Significance of Dirichlet Series Solution for a Boundary Value Problem
|
|
- Mary Sims
- 5 years ago
- Views:
Transcription
1 IOSR Journal of Engneerng (IOSRJEN) ISSN (e): 5-3 ISSN (p): Vol. 6 Issue 6(June. 6) V PP Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem Achala L. Nargund* and Pramod S.* *P.G. Department of Mathematcs and Research Centre n Appled Mathematcs M.E.S College of Arts Commerce and Scence Bengaluru-563 Abstract: Drchlet seres s an exponental power seres ntroduced by P. G. L. Drchlet a German mathematcan. Usng ths power seres we study the boundary-layer equaton of flow over a nonlnearly stretchng sheet n the presence of magnetc feld. The soluton obtaned by ths method s n good agreement wth exstng solutons. Keywords: Boundary Layer Equatons Adoman decomposton method Homotopy Analyss Method Drchlet Seres Newton-Raphson Method. I. INTRODUCTION The boundary layer flow caused by a contnuously stretchng sheet s often encountered n many engneerng and ndustral processes. These flows are exstng n the polymer ndustry n the manufacture of sheetng materal through an extruson process and coolng of an nfnte metallc plate. Most boundary layer models can be reduced to systems of nonlnear ordnary dfferental equatons whch are usually solved ether by numercal methods or by analytc methods. Analytc methods have sgnfcant advantages over pure numercal methods n provdng more convergent solutons. In the modern developments of the theory of power seres a great part has been played by a varety of methods of summaton of oscllatng seres whch we assocate wth the names of Frobenus Holder Cesaro Borel Lndelof MttagLeffler and Le Roy. Of these defntons the smplest and the most natural s that whch defnes the sum of an oscllatng seres as the lmt of the arthmetc mean of ts frst n partal sums. Ths defnton was generalzed n two dfferent ways by Holder and by Cesaro who thus arrved at two systems of defntons the complete equvalence of whch has been establshed only recently by Knopp Schnee Ford and Schur. The range of applcaton of Cesaro s methods s lmted n a way whch forbds ther applcaton to the problem of the analytcal contnuaton of the functon represented by a Taylor s seres. A power seres outsde ts crcle of convergence dverges too crudely for the applcaton of such methods: more powerful though less delcate methods such as Borel s are requred. But Cesaro s methods have proved of hghest value n the study of power seres on the crcle of convergence and closely connected problems of the theory of Fourer seres. And t s natural to suppose that n the theory of Drchlet Seres where we are dealng wth seres whose convergence or dvergence s of a much more delcate character than s n general that of power seres they wll fnd a wder feld of applcaton [5] [6]. Drchlet seres soluton s an exponental seres soluton whch are most useful especally n obtanng derved quanttes than pure numercal schemes. The accuracy and the unqueness of the soluton so obtaned can be confrmed usng other equally powerful sem numercal schemes. Ths method explaned by P. L. Sachdev [9]. Sachdev. et. al () proposed the Drchlet seres soluton approach to unform flow past a sem-nfnte flat plate. Here they have found the soluton of free conventon flows n saturated porous meda and also soluton of Falkner-Skan equaton n the axsymmetrc flow due to stretchng flat surface []. Sachdev. et. al (5) proposed the Drchlet seres solutons to the boundary value problems for thrd order nonlnear ordnary dfferental equatons over an nfnte nterval. In ths paper they found the soluton of Falkner-Skan equaton occurs n the magneto hydrodynamcs []. Awang. et. al [] have studed the boundary layer equaton of flow over a nonlnearly stretchng sheet n the presence of chemcal reacton and a magnetc feld usng Adoman Decomposton Method (ADM). S. B. Sathyanarayana and L. N. Achala [] nvestgated the soluton by Homotopy Analyss Method (HAM) for the boundary layer flow of a vscous flow over a nonlnearly stretchng sheet n the absence of a chemcal reacton and n presence of magnetc feld. We are nterested n applyng the Drchlet Seres Soluton method to obtan an approxmate analytc soluton of the boundary layer vscous flow over a nonlnearly stretchng sheet n the Internatonal organzaton of Scentfc Research 8 P a g e
2 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem absence of a chemcal reacton and n presence of magnetc feld. Comparson of the present soluton wth the solutons obtaned by Awang. et. al [] n the absence of a chemcal reacton and S. B. Sathyanarayana and L. N. Achala [] by HAM were also made. II. GOVERNING EQUATIONS Here we consder the steady two-dmensonal ncompressble flow of an electrcally conductng vscous flud past a nonlnearly sem-nfnte stretchng sheet under the nfluence of a constant transverse appled magnetc feld. The magnetc Reynolds number s assumed small and neglgble n comparson to the appled magnetc feld. The governng boundary layer equatons are u x v y = () u u u B u v = v u m x y y () where x and y are dstances along and perpendcular to the sheet respectvely u and v are component of the velocty along x and y drectons respectvely v knematc vscosty flud densty electrcal m conductvty B strength of the magnetc feld. The correspondng boundary condtons for nonlnear stretchng sheet are as follow u ( x ) = a x cx v ( x ) = (3) u a s y (4) where d and c are constants. We ntroduce the smlarty transformatons [] a y u a x f c x g = = ' ( ) ' ( ) (5) m cx B (6) m v = a f ( ) g ( ) N = a / a m substtutng equatons (5) and (6) n () and () we obtan the followng ordnary dfferental equatons f ''' ff '' f ' N f ' = (7) g ''' fg '' 3 f ' g ' f '' g N g ' = (8) subject to boundary condtons (3) and (4) f ( ) = f ' ( ) = f ' ( ) = (9) g ( ) = g ' ( ) = g ' ( ) = () where f and g are functons related to the velocty fled N s a magnetc parameter and the prmes denote dfferentaton wth respect to. Internatonal organzaton of Scentfc Research 9 P a g e
3 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem III. DIRICHLET SERIES APPROACH TO BOUNDARY VALUE PROBLEM OVER AN INFINITE INTERVAL We assume the Drchlet seres solutons to equatons (7) and (8) satsfyng f '( ) = and g '( ) = [3] [4] n the form f ( ) = b d e () = g ( ) = l p e () = where > d and p are parameters. Substtutng () and () n (7) and (8) we get 3 [ N ] b d e [ k k ] b b d e = (3) k k = = k = and 3 [ N N ] l p e b d e = = = k = [6 k 3 k ] b l d p e = k k k (4) For = equatons (3) and (4) reduces to [ N ] b d e = (5) bd =. (6) To avod trval soluton we set b = l =. Hence from equatons (5) and (6) we can wrte = N (7) = (8) where b and d. Substtutng equatons (7) and (8) n equatons (3) and (4) we obtan recursve relatons for the coeffcents b and l ( = ) = [ ] (9) k k ( )( N ) k = b k k b b and 3 d k = [ ] ( ). () k k ( )( N ) k = p l k k b l If the seres () and () converge absolutely when > for some then these seres converge absolutely and unformly n the half plane R e ( ) R e ( ) such that f ' ( ) = and g ' ( ) = [3] [4]. A general dscusson of the convergence etc. of the Drchlet seres () and () can be found n [5] [6]. The unknown parameters d p are determned from the remanng boundary condtons (9) and () at Internatonal organzaton of Scentfc Research P a g e
4 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem = as follows N f ( ) = b d () = f ' ( ) = ( ) b d () = g ( ) = l p (3) = g ' ( ) = ( ) l p. (4) = The numercal values of d and p are calculated by applyng Newton - Raphson method to equatons () () and (4) (Table ). Substtutng equatons (7) and (8) n equatons () and () then the Drchlet Seres solutons for (7) and (8) wll be N f ( ) = b d e (5) = g ( ) = l p e (6) = where b and l can be calculated by usng equatons (9) and (). The shear stress at the surface s gven by 3 f '' ( ) = b d. (7) = The exact soluton of (7) subject to boundary condtons (9) s [6] f ( ) = [ exp ( N )] (8) N f '' ( ) = N. (9) Obtaned Drchlet seres soluton (5) and exact soluton (8) are compared graphcally for the dfferent values of N n Fgure. The exact shear stress gven n (9) s compared numercally wth our Drchlet seres shear stress (9) n Table. IV. NUMERICAL RESULTS AND CONCLUSIONS In the present paper we have gven approxmate analytc soluton of the boundary layer vscous flow over a nonlnearly stretchng sheet n the absence of a chemcal reacton and n presence of magnetc feld n the form of Drchlet seres (5) and (6). The calculated values of f ''( ) representng shear stress at the surface for the dfferent sets of values of N d and are gven n Table. Comparson of the values obtaned by the Drchlet seres method wth other methods gven n Table. The velocty f '( ) of exact soluton (8) and Drchlet seres soluton (5) are compared graphcally for the dfferent values of N n Fgure. Internatonal organzaton of Scentfc Research P a g e
5 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem Fgures represents the component of velocty u ( x y ) (5) and Fgures represents the component of velocty v ( x y ) (6) for the dfferent values N. Both u ( x y ) and v ( x y ) are obtaned by substtutng Drchlet seres (5) and (6) n equatons(5) and (6). We can observe that the component of velocty v ( x y ) movng upwards as N ncreases. The soluton obtaned by usng the Drchlet seres method matches wth the soluton obtaned by usng Adoman Decomposton Method [] Homotopy Analyss Method [] and the exact soluton [6]. We conclude that the Drchlet seres method s a strong analytc method to solve nonlnear dfferental equatons and t produces good convergent soluton. Table : Comparson of the values of f '' ( ) obtaned by the Drchlet seres method and exact soluton for the dfferent values of N and d. N d ' f ( ) ' f ( ) Drchlet Exact Table : Comparson of the values of f '' ( ) obtaned by usng the Drchlet Seres Method and other methods. N Drchlet Seres Exact ADM HAM Fgure : Velocty plot of f ( ) for dfferent N Internatonal organzaton of Scentfc Research P a g e
6 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem Fgure : Velocty plot of f '( ) for dfferent N Fgure 3: u ( x y ) for N = Fgure 4: v ( x y ) for N = Internatonal organzaton of Scentfc Research 3 P a g e
7 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem Fgure 5: u ( x y ) for N =.5 Fgure 6: v ( x y ) for N =.5 Fgure 7: u ( x y ) for N =9 Internatonal organzaton of Scentfc Research 4 P a g e
8 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem Fgure 8: v ( x y ) for N =9 Fgure 9: u ( x y ) for N = 5 Fgure : v ( x y ) for N = 5 V. ACKNOWLEDGEMENT Internatonal organzaton of Scentfc Research 5 P a g e
9 Sgnfcance of Drchlet Seres Soluton for a Boundary Value Problem The authors are thankful to Vson Group of Scence and Technology (VGST) for provdng fnancal assstance through GRD 5 CISE. REFERENCES [] S. Awang Kechl and I. Hashm Seres soluton of flow over nonlnearly stretchng Sheet wth chemcal reacton and magnetc feld Physcs Letters A [] S. B. Sathyanarana and L. N. Achala Homotopy analyss method for flow over nonlnearly stretchng sheet wth magnetc Feld Journal of Appled Mathematcs and Flud mechancs ISSN Volume 3 Number pp. 5-. [3] T.K.Kravchenko A.I.Yablonsk Soluton of an nfnte boundary value problem for thrd order equaton Dfferental nye Uranenya vol. pp [4] T.K. Kravchenko A.I.Yablonsk A boundary value problem on a sem-nfnte nterval Dfferental nye Uranenya vol. 8() pp [5] S.Resz Introducton to Drchlet seres Camb. Unv. Press 957. [6] G.H. Hardy M. Resz The general theory of Drchlet s seres Cambrdge Unv. Press 95. [7] J.H. Merkn A note on the soluton of a dfferental equaton arsng n boundary layer theory J. Engg. Mathematcs [8] P.L. Sachdev Nonlnear ordnary dfferental equatons and ther applcatons Marcel Dekker INC 99. [9] P.L. Sachdev N. M. Bujurke and N. P. Pa Drchlet seres soluton of equatons arsng n boundary layer theory Mathematcal and computer modellng [] V. M. Falkner and S. W. Skan Solutons of the boundary layer equatons Phl. Soc. Mag. : [] P. L. Sachdev N. M. Bujurke and V. B. Awat Boundary value problems for thrd order nonlnear ordnary dfferental equatons Studes n Appled Mathematcs Vol. 5 No. 3 pp [] N. M. Bujurke R. B. Kudenatt and V. B. Awat Drchlet seres soluton of mhd flow over a nonlnear stretchng sheet Internatonal journal of appled mathematcs and engneerng scences Vol. 5 No January-June. [3] N. M. Bujurke R. B. Kudenatt and V. B. Awat An exponental seres method for the soluton of free convecton boundary layer flow n a saturated porous medum Amercan journal of computatonal mathematcs 4-. [4] N. M. Bujurke and V. B. Awat Approxmate analytcal solutons of MHD flow of a vscous flud on a nonlnear porous shrnkng sheet Bulletn of the nternatonal mathematcal vrtual nsttute vol [5] R. B.Kudenatt V. B.Awat and N. M.Bujurke Exact analytcal solutons of class of boundary layer equatons for a stretchng surface Appl Math Comp vol. 8 pp [6] F. T. Akyldz H. Bellout K. Vajravelu J. Math. Anal. Appl Internatonal organzaton of Scentfc Research 6 P a g e
A 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 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 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 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 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 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 informationIrregular vibrations in multi-mass discrete-continuous systems torsionally deformed
(2) 4 48 Irregular vbratons n mult-mass dscrete-contnuous systems torsonally deformed Abstract In the paper rregular vbratons of dscrete-contnuous systems consstng of an arbtrary number rgd bodes connected
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 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 informationEffect of variable thermal conductivity on heat and mass transfer flow over a vertical channel with magnetic field intensity
Appled and Computatonal Mathematcs 014; 3(): 48-56 Publshed onlne Aprl 30 014 (http://www.scencepublshnggroup.com/j/acm) do: 10.11648/j.acm.014030.1 Effect of varable thermal conductvty on heat and mass
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 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 informationMHD STEADY FLOW IN A CHANNEL WITH SLIP AT THE PERMEABLE BOUNDARIES
GENERAL PHYSICS MHD STEADY FLOW IN A CHANNEL WITH SLIP AT THE PERMEABLE BOUNDARIES O.D. MAKINDE, E. OSALUSI Appled Mathematcs Department, Unversty of Lmpopo, Prvate Bag X116, Sovenga 77, South Afrca Receved
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 informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
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 informationMATH 5630: Discrete Time-Space Model Hung Phan, UMass Lowell March 1, 2018
MATH 5630: Dscrete Tme-Space Model Hung Phan, UMass Lowell March, 08 Newton s Law of Coolng Consder the coolng of a well strred coffee so that the temperature does not depend on space Newton s law of collng
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 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 informationSTUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS
Blucher Mechancal Engneerng Proceedngs May 0, vol., num. www.proceedngs.blucher.com.br/evento/0wccm STUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS Takahko Kurahash,
More informationn α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0
MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector
More informationMore metrics on cartesian products
More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of
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 informationA Numerical Study of Heat Transfer and Fluid Flow past Single Tube
A Numercal Study of Heat ransfer and Flud Flow past Sngle ube ZEINAB SAYED ABDEL-REHIM Mechancal Engneerng Natonal Research Center El-Bohos Street, Dokk, Gza EGYP abdelrehmz@yahoo.com Abstract: - A numercal
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 informationBuckling analysis of single-layered FG nanoplates on elastic substrate with uneven porosities and various boundary conditions
IOSR Journal of Mechancal and Cvl Engneerng (IOSR-JMCE) e-issn: 78-1684,p-ISSN: 30-334X, Volume 15, Issue 5 Ver. IV (Sep. - Oct. 018), PP 41-46 www.osrjournals.org Bucklng analyss of sngle-layered FG nanoplates
More informationPrinciples of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer
Prncples of Food and Boprocess Engneerng (FS 31) Solutons to Example Problems on Heat Transfer 1. We start wth Fourer s law of heat conducton: Q = k A ( T/ x) Rearrangng, we get: Q/A = k ( T/ x) Here,
More informationNumerical Solution of One-Dimensional Heat and Wave Equation by Non-Polynomial Quintic Spline
Internatonal Journal of Mathematcal Modellng & Computatons Vol. 05, No. 04, Fall 2015, 291-305 Numercal Soluton of One-Dmensonal Heat and Wave Equaton by Non-Polynomal Quntc Splne J. Rashdna a, and M.
More informationarxiv: v1 [math.co] 12 Sep 2014
arxv:1409.3707v1 [math.co] 12 Sep 2014 On the bnomal sums of Horadam sequence Nazmye Ylmaz and Necat Taskara Department of Mathematcs, Scence Faculty, Selcuk Unversty, 42075, Campus, Konya, Turkey March
More informationInductance Calculation for Conductors of Arbitrary Shape
CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors
More informationVisco-Rubber Elastic Model for Pressure Sensitive Adhesive
Vsco-Rubber Elastc Model for Pressure Senstve Adhesve Kazuhsa Maeda, Shgenobu Okazawa, Koj Nshgch and Takash Iwamoto Abstract A materal model to descrbe large deformaton of pressure senstve adhesve (PSA
More informationComputers and Mathematics with Applications
Computers and Mathematcs wth Applcatons 56 (2008 3204 3220 Contents lsts avalable at ScenceDrect Computers and Mathematcs wth Applcatons journal homepage: www.elsever.com/locate/camwa An nnovatve egenvalue
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 informationSTATIC ANALYSIS OF TWO-LAYERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION
STATIC ANALYSIS OF TWO-LERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION Ákos József Lengyel István Ecsed Assstant Lecturer Emertus Professor Insttute of Appled Mechancs Unversty of Mskolc Mskolc-Egyetemváros
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 informationThree-dimensional eddy current analysis by the boundary element method using vector potential
Physcs Electrcty & Magnetsm felds Okayama Unversty Year 1990 Three-dmensonal eddy current analyss by the boundary element method usng vector potental H. Tsubo M. Tanaka Okayama Unversty Okayama Unversty
More informationFixed point method and its improvement for the system of Volterra-Fredholm integral equations of the second kind
MATEMATIKA, 217, Volume 33, Number 2, 191 26 c Penerbt UTM Press. All rghts reserved Fxed pont method and ts mprovement for the system of Volterra-Fredholm ntegral equatons of the second knd 1 Talaat I.
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
More informationA Solution of Porous Media Equation
Internatonal Mathematcal Forum, Vol. 11, 016, no. 15, 71-733 HIKARI Ltd, www.m-hkar.com http://dx.do.org/10.1988/mf.016.6669 A Soluton of Porous Meda Equaton F. Fonseca Unversdad Naconal de Colomba Grupo
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 information( ) = ( ) + ( 0) ) ( )
EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.
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 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 informationFUZZY GOAL PROGRAMMING VS ORDINARY FUZZY PROGRAMMING APPROACH FOR MULTI OBJECTIVE PROGRAMMING PROBLEM
Internatonal Conference on Ceramcs, Bkaner, Inda Internatonal Journal of Modern Physcs: Conference Seres Vol. 22 (2013) 757 761 World Scentfc Publshng Company DOI: 10.1142/S2010194513010982 FUZZY GOAL
More informationTurbulence and its Modelling
School of Mechancal Aerospace and Cvl Engneerng 3rd Year Flud Mechancs Introducton In earler lectures we have consdered how flow nstabltes develop, and noted that above some crtcal Reynolds number flows
More informationThe binomial transforms of the generalized (s, t )-Jacobsthal matrix sequence
Int. J. Adv. Appl. Math. and Mech. 6(3 (2019 14 20 (ISSN: 2347-2529 Journal homepage: www.jaamm.com IJAAMM Internatonal Journal of Advances n Appled Mathematcs and Mechancs The bnomal transforms of the
More informationTHE STURM-LIOUVILLE EIGENVALUE PROBLEM - A NUMERICAL SOLUTION USING THE CONTROL VOLUME METHOD
Journal of Appled Mathematcs and Computatonal Mechancs 06, 5(), 7-36 www.amcm.pcz.pl p-iss 99-9965 DOI: 0.75/jamcm.06..4 e-iss 353-0588 THE STURM-LIOUVILLE EIGEVALUE PROBLEM - A UMERICAL SOLUTIO USIG THE
More informationTurbulent Flow. Turbulent Flow
http://www.youtube.com/watch?v=xoll2kedog&feature=related http://br.youtube.com/watch?v=7kkftgx2any http://br.youtube.com/watch?v=vqhxihpvcvu 1. Caothc fluctuatons wth a wde range of frequences and
More informationDirichlet s Theorem In Arithmetic Progressions
Drchlet s Theorem In Arthmetc Progressons Parsa Kavkan Hang Wang The Unversty of Adelade February 26, 205 Abstract The am of ths paper s to ntroduce and prove Drchlet s theorem n arthmetc progressons,
More informationAssessment of Site Amplification Effect from Input Energy Spectra of Strong Ground Motion
Assessment of Ste Amplfcaton Effect from Input Energy Spectra of Strong Ground Moton M.S. Gong & L.L Xe Key Laboratory of Earthquake Engneerng and Engneerng Vbraton,Insttute of Engneerng Mechancs, CEA,
More informationIndeterminate pin-jointed frames (trusses)
Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all
More informationGrid Generation around a Cylinder by Complex Potential Functions
Research Journal of Appled Scences, Engneerng and Technolog 4(): 53-535, 0 ISSN: 040-7467 Mawell Scentfc Organzaton, 0 Submtted: December 0, 0 Accepted: Januar, 0 Publshed: June 0, 0 Grd Generaton around
More informationFLOW AND HEAT TRANSFER OF THREE IMMISCIBLE FLUIDS IN THE PRESENCE OF UNIFORM MAGNETIC FIELD
THERMAL SCIENCE: Year 04, Vol. 8, No., pp. 09-08 09 FLOW AND HEAT TRANSFER OF THREE IMMISCIBLE FLUIDS IN THE PRESENCE OF UNIFORM MAGNETIC FIELD by Dragša D. NIKODIJEVI], vojn M. STAMENKOVI], Mloš M. JOVANOVI],
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 informationFinite Element Modelling of truss/cable structures
Pet Schreurs Endhoven Unversty of echnology Department of Mechancal Engneerng Materals echnology November 3, 214 Fnte Element Modellng of truss/cable structures 1 Fnte Element Analyss of prestressed structures
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 informationIntroduction to Computational Fluid Dynamics
Introducton to Computatonal Flud Dynamcs M. Zanub 1, T. Mahalakshm 2 1 (PG MATHS), Department of Mathematcs, St. Josephs College of Arts and Scence for Women-Hosur, Peryar Unversty 2 Assstance professor,
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 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 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 informationχ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body
Secton.. Moton.. The Materal Body and Moton hyscal materals n the real world are modeled usng an abstract mathematcal entty called a body. Ths body conssts of an nfnte number of materal partcles. Shown
More informationOn Tiling for Some Types of Manifolds. and their Folding
Appled Mathematcal Scences, Vol. 3, 009, no. 6, 75-84 On Tlng for Some Types of Manfolds and ther Foldng H. Rafat Mathematcs Department, Faculty of Scence Tanta Unversty, Tanta Egypt hshamrafat005@yahoo.com
More informationExistence results for a fourth order multipoint boundary value problem at resonance
Avalable onlne at www.scencedrect.com ScenceDrect Journal of the Ngeran Mathematcal Socety xx (xxxx) xxx xxx www.elsever.com/locate/jnnms Exstence results for a fourth order multpont boundary value problem
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 informationMagnetic Field Around The New 400kV OH Power Transmission Lines In Libya
ECENT ADVANCES n ENEGY & ENVIONMENT Magnetc Feld Around The New kv OH Power Transmsson Lnes In Lbya JAMAL M. EHTAIBA * SAYEH M. ELHABASHI ** Organzaton for Development of Admnstratve Centers, ODAC MISUATA
More informationMixed Convection of the Stagnation-point Flow Towards a Stretching Vertical Permeable Sheet
Malaysan Mxed Journal Convecton of Mathematcal of Stagnaton-pont Scences 1(): Flow 17 - Towards 6 (007) a Stretchng Vertcal Permeable Sheet Mxed Convecton of the Stagnaton-pont Flow Towards a Stretchng
More informationProcedia Computer Science
Avalable onlne at www.scencedrect.com Proceda Proceda Computer Computer Scence Scence 1 (01) 00 (009) 589 597 000 000 Proceda Computer Scence www.elsever.com/locate/proceda Internatonal Conference on Computatonal
More informationCopyright 2014 Tech Science Press CMC, vol.43, no.2, pp.87-95, 2014
Copyrght 2014 Tech Scence Press CMC, vol.43, no.2, pp.87-95, 2014 Analytcal Treatment of the Isotropc and Tetragonal Lattce Green Functons for the Face-centered Cubc, Body-centered Cubc and Smple Cubc
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 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 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 information829. An adaptive method for inertia force identification in cantilever under moving mass
89. An adaptve method for nerta force dentfcaton n cantlever under movng mass Qang Chen 1, Mnzhuo Wang, Hao Yan 3, Haonan Ye 4, Guola Yang 5 1,, 3, 4 Department of Control and System Engneerng, Nanng Unversty,
More informationColor Rendering Uncertainty
Australan Journal of Basc and Appled Scences 4(10): 4601-4608 010 ISSN 1991-8178 Color Renderng Uncertanty 1 A.el Bally M.M. El-Ganany 3 A. Al-amel 1 Physcs Department Photometry department- NIS Abstract:
More informationA 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 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 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 informationNumerical Simulation of One-Dimensional Wave Equation by Non-Polynomial Quintic Spline
IOSR Journal of Matematcs (IOSR-JM) e-issn: 78-578, p-issn: 319-765X. Volume 14, Issue 6 Ver. I (Nov - Dec 018), PP 6-30 www.osrournals.org Numercal Smulaton of One-Dmensonal Wave Equaton by Non-Polynomal
More informationAvailable online at ScienceDirect. Procedia Materials Science 10 (2015 )
Avalable onlne at www.scencedrect.com ScenceDrect Proceda Materals Scence (5 ) 43 53 nd Internatonal Conference on Nanomaterals and Technologes (CNT 4) Influence of thermal and magnetc feld on vbraton
More informationRestricted divisor sums
ACTA ARITHMETICA 02 2002) Restrcted dvsor sums by Kevn A Broughan Hamlton) Introducton There s a body of work n the lterature on varous restrcted sums of the number of dvsors of an nteger functon ncludng
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 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 informationThe Analytical Solution of a System of Nonlinear Differential Equations
Int. Journal of Math. Analyss, Vol. 1, 007, no. 10, 451-46 The Analytcal Soluton of a System of Nonlnear Dfferental Equatons Yunhu L a, Fazhan Geng b and Mnggen Cu b1 a Dept. of Math., Harbn Unversty Harbn,
More informationJoint Statistical Meetings - Biopharmaceutical Section
Iteratve Ch-Square Test for Equvalence of Multple Treatment Groups Te-Hua Ng*, U.S. Food and Drug Admnstraton 1401 Rockvlle Pke, #200S, HFM-217, Rockvlle, MD 20852-1448 Key Words: Equvalence Testng; Actve
More informationSpin-rotation coupling of the angularly accelerated rigid body
Spn-rotaton couplng of the angularly accelerated rgd body Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 E-mal: louaelzen@gmal.com November 1, 2017 All Rghts Reserved. Abstract Ths paper s
More informationAppendix for Causal Interaction in Factorial Experiments: Application to Conjoint Analysis
A Appendx for Causal Interacton n Factoral Experments: Applcaton to Conjont Analyss Mathematcal Appendx: Proofs of Theorems A. Lemmas Below, we descrbe all the lemmas, whch are used to prove the man theorems
More informationInner Product. Euclidean Space. Orthonormal Basis. Orthogonal
Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,
More informationA MODIFIED METHOD FOR SOLVING SYSTEM OF NONLINEAR EQUATIONS
Journal of Mathematcs and Statstcs 9 (1): 4-8, 1 ISSN 1549-644 1 Scence Publcatons do:1.844/jmssp.1.4.8 Publshed Onlne 9 (1) 1 (http://www.thescpub.com/jmss.toc) A MODIFIED METHOD FOR SOLVING SYSTEM OF
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 informationA constant recursive convolution technique for frequency dependent scalar wave equation based FDTD algorithm
J Comput Electron (213) 12:752 756 DOI 1.17/s1825-13-479-2 A constant recursve convoluton technque for frequency dependent scalar wave equaton bed FDTD algorthm M. Burak Özakın Serkan Aksoy Publshed onlne:
More informationLecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES
COMPUTATIONAL FLUID DYNAMICS: FDM: Appromaton of Second Order Dervatves Lecture APPROXIMATION OF SECOMD ORDER DERIVATIVES. APPROXIMATION OF SECOND ORDER DERIVATIVES Second order dervatves appear n dffusve
More informationNew Method for Solving Poisson Equation. on Irregular Domains
Appled Mathematcal Scences Vol. 6 01 no. 8 369 380 New Method for Solvng Posson Equaton on Irregular Domans J. Izadan and N. Karamooz Department of Mathematcs Facult of Scences Mashhad BranchIslamc Azad
More informationMathematical Preparations
1 Introducton Mathematcal Preparatons The theory of relatvty was developed to explan experments whch studed the propagaton of electromagnetc radaton n movng coordnate systems. Wthn expermental error the
More informationHaar Wavelet Collocation Method for the Numerical Solution of Nonlinear Volterra-Fredholm-Hammerstein Integral Equations
Global Journal of Pure and Appled Mathematcs. ISS 0973-768 Volume 3, umber 2 (207), pp. 463-474 Research Inda Publcatons http://www.rpublcaton.com Haar Wavelet Collocaton Method for the umercal Soluton
More informationAppendix B. The Finite Difference Scheme
140 APPENDIXES Appendx B. The Fnte Dfference Scheme In ths appendx we present numercal technques whch are used to approxmate solutons of system 3.1 3.3. A comprehensve treatment of theoretcal and mplementaton
More informationFoundations of Arithmetic
Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an
More informationThe internal structure of natural numbers and one method for the definition of large prime numbers
The nternal structure of natural numbers and one method for the defnton of large prme numbers Emmanul Manousos APM Insttute for the Advancement of Physcs and Mathematcs 3 Poulou str. 53 Athens Greece Abstract
More informationarxiv: v1 [physics.flu-dyn] 16 Sep 2013
Three-Dmensonal Smoothed Partcle Hydrodynamcs Method for Smulatng Free Surface Flows Rzal Dw Prayogo a,b, Chrstan Fredy Naa a a Faculty of Mathematcs and Natural Scences, Insttut Teknolog Bandung, Jl.
More informationThe Finite Element Method
The Fnte Element Method GENERAL INTRODUCTION Read: Chapters 1 and 2 CONTENTS Engneerng and analyss Smulaton of a physcal process Examples mathematcal model development Approxmate solutons and methods of
More informationTHE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD
Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS
More informationConsideration of 2D Unsteady Boundary Layer Over Oscillating Flat Plate
Proceedngs of the th WSEAS Internatonal Conference on Flud Mechancs and Aerodynamcs, Elounda, Greece, August -, (pp-) Consderaton of D Unsteady Boundary Layer Over Oscllatng Flat Plate N.M. NOURI, H.R.
More information