A Solution of Porous Media Equation
|
|
- Earl Wood
- 5 years ago
- Views:
Transcription
1 Internatonal Mathematcal Forum, Vol. 11, 016, no. 15, HIKARI Ltd, A Soluton of Porous Meda Equaton F. Fonseca Unversdad Naconal de Colomba Grupo de Cenca de Materales y Superfces epartamento de Físca Bogotá-Colomba Copyrght c 016 F. Fonseca. Ths artcle s dstrbuted under the Creatve Commons Attrbuton Lcense, whch permts unrestrcted use, dstrbuton, and reproducton n any medum, provded the orgnal work s properly cted. Abstract We solve the nonlnear porous meda equaton usng lattce Boltzmann for a d1q3 lattce velocty method. We fnd the equlbrum dstrbuton accordng to the porous meda equaton. Also, we use the tanh method n order to fnd several famles of soltary wave solutons. We present results for two colldng solutons, usng LB method, whch s n agreement wth the tanh soluton. Mathematcs Subject Classfcaton: 35-XX, 34-XX, 76xx Keywords: Porous Meda Equaton, Lattce-Boltzmann, Tanh Functon 1 Introducton ffuson s a common n many research felds n physcs, chemstry, bology, fnance and ngeneerng use ther methods and results [1]. A lot of nvestgaton has been made n the theory of nonlnear dffuson equatons such as classcal methods [], nonclasscal methods [3], generalzed condtonal symmetry [4] nonlocal symmetry method [5], and the truncated Panleve approach [6], etc. For a further and deep research on the mathematcal propertes of porous meda equaton should be consulted reference [7], and references theren. Also, n the search for solutons to these complex nonlnear equatons, we can fnd the so called soltary wave solutons. Among them, one of the most knwon and appled s the Tanh method [8], used n ths work.
2 7 F. Fonseca On the other hand, lattce-boltzmann LB) technque s the dscretzed verson of the Boltzmann equaton, who responses for the spato-temporal evoluton of the statstcal dstrbuton functon, whch s a qute complex ntegrodfferental equaton. LB over the years has proven ts effectveness and adaptablty to fnd solutons to a large number of problems n physcs [9]. The lattce Boltzmann model The lattce Boltzmann equaton s gven by: f x + e t, t + t) f x, t) = Ω x, t) The term Ω x, t)) represents the B.G.K. approxmaton, [10], s: Ω x, t)) = 1 τ f x, t) f eq x, t)) ) Where f x, t) s the dstrbuton functon for partcles wth velocty e at poston x and tme t, and t s the tme step. τ s a nondmensonal relaxaton tme, weghtng the approacng rate to the statstcal equlbrum, and f eq x, t) s equlbrum dstrbuton functon. Usng a unt tme gven by ɛ = δt/e, where e s the velocty dscretzed on a mesh. Then, the lattce-boltzmann equaton s: f x + e ɛ, t + ɛ) f x, t) = Ω x, t) 3) Expandng n a Taylor seres, the dstrbuton functon, up to order fourth, we have: f x + e ɛ, t + ɛ) f x, t) = ɛ + ɛ t + e x ) f + ɛ3 6 t + e x ) 3 t + e f + Oɛ 4 ) x ) f 4) ong a perturbatve expanson of the dervatves n tme n powers of ɛ, we get: And assumng: f = f 0) + ɛf + ɛ f ) + ɛ 3 f 3) 5) f 0) Where the temporal scales are defned as: = f eq) 6)
3 A soluton of porous meda equaton 73 t 0 = t t 1 = ɛt t = ɛt t 3 = ɛt 3 7) And the perturbatve expanson n parameter ɛ of the temporal dervatve operator t = + ɛ 1 + ɛ + ɛ 3 8) t 0 t 1 t t 3 Replacng eqs. 5) and 8) n eq. 4), we get at frst, second and thrd order n ɛ, respectvely, the next set of equatons: f 0 t 0 + e f 0 x = 1 τ f 1 9) f 0 τ1 1 ) t 1 τ ) + e f = 1 t 0 x τ f 10) f 0 t 1 τ τ ) f τ) + e t t 0 x ) 3 + e f 0 t 0 x = 1 τ f 3 3 The moments of the dstrbuton Where φ, u are the macroscopc quanttes defned as: l f 0) = φ = ) + 1 f eq) 1) e f 0) = 0 13) e l, e l,j f 0) l = λφ m δ j 14) Where δ j s Kronecker s delta. ong some algebra, we get: ) ɛ φ ɛτ1 1 t 1 τ ) f x e e j = 1 f ) 15) τ Assumng f ) = βτφ n 16)
4 74 F. Fonseca Fgure 1: The lattce velocty scheme 1Q3. Then If we chose as: φ t = ɛλτ 1 ) φ m x + βφ n 17) = ɛλτ 1 ) 18) Then eq. 17) s the generalzed porous meda equaton [7]: 4 The dstrbuton functon φ t = φ m x + βφ n 19) We use a d1q3, see fgure ), one-dmensonal velocty scheme wth e α = {0, c, c}. Then, the one partcle equlbrum dstrbuton functon s defned as: f eq) = 5 Soltary wave soluton λ φ m = 0 c φ λ φ m = 1 c φ λ φ m = c We choose n eq. 19) wth m =, and n = 4, then: 0) Usng φ t = φ x + βφ4
5 A soluton of porous meda equaton 75 The dervatves change lke: ξ = x at + ξ 0 ) t = a ξ ; x = ξ ; x = ξ 3) Now, we apply the tanh method [8]. varable: Then, we ntroduce an ndependent The dervatves of ξ n terms of Y, are: Y x, t) = tanh ξ) 4) d dξ = 1 Y ) d dy, d dξ = Y 1 Y ) d dy + 1 Y ) d 5) dy The solutons are postulated [8] as: φξ) = m a Y 6) =1 Now, usng eqs. 3) and eq. 5) n eq., we get: a1 Y ) dφ dy = Y 1 Y ) dφ dy + 1 Y ) d φ dy + βφ4 7) The parameter m, n eq. 6), s obtaned by the balance of the hghest-order lnear term wth the nonlnear terms n the transformed equatons. So, we have: Then, eq. 6) s: Y 4 d φ dy φ4 4 + m = 4m m = 1 8) φξ) = a 0 + a 1 Y φξ) = a 0 + a 1 a 0 Y + a 1Y 9)
6 76 F. Fonseca Replacng a1 Y )a 1 = 4Y a 1 a 0 + a 1Y a 1 a 0 + a 1Y )Y ) 30) +a 11 Y + Y 4 ) + βa Y a 3 0a 1 + 6Y a 0a 1 +4Y 3 a 0 a Y 4 a 4 Groupng the coeffcents, n eq 30), n powers of Y and equatng ther coeefcents to zero, we get a set of nonlnear equatons. ong some algebra the solutons are: a 01, = ± β, a 1 1, = ± β, a 6 1 3,4 = ± β 3 a 15 = aβ β a β 8, a 16 = aβ + β a β 8 4β 4β 3) a 17 = a, a 0 3 = a + β ) 1/4 1/4, a 0 4 = a + β ) 1/4 1/4 33) a 05 = a + β ) 1/4 1/4, a 06 = a + β ) 1/4 1/4 34) a 07 = a β ) 1/4 1/4, a 0 8 = a β ) 1/4 1/4 35) a 09 = a β ) 1/4 1/4, a 010 = a β ) 1/4 1/4 36) a 011 = a + 1 ) 1/4 6 b b b 1/4 37)
7 A soluton of porous meda equaton 77 a + 1 ) 1/4 6 b b a 01 = 38) b 1/4 a 013 = a 014 = a + 1 ) 1/4 6 b b 39) b 1/4 a + 1 ) 1/4 6 b b b 1/4 40) a 015 = a ) 1/4 6 b b b 1/4 4 a ) 1/4 6 b b a 016 = 4) b 1/4 Usng a 11,,3,4 : a 017 = a 018 = a ) 1/4 6 b b 43) b 1/4 a ) 1/4 6 b b b 1/4 44) ong the next defntons: a 019,...,6 = ± a + 8a 1 6βa 1 45) l 1 = 187a 4 b a b b ) a 8 b a 6 b a 4 b 8 6
8 78 F. Fonseca Fgure : Two colldng functons, eq. 5), usng LB method. l = 7a b b 4 47) l 3 = 16 7b + 4 l ) 7b 3 l 1 ) + l 1/3 48) 1/3 54b 3 l 4 = 3 7b 4 l ) 7b 3 l 1 ) l 1/3 a 1/3 54b 3 3b 49) l 3 We get: l 5 = 3 7b 4 l ) 7b 3 l 1 ) + l 1/3 a 1/3 54b 3 3b 50) l 3 a 031 = 3b + 1 l3 1 l4 5
9 A soluton of porous meda equaton 79 a 131 = a 4 + a 3b 4 l 3 3 l 3 9a b l3 3 l 1 ) 1/3 4 b l 3 ) 3/ + 18b4 l 3 + l 1/3 l 3 9a b l b4 3 l 1 ) 1/3 l 1 ) 1/3 3 l 1 ) 1/3 l4 5) + l 1/3 l 4 + b l 3 l b l 4 ) 3/ )/a) a 03 = 3b + 1 l3 1 l4 53) a 13 = a 4 + a 3b 4 l 3 3 l 3 9a b l3 3 l 1 ) 1/3 4 b l 3 ) 3/ + 18b4 l 3 + l 1/3 l 3 9a b l b4 3 l 1 ) 1/3 l 1 ) 1/3 3 l 1 ) 1/3 l4 54) + l 1/3 l 4 + b l 3 l b l 4 ) 3/ )/a) a 033 = 3b + 1 l3 + 1 l4 55) a 133 = a 4 + a 3b 4 l 3 3 l 9a b l3 3 l 1 ) 1/3 4 b l 4 ) 3/ 56) + l 1/3 l 3 l 1/3 l 4 l4 3 4 b l 3 ) 3/ + 9a b l 4 18b4 l 1 ) 1/3 3 l 1 ) 1/3 b l 3 l4 + 18b4 l 3 3 l 1 ) 1/3 )/a) a 034 = 3b + 1 l3 + 1 l4 57) a 134 = 4 3 l 3 9a b l b4 l3 58) l 1 ) 1/3 3 l 1 ) 1/3 3 4 b l 4 ) 3/ 3 4 b l 3 ) 3/ + 9a b l 4 18b4 l 1 ) 1/3 3 l 1 ) 1/3 a 4 + a 3b l 1/3 l4 l 3 l4 b l 3 l4 + l 1/3 l 3 )/a)
10 730 F. Fonseca a 035 = 3b 1 l3 1 l5 59) a 135 = l 3 + 9a b l 3 18b4 l3 60) l 1 ) 1/3 3 l 1 ) 1/3 l 1/3 l b l 3 ) 3/ 9a b l 5 l 1 ) 1/3 + 18b4 l 5 + l 1/3 l 4 b l 3 l 1 ) 1/3 3 l b l 5 ) 3/ a 4 a 3b l 3 )/a) a 036 = 3b 1 l3 1 l5 6 a 136 = a 3b + 4 l 3 3 l 3 + 9a b l3 18b4 l3 6) l 1 ) 1/3 3 l 1 ) 1/3 a 4 l 1/3 l b l 3 ) 3/ 9a b l b4 l 1 ) 1/3 3 l 1 ) 1/3 l5 + l 1/3 l 5 b l 3 l b l 5 ) 3/ )/a) a 037 = 3b 1 l3 + 1 l5 63) a 137 = a 4 a 3b + 4 l 3 3 l 3 + 9a b l3 64) l 1 ) 1/3 l 1/3 l 3 3 l 1 ) 1/3 18b4 l b l 3 ) 3/ + 9a b l 5 l 1 ) 1/3 18b4 l 5 l 1/3 l 5 + b l 3 l 1 ) 1/3 3 l5 3 4 b l 5 ) 3/ )/a)
11 A soluton of porous meda equaton 731 a 038 = 3b 1 l3 + 1 l5 65) a 138 = a 3b + 4 l 3 3 l 3 + 9a b l3 18b4 l3 66) l 1 ) 1/3 3 l 1 ) 1/3 l 1/3 l 3 l b l 3 ) 3/ + 9a b l 5 18b4 l 1 ) 1/3 3 l 1 ) 1/3 a 4 l 1/3 l5 + b l 3 l5 3 4 b l 5 ) 3/ )/a) We fnd thrty eght famles of solutons usng Tanh method. famles are: So, the φ 1 a 01, a 15 ), φ a 01, a 16 ), φ 3 a 0, a 15 ) 67) φ 4 a 0, a 16 ), φ 5 a 01, a 17 ), φ 6 a 0, a 17 ) 68) φ 7 a 03, a 11 ), φ 8 a 04, a 11 ), φ 9 a 05, a 11 ) 69) φ 10 a 06, a 11 ), φ 11 a 07, a 1 ), φ 1 a 08, a 1 ) 70) φ 13 a 09, a 1 ), φ 14 a 010, a 1 ), φ 15 a 011, a 13 ) 7 φ 16 a 01, a 13 ), φ 17 a 013, a 13 ), φ 18 a 014, a 13 ) 7) φ 19 a 015, a 14 ), φ 0 a 016, a 14 ), φ 1 a 017, a 14 ) 73) φ a 018, a 14 ), φ 3 a 019, a 11 ), φ 4 a 00, a 11 ) 74)
12 73 F. Fonseca φ 5 a 01, a 1 ), φ 6 a 0, a 1 ), φ 7 a 03, a 13 ) 75) φ 8 a 04, a 13 ), φ 9 a 05, a 14 ), φ 30 a 05, a 14 ) 76) φ 31 a 031, a 131 ), φ 3 a 03, a 13 ), φ 33 a 033, a 133 ) 77) φ 34 a 034, a 134 ), φ 35 a 035, a 135 ), φ 36 a 036, a 136 ) 78) 6 Conclusons φ 37 a 037, a 137 ), φ 38 a 038, a 138 ) 79) We solve the general nonlnear porous meda equaton usng lattce-boltzmann and the Tanh method. Also, we get thrty eght famles of solutons usng Tanh method. As far as we know, ths procedure s totally orgnal and stablshes a contrbuton to the soluton to the porous meda equaton. As a future work, the model could be extended to two and three dmensons. Acknowledgements. Ths research was supported by Unversdad Naconal de Colomba n Hermes project 350. References [1] J. Janssen, O. Manca and R. Manca, Appled ffuson Processes from Engneerng to Fnance, John Wley & Sons, [] V.A. orodntsyn, On nvarant solutons of the equatons on non-lnear heat conducton wth a source, USSR Computatonal Mathematcs and Mathematcal Physcs, 198), [3] W.I. Fushchch, W.M. Shtelen, N.I. Serov, Symmetry Analyss and Exact Solutons of Equatons of Nonlnear Mathematcal Physcs, Kluwer Academc, ordrecht,
13 A soluton of porous meda equaton 733 [4] R.Z. Zhdanov, Condtonal Le-Bäcklund symmetry and reducton of evoluton equatons, Journal of Physcs A: Mathematcal and General, ), [5] G.W. Bluman, J.. Red, S. Kume, New classes of symmetres for partal dfferental equatons, J. Math. Phys., ), [6] F. Carello, M. Tabor, Panlevé expansons for nonntegrable evoluton equatons, Physca : Nonlnear Phenomena, ), [7] J.L. Vázquez, The Porous Medum Equaton: Mathematcal Theory, Oxford Mathematcal a Monographs, [8] W. Malflet and W. Hereman, The Tanh Method: I. Exact solutons of Nonlnear Evoluton and Wave Equatons, Physca Scrpta, ), [9] Sauro Succ, The Lattce Boltzmann Equaton for Flud ynamcs and Beyond, Numercal Mathematcs and Scentfc Computaton, Oxford Unversty Press, 001. [10] P.L. Bathnagar, E.P. Gross and M. Krook, A model for collson processes n gases. I. Small ampltude processes n charged and neutral onecomponent systems, Physcal Revew, ), Receved: June, 016; Publshed: July 6, 016
A Solution of the Harry-Dym Equation Using Lattice-Boltzmannn and a Solitary Wave Methods
Appled Mathematcal Scences, Vol. 11, 2017, no. 52, 2579-2586 HIKARI Ltd, www.m-hkar.com https://do.org/10.12988/ams.2017.79280 A Soluton of the Harry-Dym Equaton Usng Lattce-Boltzmannn and a Soltary Wave
More informationThe Solution of the Two-Dimensional Gross-Pitaevskii Equation Using Lattice-Boltzmann and He s Semi-Inverse Method
Internatonal Journal of Mathematcal Analyss Vol., 7, no., 69-77 HIKARI Ltd, www.m-hkar.com https://do.org/.988/jma.7.634 The Soluton of the Two-Dmensonal Gross-Ptaevsk Equaton Usng Lattce-Boltzmann and
More information(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate
Internatonal Journal of Mathematcs and Systems Scence (018) Volume 1 do:10.494/jmss.v1.815 (Onlne Frst)A Lattce Boltzmann Scheme for Dffuson Equaton n Sphercal Coordnate Debabrata Datta 1 *, T K Pal 1
More informationAsymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation
Nonl. Analyss and Dfferental Equatons, ol., 4, no., 5 - HIKARI Ltd, www.m-har.com http://dx.do.org/.988/nade.4.456 Asymptotcs of the Soluton of a Boundary alue Problem for One-Characterstc Dfferental Equaton
More informationInternational Conference on Advanced Computer Science and Electronics Information (ICACSEI 2013) equation. E. M. E. Zayed and S. A.
Internatonal Conference on Advanced Computer Scence and Electroncs Informaton (ICACSEI ) The two varable (G'/G/G) -expanson method for fndng exact travelng wave solutons of the (+) dmensonal nonlnear potental
More informationQuantum Particle Motion in Physical Space
Adv. Studes Theor. Phys., Vol. 8, 014, no. 1, 7-34 HIKARI Ltd, www.-hkar.co http://dx.do.org/10.1988/astp.014.311136 Quantu Partcle Moton n Physcal Space A. Yu. Saarn Dept. of Physcs, Saara State Techncal
More informationThe Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices
Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan
More informationThe Order Relation and Trace Inequalities for. Hermitian Operators
Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence
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 informationExistence of Two Conjugate Classes of A 5 within S 6. by Use of Character Table of S 6
Internatonal Mathematcal Forum, Vol. 8, 2013, no. 32, 1591-159 HIKARI Ltd, www.m-hkar.com http://dx.do.org/10.12988/mf.2013.3359 Exstence of Two Conjugate Classes of A 5 wthn S by Use of Character Table
More informationResearch Article A Multilevel Finite Difference Scheme for One-Dimensional Burgers Equation Derived from the Lattice Boltzmann Method
Appled Mathematcs Volume 01, Artcle ID 9590, 13 pages do:10.1155/01/9590 Research Artcle A Multlevel Fnte Dfference Scheme for One-Dmensonal Burgers Equaton Derved from the Lattce Boltzmann Method Qaoe
More informationResearch Article Green s Theorem for Sign Data
Internatonal Scholarly Research Network ISRN Appled Mathematcs Volume 2012, Artcle ID 539359, 10 pages do:10.5402/2012/539359 Research Artcle Green s Theorem for Sgn Data Lous M. Houston The Unversty of
More informationComparison of the Population Variance Estimators. of 2-Parameter Exponential Distribution Based on. Multiple Criteria Decision Making Method
Appled Mathematcal Scences, Vol. 7, 0, no. 47, 07-0 HIARI Ltd, www.m-hkar.com Comparson of the Populaton Varance Estmators of -Parameter Exponental Dstrbuton Based on Multple Crtera Decson Makng Method
More informationDETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM
Ganj, Z. Z., et al.: Determnaton of Temperature Dstrbuton for S111 DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM by Davood Domr GANJI
More informationA new Approach for Solving Linear Ordinary Differential Equations
, ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of
More informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationNew Exact Traveling Wave Solutions for Two Nonlinear Evolution Equations
Internatonal Conference on Computer Technology and Scence (ICCTS ) IPCSIT vol. 47 () () IACSIT Press, Sngapore DOI:.7763/IPCSIT..V47.66 New Exact Travelng Wave Solutons for Two Nonlnear Evoluton Equatons
More informationResearch Article Relative Smooth Topological Spaces
Advances n Fuzzy Systems Volume 2009, Artcle ID 172917, 5 pages do:10.1155/2009/172917 Research Artcle Relatve Smooth Topologcal Spaces B. Ghazanfar Department of Mathematcs, Faculty of Scence, Lorestan
More informationSolution of the Hirota Equation Using Lattice-Boltzmann and the Exponential Function Methods
Advanced Studies in Theoretical Physics Vol. 11, 2017, no. 7, 307-315 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/astp.2017.7418 Solution of the Hirota Equation Using Lattice-Boltzmann and the
More informationSharp integral inequalities involving high-order partial derivatives. Journal Of Inequalities And Applications, 2008, v. 2008, article no.
Ttle Sharp ntegral nequaltes nvolvng hgh-order partal dervatves Authors Zhao, CJ; Cheung, WS Ctaton Journal Of Inequaltes And Applcatons, 008, v. 008, artcle no. 5747 Issued Date 008 URL http://hdl.handle.net/07/569
More information), it produces a response (output function g (x)
Lnear Systems Revew Notes adapted from notes by Mchael Braun Typcally n electrcal engneerng, one s concerned wth functons of tme, such as a voltage waveform System descrpton s therefore defned n the domans
More informationGeorgia Tech PHYS 6124 Mathematical Methods of Physics I
Georga Tech PHYS 624 Mathematcal Methods of Physcs I Instructor: Predrag Cvtanovć Fall semester 202 Homework Set #7 due October 30 202 == show all your work for maxmum credt == put labels ttle legends
More informationResearch Article Cubic B-Spline Collocation Method for One-Dimensional Heat and Advection-Diffusion Equations
Appled Mathematcs Volume 22, Artcle ID 4587, 8 pages do:.55/22/4587 Research Artcle Cubc B-Splne Collocaton Method for One-Dmensonal Heat and Advecton-Dffuson Equatons Joan Goh, Ahmad Abd. Majd, and Ahmad
More informationThe Exact Formulation of the Inverse of the Tridiagonal Matrix for Solving the 1D Poisson Equation with the Finite Difference Method
Journal of Electromagnetc Analyss and Applcatons, 04, 6, 0-08 Publshed Onlne September 04 n ScRes. http://www.scrp.org/journal/jemaa http://dx.do.org/0.46/jemaa.04.6000 The Exact Formulaton of the Inverse
More informationThe Tangential Force Distribution on Inner Cylinder of Power Law Fluid Flowing in Eccentric Annuli with the Inner Cylinder Reciprocating Axially
Open Journal of Flud Dynamcs, 2015, 5, 183-187 Publshed Onlne June 2015 n ScRes. http://www.scrp.org/journal/ojfd http://dx.do.org/10.4236/ojfd.2015.52020 The Tangental Force Dstrbuton on Inner Cylnder
More informationCase Study of Markov Chains Ray-Knight Compactification
Internatonal Journal of Contemporary Mathematcal Scences Vol. 9, 24, no. 6, 753-76 HIKAI Ltd, www.m-har.com http://dx.do.org/.2988/cms.24.46 Case Study of Marov Chans ay-knght Compactfcaton HaXa Du and
More informationStatistical inference for generalized Pareto distribution based on progressive Type-II censored data with random removals
Internatonal Journal of Scentfc World, 2 1) 2014) 1-9 c Scence Publshng Corporaton www.scencepubco.com/ndex.php/ijsw do: 10.14419/jsw.v21.1780 Research Paper Statstcal nference for generalzed Pareto dstrbuton
More informationA PROCEDURE FOR SIMULATING THE NONLINEAR CONDUCTION HEAT TRANSFER IN A BODY WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY.
Proceedngs of the th Brazlan Congress of Thermal Scences and Engneerng -- ENCIT 006 Braz. Soc. of Mechancal Scences and Engneerng -- ABCM, Curtba, Brazl,- Dec. 5-8, 006 A PROCEDURE FOR SIMULATING THE NONLINEAR
More informationEntropy generation in a chemical reaction
Entropy generaton n a chemcal reacton E Mranda Área de Cencas Exactas COICET CCT Mendoza 5500 Mendoza, rgentna and Departamento de Físca Unversdad aconal de San Lus 5700 San Lus, rgentna bstract: Entropy
More informationNumerical Solution of Ordinary Differential Equations
Numercal Methods (CENG 00) CHAPTER-VI Numercal Soluton of Ordnar Dfferental Equatons 6 Introducton Dfferental equatons are equatons composed of an unknown functon and ts dervatves The followng are examples
More informationPerfect Fluid Cosmological Model in the Frame Work Lyra s Manifold
Prespacetme Journal December 06 Volume 7 Issue 6 pp. 095-099 Pund, A. M. & Avachar, G.., Perfect Flud Cosmologcal Model n the Frame Work Lyra s Manfold Perfect Flud Cosmologcal Model n the Frame Work Lyra
More informationTransfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system
Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng
More informationGroup Analysis of Ordinary Differential Equations of the Order n>2
Symmetry n Nonlnear Mathematcal Physcs 997, V., 64 7. Group Analyss of Ordnary Dfferental Equatons of the Order n> L.M. BERKOVICH and S.Y. POPOV Samara State Unversty, 4430, Samara, Russa E-mal: berk@nfo.ssu.samara.ru
More informationMagnetic Diffusion using Lattice-Boltzmann
Revsta Mexcana de Físca S 58 2 188 14 DICIEMBRE 212 Magnetc Dffuson usng Lattce-Boltzmann F. Fonseca Physcs Department, Unversdad Naconal de Colomba, Bogotá Colomba. e-mal: frfonsecaf@unal.edu.co Recbdo
More informationUniversity of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015
Lecture 2. 1/07/15-1/09/15 Unversty of Washngton Department of Chemstry Chemstry 453 Wnter Quarter 2015 We are not talkng about truth. We are talkng about somethng that seems lke truth. The truth we want
More informationModule 1 : The equation of continuity. Lecture 1: Equation of Continuity
1 Module 1 : The equaton of contnuty Lecture 1: Equaton of Contnuty 2 Advanced Heat and Mass Transfer: Modules 1. THE EQUATION OF CONTINUITY : Lectures 1-6 () () () (v) (v) Overall Mass Balance Momentum
More informationImplicit Integration Henyey Method
Implct Integraton Henyey Method In realstc stellar evoluton codes nstead of a drect ntegraton usng for example the Runge-Kutta method one employs an teratve mplct technque. Ths s because the structure
More informationNON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS
IJRRAS 8 (3 September 011 www.arpapress.com/volumes/vol8issue3/ijrras_8_3_08.pdf NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS H.O. Bakodah Dept. of Mathematc
More informationSIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME. Abstract
SIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME PACS REFERENCE: 43.20.Mv Andreas Wlde Fraunhofer Insttut für Integrerte Schaltungen, Außenstelle EAS Zeunerstr.
More informationCOMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD
COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,
More informationApplication of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems
Mathematca Aeterna, Vol. 1, 011, no. 06, 405 415 Applcaton of B-Splne to Numercal Soluton of a System of Sngularly Perturbed Problems Yogesh Gupta Department of Mathematcs Unted College of Engneerng &
More informationThe Two-scale Finite Element Errors Analysis for One Class of Thermoelastic Problem in Periodic Composites
7 Asa-Pacfc Engneerng Technology Conference (APETC 7) ISBN: 978--6595-443- The Two-scale Fnte Element Errors Analyss for One Class of Thermoelastc Problem n Perodc Compostes Xaoun Deng Mngxang Deng ABSTRACT
More informationHongyi Miao, College of Science, Nanjing Forestry University, Nanjing ,China. (Received 20 June 2013, accepted 11 March 2014) I)ϕ (k)
ISSN 1749-3889 (prnt), 1749-3897 (onlne) Internatonal Journal of Nonlnear Scence Vol.17(2014) No.2,pp.188-192 Modfed Block Jacob-Davdson Method for Solvng Large Sparse Egenproblems Hongy Mao, College of
More informationCHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE
CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng
More informationOne-sided finite-difference approximations suitable for use with Richardson extrapolation
Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,
More informationResearch Article A Combination Method of Mixed Multiscale Finite-Element and Laplace Transform for Flow in a Dual-Permeability System
Internatonal Scholarly Research Network ISRN Appled Mathematcs Volume 22, Artcle ID 22893, pages do:.542/22/22893 Research Artcle A Combnaton Method of Mxed Multscale Fnte-Element and Laplace ransform
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationGlobal Sensitivity. Tuesday 20 th February, 2018
Global Senstvty Tuesday 2 th February, 28 ) Local Senstvty Most senstvty analyses [] are based on local estmates of senstvty, typcally by expandng the response n a Taylor seres about some specfc values
More informationThermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)
hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In
More informationSolving Fractional Nonlinear Fredholm Integro-differential Equations via Hybrid of Rationalized Haar Functions
ISSN 746-7659 England UK Journal of Informaton and Computng Scence Vol. 9 No. 3 4 pp. 69-8 Solvng Fractonal Nonlnear Fredholm Integro-dfferental Equatons va Hybrd of Ratonalzed Haar Functons Yadollah Ordokhan
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationUniqueness of Weak Solutions to the 3D Ginzburg- Landau Model for Superconductivity
Int. Journal of Math. Analyss, Vol. 6, 212, no. 22, 195-114 Unqueness of Weak Solutons to the 3D Gnzburg- Landau Model for Superconductvty Jshan Fan Department of Appled Mathematcs Nanjng Forestry Unversty
More informationA boundary element method with analytical integration for deformation of inhomogeneous elastic materials
Journal of Physcs: Conference Seres PAPER OPEN ACCESS A boundary element method wth analytcal ntegraton for deformaton of nhomogeneous elastc materals To cte ths artcle: Moh. Ivan Azs et al 2018 J. Phys.:
More informationUsing T.O.M to Estimate Parameter of distributions that have not Single Exponential Family
IOSR Journal of Mathematcs IOSR-JM) ISSN: 2278-5728. Volume 3, Issue 3 Sep-Oct. 202), PP 44-48 www.osrjournals.org Usng T.O.M to Estmate Parameter of dstrbutons that have not Sngle Exponental Famly Jubran
More informationSystem in Weibull Distribution
Internatonal Matheatcal Foru 4 9 no. 9 94-95 Relablty Equvalence Factors of a Seres-Parallel Syste n Webull Dstrbuton M. A. El-Dacese Matheatcs Departent Faculty of Scence Tanta Unversty Tanta Egypt eldacese@yahoo.co
More informationA NUMERICAL COMPARISON OF LANGRANGE AND KANE S METHODS OF AN ARM SEGMENT
Internatonal Conference Mathematcal and Computatonal ology 0 Internatonal Journal of Modern Physcs: Conference Seres Vol. 9 0 68 75 World Scentfc Publshng Company DOI: 0.4/S009450059 A NUMERICAL COMPARISON
More informationConvexity preserving interpolation by splines of arbitrary degree
Computer Scence Journal of Moldova, vol.18, no.1(52), 2010 Convexty preservng nterpolaton by splnes of arbtrary degree Igor Verlan Abstract In the present paper an algorthm of C 2 nterpolaton of dscrete
More informationResearch Article Exact Partition Function for the Random Walk of an Electrostatic Field
Hndaw Advances n Mathematcal Physcs Volume 2017, Artcle ID 6970870, 5 pages https://do.org/10.1155/2017/6970870 Research Artcle Exact Partton Functon for the Random Walk of an Electrostatc Feld Gabrel
More informationEXACT TRAVELLING WAVE SOLUTIONS FOR THREE NONLINEAR EVOLUTION EQUATIONS BY A BERNOULLI SUB-ODE METHOD
www.arpapress.co/volues/vol16issue/ijrras_16 10.pdf EXACT TRAVELLING WAVE SOLUTIONS FOR THREE NONLINEAR EVOLUTION EQUATIONS BY A BERNOULLI SUB-ODE METHOD Chengbo Tan & Qnghua Feng * School of Scence, Shandong
More informationLecture 20: Noether s Theorem
Lecture 20: Noether s Theorem In our revew of Newtonan Mechancs, we were remnded that some quanttes (energy, lnear momentum, and angular momentum) are conserved That s, they are constant f no external
More informationMonotonic Interpolating Curves by Using Rational. Cubic Ball Interpolation
Appled Mathematcal Scences, vol. 8, 204, no. 46, 7259 7276 HIKARI Ltd, www.m-hkar.com http://dx.do.org/0.2988/ams.204.47554 Monotonc Interpolatng Curves by Usng Ratonal Cubc Ball Interpolaton Samsul Arffn
More informationOn the spectral norm of r-circulant matrices with the Pell and Pell-Lucas numbers
Türkmen and Gökbaş Journal of Inequaltes and Applcatons (06) 06:65 DOI 086/s3660-06-0997-0 R E S E A R C H Open Access On the spectral norm of r-crculant matrces wth the Pell and Pell-Lucas numbers Ramazan
More informationSignificance of Dirichlet Series Solution for a Boundary Value Problem
IOSR Journal of Engneerng (IOSRJEN) ISSN (e): 5-3 ISSN (p): 78-879 Vol. 6 Issue 6(June. 6) V PP 8-6 www.osrjen.org Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem Achala L. Nargund* and
More informationNew Exact Solutions of the Kawahara Equation using Generalized F-expansion Method
Journal of Mathematcal Control Scence and Applcatons (JMCSA) Vol. No. 1 (January-June, 16), ISSN : 97-57 Journal of Mathematcal Control Scence and Applcatons (JMCSA) Vol. 1, No. 1, June 7, pp. 189-1 Internatonal
More informationPOLYNOMIAL BASED DIFFERENTIAL QUADRATURE FOR NUMERICAL SOLUTIONS OF KURAMOTO-SIVASHINSKY EQUATION
POLYOMIAL BASED DIFFERETIAL QUADRATURE FOR UMERICAL SOLUTIOS OF KURAMOTO-SIVASHISKY EQUATIO Gülsemay YİĞİT 1 and Mustafa BAYRAM *, 1 School of Engneerng and atural Scences, Altınbaş Unversty, Istanbul,
More informationPrimer on High-Order Moment Estimators
Prmer on Hgh-Order Moment Estmators Ton M. Whted July 2007 The Errors-n-Varables Model We wll start wth the classcal EIV for one msmeasured regressor. The general case s n Erckson and Whted Econometrc
More informationInternational Journal of Algebra, Vol. 8, 2014, no. 5, HIKARI Ltd,
Internatonal Journal of Algebra, Vol. 8, 2014, no. 5, 229-238 HIKARI Ltd, www.m-hkar.com http://dx.do.org/10.12988/ja.2014.4212 On P-Duo odules Inaam ohammed Al Had Department of athematcs College of Educaton
More informationNumerical Simulation of Lid-Driven Cavity Flow Using the Lattice Boltzmann Method
Proceedngs of the 3th WSEAS Internatonal Conference on APPLIED MATHEMATICS (MATH'8) Numercal Smulaton of Ld-Drven Cavty Flow Usng the Lattce Boltzmann Method M.A. MUSSA, S. ABDULLAH *, C.S. NOR AZWADI
More informationComparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy
Comparatve Studes of Law of Conservaton of Energy and Law Clusters of Conservaton of Generalzed Energy No.3 of Comparatve Physcs Seres Papers Fu Yuhua (CNOOC Research Insttute, E-mal:fuyh1945@sna.com)
More informationAn identification algorithm of model kinetic parameters of the interfacial layer growth in fiber composites
IOP Conference Seres: Materals Scence and Engneerng PAPER OPE ACCESS An dentfcaton algorthm of model knetc parameters of the nterfacal layer growth n fber compostes o cte ths artcle: V Zubov et al 216
More informationHomogenization of reaction-diffusion processes in a two-component porous medium with a non-linear flux-condition on the interface
Homogenzaton of reacton-dffuson processes n a two-component porous medum wth a non-lnear flux-condton on the nterface Internatonal Conference on Numercal and Mathematcal Modelng of Flow and Transport n
More informationCOMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS
Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS
More informationNumerical Solutions of a Generalized Nth Order Boundary Value Problems Using Power Series Approximation Method
Appled Mathematcs, 6, 7, 5-4 Publshed Onlne Jul 6 n ScRes. http://www.scrp.org/journal/am http://.do.org/.436/am.6.77 umercal Solutons of a Generalzed th Order Boundar Value Problems Usng Power Seres Approxmaton
More information2 Finite difference basics
Numersche Methoden 1, WS 11/12 B.J.P. Kaus 2 Fnte dfference bascs Consder the one- The bascs of the fnte dfference method are best understood wth an example. dmensonal transent heat conducton equaton T
More informationCanonical transformations
Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,
More informationOpen Systems: Chemical Potential and Partial Molar Quantities Chemical Potential
Open Systems: Chemcal Potental and Partal Molar Quanttes Chemcal Potental For closed systems, we have derved the followng relatonshps: du = TdS pdv dh = TdS + Vdp da = SdT pdv dg = VdP SdT For open systems,
More information2.29 Numerical Fluid Mechanics Fall 2011 Lecture 12
REVIEW Lecture 11: 2.29 Numercal Flud Mechancs Fall 2011 Lecture 12 End of (Lnear) Algebrac Systems Gradent Methods Krylov Subspace Methods Precondtonng of Ax=b FINITE DIFFERENCES Classfcaton of Partal
More informationPhysics 607 Exam 1. ( ) = 1, Γ( z +1) = zγ( z) x n e x2 dx = 1. e x2
Physcs 607 Exam 1 Please be well-organzed, and show all sgnfcant steps clearly n all problems. You are graded on your wor, so please do not just wrte down answers wth no explanaton! Do all your wor on
More informationResearch Article The Solution of Two-Point Boundary Value Problem of a Class of Duffing-Type Systems with Non-C 1 Perturbation Term
Hndaw Publshng Corporaton Boundary Value Problems Volume 9, Artcle ID 87834, 1 pages do:1.1155/9/87834 Research Artcle The Soluton of Two-Pont Boundary Value Problem of a Class of Duffng-Type Systems wth
More informationON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION
Advanced Mathematcal Models & Applcatons Vol.3, No.3, 2018, pp.215-222 ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EUATION
More informationElectron-Impact Double Ionization of the H 2
I R A P 6(), Dec. 5, pp. 9- Electron-Impact Double Ionzaton of the H olecule Internatonal Scence Press ISSN: 9-59 Electron-Impact Double Ionzaton of the H olecule. S. PINDZOLA AND J. COLGAN Department
More informationCausal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim
Causal Damonds M. Aghl, L. Bombell, B. Plgrm Introducton The correcton to volume of a causal nterval due to curvature of spacetme has been done by Myrhem [] and recently by Gbbons & Solodukhn [] and later
More informationApplication of the lattice Boltzmann method for solving conduction problems with heat flux boundary condition.
November 5-7, 9 - Sousse Tunsa Applcaton of the lattce Boltzmann method for solvng conducton problems wth heat flux boundary condton. Raoudha CHAABANE, Faouz ASKRI, Sass Ben NASRALLAH Laboratore d Etudes
More informationLecture 12: Discrete Laplacian
Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly
More informationPhysics 5153 Classical Mechanics. Principle of Virtual Work-1
P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal
More informationProblem Points Score Total 100
Physcs 450 Solutons of Sample Exam I Problem Ponts Score 1 8 15 3 17 4 0 5 0 Total 100 All wor must be shown n order to receve full credt. Wor must be legble and comprehensble wth answers clearly ndcated.
More informationSeptic B-Spline Collocation Method for the Numerical Solution of the Modified Equal Width Wave Equation
Appled Mathematcs 79-749 do:.46/am..698 Publshed Onlne June (http://www.scrp.org/ournal/am) Septc B-Splne Collocaton Method for the umercal Soluton of the Modfed Equal Wdth Wave Equaton Abstract Turab
More information2-π STRUCTURES ASSOCIATED TO THE LAGRANGIAN MECHANICAL SYSTEMS UDC 531.3: (045)=111. Victor Blãnuţã, Manuela Gîrţu
FACTA UNIVERSITATIS Seres: Mechancs Automatc Control and Robotcs Vol. 6 N o 1 007 pp. 89-95 -π STRUCTURES ASSOCIATED TO THE LAGRANGIAN MECHANICAL SYSTEMS UDC 531.3:53.511(045)=111 Vctor Blãnuţã Manuela
More informationModelli Clamfim Equazione del Calore Lezione ottobre 2014
CLAMFIM Bologna Modell 1 @ Clamfm Equazone del Calore Lezone 17 15 ottobre 2014 professor Danele Rtell danele.rtell@unbo.t 1/24? Convoluton The convoluton of two functons g(t) and f(t) s the functon (g
More informationA note on almost sure behavior of randomly weighted sums of φ-mixing random variables with φ-mixing weights
ACTA ET COMMENTATIONES UNIVERSITATIS TARTUENSIS DE MATHEMATICA Volume 7, Number 2, December 203 Avalable onlne at http://acutm.math.ut.ee A note on almost sure behavor of randomly weghted sums of φ-mxng
More informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationResearch Article A Generalized Sum-Difference Inequality and Applications to Partial Difference Equations
Hndaw Publshng Corporaton Advances n Dfference Equatons Volume 008, Artcle ID 695495, pages do:0.55/008/695495 Research Artcle A Generalzed Sum-Dfference Inequalty and Applcatons to Partal Dfference Equatons
More informationProjective change between two Special (α, β)- Finsler Metrics
Internatonal Journal of Trend n Research and Development, Volume 2(6), ISSN 2394-9333 www.jtrd.com Projectve change between two Specal (, β)- Fnsler Metrcs Gayathr.K 1 and Narasmhamurthy.S.K 2 1 Assstant
More informationChapter 4 The Wave Equation
Chapter 4 The Wave Equaton Another classcal example of a hyperbolc PDE s a wave equaton. The wave equaton s a second-order lnear hyperbolc PDE that descrbes the propagaton of a varety of waves, such as
More informationNote: Please use the actual date you accessed this material in your citation.
MIT OpenCourseWare http://ocw.mt.edu 6.13/ESD.13J Electromagnetcs and Applcatons, Fall 5 Please use the followng ctaton format: Markus Zahn, Erch Ippen, and Davd Staeln, 6.13/ESD.13J Electromagnetcs and
More informationSOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE 2-TANGENT BUNDLE
STUDIA UNIV. BABEŞ BOLYAI MATHEMATICA Volume LIII Number March 008 SOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE -TANGENT BUNDLE GHEORGHE ATANASIU AND MONICA PURCARU Abstract. In
More informationTrees and Order Conditions
Trees and Order Condtons Constructon of Runge-Kutta order condtons usng Butcher trees and seres. Paul Tranqull 1 1 Computatonal Scence Laboratory CSL) Department of Computer Scence Vrgna Tech. Trees and
More informationNovember 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project
SE 8 Fnal Project Story Shear Frame u m Gven: u m L L m L L EI ω ω Solve for m Story Bendng Beam u u m L m L Gven: m L L EI ω ω Solve for m 3 3 Story Shear Frame u 3 m 3 Gven: L 3 m m L L L 3 EI ω ω ω
More informationBinomial transforms of the modified k-fibonacci-like sequence
Internatonal Journal of Mathematcs and Computer Scence, 14(2019, no. 1, 47 59 M CS Bnomal transforms of the modfed k-fbonacc-lke sequence Youngwoo Kwon Department of mathematcs Korea Unversty Seoul, Republc
More information