Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy
|
|
- Ashley Fisher
- 5 years ago
- Views:
Transcription
1 Arcle Inernaonal Journal of Modern Mahemacal Scences, 4, (): - Inernaonal Journal of Modern Mahemacal Scences Journal homepage: ISSN: 66-86X Florda, USA Approxmae Analyc Soluon of (+) - Dmensonal Zakharov-Kuznesov(Zk) Equaons Usng Homoopy Perurbaon Mehod wh Hyperbolc & Perodc Inal Condons E.S. Fahmy Basc Scence Deparmen, Faculy of Engneerng, Ocober 6 Unversy E-Mal: esfahmy@yahoo.com Arcle hsory: Receved 4 December, Receved n revsed form 8 March 4, Acceped 4 March 4, Publshed Aprl 4. Absrac: In hs paper, we consruc an approxmae analyc soluon of (+) dmensonal Zakhorov-Kuznesov equaons usng Homoopy eraon mehod wh hyperbolc & perodc nal condons and he resul s compared wh he exac soluons obaned by sne-cosne mehod. Keywords: Homoopy eraon mehod; Zakhorov-Kuznesov equaons; sne-cosne mehod.. Inroducon The kdv equaon s consdered a spaally one-dmensonal model. The bes known wodmensonal generalzaons of kdv equaon are Kadomosov-Pevshvll (KP) equaons. Wazwaz [] exended he coupled Zakhorov-Kuznesov(ZK) equaons. The coupled ZK equaons descrbe he nonlnear developmen of on-acousc waves n magnezed plasma under he resrcons of small wave amplude, weak dsperson, and srong magnec felds. The physcal Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
2 In. J. Modern Mah. Sc. 4, (): - phenomena for hs equaon were nvesgaed n [-4]. In hs paper we nroduce (+) - dmensonal ZK-equaons whch s gven as u ( uv ) ( vw ) ( u u ), x x xxx yyx v ( uw ) ( v v ), x xxx yyx w ( uv ) ( w w ). x xxx yyx () where,, and are arbary consans. In [5-] many soluons was obaned and one of hs soluons s he exac soluons obaned by sne-cosne mehod [5], egh cases of exac soluons was nroduced. In hs work we consder wo cases of hese soluons o be he nal condons for Homoopy perurbaon mehod [-]. The Homoopy mehod was nroduced by He [-6] n whose mehod he soluon was consdered as he summaon of an nfne seres whch usually converges readly o he exac soluon. Ths paper s organzed n he followng way: n secon we descrbe he Homoopy perurbaon mehod, n secon, we apply he Homoopy mehod o oban an analyc approxmae soluon for ZK- equaons () under wo knds of nal condons and we dscuss our numercal resuls usng fguers, show ha he approxmae soluons s comparson wh he exac soluons.. He Homoopy Perurbaon Mehod Consder he followng nonlnear dfferenal equaon A( u) f ( r), r () Wh he boundary condons: u B ( u, ), n where A r s he general dfferenal operaor, B funcon and s he boundary of he donan. Equaon () can be wren as () s he boundary operaor and f ( r ), s analyc L( u) N ( u) f ( r), (4) where Lu ( ) s he lnear par and N ( u ) s he nonlnear par. By usng Homoopy echnque, we can defne H ( v, p) ( p)[ L( u) L ( u)] p[ A( v ) f ( r)], r (5) Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
3 In. J. Modern Mah. Sc. 4, (): - Or H ( v, p) L( u) L ( u) pl ( u) p( N ( v ) f ( r)), r (6) where p [,] s an embeddng condon, hen from equaons (5,6) we ge H ( v,) L( u ) L ( u ), H ( v,) A( u ) f ( r). (7) Accordng o he Homoopy echnque, we can frs use he parameer p as a small parameer and wre equaon () as a power seres n p, we have v v pv p v (8) If p n he above equaon, we ge approxmae soluon of (4) n he followng form: u lmv v pv p v (9) p The combnaon of he perurbaon mehod and he Homoopy mehod s called Homoopy perurbaon mehod whch elmnaons of he radonal mehod.. Mehod of Soluon By rewren equaon () as u ( uv vu ) ( vw wv ) ( u u ), x x x x xxx yyx v ( uw wu ) ( v v ), x x xxx yyx w ( uv vu ) ( w w ). x x xxx yyx () Applyng he Homoopy mehod, we can pu,, () u p u v p v w p w Subsung no equaon (), we ge Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
4 In. J. Modern Mah. Sc. 4, (): - 4 x x ( p u ) u ( x, y,) [ p ( (( p u )( p v ) ( p v )( p u ) ) d p v v x ( ) ( x x p ( (( p w )( p v ) ( p v )( p w ) ) d xxx yyx p (( p u ) ( p u ) ) d xxx yyx x x x x, y,) [ p ( (( p u )( p w ) ( p w )( p u ) ) d p (( p v ) ( p v ) ) d ( p w ) w ( x, y,) [ p ( (( p u )( p v ) ( p v )( p u ) ) d p (( p v ) ( p v ) ) d xxx yyx () Comarng he coeffcen of he same powers of p, we ge he followng se of equaons u ( x, y, ) u ( x, y,), u ( x, y, ) [ ( u v v u ) ( v w w v ) ( u u )] d, x x x x xxx yyx u ( x, y, ) [ ( u v v u u v v u ) x x x x + ( v w w v v w w v ) ( u u )] d x x x x xxx yyx For v ( x, y, ) : v ( x, y, ) v ( x, y,), v ( x, y, ) [ ( u w w u ) ( v v )] d, x x xxx yyx v ( x, y, ) [ ( u w w u u w w u ) ( v v )] d x x x x xxx yyx And for w ( x, y, ) : w ( x, y, ) w ( x, y,), w ( x, y, ) [ ( u v v u ) ( w w )] d, x x xxx yyx w ( x, y, ) [ ( u v v u u v v u ) ( w w )] d x x x x xxx yyx ().. Case One Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
5 In. J. Modern Mah. Sc. 4, (): - 5 form: From [5], we can oban he hyperbolc nal condon of ZK equaons n he followng u x y k x y (,,) sech ( ( )), v x y k x y (,,) sech ( ( )), w x y k x y (,,) sech ( ( )). (4) Where k c k c /, / 4 ( 4, k c c / 4 ( 4, and / 8. (5) Then equaon () gves us he frs few approxmaons of u( x, y, ) : u x y k x y (,,) sech ( ( )), u ( x, y,) 4 ( k k k k k k cosh ( ( x y )) 4 4 sech ( ( x y ))anh ( ( x y )) u ( x, y,) ( 46 k 96 k k 4k k 4k k 4 (8 k 7 k ( k k ) ( k k + k ( k k ) k ( k k )cosh( ( x y )) ( cosh( ( x y )) k cosh(6 ( x y ))sech (6 ( x y )). 4 8 (6) The frs few approxmaons of v ( x, y, ) : v x y k x y (,,) sech ( ( )), v ( x, y,) 4 ( k k k k cosh( ( x y )) 4 sech ( ( x y ))anh( ( x y )) v ( x, y,) ( 46 k 96 k k 4k k k 4k k 4k k 4 (8 k 7 k k k k ( k k k k )) cosh( ( x y )) ( k k k )cosh(4 ( x y )) k cosh(6 ( x y ))sech ( ( x y )). 4 8 (7) The frs few approxmaons of w ( x, y, ) : Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
6 In. J. Modern Mah. Sc. 4, (): - 6 w x y k x y (,,) sech ( ( )), w ( x, y,) 4 ( k k k k cosh( ( x y )) 4 sech ( ( x y ))anh( ( x y )) w ( x, y,) ( 46 k 96 k k 4k k k 4k k 4 k k 4 (8 k 7 k k ( k k k k k k )) cosh( ( x y )) ( k k k )cosh(4 ( x y )) k cosh(6 ( x y ))sech ( ( x y )). 4 8 (8) Thus, we oban he hyperbolc approxmae soluons of () as followng u ( x, y, ) k sech ( ( x y )) 4 ( k k k k k k cosh ( ( x y ))sech ( ( x y ))anh ( ( x y )) 4 4 ( 46 k 96 k k 4k k 4k k 4 (8 k 7 k ( k k ) ( k k + k ( k k ) k ( k k )cosh( ( x y )) ( cosh( ( x y )) k cosh(6 ( x y ))sech (6 ( x y )). 4 8 v ( x, y, ) k sech ( ( x y )) 4 ( k k k k cosh( ( x y )) sech ( ( x y ))anh( ( x y )) ( 46 k 96 k k 4 4 4k k k 4k k 4 k k (8 k 7 k k ( k k k k ))cosh( ( x y )) ( k k k ) cosh(4 ( x y )) k cosh(6 ( x y ))sech ( ( x y )). 4 8 k k w ( x, y, ) k sech ( ( x y )) 4 ( k k k k 4 cosh( ( x y ))sech ( ( x y ))anh( ( x y )) ( 46 k 96 k k 4k k k 4 4k k 4 k k (8 k 7 k k ( k k k k k k ))cosh( ( x y )) ( k k k )cosh(4 ( x y )) k cosh(6 ( x y ))sech ( ( x y )). 4 8 (9) Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
7 In. J. Modern Mah. Sc. 4, (): [a]: The approxmae soluon u( x, y, ), s comparson wh he exac soluon [b]: The approxmae soluon v ( x, y, ), s comparson wh he exac soluon [c]: The approxmae soluon w ( x, y, ), s comparson wh he exac soluon Fgure : The approxmae soluons s comparson wh he exac soluons for hyperbolc nal condons a.,. and y. Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
8 In. J. Modern Mah. Sc. 4, (): Case Two From [5], we can oban he perodc nal condon of ZK equaons n he followng form: u x y k x y (,,) sec ( ( )), v x y k x y (,,) sec ( ( )), w x y k x y (,,) sec ( ( )). () Where k c k c /, / 4 ( 4 ), k c c / 4 ( 4, and / 8. Then equaon () gves us he frs few approxmaons of u( x, y, ) : u x y k x y (,,) sec ( ( )), u ( x, y,) 4 ( k k k k k k cos ( ( x y )) 4 4 sec ( ( x y ))an ( ( x y )) u ( x, y,) ( 8 k 7 k ( k k ) ( k k 4 k ( k k ) k ( k k )cos( ( x y )) ((64 k k k 74 k ( k k ) k ( k k ) k ( k k ) ( k k k k k )cos(4 ( x y )) k cos(6 ( x y ))sec ( ( x y )). 4 8 () The frs few approxmaons of v ( x, y, ) : v x y k x y (,,) sec ( ( )), v ( x, y,) 4 ( k k k k k k cos( ( x y )) 4 4 sec ( ( x y ))an ( ( x y )) v ( x, y,) ( 8 k 7 k k k ( k k k 4 k ))cos( ( x y )) ((64 k 74 k k k ( k k k k )) ( k k k ) cos(4 ( x y )) k cos(6 ( x y ))sec ( ( x y )). 4 8 () The frs few approxmaons of w ( x, y, ) : Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
9 In. J. Modern Mah. Sc. 4, (): - 9 w x y k x y (,,) sec ( ( )), w ( x, y,) 4 ( k k k k cos( ( x y )) 4 4 sec ( ( x y ))an ( ( x y )) w ( x, y,) ( 8 k 7 k k ( k k k k 4 kk ))cos( ( x y )) ((64 k 74 k k k ( k k k k )) ( k k k ) cos(4 ( x y )) k cos(6 ( x y ))sec ( ( x y )). 4 8 () Thus, we oban he hyperbolc approxmae soluons of () as followng u ( x, y, ) k sec ( ( x y )) 4 ( k k k k k k cos ( ( x y ))sec ( ( x y ))an ( ( x y )) 4 4 ( 8 k 7 k ( k k ) ( k k k ( k 4 k ) k ( k k )cos( ( x y )) ((64 k k k 74 k ( k k ) k ( k k ) k ( k k ) ( k k k 8 k k )cos(4 ( x y )) k cos(6 ( x y ))sec ( ( x y )). 4 v ( x, y, ) k sec ( ( x y )) 4 ( k k k k k k cos( ( x y ))sec ( ( x y ))an ( ( x y )) 4 4 ( 8 k 7 k k k 4 ( k k k k ))cos( ( x y )) ((64 k 74 k k k ( k k k k )) ( k k k )cos(4 ( x y )) k 4 8 cos(6 ( x y ))sec ( ( x y )). w ( x, y, ) k sec ( ( x y )) 4 ( k k k k cos( ( x y ))sec ( ( x y ))an ( ( x y )) 4 4 ( 8 k 7 k k ( k k k k kk 4 ))cos( ( x y )) ((64 k 74 k k k ( k k k k )) ( k k k ) cos(4 ( x y )) k cos(6 ( x y ))sec ( ( x y )). 4 8 (4) Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
10 In. J. Modern Mah. Sc. 4, (): [a]: The approxmae soluon 5 5 u( x, y, ), s comparson wh he exac soluon [b]: The approxmae soluon v ( x, y, ), s comparson wh he exac soluon [c]: The approxmae soluon w ( x, y, ), s comparson wh he exac soluon Fgure : The approxmae soluons s comparson wh he exac soluons for hyperbolc nal condons a.,. and y. 4. Conclusons Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
11 In. J. Modern Mah. Sc. 4, (): - In hs paper we consruced an analyc approxmae soluons for (+) dmensonal Zakhorov-Kuznesov(zk)-equaons usng Homoopy perurbaon mehod, under wo knds of nal condons, we have obaned resuls wh excellen accuracy as shown n fgures, where he approxmae soluons are successfully confrm o he exac soluons. References [] A. M. Wazwaz, Compleely negerable coupled kdv and coupled kp-sysem, Commun Nonlnear Sc. do:.6 lj. cnsns. 9. [] J. WU, New explc ravellng wave soluons for hree nonlnear evaluaon equaon. Appl. mah. compu., 7(): [] Z Y. Qn, A fne - dmensonal negerable sysem relaed o a new coupled kdv equaon. Phys. Le. A, 55(6): [4] A. M. Wazwaz, The exended anh mehod for abundan solary wave soluons of nonlnear wave equaons, Appl. Mah. Compu., 87(7): -4. [5] Y. Xe, S. Tang, Sne-Cosne mehod for new Coupled Zk-sysem, App. Mah. Scence. 5()(): [6] S. Monro, E. J. Parkes, The dervaon of a modfed ZakharovK- zunesov equaon and he sably of s soluons, Journal of Plasma Physcs, 6()(999): 5-7. [7] S. Munro, EJ. Parkes. Sably of solary-wave soluons o a modfed ZakharovCK - uznesov equaon, J Plasma Phys., 64(): [8] C. M. Khalgue, Exac Explc Soluons and Conservaon Lows for a coupled Zakhorov- Kuzneov sysem, problems n Engneerng, (), ID. 467, 5 pages. [9] M. Inc, Exac soluons wh solary paerns for he Zakharov-Kuznesov equaons wh fully nonlnear dsperson, Chaos Solons Fracals, (5)(7): [] J. Wu. New explc ravellng wave soluons for hree nonlnear evoluon equaons, Appl Mah Compu., 7(): , [] Kanglgl, F and F. A yaz, Solary wave Soluon for kdv and M kdv equaons by dfferenonal ransform mehod, Chaos solons and fracals, do :6/j. Chaos..9. [] J. H. He, Homoopy perurbaon mehod for nonlnear oscllaors wh dsconnues, Appled Mahemacs and Compuaon, 5()( 4): [] J. H. He, Comparson of Homoopy perurbaon mehod and Homoopy analyss mehod, Appled Mahemacs and Compuaon, 56()( 4): [4] J.H.He, Asympoology by Homoopy perurbaon mehod, Appled Mahemacs and Compuaon, 56()(4): Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
12 In. J. Modern Mah. Sc. 4, (): - [5] J.H.He, Homoopy perurbaon mehod for solvng boundary value problems, Physcs Leers. A, 5(-)(6): [6] J.H.He, Applcaon of Homoopy perurbaon mehod o nonlnear wave equaons, Chaos, Solons and Fracals, 6()(5): [7] Targ. M. Elzak and J. Bazar, Homoopy Perurbaon Mehod and Elzak Transform for Solvng Sysem of Nonlnear Paral Dfferenal Equaons, World Appl. Sc. J.,4(7)(): [8] Sharma, P.R. and Grraj Meh,. Applcaons of Homoopy Perurbaon mehod o Paral dfferenal equaons, Asan Journal of Mahemacs and Sascs, 4()(): 4-5. [9] J. Bazar, F. Badpemaa, F. Azm, Applcaon of he homoopy perurbaon mehod o Zakharov-Kuznesov equaons, Compuers and Mahemacs wh Applcaons, 58(9): [] D.D.Ganj, H. Babazadeh, F. Noor, M.MProuze, M.Janpour, An Applcaon of Homoopy perurbaon mehod for Non-lnear Blasus equaon o Boundary Layer Flow Over a Fla, plae, In. J. of nonlnear Sc, (7)(4)(9): Copyrgh 4 by Modern Scenfc Press Company, Florda, USA
M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria
IOSR Journal of Mahemacs (IOSR-JM e-issn: 78-578, p-issn: 9-765X. Volume 0, Issue 4 Ver. IV (Jul-Aug. 04, PP 40-44 Mulple SolonSoluons for a (+-dmensonalhroa-sasuma shallow waer wave equaon UsngPanlevé-Bӓclund
More informationA NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION
S19 A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION by Xaojun YANG a,b, Yugu YANG a*, Carlo CATTANI c, and Mngzheng ZHU b a Sae Key Laboraory for Geomechancs and Deep Underground Engneerng, Chna Unversy
More informationCubic Bezier Homotopy Function for Solving Exponential Equations
Penerb Journal of Advanced Research n Compung and Applcaons ISSN (onlne: 46-97 Vol. 4, No.. Pages -8, 6 omoopy Funcon for Solvng Eponenal Equaons S. S. Raml *,,. Mohamad Nor,a, N. S. Saharzan,b and M.
More informationOn computing differential transform of nonlinear non-autonomous functions and its applications
On compung dfferenal ransform of nonlnear non-auonomous funcons and s applcaons Essam. R. El-Zahar, and Abdelhalm Ebad Deparmen of Mahemacs, Faculy of Scences and Humanes, Prnce Saam Bn Abdulazz Unversy,
More informationHEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD
Journal of Appled Mahemacs and Compuaonal Mechancs 3, (), 45-5 HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Sansław Kukla, Urszula Sedlecka Insue of Mahemacs,
More informationExistence and Uniqueness Results for Random Impulsive Integro-Differential Equation
Global Journal of Pure and Appled Mahemacs. ISSN 973-768 Volume 4, Number 6 (8), pp. 89-87 Research Inda Publcaons hp://www.rpublcaon.com Exsence and Unqueness Resuls for Random Impulsve Inegro-Dfferenal
More informationA DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE
S13 A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE by Hossen JAFARI a,b, Haleh TAJADODI c, and Sarah Jane JOHNSTON a a Deparen of Maheacal Scences, Unversy
More informationMethod of upper lower solutions for nonlinear system of fractional differential equations and applications
Malaya Journal of Maemak, Vol. 6, No. 3, 467-472, 218 hps://do.org/1.26637/mjm63/1 Mehod of upper lower soluons for nonlnear sysem of fraconal dfferenal equaons and applcaons D.B. Dhagude1 *, N.B. Jadhav2
More informationFRACTIONAL OPTICAL SOLITARY WAVE SOLUTIONS OF THE HIGHER-ORDER NONLINEAR SCHRÖDINGER EQUATION
THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY Seres A OF THE ROMANIAN ACADEMY Volume Number /00x pp. 9 00 FRACTIONAL OPTICAL SOLITARY WAVE SOLUTIONS OF THE HIGHER-ORDER NONLINEAR SCHRÖDINGER
More informationOn One Analytic Method of. Constructing Program Controls
Appled Mahemacal Scences, Vol. 9, 05, no. 8, 409-407 HIKARI Ld, www.m-hkar.com hp://dx.do.org/0.988/ams.05.54349 On One Analyc Mehod of Consrucng Program Conrols A. N. Kvko, S. V. Chsyakov and Yu. E. Balyna
More informationGENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim
Korean J. Mah. 19 (2011), No. 3, pp. 263 272 GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS Youngwoo Ahn and Kae Km Absrac. In he paper [1], an explc correspondence beween ceran
More information( ) () we define the interaction representation by the unitary transformation () = ()
Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger
More informationGeneralized double sinh-gordon equation: Symmetry reductions, exact solutions and conservation laws
IJS (05) 9A: 89-96 Iranan Journal of Scence & echnology hp://ss.shrazu.ac.r Generalzed double snh-gordon equaon: Symmery reducons eac soluons and conservaon laws G. Magalawe B. Muaeea and C. M. Khalque
More information[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5
TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres
More informationP R = P 0. The system is shown on the next figure:
TPG460 Reservor Smulaon 08 page of INTRODUCTION TO RESERVOIR SIMULATION Analycal and numercal soluons of smple one-dmensonal, one-phase flow equaons As an nroducon o reservor smulaon, we wll revew he smples
More informationFTCS Solution to the Heat Equation
FTCS Soluon o he Hea Equaon ME 448/548 Noes Gerald Reckenwald Porland Sae Unversy Deparmen of Mechancal Engneerng gerry@pdxedu ME 448/548: FTCS Soluon o he Hea Equaon Overvew Use he forward fne d erence
More informationPerformance Analysis for a Network having Standby Redundant Unit with Waiting in Repair
TECHNI Inernaonal Journal of Compung Scence Communcaon Technologes VOL.5 NO. July 22 (ISSN 974-3375 erformance nalyss for a Nework havng Sby edundan Un wh ang n epar Jendra Sngh 2 abns orwal 2 Deparmen
More informationOrdinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s
Ordnary Dfferenal Equaons n Neuroscence wh Malab eamples. Am - Gan undersandng of how o se up and solve ODE s Am Undersand how o se up an solve a smple eample of he Hebb rule n D Our goal a end of class
More informationCoupled Method for Solving Time-Fractional Navier-Stokes Equation
INTERNATIONAL JOURNAL OF CIRCUITS, SYSTEMS AND SIGNAL PROCESSING Volume, 8 Coupled Mehod for Solng Tme-Fraconal Naer-Sokes Equaon S. O. Edek, and G. O. Aknlab Absrac Ths paper wnesses he couplng of wo
More informationResearch Article Numerical Approximation of Higher-Order Solutions of the Quadratic Nonlinear Stochastic Oscillatory Equation Using WHEP Technique
Hndaw Publshng Corporaon Journal of Appled Mahemacs Volume 3, Arcle ID 68537, pages hp://dx.do.org/.55/3/68537 Research Arcle Numercal Approxmaon of Hgher-Order Soluons of he Quadrac Nonlnear Sochasc Oscllaory
More informationExistence of Time Periodic Solutions for the Ginzburg-Landau Equations. model of superconductivity
Journal of Mahemacal Analyss and Applcaons 3, 3944 999 Arcle ID jmaa.999.683, avalable onlne a hp:www.dealbrary.com on Exsence of me Perodc Soluons for he Gnzburg-Landau Equaons of Superconducvy Bxang
More informationMohammad H. Al-Towaiq a & Hasan K. Al-Bzoor a a Department of Mathematics and Statistics, Jordan University of
Ths arcle was downloaded by: [Jordan Unv. of Scence & Tech] On: 05 Aprl 05, A: 0:4 Publsher: Taylor & Francs Informa Ld Regsered n England and ales Regsered umber: 07954 Regsered offce: Mormer House, 37-4
More informationImplementation of Quantized State Systems in MATLAB/Simulink
SNE T ECHNICAL N OTE Implemenaon of Quanzed Sae Sysems n MATLAB/Smulnk Parck Grabher, Mahas Rößler 2*, Bernhard Henzl 3 Ins. of Analyss and Scenfc Compung, Venna Unversy of Technology, Wedner Haupsraße
More informationComparison of Differences between Power Means 1
In. Journal of Mah. Analyss, Vol. 7, 203, no., 5-55 Comparson of Dfferences beween Power Means Chang-An Tan, Guanghua Sh and Fe Zuo College of Mahemacs and Informaon Scence Henan Normal Unversy, 453007,
More informationAPPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC CORRECTION
THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY Seres A OF THE ROMANIAN ACADEMY Volume 6 Number /5 pp 8 86 APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC
More informationSome Numerical Methods For Solving Fractional Parabolic Partial Differential Equations
Eng.& Tech. Journal,Vol.28, No.2, 2 Some Numercal Mehods For Solvng Fraconal Parabolc Paral Dfferenal Dr. Osama H.Mohammed*, Ibsam K.Hanan* & Akram A. Al-Sabbagh* Receved on: 7//29 Acceped on:/4/2 Absrac
More informationOn the numerical treatment ofthenonlinear partial differentialequation of fractional order
IOSR Journal of Mahemacs (IOSR-JM) e-iss: 2278-5728, p-iss: 239-765X. Volume 2, Issue 6 Ver. I (ov. - Dec.26), PP 28-37 www.osrjournals.org On he numercal reamen ofhenonlnear paral dfferenalequaon of fraconal
More informationV.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS
R&RATA # Vol.) 8, March FURTHER AALYSIS OF COFIDECE ITERVALS FOR LARGE CLIET/SERVER COMPUTER ETWORKS Vyacheslav Abramov School of Mahemacal Scences, Monash Unversy, Buldng 8, Level 4, Clayon Campus, Wellngon
More informationRelative controllability of nonlinear systems with delays in control
Relave conrollably o nonlnear sysems wh delays n conrol Jerzy Klamka Insue o Conrol Engneerng, Slesan Techncal Unversy, 44- Glwce, Poland. phone/ax : 48 32 37227, {jklamka}@a.polsl.glwce.pl Keywor: Conrollably.
More informationSolution in semi infinite diffusion couples (error function analysis)
Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of
More informationVolatility Interpolation
Volaly Inerpolaon Prelmnary Verson March 00 Jesper Andreasen and Bran Huge Danse Mares, Copenhagen wan.daddy@danseban.com brno@danseban.com Elecronc copy avalable a: hp://ssrn.com/absrac=69497 Inro Local
More informationSolution of the Schrödinger Equation for a Linear Potential using the Extended Baker-Campbell-Hausdorff Formula
Appl. Mah. Inf. Sc. 9, No. 1, 175-181 015 175 Appled Mahemacs & Informaon Scences An Inernaonal Journal hp://dx.do.org/10.1785/ams/0901 Soluon of he Schrödnger Equaon for a Lnear Poenal usng he Exended
More informationLecture 18: The Laplace Transform (See Sections and 14.7 in Boas)
Lecure 8: The Lalace Transform (See Secons 88- and 47 n Boas) Recall ha our bg-cure goal s he analyss of he dfferenal equaon, ax bx cx F, where we emloy varous exansons for he drvng funcon F deendng on
More informationSOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β
SARAJEVO JOURNAL OF MATHEMATICS Vol.3 (15) (2007), 137 143 SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β M. A. K. BAIG AND RAYEES AHMAD DAR Absrac. In hs paper, we propose
More informationLet s treat the problem of the response of a system to an applied external force. Again,
Page 33 QUANTUM LNEAR RESPONSE FUNCTON Le s rea he problem of he response of a sysem o an appled exernal force. Agan, H() H f () A H + V () Exernal agen acng on nernal varable Hamlonan for equlbrum sysem
More informationScattering at an Interface: Oblique Incidence
Course Insrucor Dr. Raymond C. Rumpf Offce: A 337 Phone: (915) 747 6958 E Mal: rcrumpf@uep.edu EE 4347 Appled Elecromagnecs Topc 3g Scaerng a an Inerface: Oblque Incdence Scaerng These Oblque noes may
More informationThis document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore.
Ths documen s downloaded from DR-NTU, Nanyang Technologcal Unversy Lbrary, Sngapore. Tle A smplfed verb machng algorhm for word paron n vsual speech processng( Acceped verson ) Auhor(s) Foo, Say We; Yong,
More informationSampling Procedure of the Sum of two Binary Markov Process Realizations
Samplng Procedure of he Sum of wo Bnary Markov Process Realzaons YURY GORITSKIY Dep. of Mahemacal Modelng of Moscow Power Insue (Techncal Unversy), Moscow, RUSSIA, E-mal: gorsky@yandex.ru VLADIMIR KAZAKOV
More informationIn the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!
ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL The frs hng o es n wo-way ANOVA: Is here neracon? "No neracon" means: The man effecs model would f. Ths n urn means: In he neracon plo (wh A on he horzonal
More informationJ i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.
umercal negraon of he dffuson equaon (I) Fne dfference mehod. Spaal screaon. Inernal nodes. R L V For hermal conducon le s dscree he spaal doman no small fne spans, =,,: Balance of parcles for an nernal
More informationDiffusion of Heptane in Polyethylene Vinyl Acetate: Modelisation and Experimentation
IOSR Journal of Appled hemsry (IOSR-JA) e-issn: 78-5736.Volume 7, Issue 6 Ver. I. (Jun. 4), PP 8-86 Dffuson of Hepane n Polyehylene Vnyl Aceae: odelsaon and Expermenaon Rachd Aman *, Façal oubarak, hammed
More informationChapter Lagrangian Interpolation
Chaper 5.4 agrangan Inerpolaon Afer readng hs chaper you should be able o:. dere agrangan mehod of nerpolaon. sole problems usng agrangan mehod of nerpolaon and. use agrangan nerpolans o fnd deraes and
More informationNotes on the stability of dynamic systems and the use of Eigen Values.
Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon
More informationJohn Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany
Herarchcal Markov Normal Mxure models wh Applcaons o Fnancal Asse Reurns Appendx: Proofs of Theorems and Condonal Poseror Dsrbuons John Geweke a and Gann Amsano b a Deparmens of Economcs and Sascs, Unversy
More informationFirst-order piecewise-linear dynamic circuits
Frs-order pecewse-lnear dynamc crcus. Fndng he soluon We wll sudy rs-order dynamc crcus composed o a nonlnear resse one-por, ermnaed eher by a lnear capacor or a lnear nducor (see Fg.. Nonlnear resse one-por
More informationTHE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS
THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he
More information3. OVERVIEW OF NUMERICAL METHODS
3 OVERVIEW OF NUMERICAL METHODS 3 Inroducory remarks Ths chaper summarzes hose numercal echnques whose knowledge s ndspensable for he undersandng of he dfferen dscree elemen mehods: he Newon-Raphson-mehod,
More informationDelay-Range-Dependent Stability Analysis for Continuous Linear System with Interval Delay
Inernaonal Journal of Emergng Engneerng esearch an echnology Volume 3, Issue 8, Augus 05, PP 70-76 ISSN 349-4395 (Prn) & ISSN 349-4409 (Onlne) Delay-ange-Depenen Sably Analyss for Connuous Lnear Sysem
More information@FMI c Kyung Moon Sa Co.
Annals of Fuzzy Mahemacs and Informacs Volume 8, No. 2, (Augus 2014), pp. 245 257 ISSN: 2093 9310 (prn verson) ISSN: 2287 6235 (elecronc verson) hp://www.afm.or.kr @FMI c Kyung Moon Sa Co. hp://www.kyungmoon.com
More informationTesting a new idea to solve the P = NP problem with mathematical induction
Tesng a new dea o solve he P = NP problem wh mahemacal nducon Bacground P and NP are wo classes (ses) of languages n Compuer Scence An open problem s wheher P = NP Ths paper ess a new dea o compare he
More informationSELFSIMILAR PROCESSES WITH STATIONARY INCREMENTS IN THE SECOND WIENER CHAOS
POBABILITY AD MATEMATICAL STATISTICS Vol., Fasc., pp. SELFSIMILA POCESSES WIT STATIOAY ICEMETS I TE SECOD WIEE CAOS BY M. M A E J I M A YOKOAMA AD C. A. T U D O LILLE Absrac. We sudy selfsmlar processes
More informationLinear Response Theory: The connection between QFT and experiments
Phys540.nb 39 3 Lnear Response Theory: The connecon beween QFT and expermens 3.1. Basc conceps and deas Q: ow do we measure he conducvy of a meal? A: we frs nroduce a weak elecrc feld E, and hen measure
More informationNATIONAL UNIVERSITY OF SINGAPORE PC5202 ADVANCED STATISTICAL MECHANICS. (Semester II: AY ) Time Allowed: 2 Hours
NATONAL UNVERSTY OF SNGAPORE PC5 ADVANCED STATSTCAL MECHANCS (Semeser : AY 1-13) Tme Allowed: Hours NSTRUCTONS TO CANDDATES 1. Ths examnaon paper conans 5 quesons and comprses 4 prned pages.. Answer all
More informationCH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC
CH.3. COMPATIBILITY EQUATIONS Connuum Mechancs Course (MMC) - ETSECCPB - UPC Overvew Compably Condons Compably Equaons of a Poenal Vecor Feld Compably Condons for Infnesmal Srans Inegraon of he Infnesmal
More informationHandout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs.
Handou # 6 (MEEN 67) Numercal Inegraon o Fnd Tme Response of SDOF mechancal sysem Sae Space Mehod The EOM for a lnear sysem s M X DX K X F() () X X X X V wh nal condons, a 0 0 ; 0 Defne he followng varables,
More informationReview of Numerical Schemes for Two Point Second Order Non-Linear Boundary Value Problems
Proceedngs of e Pasan Academ of Scences 5 (: 5-58 (5 Coprg Pasan Academ of Scences ISS: 377-969 (prn, 36-448 (onlne Pasan Academ of Scences Researc Arcle Revew of umercal Scemes for Two Pon Second Order
More informationNew M-Estimator Objective Function. in Simultaneous Equations Model. (A Comparative Study)
Inernaonal Mahemacal Forum, Vol. 8, 3, no., 7 - HIKARI Ld, www.m-hkar.com hp://dx.do.org/.988/mf.3.3488 New M-Esmaor Objecve Funcon n Smulaneous Equaons Model (A Comparave Sudy) Ahmed H. Youssef Professor
More informationMechanics Physics 151
Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ
More informationCONSISTENT EARTHQUAKE ACCELERATION AND DISPLACEMENT RECORDS
APPENDX J CONSSTENT EARTHQUAKE ACCEERATON AND DSPACEMENT RECORDS Earhqake Acceleraons can be Measred. However, Srcres are Sbjeced o Earhqake Dsplacemens J. NTRODUCTON { XE "Acceleraon Records" }A he presen
More informationAppendix H: Rarefaction and extrapolation of Hill numbers for incidence data
Anne Chao Ncholas J Goell C seh lzabeh L ander K Ma Rober K Colwell and Aaron M llson 03 Rarefacon and erapolaon wh ll numbers: a framewor for samplng and esmaon n speces dversy sudes cology Monographs
More informationA New Generalized Gronwall-Bellman Type Inequality
22 Inernaonal Conference on Image, Vson and Comung (ICIVC 22) IPCSIT vol. 5 (22) (22) IACSIT Press, Sngaore DOI:.7763/IPCSIT.22.V5.46 A New Generalzed Gronwall-Bellman Tye Ineualy Qnghua Feng School of
More informationFI 3103 Quantum Physics
/9/4 FI 33 Quanum Physcs Aleander A. Iskandar Physcs of Magnesm and Phooncs Research Grou Insu Teknolog Bandung Basc Conces n Quanum Physcs Probably and Eecaon Value Hesenberg Uncerany Prncle Wave Funcon
More informationNumerical solution of second-order hyperbolic telegraph equation via new cubic trigonometric B-splines approach
Nazr e al., Cogen Mahemacs 17, : 13861 hps://do.org/18/3311835.17.13861 APPLIED & INTERDISCIPLINARY MATHEMATICS RESEARCH ARTICLE Numercal soluon of second-order hyperbolc elegraph equaon va new cubc rgonomerc
More information2/20/2013. EE 101 Midterm 2 Review
//3 EE Mderm eew //3 Volage-mplfer Model The npu ressance s he equalen ressance see when lookng no he npu ermnals of he amplfer. o s he oupu ressance. I causes he oupu olage o decrease as he load ressance
More informationWronskian Determinant Solutions for the (3 + 1)-Dimensional Boiti-Leon-Manna-Pempinelli Equation
Jornal of Appled Mahemacs and Physcs 0 8-4 Pblshed Onlne ovember 0 (hp://www.scrp.org/jornal/jamp) hp://d.do.org/0.46/jamp.0.5004 Wronskan Deermnan Solons for he ( + )-Dmensonal Bo-Leon-Manna-Pempnell
More informationUNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 2017 EXAMINATION
INTERNATIONAL TRADE T. J. KEHOE UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 27 EXAMINATION Please answer wo of he hree quesons. You can consul class noes, workng papers, and arcles whle you are workng on he
More informationDelay Dependent Robust Stability of T-S Fuzzy. Systems with Additive Time Varying Delays
Appled Maemacal Scences, Vol. 6,, no., - Delay Dependen Robus Sably of -S Fuzzy Sysems w Addve me Varyng Delays Idrss Sad LESSI. Deparmen of Pyscs, Faculy of Scences B.P. 796 Fès-Alas Sad_drss9@yaoo.fr
More informationF-Tests and Analysis of Variance (ANOVA) in the Simple Linear Regression Model. 1. Introduction
ECOOMICS 35* -- OTE 9 ECO 35* -- OTE 9 F-Tess and Analyss of Varance (AOVA n he Smple Lnear Regresson Model Inroducon The smple lnear regresson model s gven by he followng populaon regresson equaon, or
More informationJanuary Examinations 2012
Page of 5 EC79 January Examnaons No. of Pages: 5 No. of Quesons: 8 Subjec ECONOMICS (POSTGRADUATE) Tle of Paper EC79 QUANTITATIVE METHODS FOR BUSINESS AND FINANCE Tme Allowed Two Hours ( hours) Insrucons
More informationA Simulation Based Optimal Control System For Water Resources
Cy Unversy of New York (CUNY) CUNY Academc Works Inernaonal Conference on Hydronformacs 8--4 A Smulaon Based Opmal Conrol Sysem For Waer Resources Aser acasa Maro Morales-Hernández Plar Brufau Plar García-Navarro
More informationMALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES. Institute for Mathematical Research, Universiti Putra Malaysia, UPM Serdang, Selangor, Malaysia
Malaysan Journal of Mahemacal Scences 9(2): 277-300 (2015) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Journal homeage: h://ensemumedumy/journal A Mehod for Deermnng -Adc Orders of Facorals 1* Rafka Zulkal,
More informationVariants of Pegasos. December 11, 2009
Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on
More informationComb Filters. Comb Filters
The smple flers dscussed so far are characered eher by a sngle passband and/or a sngle sopband There are applcaons where flers wh mulple passbands and sopbands are requred Thecomb fler s an example of
More informationStochastic Maxwell Equations in Photonic Crystal Modeling and Simulations
Sochasc Maxwell Equaons n Phoonc Crsal Modelng and Smulaons Hao-Mn Zhou School of Mah Georga Insue of Technolog Jon work wh: Al Adb ECE Majd Bade ECE Shu-Nee Chow Mah IPAM UCLA Aprl 14-18 2008 Parall suppored
More informationSolving Parabolic Partial Delay Differential. Equations Using The Explicit Method And Higher. Order Differences
Jornal of Kfa for Maemacs and Compe Vol. No.7 Dec pp 77-5 Solvng Parabolc Paral Delay Dfferenal Eqaons Usng e Eplc Meod And Hger Order Dfferences Asss. Prof. Amal Kalaf Haydar Kfa Unversy College of Edcaon
More informationMANY real-world applications (e.g. production
Barebones Parcle Swarm for Ineger Programmng Problems Mahamed G. H. Omran, Andres Engelbrech and Ayed Salman Absrac The performance of wo recen varans of Parcle Swarm Opmzaon (PSO) when appled o Ineger
More informationIncluding the ordinary differential of distance with time as velocity makes a system of ordinary differential equations.
Soluons o Ordnary Derenal Equaons An ordnary derenal equaon has only one ndependen varable. A sysem o ordnary derenal equaons consss o several derenal equaons each wh he same ndependen varable. An eample
More informationNeural Networks-Based Time Series Prediction Using Long and Short Term Dependence in the Learning Process
Neural Neworks-Based Tme Seres Predcon Usng Long and Shor Term Dependence n he Learnng Process J. Puchea, D. Paño and B. Kuchen, Absrac In hs work a feedforward neural neworksbased nonlnear auoregresson
More informationFuzzy Set Theory in Modeling Uncertainty Data. via Interpolation Rational Bezier Surface Function
Appled Mahemacal Scences, Vol. 7, 013, no. 45, 9 38 HIKARI Ld, www.m-hkar.com Fuzzy Se Theory n Modelng Uncerany Daa va Inerpolaon Raonal Bezer Surface Funcon Rozam Zakara Deparmen of Mahemacs, Faculy
More informationChapter 6: AC Circuits
Chaper 6: AC Crcus Chaper 6: Oulne Phasors and he AC Seady Sae AC Crcus A sable, lnear crcu operang n he seady sae wh snusodal excaon (.e., snusodal seady sae. Complee response forced response naural response.
More informationNovel Technique for Dynamic Analysis of Shear-Frames Based on Energy Balance Equations
Novel Technque for Dynamc Analyss of Shear-Frames Based on Energy Balance Equaons Mohammad Jall Sadr Abad, Mussa Mahmoud,* and Earl Dowell 3. Ph.D. Suden, Deparmen of Cvl Engneerng, Shahd Rajaee Teacher
More informationObserver Design for Nonlinear Systems using Linear Approximations
Observer Desgn for Nonlnear Ssems sng Lnear Appromaons C. Navarro Hernandez, S.P. Banks and M. Aldeen Deparmen of Aomac Conrol and Ssems Engneerng, Unvers of Sheffeld, Mappn Sree, Sheffeld S 3JD. e-mal:
More informationMotion of Wavepackets in Non-Hermitian. Quantum Mechanics
Moon of Wavepaces n Non-Herman Quanum Mechancs Nmrod Moseyev Deparmen of Chemsry and Mnerva Cener for Non-lnear Physcs of Complex Sysems, Technon-Israel Insue of Technology www.echnon echnon.ac..ac.l\~nmrod
More informationON THE WEAK LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS
ON THE WEA LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS FENGBO HANG Absrac. We denfy all he weak sequenal lms of smooh maps n W (M N). In parcular, hs mples a necessary su cen opologcal
More informationResearch Article Adaptive Synchronization of Complex Dynamical Networks with State Predictor
Appled Mahemacs Volume 3, Arcle ID 39437, 8 pages hp://dxdoorg/55/3/39437 Research Arcle Adapve Synchronzaon of Complex Dynamcal eworks wh Sae Predcor Yunao Sh, Bo Lu, and Xao Han Key Laboraory of Beng
More informationAn introduction to Support Vector Machine
An nroducon o Suppor Vecor Machne 報告者 : 黃立德 References: Smon Haykn, "Neural Neworks: a comprehensve foundaon, second edon, 999, Chaper 2,6 Nello Chrsann, John Shawe-Tayer, An Inroducon o Suppor Vecor Machnes,
More informationA Hybrid Variational Iteration Method for Blasius Equation
Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method
More information( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model
BGC1: Survval and even hsory analyss Oslo, March-May 212 Monday May 7h and Tuesday May 8h The addve regresson model Ørnulf Borgan Deparmen of Mahemacs Unversy of Oslo Oulne of program: Recapulaon Counng
More informationAdvanced Macroeconomics II: Exchange economy
Advanced Macroeconomcs II: Exchange economy Krzyszof Makarsk 1 Smple deermnsc dynamc model. 1.1 Inroducon Inroducon Smple deermnsc dynamc model. Defnons of equlbrum: Arrow-Debreu Sequenal Recursve Equvalence
More informationBorn Oppenheimer Approximation and Beyond
L Born Oppenhemer Approxmaon and Beyond aro Barba A*dex Char Professor maro.barba@unv amu.fr Ax arselle Unversé, nsu de Chme Radcalare LGHT AD Adabac x dabac x nonadabac LGHT AD From Gree dabaos: o be
More informationResponse of MDOF systems
Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss
More informationDual Approximate Dynamic Programming for Large Scale Hydro Valleys
Dual Approxmae Dynamc Programmng for Large Scale Hydro Valleys Perre Carpener and Jean-Phlppe Chanceler 1 ENSTA ParsTech and ENPC ParsTech CMM Workshop, January 2016 1 Jon work wh J.-C. Alas, suppored
More informationDynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005
Dynamc Team Decson Theory EECS 558 Proec Shruvandana Sharma and Davd Shuman December 0, 005 Oulne Inroducon o Team Decson Theory Decomposon of he Dynamc Team Decson Problem Equvalence of Sac and Dynamc
More informationJournal of Theoretical and Applied Information Technology.
Journal of heorecal and Appled Informaon echnology 5-9 JAI. All rghs reserved. www.ja.org NEW APPROXIMAION FOR ANDOFF RAE AND NUMBER OF ANDOFF PROBABILIY IN CELLULAR SYSEMS UNDER GENERAL DISRIBUIONS OF
More informationSolving the multi-period fixed cost transportation problem using LINGO solver
Inernaonal Journal of Pure and Appled Mahemacs Volume 119 No. 12 2018, 2151-2157 ISSN: 1314-3395 (on-lne verson) url: hp://www.pam.eu Specal Issue pam.eu Solvng he mul-perod fxed cos ransporaon problem
More informatione-journal Reliability: Theory& Applications No 2 (Vol.2) Vyacheslav Abramov
June 7 e-ournal Relably: Theory& Applcaons No (Vol. CONFIDENCE INTERVALS ASSOCIATED WITH PERFORMANCE ANALYSIS OF SYMMETRIC LARGE CLOSED CLIENT/SERVER COMPUTER NETWORKS Absrac Vyacheslav Abramov School
More informationAn Improved Flower Pollination Algorithm for Solving Integer Programming Problems
Appl. Mah. Inf. Sc. Le. 3, No. 1, 31-37 (015 31 Appled Mahemacs & Informaon Scences Leers An Inernaonal Journal hp://dx.do.org/10.1785/amsl/030106 An Improved Flower Pollnaon Algorhm for Solvng Ineger
More informationSupplementary Material to: IMU Preintegration on Manifold for E cient Visual-Inertial Maximum-a-Posteriori Estimation
Supplemenary Maeral o: IMU Prenegraon on Manfold for E cen Vsual-Ineral Maxmum-a-Poseror Esmaon echncal Repor G-IRIM-CP&R-05-00 Chrsan Forser, Luca Carlone, Fran Dellaer, and Davde Scaramuzza May 0, 05
More informationChapter 2 Linear dynamic analysis of a structural system
Chaper Lnear dynamc analyss of a srucural sysem. Dynamc equlbrum he dynamc equlbrum analyss of a srucure s he mos general case ha can be suded as akes no accoun all he forces acng on. When he exernal loads
More informationTrack Properities of Normal Chain
In. J. Conemp. Mah. Scences, Vol. 8, 213, no. 4, 163-171 HIKARI Ld, www.m-har.com rac Propes of Normal Chan L Chen School of Mahemacs and Sascs, Zhengzhou Normal Unversy Zhengzhou Cy, Hennan Provnce, 4544,
More information