs [ ] S = ω : lim = p, Strog law of larg umbrs

More information

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1 Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida

More information

Chapter 4 - The Fourier Series

Chapter 4 - The Fourier Series M. J. Robrts - 8/8/4 Chaptr 4 - Th Fourir Sris Slctd Solutios (I this solutio maual, th symbol,, is usd for priodic covolutio bcaus th prfrrd symbol which appars i th txt is ot i th fot slctio of th word

More information

BOUNDS FOR THE COMPONENTWISE DISTANCE TO THE NEAREST SINGULAR MATRIX

BOUNDS FOR THE COMPONENTWISE DISTANCE TO THE NEAREST SINGULAR MATRIX SIAM J. Matrix Aal. Appl. (SIMAX), 8():83 03, 997 BOUNDS FOR THE COMPONENTWISE DISTANCE TO THE NEAREST SINGULAR MATRIX S. M. RUMP Abstract. Th ormwis distac of a matrix A to th arst sigular matrix is wll

More information

A Note on Quantile Coupling Inequalities and Their Applications

A Note on Quantile Coupling Inequalities and Their Applications A Not o Quatil Couplig Iqualitis ad Thir Applicatios Harriso H. Zhou Dpartmt of Statistics, Yal Uivrsity, Nw Hav, CT 06520, USA. E-mail:huibi.zhou@yal.du Ju 2, 2006 Abstract A rlatioship btw th larg dviatio

More information

Numerov-Cooley Method : 1-D Schr. Eq. Last time: Rydberg, Klein, Rees Method and Long-Range Model G(v), B(v) rotation-vibration constants.

Numerov-Cooley Method : 1-D Schr. Eq. Last time: Rydberg, Klein, Rees Method and Long-Range Model G(v), B(v) rotation-vibration constants. Numrov-Cooly Mthod : 1-D Schr. Eq. Last tim: Rydbrg, Kli, Rs Mthod ad Log-Rag Modl G(v), B(v) rotatio-vibratio costats 9-1 V J (x) pottial rgy curv x = R R Ev,J, v,j, all cocivabl xprimts wp( x, t) = ai

More information

Triple Play: From De Morgan to Stirling To Euler to Maclaurin to Stirling

Triple Play: From De Morgan to Stirling To Euler to Maclaurin to Stirling Tripl Play: From D Morga to Stirlig To Eulr to Maclauri to Stirlig Augustus D Morga (186-1871) was a sigificat Victoria Mathmaticia who mad cotributios to Mathmatics History, Mathmatical Rcratios, Mathmatical

More information

Ma 530 Introduction to Power Series

Ma 530 Introduction to Power Series Ma 530 Itroductio to Power Series Please ote that there is material o power series at Visual Calculus. Some of this material was used as part of the presetatio of the topics that follow. What is a Power

More information

ASSERTION AND REASON

ASSERTION AND REASON ASSERTION AND REASON Som qustios (Assrtio Rso typ) r giv low. Ech qustio cotis Sttmt (Assrtio) d Sttmt (Rso). Ech qustio hs choics (A), (B), (C) d (D) out of which ONLY ONE is corrct. So slct th corrct

More information

Fourth Part: The Interplay of Algebra and Logic

Fourth Part: The Interplay of Algebra and Logic Fourth Part: Th Intrplay of Algbra and Logic Francsco Paoli TACL 2013 Francsco Paoli (Univ. of Cagliari) Tutorial on algbraic logic TACL 2013 1 / 18 Adissibility of cut Cut liination, in proof-thortic

More information

CHAPTER 5. Theory and Solution Using Matrix Techniques

CHAPTER 5. Theory and Solution Using Matrix Techniques A SERIES OF CLASS NOTES FOR 2005-2006 TO INTRODUCE LINEAR AND NONLINEAR PROBLEMS TO ENGINEERS, SCIENTISTS, AND APPLIED MATHEMATICIANS DE CLASS NOTES 3 A COLLECTION OF HANDOUTS ON SYSTEMS OF ORDINARY DIFFERENTIAL

More information