On Fractional Governing Equations of Spherical Particles Settling in Water

Size: px
Start display at page:

Download "On Fractional Governing Equations of Spherical Particles Settling in Water"

Transcription

1 Ameica Joual of Egieeig, Techology ad Sociey 7; 4(6): 5-9 hp:// ISSN: (Pi); ISSN: 38-68X (Olie) O Facioal Goveig Equaios of Spheical Paicles Selig i Wae Kama Ayub, M. Yaqub Kha, Qazi Mahmood Ul-Hassa, Memmoa Yaqub 3 Depame of Mahemaics, Riphah Ieaioal Uivesiy, Islamabad, Pakisa Depame of Mahemaics, Uivesiy of Wah, Wah Ca., Pakisa 3 Depame of Mahemaics, Allama Iqbal Ope Uivesiy, Islamabad, Pakisa addess kamaayub88@gmail.com (K. Ayub) To cie his aicle Kama Ayub, M. Yaqub Kha, Qazi Mahmood Ul-Hassa, Memmoa Yaqub. O Facioal Goveig Equaios of Spheical Paicles Selig i Wae. Ameica Joual of Egieeig, Techology ad Sociey. Vol. 4, No. 6, 7, pp Received: Mach 4, 7; Acceped: May 4, 7; Published: Novembe 7, 7 Absac This pape shows a sucue o ge he esul o he ueve sele acios of few solid spheical paicles decliig i wae as a Newoia fluid by homoopy aalysis mehod. The paial deivaive is descibed i Modified Riema liouville sese. This mehod pefoms vey well i compeece. Numeical esuls eplai he whole cosisecy i used algoihm. Keywods Homoopy Aalysis Mehod, Spheical Paicles, Dag Coefficie, Facioal Calculus, Sedimeaio Pheomeo, Modified Riema-Liouville Facioal Deivaive. Ioducio I cue ime, he facioal ode diffeeial equaios have bee happeig i may subsaial ad egieeig poblems such like fequecy depede damp aciviies of maeial, diffusio pocesses, moio of a lage hi plae i a Newoia fluid, ceepig ad elaaio fucios fo viscoelasic maeials. Fo moe deails o he applicaios of facioal deivaives i vaiey ad saisical mechaics see [-4]. Mos facioal diffeeial equaios do o have accuae aalyical soluios, heefoe appoimae ad umeical echiques mus be used. Leaig of egossed bodies moio i fluids has log bee a subjec of gea iees due o is massive applicaios i aue ad idusy e.g. Sedime aspo ad deposiio i pipelies. The selig of a eiy, icludig a solid paicle, bubble, o dop, boh i a Newoia fluid ad i a o-newoia fluid, is epoed by Bidge ad Bee [5] ad Chhaba [6]. Haide ad Levespiel [7] offeed seveal heave coefficies fo spheical ad o-spheical paicles [8]. A paicle fallig veically i a fluid ude he ifluece of gaviy will acceleae uil he gaviaioal foce is easoable by he suggle foces, icludig buoyacy ad dag foces. Whe he paicle eaches o a cosa velociy, i s called as emial velociy o selig velociy. The familiaiy of he emial velociy of solids decliig i liquids is equied i may idusial applicaios such as mieal pocessig, solid-liquid miig, hydaulic aspo, sluy sysems, aspig wae jes, fluidized bed eacos ad so o. I is uambiguous ha mos of he pevious ivesigaios ae caied ou fo seady-sae codiios, whee he paicles aai o emial velociy, ad sligh of hem has bee epoed abou he useady moio of spheical objecs.. Mahemaical Fomulaio Fo modelig he paicle sedime pheomeo, coside a small, igid spheical, o-defomable shape of diamee D, mass m ad desiy as paicle which is fallig i ifiie ee filled wae as a icompessible Newoia fluid. Desiy of wae ρ ad is viscosiy µ ae kow. We jus cosideed he gaviy, buoyacy ad dag foces o paicle ad assumed ρ < < ρ. s ρ s Rewiig foce balace fo paicle, he equaio of moio is as follows

2 6 Kama Ayub e al.: O Facioal Goveig Equaios of Spheical Paicles Selig i Wae d w ρ 3 m = mg π D ρcd w π D ρ w, d ρs 8 whee is he dag coefficie, i he igh had side of he Eq. (), he fis em epeses he buoyacy affec, he secod em coespods o dag esisace, ad he las em is due o he added mass effec which is due o acceleaio of fluid aoud he paicle. The mai difficuly o solve Eq. () is o-liea ems due o he o-lieaiy aue of he dag coefficie () Feeia e al. [9], i hei aalyical sudy, suggesed a coelaio fo of spheical paicles which has good ageeme wih he epeimeal daa i a 5 wide age of Reyolds umbe, Re ad is give by CD 4 = Re Re + 48 The mass of he spheical paicle is () 3 m = π D ρs (3) 6 Subsiuig Equaios () ad (3) io Eq. (), we have whee d w a bw cw d, w( ) d + + = = (4) 3 a = π D ( ρs + ρ ) (5) b = 3π D µ (6) c = π D ρ (7) 6 3 d = π D g ( ρs ρ ) (8) 6 I ece yeas hee has bee a gea deal of iees i facioal diffeeial equaios. These equaios aise i coiuous ime adom walks, modelig of aomalous diffusive ad sub diffusive sysems, uificaio of diffusio ad wave popagaio pheomeo, ad simplificaio of he esuls ad moe applicaios wee sudied i [, ]. Ou coce i his wok is o coside he aalyical soluio of he oliea diffeeial equaio wih imefacioal deivaives of he fom: + + = = <,> (9) Equaio (9) educes o he classical oliea diffeeial equaio (4) fo =. The objecive of his pape is o eed he applicaio of he homoopy aalysis mehod (HAM) by usig modified Reima-Liouville deivaive [- 6] o obai aalyic soluios o he ime-facioal equaio of some spheical paicles selig i wae. The homoopy aalysis mehod is a compuaioal mehod ha yields aalyical soluios ad has ceai advaages ove sadad umeical mehods. I is fee fom oudig off eos, as i does o ivolve disceizaio, ad does o equie lage compue obaied memoy o powe. The mehod ioduces he soluio i he fom of a covege facioal seies wih elegaly compuable ems. The HAM is developed i 99 by Liao i [7-6]. By he pese mehod, umeical esuls ca be obaied wih usig a few ieaios. The HAM coais he auiliay paamee ħ, which povides us wih a simple way o adjus ad cool he covegece egio of soluio seies fo lage values of. Ulike, ohe umeical mehods ae give low degee of accuacy fo lage values of. Theefoe, he HAM hadles liea ad oliea poblems wihou ay assumpio ad esicio. 3. Modified Riema-Liouville Deivaive Assume h: R R, h( ) deoe a coiuous (bu o ecessaily diffeeiable) fucio ad le he paiio h > i he ieval [,]. Though he facioal Riema Liouville iegal I h( ) = ( ψ) f ( ψ) dψ, > () Γα The modified Riema-Liouville deivaive is defied as d D h( ) = ( ψ) ( f ( ψ) f ()) dψ, () Γ( ) d Whee [,], < ad G. Jumaie s deivaive is defied hough he facioal diffeece k = ( FW ) h( ) = ( ) f[ + ( k) h], () k Whee FW h( ) = h( + h). The he facioal deivaive is defied as he followig limi, f ( ) f ( ) = lim h (3) h The poposed modified Riema Liouville deivaive as show i equaio () is sicly equivale o equaio. (3). Meawhile, we would ioduce some popeies of he facioal modified Riema Liouville deivaive i equaios. (4) ad (5). (i) Facioal Leibiz poduc law

3 Ameica Joual of Egieeig, Techology ad Sociey 7; 4(6): ( ) ( ) w v wv D ( wv) = + (4) (ii) Facioal Leibiz fomulaio I D h( ) = h( ) h(), < (5) Theefoe, he iegaio by pa ca be used duig he facioal calculus ( ) ( ) b a b I w v ( wv)/ b I a = wv (6) a (iii) Iegaio wih espec o( dψ ). Assume h( ) deoe a coiuous R R fucio, we use he followig equaliy fo he iegal wih espec o( dw) α I h( ) = ( ψ) f ( ψ) dψ, < ΓΒ = f ( ψ ) d ( ψ ) Γ ( + ) 4. Homoopy Aalysis Mehod (HAM) We coside he followig diffeeial equaio ( ) (7) HD w, =, (8) Whee HD is a oliea opeao fo his poblem, ad w, is a ukow deoe a idepede vaiables, ( ) fucio. I he fame of HAM, we ca cosuc he followig zeoh-ode defomaio: ( q) L( w( q) w ( )) q H ( ) HD( w( q) ), ;, = ħ,, ;, (9) whee [,] q is he embeddig paamee, ħ is a auiliay paamee, H (, ) is a auiliay fucio, L is a auiliay liea opeao, w (, ) is a iiial guess of w(, ) ad w(, ; q ) is a ukow fucio of he idepede vaiables, ad q. Obviously, whe q = ad q =, i holds (, ;) = w (, ), w( ) w( ) w, ; =,, () Usig he paamee q, we epad W (, ; q ) i Taylo seies as follows: whee w, ; q = w, + w, q, () ( ) ( ) ( ) = ( ; ) w q w =! q q = () Assume ha he auiliay liea opeao, he iiial guess, H, he auiliay paamee ħ ad he auiliay fucio ( ) ae seleced such ha he seies (9) is covege aq =, he due o () we have Le us defie he veco (, ) (, ) (, ) w = w + w (3) { = (, ) (, ), (, ),..., (, )} w = w w w (4) Diffeeiaig () imes wih espec o he embeddig paamee q, he seig q = ad fially dividig hem by!, we have he so-called h-ode defomaio equaio whee ( ) ( ) = ( ) ( ) L W, χw, ħ H, R w, (5) R w ( ) =! ( ) ( ( ; )) HD w q q, ad χ = >., (6) q = (7) Fially, fo he pupose of compuaio, we will appoimae he HAM soluio (3) by he followig ucaed seies: ϕ 5. Applicaios ( ) w ( ) =. (8) k= I his secio, we demosae he efficiecy ad effeciveess of he Homoopy aalysis mehod wih modified Riema Liouville deivaive. Fo he case, a = b = c = d =, eq. (9) becomes k d w( ) + w( ) + w ( ) =, <, (9) d Subjec o he iiial codiio w () =. Cosucig he followig Homoopy, Accodig o (9), he zeoh-ode defomaio ca be give by

4 8 Kama Ayub e al.: O Facioal Goveig Equaios of Spheical Paicles Selig i Wae ( ) ( q) L w(, ; q) w (, ) ( ) ( ) ( ) ( ) ( ) = qħh, D w, ; q + w, ; q + w, ; q w, = We ca sa wih a iiial appoimaio ( ) ad we choose he auiliay liea opeao wih he popey ( ( )) = D w( q) L w, ; q, ;, L( C ) =, whee C is a iegal cosa. We also choose he auiliay fucio o be H (, ) =. Hece, he h-ode defomaio ca be give by whee ( ) ( ) = ( ) ( ) L w, χw, ħ H, R uw, R ( w ) = D ( w ) + w + ww (3) i j i= Now he soluio of he h-ode defomaio equaios (4) fo become ( ) χ ( ) ( ) w, = w, + ħ L R w. (3) Cosequely, (foħ = ) he fis few ems of he HAM seies soluio ae as follows: w (, ) =, w (, ) =, Γ ( + ) w (, ) =, Γ ( + ) Γ ( + ) 3 w3 (, ) =, Γ ( + 3 ) Γ ( + ) Γ ( + 3 ) Γ ( + ) Γ ( + 3 ) 4 w4 (, ) = + +, α Γ ( + 4 ) Γ ( + ) Γ ( + 4 ) Γ ( + 4 ) Γ ( + ) Γ ( + ) ad so o. Hece, he HAM seies soluio (fo ħ = ) is ( ) ( ) ( ) ( ) w, = w, + w, + w, +.. Γ ( + ) 3 w( ) = + Γ ( + ) Γ ( + ) ( 3 ) ( ) ( 3 ) Γ + Γ + Γ + Γ ( + ) Γ ( + 3 ) , Γ ( + 4 ) Γ ( + ) Γ ( + 4 ) Γ ( + 4 ) Γ ( + ) Γ ( + ) (3) Fo =, he equaio (3) ca be educed as w( ) = +... (33) Coclusio I give pape, we use HAM o ge he soluios of he Equaio of some spheical paicles selig i wae. The HAM is saighfowad wihou esicive assumpios, ad he compoes of he seies soluio ca be easily compued usig ay mahemaical symbolic package. The pape peses ha homoopy aalysis mehod ca easily be used o cosuc soluios fo a boad class of oliea poblems wih facioal deivaives. Nomeclaue a, b, c, d Cosas Acc Acceleaio [ m s ] Time [s] w Velociy [ m s] Dag Paicle diamee D coefficie [m] Acc due o g gaviy [ ] m Paicle mass [kg] m s Dyamic µ kg ρ Fluid desiy [ kg ] 3 viscosiy [ ] m ms Spheical paicle desiy [kg/m 3 ] ρ s Refeeces [] I. Podluby, Facioal Diffeeial Equaios, Academic Pess, New Yok, 999. [] J. H. He, Noliea oscillaio wih facioal deivaive ad is applicaios, Ieaioal Cofeece o Vibaig Egieeig 98, Dalia, Chia, 998, pp [3] J. H. He, some applicaios of oliea facioal diffeeial equaios ad hei Appoimaios, Bull. Sci. Techol., 5() (999), [4] J. H. He, appoimae aalyical soluio fo seepage flow wih facioal deivaives i poous Media, Compu. Mehods Appl. Mech. Egg., 67 (998), [5] J. S. Bidge, S. J. Bee, A model fo he eaime ad aspo of sedime gais of mied sizes, shapes, ad desiies, Wae Resou. Res. 8 () (99) [6] R. P. Chhaba, Bubbles, Dops ad Paicles i No- Newoia Fluids, CRC Pess, Boca Rao, FL, 993. [7] Haide, O. Levespiel, Dag coefficies ad emial velociy of spheical ad o-spheical paicles, Powde Tech. 58 (989) [8] M. Jalaal, D. D. Gaji, G. Ahmadi, Aalyical ivesigaio o acceleaio moio of a veically fallig spheical paicle i icompessible Newoia media, Adv. Powde Tech. ()

5 Ameica Joual of Egieeig, Techology ad Sociey 7; 4(6): [9] J. M. Feeia, M. Duae Naia, R. P. Chhaba, A aalyical sudy of he asie moio of a dese igid sphee i a icompessible Newoia fluid, Chem. Eg. Commu. 68 () (998). [] S. Abbasbady, Appoimae soluio fo he oliea model of diffusio ad eacio i poous caalyss by meas of he homoopy aalysis mehod. Chem. Eg. J. 7. doi:.6/j.cej [] A. M. Wazwaz, Blow-up fo soluios of some liea wave equaios wih mied oliea Bouday codiios. Appl Mah Compu ; 3:57 9. [] G. Jumaie, Table of some basic facioal calculus fomulae deived fom a modified Riema Liouville deivaive fo o-diffeeiable fucios, Appl. Mah. Le. (9) [3] B. J. Wes, M. Bologab, P. Gigolii, Physics of Facioal Opeaos, Spige, New Yok, 3. [4] K. S. Mille, B. Ross, a Ioducio o he Facioal Calculus ad Facioal Diffeeial Equaios, Wiley, New Yok, 993. [5] S. G. Samko, A. A. Kilbas, O. I. Maichev, Facioal Iegals ad Deivaives: Theoy ad Applicaios, Godo ad Beach, Yvedo, 993. [6] S. Momai, Z. Odiba, I. Hashim, Algoihms fo oliea facioal paial diffeeial equaios: A selecio of umeical mehods, Topological Mehods i Noliea Aalysis 3 (8). [7] S. J. Liao The poposed homoopy aalysis echique fo he soluio of oliea Poblems. Ph.D. hesis, Shaghai Jiao Tog Uivesiy; 99. [8] S. J. Liao A appoimae soluio echique which does o deped upo small Paamees: a special eample. I J Noliea Mech 995; 3:37 8. [9] S. J. Liao A appoimae soluio echique which does o deped upo small paamees (II): A applicaio i fluid mechaics. I. J. Noliea Mech. 997; 3:85. [] S. J. Liao A eplici, oally aalyic appoimaio of Blasius viscous flow poblems. I. J. Noliea Mech. 999; 34 (4): [] S. J. Liao Beyod peubaio: ioducio o he homoopy aalysis mehod. Boca Rao: Chapma & Hall, CRC Pess; 3. [] S. J. Liao O he homoopy aalysis mehod fo oliea poblems. Appl. Mah. Compu. 4; 47: [3] S. J. Liao Campo A. Aalyic soluios of he empeaue disibuio i Blasius viscous flow poblems. J. Fluid Mech. ; 453:4 5. [4] M. Dehgha, J. Maaa, A. Saadamadi Applicaio of semiaalyic mehods fo he Fizhugh Nagumo equaio which models he asmissio of eve impulses Mah. Mehods Appl. Sci., 33 (), pp [5] R. L. Fosdick, K. R. Rajagopal Themodyamics ad sabiliy of fluids of hid gadepoc. Roy. Soc. Lod. A, 339 (98), pp [6] R. A. Va Gode, K. Vajavelu O he selecio of auiliay fucios opeaos ad co-vegece cool paamees i he applicaio of he homoopy aalysis mehod o oliea diffeeial equaios: a geeal appoach Commu. Noliea Sci. Nume. Simul, 4 (9), pp

Supplementary Information

Supplementary Information Supplemeay Ifomaio No-ivasive, asie deemiaio of he coe empeaue of a hea-geeaig solid body Dea Ahoy, Daipaya Saka, Aku Jai * Mechaical ad Aeospace Egieeig Depame Uivesiy of Texas a Aligo, Aligo, TX, USA.

More information

Comparing Different Estimators for Parameters of Kumaraswamy Distribution

Comparing Different Estimators for Parameters of Kumaraswamy Distribution Compaig Diffee Esimaos fo Paamees of Kumaaswamy Disibuio ا.م.د نذير عباس ابراهيم الشمري جامعة النهرين/بغداد-العراق أ.م.د نشات جاسم محمد الجامعة التقنية الوسطى/بغداد- العراق Absac: This pape deals wih compaig

More information

On a Z-Transformation Approach to a Continuous-Time Markov Process with Nonfixed Transition Rates

On a Z-Transformation Approach to a Continuous-Time Markov Process with Nonfixed Transition Rates Ge. Mah. Noes, Vol. 24, No. 2, Ocobe 24, pp. 85-96 ISSN 229-784; Copyigh ICSRS Publicaio, 24 www.i-css.og Available fee olie a hp://www.gema.i O a Z-Tasfomaio Appoach o a Coiuous-Time Maov Pocess wih Nofixed

More information

The Central Limit Theorems for Sums of Powers of Function of Independent Random Variables

The Central Limit Theorems for Sums of Powers of Function of Independent Random Variables ScieceAsia 8 () : 55-6 The Ceal Limi Theoems fo Sums of Poes of Fucio of Idepede Radom Vaiables K Laipapo a ad K Neammaee b a Depame of Mahemaics Walailak Uivesiy Nakho Si Thammaa 86 Thailad b Depame of

More information

Spectrum of The Direct Sum of Operators. 1. Introduction

Spectrum of The Direct Sum of Operators. 1. Introduction Specu of The Diec Su of Opeaos by E.OTKUN ÇEVİK ad Z.I.ISMILOV Kaadeiz Techical Uivesiy, Faculy of Scieces, Depae of Maheaics 6080 Tabzo, TURKEY e-ail adess : zaeddi@yahoo.co bsac: I his wok, a coecio

More information

Numerical Solution of Sine-Gordon Equation by Reduced Differential Transform Method

Numerical Solution of Sine-Gordon Equation by Reduced Differential Transform Method Poceedigs of he Wold Cogess o Egieeig Vol I WCE, July 6-8,, Lodo, U.K. Nueical Soluio of Sie-Godo Equaio by Reduced Diffeeial Tasfo Mehod Yıldıay Kesi, İbahi Çağla ad Ayşe Beül Koç Absac Reduced diffeeial

More information

Available online at J. Math. Comput. Sci. 2 (2012), No. 4, ISSN:

Available online at   J. Math. Comput. Sci. 2 (2012), No. 4, ISSN: Available olie a h://scik.og J. Mah. Comu. Sci. 2 (22), No. 4, 83-835 ISSN: 927-537 UNBIASED ESTIMATION IN BURR DISTRIBUTION YASHBIR SINGH * Deame of Saisics, School of Mahemaics, Saisics ad Comuaioal

More information

Homotopy Analysis Method for Solving Fractional Sturm-Liouville Problems

Homotopy Analysis Method for Solving Fractional Sturm-Liouville Problems Ausralia Joural of Basic ad Applied Scieces, 4(1): 518-57, 1 ISSN 1991-8178 Homoopy Aalysis Mehod for Solvig Fracioal Surm-Liouville Problems 1 A Neamay, R Darzi, A Dabbaghia 1 Deparme of Mahemaics, Uiversiy

More information

PRICING AMERICAN PUT OPTION WITH DIVIDENDS ON VARIATIONAL INEQUALITY

PRICING AMERICAN PUT OPTION WITH DIVIDENDS ON VARIATIONAL INEQUALITY Joual of Mahemaical cieces: Aaces a Applicaios olume 37 06 Pages 9-36 Aailable a hp://scieificaacescoi DOI: hp://oiog/0864/msaa_700609 PRICIG AMERICA PUT OPTIO ITH DIIDED O ARIATIOAL IEQUALITY XIAOFAG

More information

S, we call the base curve and the director curve. The straight lines

S, we call the base curve and the director curve. The straight lines Developable Ruled Sufaces wih Daboux Fame i iowsi -Space Sezai KIZILTUĞ, Ali ÇAKAK ahemaics Depame, Faculy of As ad Sciece, Ezica Uivesiy, Ezica, Tuey ahemaics Depame, Faculy of Sciece, Aau Uivesiy, Ezuum,

More information

Existence and Smoothness of Solution of Navier-Stokes Equation on R 3

Existence and Smoothness of Solution of Navier-Stokes Equation on R 3 Ieaioal Joual of Mode Noliea Theoy ad Applicaio, 5, 4, 7-6 Published Olie Jue 5 i SciRes. hp://www.scip.og/joual/ijma hp://dx.doi.og/.436/ijma.5.48 Exisece ad Smoohess of Soluio of Navie-Sokes Equaio o

More information

On imploding cylindrical and spherical shock waves in a perfect gas

On imploding cylindrical and spherical shock waves in a perfect gas J. Fluid Mech. (2006), vol. 560, pp. 103 122. c 2006 Cambidge Uivesiy Pess doi:10.1017/s0022112006000590 Pied i he Uied Kigdom 103 O implodig cylidical ad spheical shock waves i a pefec gas By N. F. PONCHAUT,

More information

Capítulo. of Particles: Energy and Momentum Methods

Capítulo. of Particles: Energy and Momentum Methods Capíulo 5 Kieics of Paicles: Eegy ad Momeum Mehods Mecáica II Coes Ioducio Wok of a Foce Piciple of Wok & Eegy pplicaios of he Piciple of Wok & Eegy Powe ad Efficiecy Sample Poblem 3. Sample Poblem 3.

More information

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM Available a hp://pvamu.edu/aam Appl. Appl. Mah. ISSN: 193-9466 Vol. 5, No. Issue (December 1), pp. 575 584 (Previously, Vol. 5, Issue 1, pp. 167 1681) Applicaios ad Applied Mahemaics: A Ieraioal Joural

More information

The Non-Truncated Bulk Arrival Queue M x /M/1 with Reneging, Balking, State-Dependent and an Additional Server for Longer Queues

The Non-Truncated Bulk Arrival Queue M x /M/1 with Reneging, Balking, State-Dependent and an Additional Server for Longer Queues Alied Maheaical Sciece Vol. 8 o. 5 747-75 The No-Tucaed Bul Aival Queue M x /M/ wih Reei Bali Sae-Deede ad a Addiioal Seve fo Loe Queue A. A. EL Shebiy aculy of Sciece Meofia Uiveiy Ey elhebiy@yahoo.co

More information

Relations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems

Relations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems Tish Joal of Aalysis ad Nmbe Theoy 27 Vol 5 No 4 26-3 Available olie a hp://pbssciepbcom/ja/5/4/2 Sciece ad Edcaio Pblishig DOI:269/ja-5-4-2 Relaios o he Aposol Type (p -Fobeis-Ele Polyomials ad Geealizaios

More information

Comparison between Fourier and Corrected Fourier Series Methods

Comparison between Fourier and Corrected Fourier Series Methods Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1

More information

Exact Solution of Unsteady Tank Drainage for Ellis Fluid

Exact Solution of Unsteady Tank Drainage for Ellis Fluid Joual of Applied Fluid Mechaics, Vol, No 6, pp 69-66, Available olie a wwwjafmoliee, IN 75-57, EIN 75-65 DOI: 95/jafm69 Exac oluio of Useady ak Daiae fo Ellis Fluid K N Memo,, F hah ad A M iddiqui Depame

More information

6.2 Improving Our 3-D Graphics Pipeline

6.2 Improving Our 3-D Graphics Pipeline 6.2. IMPROVING OUR 3-D GRAPHICS PIPELINE 8 6.2 Impovig Ou 3-D Gaphics Pipelie We iish ou basic 3D gaphics pipelie wih he implemeaio o pespecive. beoe we do his, we eview homogeeous coodiaes. 6.2. Homogeeous

More information

ON POINTWISE APPROXIMATION OF FUNCTIONS BY SOME MATRIX MEANS OF FOURIER SERIES

ON POINTWISE APPROXIMATION OF FUNCTIONS BY SOME MATRIX MEANS OF FOURIER SERIES M aheaical I equaliies & A pplicaios Volue 19, Nube 1 (216), 287 296 doi:1.7153/ia-19-21 ON POINTWISE APPROXIMATION OF FUNCTIONS BY SOME MATRIX MEANS OF FOURIER SERIES W. ŁENSKI AND B. SZAL (Couicaed by

More information

Analytical solution of tank drainage for electrically conducting power law fluid

Analytical solution of tank drainage for electrically conducting power law fluid Pepis www.pepis.o NO PEE-EVIEWED Posed: 5 Febuay 8 doi:.944/pepis8..v Aalyical soluio of ak daiae fo elecically coduci powe law fluid K. N. Memo,*, A. M. Siddiqui, Syed Feoz Shah, S. Islam 4 Depame of

More information

GENERALIZED FRACTIONAL INTEGRAL OPERATORS AND THEIR MODIFIED VERSIONS

GENERALIZED FRACTIONAL INTEGRAL OPERATORS AND THEIR MODIFIED VERSIONS GENERALIZED FRACTIONAL INTEGRAL OPERATORS AND THEIR MODIFIED VERSIONS HENDRA GUNAWAN Absac. Associaed o a fucio ρ :(, ) (, ), le T ρ be he opeao defied o a suiable fucio space by T ρ f(x) := f(y) dy, R

More information

Outline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem

Outline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem adial diffsio eqaio Febay 4 9 Diffsio Eqaios i ylidical oodiaes ay aeo Mechaical Egieeig 5B Seia i Egieeig Aalysis Febay 4, 9 Olie eview las class Gadie ad covecio boday codiio Diffsio eqaio i adial coodiaes

More information

ON GENERALIZED FRACTIONAL INTEGRAL OPERATORS. ( ρ( x y ) T ρ f(x) := f(y) R x y n dy, R x y n ρ( y )(1 χ )

ON GENERALIZED FRACTIONAL INTEGRAL OPERATORS. ( ρ( x y ) T ρ f(x) := f(y) R x y n dy, R x y n ρ( y )(1 χ ) Scieiae Mahemaicae Japoicae Olie, Vol., 24), 37 38 37 ON GENERALIZED FRACTIONAL INTEGRAL OPERATORS ERIDANI, HENDRA GUNAWAN 2 AND EIICHI NAKAI 3 Received Augus 29, 23; evised Apil 7, 24 Absac. We pove he

More information

New Method to Solve Partial Fractional Differential Equations

New Method to Solve Partial Fractional Differential Equations Global Joal of Pe ad Applied Mahemaics ISSN 973-768 Volme 3 Nmbe 9 7 pp 4735-4746 eseach Idia Pblicaios hp://ipblicaiocom Ne Mehod o Solve Paial Facioal iffeeial Eqaios M iahi E Edfa 3 ad K El ashid 4

More information

ABSOLUTE INDEXED SUMMABILITY FACTOR OF AN INFINITE SERIES USING QUASI-F-POWER INCREASING SEQUENCES

ABSOLUTE INDEXED SUMMABILITY FACTOR OF AN INFINITE SERIES USING QUASI-F-POWER INCREASING SEQUENCES Available olie a h://sciog Egieeig Maheaics Lees 2 (23) No 56-66 ISSN 249-9337 ABSLUE INDEED SUMMABILIY FACR F AN INFINIE SERIES USING QUASI-F-WER INCREASING SEQUENCES SKAIKRAY * RKJAI 2 UKMISRA 3 NCSAH

More information

Samuel Sindayigaya 1, Nyongesa L. Kennedy 2, Adu A.M. Wasike 3

Samuel Sindayigaya 1, Nyongesa L. Kennedy 2, Adu A.M. Wasike 3 Ieraioal Joural of Saisics ad Aalysis. ISSN 48-9959 Volume 6, Number (6, pp. -8 Research Idia Publicaios hp://www.ripublicaio.com The Populaio Mea ad is Variace i he Presece of Geocide for a Simple Birh-Deah-

More information

SOLVING OF THE FRACTIONAL NON-LINEAR AND LINEAR SCHRÖDINGER EQUATIONS BY HOMOTOPY PERTURBATION METHOD

SOLVING OF THE FRACTIONAL NON-LINEAR AND LINEAR SCHRÖDINGER EQUATIONS BY HOMOTOPY PERTURBATION METHOD SOLVING OF THE FRACTIONAL NON-LINEAR AND LINEAR SCHRÖDINGER EQUATIONS BY HOMOTOPY PERTURBATION METHOD DUMITRU BALEANU, ALIREZA K. GOLMANKHANEH,3, ALI K. GOLMANKHANEH 3 Deparme of Mahemaics ad Compuer Sciece,

More information

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of Oe of he commo descipios of cuilie moio uses ph ibles, which e mesuemes mde log he ge d oml o he ph of he picles. d e wo ohogol xes cosideed sepely fo eey is of moio. These coodies poide ul descipio fo

More information

APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY

APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY ZHEN-GUO DENG ad GUO-CHENG WU 2, 3 * School of Mahemaics ad Iformaio Sciece, Guagi Uiversiy, Naig 534, PR Chia 2 Key Laboraory

More information

Degree of Approximation of Fourier Series

Degree of Approximation of Fourier Series Ieaioal Mahemaical Foum Vol. 9 4 o. 9 49-47 HIARI Ld www.m-hiai.com h://d.doi.og/.988/im.4.49 Degee o Aoimaio o Fouie Seies by N E Meas B. P. Padhy U.. Misa Maheda Misa 3 ad Saosh uma Naya 4 Deame o Mahemaics

More information

TDCDFT: Nonlinear regime

TDCDFT: Nonlinear regime Lecue 3 TDCDFT: Noliea egime Case A. Ullich Uivesiy of Missoui Beasque Sepembe 2008 Oveview Lecue I: Basic fomalism of TDCDFT Lecue II: Applicaios of TDCDFT i liea espose Lecue III: TDCDFT i he oliea egime

More information

Contents. Level Set Method. Level Set Method. The Concept. How to Move the Contour?

Contents. Level Set Method. Level Set Method. The Concept. How to Move the Contour? CAD/Gaphics 5, Hog Kog, 7 Decembe 5 A Tuoial o Level Se ad Implici Models fo Solid Pocessig ad Modelig Michael Y. Wag Qi Xia Depame of Auomaio & Compue- Aided Egieeig The Chiese Uivesi of Hog Kog www.acae.cuhk.edu.hk/~uwag

More information

THE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN

THE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN THE SOIL STRUCTURE INTERACTION ANALYSIS BASED ON SUBSTRUCTURE METHOD IN TIME DOMAIN Musafa KUTANIS Ad Muzaffe ELMAS 2 SUMMARY I is pape, a vaiaio of e FEM wic is so-called geeal subsucue meod is caied

More information

On ARMA(1,q) models with bounded and periodically correlated solutions

On ARMA(1,q) models with bounded and periodically correlated solutions Reseach Repot HSC/03/3 O ARMA(,q) models with bouded ad peiodically coelated solutios Aleksade Weo,2 ad Agieszka Wy oma ska,2 Hugo Steihaus Cete, Woc aw Uivesity of Techology 2 Istitute of Mathematics,

More information

The Solution of the One Species Lotka-Volterra Equation Using Variational Iteration Method ABSTRACT INTRODUCTION

The Solution of the One Species Lotka-Volterra Equation Using Variational Iteration Method ABSTRACT INTRODUCTION Malaysia Joural of Mahemaical Scieces 2(2): 55-6 (28) The Soluio of he Oe Species Loka-Volerra Equaio Usig Variaioal Ieraio Mehod B. Baiha, M.S.M. Noorai, I. Hashim School of Mahemaical Scieces, Uiversii

More information

Conditional Convergence of Infinite Products

Conditional Convergence of Infinite Products Coditioal Covegece of Ifiite Poducts William F. Tech Ameica Mathematical Mothly 106 1999), 646-651 I this aticle we evisit the classical subject of ifiite poducts. Fo stadad defiitios ad theoems o this

More information

On Some Fractional Integral Operators Involving Generalized Gauss Hypergeometric Functions

On Some Fractional Integral Operators Involving Generalized Gauss Hypergeometric Functions Available at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 93-9466 Vol. 5, Issue (Decembe ), pp. 3 33 (Peviously, Vol. 5, Issue, pp. 48 47) Applicatios ad Applied Mathematics: A Iteatioal Joual (AAM) O

More information

arxiv: v4 [math.pr] 20 Jul 2016

arxiv: v4 [math.pr] 20 Jul 2016 Submied o he Aals of Applied Pobabiliy ε-strong SIMULATION FOR MULTIDIMENSIONAL STOCHASTIC DIFFERENTIAL EQUATIONS VIA ROUGH PATH ANALYSIS axiv:1403.5722v4 [mah.pr] 20 Jul 2016 By Jose Blache, Xiyu Che

More information

Multiparameter Golay 2-complementary sequences and transforms

Multiparameter Golay 2-complementary sequences and transforms Mulipaamee Golay -plemeay sequeces ad asfoms V.G. Labues, V.P. Chasovsih, E. Osheime Ual Sae Foes Egieeig Uivesiy, Sibisy a, 37, Eaeibug, Russia, 6000 Capica LLC, Pompao Beach, Floida, USA Absac. I his

More information

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to

( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to Compaiso Fuctios I this lesso, we study stability popeties of the oautoomous system = f t, x The difficulty is that ay solutio of this system statig at x( t ) depeds o both t ad t = x Thee ae thee special

More information

International Journal of Mathematics Trends and Technology (IJMTT) Volume 53 Number 5 January 2018

International Journal of Mathematics Trends and Technology (IJMTT) Volume 53 Number 5 January 2018 Ieraioal Joural of Mahemaics reds ad echology (IJM) Volume 53 Number 5 Jauary 18 Effecs of ime Depede acceleraio o he flow of Blood i rery wih periodic body acceleraio mi Gupa #1, Dr. GajedraSaraswa *,

More information

Solving Fractional Vibrational Problem Using Restarted Fractional Adomian s Decomposition Method. Jamshad Ahmad and Syed Tauseef Mohyud-Din

Solving Fractional Vibrational Problem Using Restarted Fractional Adomian s Decomposition Method. Jamshad Ahmad and Syed Tauseef Mohyud-Din Life Siee Joal ;() hp://wwwlifesieesieom Solvig Faioal Vibaioal Poblem Usig Resaed Faioal Adomia s Deomposiio Mehod Jamshad Ahmad ad Syed Taseef Mohyd-Di Depame of Mahemais Faly of Siees HITEC Uivesiy

More information

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition LINEARIZING AND APPROXIMATING THE RBC MODEL SEPTEMBER 7, 200 For f( x, y, z ), mulivariable Taylor liear expasio aroud ( x, yz, ) f ( x, y, z) f( x, y, z) + f ( x, y, z)( x x) + f ( x, y, z)( y y) + f

More information

Real-time TDDFT simulations within SIESTA. Daniel Sánchez-Portal, Rafi Ullah, Fabiano Corsetti, Miguel Pruneda and Emilio Artacho

Real-time TDDFT simulations within SIESTA. Daniel Sánchez-Portal, Rafi Ullah, Fabiano Corsetti, Miguel Pruneda and Emilio Artacho Real-ime TDDFT simulaios wihi SIESTA Daiel Sáchez-Poal, Rafi Ullah, Fabiao Cosei, Miguel Pueda ad Emilio Aacho Mai objecive Apply eal-ime simulaios wihi ime-depede desiy fucioal heoy TDDFT o sudy eleco

More information

Statistical Optics and Free Electron Lasers

Statistical Optics and Free Electron Lasers Saisical Opics ad Fee leco Lases ialuca eloi uopea XFL Los Ageles UCLA Jauay 5 h 07 Saisical Opics ad Fee leco Lases Theoy ialuca eloi UCLA Los Ageles Jauay 5 h 07 is difficul if o impossible o coceive

More information

Lecture 17: Kinetics of Phase Growth in a Two-component System:

Lecture 17: Kinetics of Phase Growth in a Two-component System: Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien

More information

Generalized Fibonacci-Type Sequence and its Properties

Generalized Fibonacci-Type Sequence and its Properties Geelized Fibocci-Type Sequece d is Popeies Ompsh Sihwl shw Vys Devshi Tuoil Keshv Kuj Mdsu (MP Idi Resech Schol Fculy of Sciece Pcific Acdemy of Highe Educio d Resech Uivesiy Udipu (Rj Absc: The Fibocci

More information

1 Notes on Little s Law (l = λw)

1 Notes on Little s Law (l = λw) Copyrigh c 26 by Karl Sigma Noes o Lile s Law (l λw) We cosider here a famous ad very useful law i queueig heory called Lile s Law, also kow as l λw, which assers ha he ime average umber of cusomers i

More information

Multivector Functions

Multivector Functions I: J. Math. Aal. ad Appl., ol. 24, No. 3, c Academic Pess (968) 467 473. Multivecto Fuctios David Hestees I a pevious pape [], the fudametals of diffeetial ad itegal calculus o Euclidea -space wee expessed

More information

Harmonic excitation (damped)

Harmonic excitation (damped) Harmoic eciaio damped k m cos EOM: m&& c& k cos c && ζ & f cos The respose soluio ca be separaed io par;. Homogeeous soluio h. Paricular soluio p h p & ζ & && ζ & f cos Homogeeous soluio Homogeeous soluio

More information

Unified Mittag-Leffler Function and Extended Riemann-Liouville Fractional Derivative Operator

Unified Mittag-Leffler Function and Extended Riemann-Liouville Fractional Derivative Operator Iteatioal Joual of Mathematic Reeach. ISSN 0976-5840 Volume 9, Numbe 2 (2017), pp. 135-148 Iteatioal Reeach Publicatio Houe http://www.iphoue.com Uified Mittag-Leffle Fuctio ad Exteded Riema-Liouville

More information

Available online at J. Math. Comput. Sci. 4 (2014), No. 4, ISSN:

Available online at   J. Math. Comput. Sci. 4 (2014), No. 4, ISSN: Available olie a hp://sci.org J. Mah. Compu. Sci. 4 (2014), No. 4, 716-727 ISSN: 1927-5307 ON ITERATIVE TECHNIQUES FOR NUMERICAL SOLUTIONS OF LINEAR AND NONLINEAR DIFFERENTIAL EQUATIONS S.O. EDEKI *, A.A.

More information

STK4080/9080 Survival and event history analysis

STK4080/9080 Survival and event history analysis STK48/98 Survival ad eve hisory aalysis Marigales i discree ime Cosider a sochasic process The process M is a marigale if Lecure 3: Marigales ad oher sochasic processes i discree ime (recap) where (formally

More information

Consider the time-varying system, (14.1)

Consider the time-varying system, (14.1) Leue 4 // Oulie Moivaio Equivale Defiiios fo Lyapuov Sabiliy Uifomly Sabiliy ad Uifomly Asympoial Sabiliy 4 Covese Lyapuov Theoem 5 Ivaiae- lie Theoem 6 Summay Moivaio Taig poblem i ool, Suppose ha x (

More information

F D D D D F. smoothed value of the data including Y t the most recent data.

F D D D D F. smoothed value of the data including Y t the most recent data. Module 2 Forecasig 1. Wha is forecasig? Forecasig is defied as esimaig he fuure value ha a parameer will ake. Mos scieific forecasig mehods forecas he fuure value usig pas daa. I Operaios Maageme forecasig

More information

By the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences

By the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences Chapte : Theoy of Modula Aithmetic 8 Sectio D Chiese Remaide Theoem By the ed of this sectio you will be able to pove the Chiese Remaide Theoem apply this theoem to solve simultaeous liea cogueces The

More information

Mean Square Convergent Finite Difference Scheme for Stochastic Parabolic PDEs

Mean Square Convergent Finite Difference Scheme for Stochastic Parabolic PDEs America Joural of Compuaioal Mahemaics, 04, 4, 80-88 Published Olie Sepember 04 i SciRes. hp://www.scirp.org/joural/ajcm hp://dx.doi.org/0.436/ajcm.04.4404 Mea Square Coverge Fiie Differece Scheme for

More information

FIXED POINT AND HYERS-ULAM-RASSIAS STABILITY OF A QUADRATIC FUNCTIONAL EQUATION IN BANACH SPACES

FIXED POINT AND HYERS-ULAM-RASSIAS STABILITY OF A QUADRATIC FUNCTIONAL EQUATION IN BANACH SPACES IJRRAS 6 () July 0 www.apapess.com/volumes/vol6issue/ijrras_6.pdf FIXED POINT AND HYERS-UAM-RASSIAS STABIITY OF A QUADRATIC FUNCTIONA EQUATION IN BANACH SPACES E. Movahedia Behbaha Khatam Al-Abia Uivesity

More information

CONTROL OF TANDEM-TYPE TWO-WHEEL VEHICLE AT VARIOUS NOTION MODES ALONG SPATIAL CURVED LAY OF LINE

CONTROL OF TANDEM-TYPE TWO-WHEEL VEHICLE AT VARIOUS NOTION MODES ALONG SPATIAL CURVED LAY OF LINE COTROL O TADEM-TYPE TWO-WHEEL EHICLE AT ARIOUS OTIO MODES ALOG SPATIAL CURED LAY O LIE АS Besha Kaves КМ Bass Т Kaves LА Toka Wheeled vehicle is cosideed as a maeial poi ude he codiios of o-uifom moveme

More information

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory Liear Time-Ivaria Sysems (LTI Sysems) Oulie Basic Sysem Properies Memoryless ad sysems wih memory (saic or dyamic) Causal ad o-causal sysems (Causaliy) Liear ad o-liear sysems (Lieariy) Sable ad o-sable

More information

B. Maddah INDE 504 Simulation 09/02/17

B. Maddah INDE 504 Simulation 09/02/17 B. Maddah INDE 54 Simulaio 9/2/7 Queueig Primer Wha is a queueig sysem? A queueig sysem cosiss of servers (resources) ha provide service o cusomers (eiies). A Cusomer requesig service will sar service

More information

INF 5460 Electronic noise Estimates and countermeasures. Lecture 13 (Mot 10) Amplifier Architectures

INF 5460 Electronic noise Estimates and countermeasures. Lecture 13 (Mot 10) Amplifier Architectures NF 5460 lecoic oise simaes ad couemeasues Lecue 3 (Mo 0) Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils

More information

Cameras and World Geometry

Cameras and World Geometry Caeas ad Wold Geoe How all is his woa? How high is he caea? Wha is he caea oaio w. wold? Which ball is close? Jaes Has Thigs o eebe Has Pihole caea odel ad caea (pojecio) ai Hoogeeous coodiaes allow pojecio

More information

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

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws. Limi of a fucio.. Oe-Sided..... Ifiie limis Verical Asympoes... Calculaig Usig he Limi Laws.5 The Squeeze Theorem.6 The Precise Defiiio of a Limi......7 Coiuiy.8 Iermediae Value Theorem..9 Refereces..

More information

Calculus BC 2015 Scoring Guidelines

Calculus BC 2015 Scoring Guidelines AP Calculus BC 5 Scorig Guidelies 5 The College Board. College Board, Advaced Placeme Program, AP, AP Ceral, ad he acor logo are regisered rademarks of he College Board. AP Ceral is he official olie home

More information

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition LINEAR APPROXIMATION OF THE BASELINE RBC MODEL FEBRUARY, 202 Iroducio For f(, y, z ), mulivariable Taylor liear epasio aroud (, yz, ) f (, y, z) f(, y, z) + f (, y, z)( ) + f (, y, z)( y y) + f (, y, z)(

More information

Robust Adaptive Control of Uncertain Nonlinear Systems in the Presence of Input Saturation and External Disturbance

Robust Adaptive Control of Uncertain Nonlinear Systems in the Presence of Input Saturation and External Disturbance 67 IEEE RANSACIONS ON AUOMAIC CONROL, VOL. 56, NO. 7, JULY Robus Adapive Cool of Uceai Noliea Sysems i he Pesece of Ipu Sauaio ad Exeal Disubace Chagyu We, Fellow, IEEE, Jig Zhou, Membe, IEEE, Zhiao Liu,

More information

Transistor configurations: There are three main ways to place a FET/BJT in an architecture:

Transistor configurations: There are three main ways to place a FET/BJT in an architecture: F3 Mo 0. Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils o povide biasig so ha he asiso has he coec

More information

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4) 7 Differeial equaios Review Solve by he mehod of udeermied coefficies ad by he mehod of variaio of parameers (4) y y = si Soluio; we firs solve he homogeeous equaio (4) y y = 4 The correspodig characerisic

More information

CAPACITY ANALYSIS OF ASYMPTOTICALLY LARGE MIMO CHANNELS. Georgy Levin

CAPACITY ANALYSIS OF ASYMPTOTICALLY LARGE MIMO CHANNELS. Georgy Levin CAPACITY ANALYSIS OF ASYMPTOTICALLY LAGE MIMO CANNELS by Geogy Levi The hesis submied o he Faculy of Gaduae ad Posdocoal Sudies i paial fulfillme of he equiemes fo he degee of DOCTO OF PILOSOPY i Elecical

More information

Advanced Physical Geodesy

Advanced Physical Geodesy Supplemetal Notes Review of g Tems i Moitz s Aalytic Cotiuatio Method. Advaced hysical Geodesy GS887 Chistophe Jekeli Geodetic Sciece The Ohio State Uivesity 5 South Oval Mall Columbus, OH 4 7 The followig

More information

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE Mohia & Samaa, Vol. 1, No. II, December, 016, pp 34-49. ORIGINAL RESEARCH ARTICLE OPEN ACCESS FIED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE 1 Mohia S. *, Samaa T. K. 1 Deparme of Mahemaics, Sudhir Memorial

More information

Strong Result for Level Crossings of Random Polynomials. Dipty Rani Dhal, Dr. P. K. Mishra. Department of Mathematics, CET, BPUT, BBSR, ODISHA, INDIA

Strong Result for Level Crossings of Random Polynomials. Dipty Rani Dhal, Dr. P. K. Mishra. Department of Mathematics, CET, BPUT, BBSR, ODISHA, INDIA Iteatioal Joual of Reseach i Egieeig ad aageet Techology (IJRET) olue Issue July 5 Available at http://wwwijetco/ Stog Result fo Level Cossigs of Rado olyoials Dipty Rai Dhal D K isha Depatet of atheatics

More information

On a Problem of Littlewood

On a Problem of Littlewood Ž. JOURAL OF MATHEMATICAL AALYSIS AD APPLICATIOS 199, 403 408 1996 ARTICLE O. 0149 O a Poblem of Littlewood Host Alze Mosbache Stasse 10, 51545 Waldbol, Gemay Submitted by J. L. Bee Received May 19, 1995

More information

Research Article On Pointwise Approximation of Conjugate Functions by Some Hump Matrix Means of Conjugate Fourier Series

Research Article On Pointwise Approximation of Conjugate Functions by Some Hump Matrix Means of Conjugate Fourier Series Hidawi Publishig Copoaio Joual of Fucio Spaces Volue 5, Aicle ID 475, 9 pages hp://dx.doi.og/.55/5/475 Reseach Aicle O Poiwise Appoxiaio of Cojugae Fucios by Soe Hup Maix Meas of Cojugae Fouie Seies W.

More information

On composite conformal mapping of an annulus to a plane with two holes

On composite conformal mapping of an annulus to a plane with two holes O composite cofomal mappig of a aulus to a plae with two holes Mila Batista (July 07) Abstact I the aticle we coside the composite cofomal map which maps aulus to ifiite egio with symmetic hole ad ealy

More information

2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)

2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i) Mah PracTes Be sure o review Lab (ad all labs) There are los of good quesios o i a) Sae he Mea Value Theorem ad draw a graph ha illusraes b) Name a impora heorem where he Mea Value Theorem was used i he

More information

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

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003 ODEs II, Suppleme o Lecures 6 & 7: The Jorda Normal Form: Solvig Auoomous, Homogeeous Liear Sysems April 2, 23 I his oe, we describe he Jorda ormal form of a marix ad use i o solve a geeral homogeeous

More information

Mapping Radius of Regular Function and Center of Convex Region. Duan Wenxi

Mapping Radius of Regular Function and Center of Convex Region. Duan Wenxi d Iteatioal Cofeece o Electical Compute Egieeig ad Electoics (ICECEE 5 Mappig adius of egula Fuctio ad Cete of Covex egio Dua Wexi School of Applied Mathematics Beijig Nomal Uivesity Zhuhai Chia 363463@qqcom

More information

Research Article A Generalized Nonlinear Sum-Difference Inequality of Product Form

Research Article A Generalized Nonlinear Sum-Difference Inequality of Product Form Joural of Applied Mahemaics Volume 03, Aricle ID 47585, 7 pages hp://dx.doi.org/0.55/03/47585 Research Aricle A Geeralized Noliear Sum-Differece Iequaliy of Produc Form YogZhou Qi ad Wu-Sheg Wag School

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

More information

Analysis of Stress in PD Front End Solenoids I. Terechkine

Analysis of Stress in PD Front End Solenoids I. Terechkine TD-05-039 Sepembe 0, 005 I. Ioducio. Aalysis of Sess i PD Fo Ed Soleoids I. Teechkie Thee ae fou diffee ypes of supecoducig soleoids used fo beam focusig i he Fod Ed of he Poo Dive. Table 1 gives a idea

More information

Additional Tables of Simulation Results

Additional Tables of Simulation Results Saisica Siica: Suppleme REGULARIZING LASSO: A CONSISTENT VARIABLE SELECTION METHOD Quefeg Li ad Ju Shao Uiversiy of Wiscosi, Madiso, Eas Chia Normal Uiversiy ad Uiversiy of Wiscosi, Madiso Supplemeary

More information

PRESSURE AND PRESSURE DERIVATIVE ANALYSIS FOR PSEUDOPLASTIC FLUIDS IN VERTICAL FRACTURED WELLS

PRESSURE AND PRESSURE DERIVATIVE ANALYSIS FOR PSEUDOPLASTIC FLUIDS IN VERTICAL FRACTURED WELLS VOL. 7, NO. 8, AUGUST 0 ISSN 89-6608 ARN Joual of Egieeig ad Applied Scieces 006-0 Asia Reseach ublishig Neo (ARN). All ighs eseved..apjouals.com RESSURE AN RESSURE ERIVATIVE ANALYSIS FOR SEUOLASTIC FLUIS

More information

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method CHAPTER 5 : SERIES 5.1 Seies 5. The Sum of a Seies 5..1 Sum of Powe of Positive Iteges 5.. Sum of Seies of Patial Factio 5..3 Diffeece Method 5.3 Test of covegece 5.3.1 Divegece Test 5.3. Itegal Test 5.3.3

More information

UNSTEADY HELICAL FLOWS OF A MAXWELL FLUID

UNSTEADY HELICAL FLOWS OF A MAXWELL FLUID PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY, Seies A, OF THE ROMANIAN ACADEMY Volue 5, Nube /4,. - UNSTEADY HELICAL FLOWS OF A MAXWELL FLUID Cosai FETECAU, Coia FETECAU Techical Uivesiy of Iasi,

More information

Finite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler

Finite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler Fiite -idetities elated to well-ow theoems of Eule ad Gauss Joha Cigle Faultät fü Mathemati Uivesität Wie A-9 Wie, Nodbegstaße 5 email: oha.cigle@uivie.ac.at Abstact We give geealizatios of a fiite vesio

More information

Fujii, Takao; Hayashi, Fumiaki; Iri Author(s) Oguro, Kazumasa.

Fujii, Takao; Hayashi, Fumiaki; Iri Author(s) Oguro, Kazumasa. TileDesigig a Opimal Public Pesio Fujii, Takao; Hayashi, Fumiaki; Ii Auho(s) Oguo, Kazumasa Ciaio Issue 3- Dae Type Techical Repo Tex Vesio publishe URL hp://hdl.hadle.e/86/54 Righ Hiosubashi Uivesiy Reposioy

More information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

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

BINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k = wwwskshieduciocom BINOMIAL HEOREM OBJEIVE PROBLEMS he coefficies of, i e esio of k e equl he k /7 If e coefficie of, d ems i e i AP, e e vlue of is he coefficies i e,, 7 ems i e esio of e i AP he 7 7 em

More information

Journal of Xiamen University (Natural Science)

Journal of Xiamen University (Natural Science) 48 4 2009 7 () Joual of Xiame Uivesiy (Naual Sciece) Vol. 48 No. 4 J ul. 2009, 3 (, 36005) :,,.,,,.,.,. : ;;; : TP 393 :A :043820479 (2009) 0420493206,( dyamic age s). ( muliage sysems),, [ ], [2 ], [3

More information

COST OPTIMIZATION OF SLAB MILLING OPERATION USING GENETIC ALGORITHMS

COST OPTIMIZATION OF SLAB MILLING OPERATION USING GENETIC ALGORITHMS COST OPTIMIZATIO OF SLAB MILLIG OPERATIO USIG GEETIC ALGORITHMS Bhavsa, S.. ad Saghvi, R.C. G H Pael College of Egieeig ad Techology, Vallah Vidyaaga 388 20, Aad, Gujaa E-mail:sake976@yahoo.co.i; ajeshsaghvi@gce.ac.i

More information

Strong Result for Level Crossings of Random Polynomials

Strong Result for Level Crossings of Random Polynomials IOSR Joual of haacy ad Biological Scieces (IOSR-JBS) e-issn:78-8, p-issn:19-7676 Volue 11, Issue Ve III (ay - Ju16), 1-18 wwwiosjoualsog Stog Result fo Level Cossigs of Rado olyoials 1 DKisha, AK asigh

More information

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP)

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP) ENGG450 Probabiliy ad Saisics for Egieers Iroducio 3 Probabiliy 4 Probabiliy disribuios 5 Probabiliy Desiies Orgaizaio ad descripio of daa 6 Samplig disribuios 7 Ifereces cocerig a mea 8 Comparig wo reames

More information

Lecture 15: Three-tank Mixing and Lead Poisoning

Lecture 15: Three-tank Mixing and Lead Poisoning Lecure 15: Three-ak Miig ad Lead Poisoig Eigevalues ad eigevecors will be used o fid he soluio of a sysem for ukow fucios ha saisfy differeial equaios The ukow fucios will be wrie as a 1 colum vecor [

More information

Duration Notes 1. To motivate this measure, observe that the duration may also be expressed as. a a T a

Duration Notes 1. To motivate this measure, observe that the duration may also be expressed as. a a T a Duio Noes Mculy defied he duio of sse i 938. 2 Le he sem of pymes cosiuig he sse be,,..., d le /( + ) deoe he discou fco. he Mculy's defiiio of he duio of he sse is 3 2 D + 2 2 +... + 2 + + + + 2... o

More information

On The Estimation of Two Missing Values in Randomized Complete Block Designs

On The Estimation of Two Missing Values in Randomized Complete Block Designs Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.

More information