International Journal of Pure and Applied Sciences and Technology

Size: px
Start display at page:

Download "International Journal of Pure and Applied Sciences and Technology"

Transcription

1 In. J. Pre Appl. Sci. echnol. () (4) pp. -8 Inernaional Jornal of Pre and Applied Sciences and echnolog ISSN 9-67 Aailable online a.ijopaasa.in Research Paper Effec of Variable Viscosi on hird Grade Flid Flo oer a Radiaie Srface ih Arrhenis Reacion Amos W. Ognsola and Benjamin A. Peer * Deparmen of Pre and Applied Mahemaics Ladoke Akinola Uniersi of echnolog Ogbomoso Nigeria * Corresponding ahor (pbenjamin8@ahoo.ca) (Receied: --4; Acceped: 7-4-4) Absrac: In his ork fecs of ariable iscosi and Arrhenis reacion on he hird grade flid oer a radiaie srface hrogh a poros medim is considered. he goerning parial differenial eqaions ere ransformed ino ordinar differenial eqaions in erms of siable similari ariable. We emploed Galerkin eighed residal mehod o sole he resling non-linear eqaions. he fecs of ariable iscosi parameer Frank-Kameneskii parameer Brinkman nmber Renolds nmber Prandl nmber and Darc nmber on he ssem of flo and he resls ere repored graphicall. Keords: hird grade flid eighed residal mehod Arrhenis reacion radiaie srface and poros medim. Inrodcion Non-Neonian flids hae receied mch aenion han Neonian flids in he recen ears de o is pracical imporance rapid deelopmen of modern indsrial maerials and echnological applicaions. I has gien insigh in he reseroir engineering hea echange beeen soil and amosphere flo of moisre hrogh poros indsrial maerials hea echangers ih flid beds preheaing coal-aer mire ceramic processing caalic reacors polmer solion molen plasics oil recoer o menion b js a fe applicaions. Some maerials behae non-neonianl namel md pasa cheese personal care prodc asphal ice cream oils and he hos of ohers. he rheological characerisics of polmer mels and solions ogeher ih he aribes of some polmeric sbsances hich has lead o he recen orld-ide processing of polmer. he rheological behaior of all he non-neonian flids canno be deermined b a single consiie eqaion.

2 In. J. Pre Appl. Sci. echnol. () (4) -8 Hea ransfer problem of hird grade flids has been sdied b seeral ahors: Makinde and Aziz [] considered he bondar laer flo of iscos nanoflid bonded b a sreching shee. Mkhopadha [] eamined he bondar laer flo and hea ransfer oards an eponeniall sreching poros shee embedded in a poros medim. Krishnend e al [] considered similari solion of mied conecie bondar laer slip flo oer a erical plae. Fosdick and Rajagopal [4] performed a complee hermodnamic analsis of consiie eqaions for he hird grade flid inoling hea ransfer process. Massodi and Chrisie [5] analzed nmericall he flo of a hird grade flid in a pipe iho hea sorce here he shear iscosi as assmed o be emperare dependen. Olajon [6] eamined he flo and naral conecion hea ransfer in a poer-la flid pas a erical plae ih hea generaion. Yrso e al [7] eamined enrop analsis for hird grade flid flo ih Vogel s models of iscosi in annlar pipe. Nadeem e al [8] analicall considered he fecs of parial slip on a forh grade flid ih ariable iscosi and Makinde [9] emploed Hermie-Pade approimaions o ealae hermal radiaion fec of inheren irreersibili in a ariable iscosi channel flo. Massodi and Chrisie [] sdied he fecs of ariable iscosi and iscos dissipaion on he flo of hird grade flid in a pipe. Nadeem e al [] sdied analical solions for pipe flo of a forh grade flid ih Renolds and Vogel s models of iscosiies. Lazars [] eamined he fecs of ariable iscosi on he eloci flid and emperare flid sing semi-implici finie difference scheme of Laminar flo in a channel filled ih saraed poros media. he resls sho ha he eloci flid and emperare flid increases as ariable iscosi parameer increases. Moiaed b he ork of Haa e al [] he considered he fec of jole heaing and hermal radiaion in flo of hird grade flid oer a radiaie srface. Folloing Szeri and Rajagopal [4] an incompressible homogeneos flid of hird grade is characerized b Cach sress τ of he folloing form: τ pi β ( ) A α ( ) A α ( ) ( ) A β ( )[ A A A A ] β ( )( ra ) A. A () here pi denoe he indeerminae par of he sress de o he consrain of incompressibili ( ) is he coficien of iscosi and α ( )α ( ) are maerial modli sall rerred o as normal sress coficiens. he kinemaic ensors A A are dined b [] hrogh ( grad ) ( grad ) τ A () d An An An ( grad ) ( grad ) An n. () d d Here denoes maerial ime deriaie and is he eloci ecor. he aboe model conains as a d special sbclass he classical linearl iscos model (he case hen all he coficiens epec are se eqal o zero). Flo of a hermodnamicall compaible flid of hird grade is gien as: ( ) i (4) here i denoes he ni ecor in he -coordinae direcion he direcion ha is chosen parallel he eernal pressre gradiens. In he absence of bod forces he balance of linear momenm d di τ b (Eqaion of Moion) (5) K d

3 In. J. Pre Appl. Sci. echnol. () (4) -8 here K is he poros medim permeabili Q r K di q L d de τ. (6) Here e denoes he inernal energ L is he eloci gradien r is he radian energ boh per ni mass and Q denoes he reacing erm. Goerning Eqaions and Mehod of Solion Folloing aaser e al [] e consider he nsead o-dimensional bondar laer flo of a magneo hdrodnamic (MHD) hrogh a poros medim. he basic goerning eqaions are as follos: (7) K B B E σ β α α 6 (8) c Q K E B k p σ β α 4 (9) he appropriae iniial and bondar condiion are as follos as as o V U () here σ is he San-Bolzmann consan k is he mean absorpion coficienq is he hea release per nis mass < V is he injecion > V is he scion c V c a c a U b a are consans E is he aciaing energ R is he niersal gas consan θ -is he dimensionless emperare k is he permeabili of he poros media K is he hermal condcii is he densi p C is he specific hea a consan pressre is he dnamic iscosi r is he iscos heaing fec direcion ψ is he Frank-Kameneskii parameer η is he similari ariable is he fecie iscosi e is he hermal epansion

4 In. J. Pre Appl. Sci. echnol. () (4) -8 4 is he flid iniial emperare or all emperare r is he rerence emperare is he absole emperare ihin he bondar laer... - emperare a he plae α α β are he flid parameers is he dimensionless eloci in he direcion Ψ is he sream fncion is he dimensionless eloci in he direcion is he free sream emperare. From Eqaions (8) and (9) e seek Renolds model of he form Mθ ( ) e () Mθ α e α β 6 σ ( EB B ) K Mθ α k e 4 qr ( ) β σ B E QC Ae K cp We inrodce he folloing ariables and parameers E R () () Ψ U f Ψ Ψ ( η) ( ) θ ( η) and η U E EQC A R 4σ r k ψ e R θ Da. (4) lo Ulo d ( R E) k K Sbsiing Eqaion (4) ino Eqaions () and () e obain d dη α f Mθ ( i ) ( i ) ( e f ) S{ f ηf } α f f ff f S f ηf 6β Re f f m ( E f ) Da 4 S Mθ θ Rd f θ f θ { ηθ 4θ } Bre ( f ) αec Pr S ( εθ ) { η } β ψ Da 4 f f f f f ff f Ecf m Ec f E e θ (5) (6)

5 In. J. Pre Appl. Sci. echnol. () (4) -8 5 Where ψ EQC A E R e 4σ α a α a β a R α α β d ( R E) k K ( c) ( c) ( c) he ransformed bondar condiion is as follos ( ) A f ( ) f ( ) f ( ) θ ( ) θ ( ) S f (8) We proceed o sole Eqaions (5) and (6) sbjec o (8) nmericall sing Galerkin-Weighed Residal Mehod as follos: c a. (7) Le f Ae i i i i i 4 θ Be (9) he resls are presened in Figres -5 Figre : Graph of he eloci fncion f for arios ales of Br.5 Pr Re A S β. Ec.5 α α m E ψ..

6 In. J. Pre Appl. Sci. echnol. () (4) -8 6 Figre : Graph of he emperare fncion θ for arios ales of Br.5 Pr Re A S β. Ec.5 α α m E ψ.. Figre : Graph of he eloci fncion f for arios ales of Br.5 Pr Re A S β. Ec.5 α α m E ψ..

7 In. J. Pre Appl. Sci. echnol. () (4) -8 7 Figre 4: Graph of he emperare fncion θ for arios ales of Br.5 Pr Re A S β. Ec.5 α α m E ψ.. Figre 5: Graph of he emperare fncion θ for arios ales of Br.5 Pr Re A S β. Ec.5 α α m E ψ Discssion of Resls/Conclsion he sd of hird grade flids is eremel imporan de o is ide arie of pracical applicaions in processes sch as filraion of polmer solions and soil remediaion hrogh he remoal of liqid pollans. From Figres -5 he resls sho ha he flid eloci and emperare increases..

8 In. J. Pre Appl. Sci. echnol. () (4) -8 8 increase in each parameers. I is noiced from Figres & 5 ha he emperare profile reach he maimm poin as Darc nmber Frank Kameneskii parameer increases. We obsered from Figre 4 ha he eloci profile has a minimm poin as Frank Kameneskii parameer increases. Conclsion I is conclded ha eloci flid and he emperare flid decreases as Frank Kameneskii parameer and ariable iscosi parameer increases. A ransien decrease in boh he flid eloci and emperare is obsered ih increase in each β α & α non-neonian parameers E Elecric parameer Br Brinkman nmber and Darc nmber hich decreases he porosi in he ssem of flo. For engineering prpose he flo model of or problem represens he oils ell and as he ψ Frank Kameneskii parameer is increasing here is qick recoer of oil from he oils ell. Also he resls of his problem are of grea ineres in prodcion processing aomobile engine for he safe of life and proper handling of he maerials dring processing. Rerences [] O.D. Makinde and A. Aziz Bondar laer flo of a nanoflid oer a non-linearl sreching shee ih a conecie bondar condiion In. J. hermal Sciences 5() 6-. [] S. Mkhopadha MHD bondar laer flo and hea ransfer oer an eponeniall sreching shee embedded in a hermall sraified medim Aleandra Eng. J. 5() [] K. Bhaachara S. Mkhopadha and G.C. Laek Similari solion of mied conecie bondar laer slip flo oer a erical plae Ain Shams Engineering Jornal 4() [4] R.L. Fosdick and K.R. Rajagopal hermodnamics and sabili of flids of hird grade Proc. R. Soc. Lond. A69(98) [5] M. Massodi and I. Chrise Hea ransfer and flo of hird grade flid in a pipe Mah. Modeling Sci. Comp. (99) [6] B.I. Olajon Flo and naral conecion hea ransfer in a poer-la flid pas a erical plae ih hea generaion In. J. Non-Linear Science 7() (9) [7] M. Yrso H. Barakoekem M. Kapc and F. Akso Enrop analsis for hird grade flid flo ih Vogel s models of iscosi in annlar pipe In. J. Non-Linear Mech. 4(8) [8] S. Nadeem and M. Ali Analical solions for pipe flo of a forh grade flid ih Renolds and Vogel s models of iscosiies Commnicaions in Non-Linear Sci. and Nmerical Simlaion 4(5) (9) 7-9. [9] O.D. Makinde Hermie-Pade approach o hermal radiaion fec on inheren irreersibili in a ariable iscosi channel flo Compers and Mahemaics ih Applicaions 58(9) -8. [] M. Massodi and I. Chrise Effecs of ariable iscosi and iscos dissipaion on he flo of hird grade flid in a pipe In. J. Non-Linear Mech. (5) (995) [] S. Nadeem. Haa N.S. Akbar and M.Y. Malik On he inflence of hea ransfer in perisalsis ih ariable iscosi In. J. Hea and Mass ransfer 5(9) [] L. Rndora Laminar flo in a channel filled ih saraed poros media Ph.D. hesis Deparmen of Mechanical Engineering Cape Peninsla Uniersi of echnolog (). [] H. asaar A. Shafig and A. Alsaedi Effec of jole heaing and hermal radiaion in flo of hird grade flid oer radiaie srface Nonlinear Analsis and Applied Mahemaics Research Grop Facl of Science Sadi Arabia 9() (4) - hp:/.plosone.org Accessed on March (4).

ME 321: FLUID MECHANICS-I

ME 321: FLUID MECHANICS-I 8/7/18 ME 31: FLUID MECHANICS-I Dr. A.B.M. Toiqe Hasan Proessor Dearmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET, Dhaka Lecre-13 8/7/18 Dierenial Analsis o Flid Moion

More information

INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING (ISSN: ), VOL. 5, NO. 2,

INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING (ISSN: ), VOL. 5, NO. 2, INTERNTIONL JOURNL OF MTHEMTICS ND SCIENTIFIC COMPUTING (ISSN: -5) VOL. 5 NO. 5 Unsead MHD Flow hrogh Poros Medim Pas an Implsivel Sared Inclined Oscillaing Plae wih Variable Temperare and Mass Diffsion

More information

TIME-SPACE DEPENDENT FRACTIONAL VISCOELASTIC MHD FLUID FLOW AND HEAT TRANSFER OVER ACCELERATING PLATE WITH SLIP BOUNDARY

TIME-SPACE DEPENDENT FRACTIONAL VISCOELASTIC MHD FLUID FLOW AND HEAT TRANSFER OVER ACCELERATING PLATE WITH SLIP BOUNDARY HERMAL SCIENCE: Year 7, Vol., No. A, pp. 7-7 IME-SPACE DEPENDEN FRACIONAL VISCOELASIC MHD FLUID FLOW AND HEA RANSFER OVER ACCELERAING PLAE WIH SLIP BOUNDARY b Shenging CHEN a, Liancn ZHENG a*, Chnri LI

More information

THERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM

THERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM elfh Inernaional Waer echnolog onference, IW1 008 Aleandria, Egp 1 HERMOPHORESIS PARILE DEPOSIION ON FLA SRFAES DE O FLID FLOW IN DAR-FORHHEIMER POROS MEDIM Rebhi A. Damseh 1 and Kamel Alzboon 1 Mechanical

More information

Heat transfer between two parallel porous plates for Couette flow under pressure gradient and Hall current

Heat transfer between two parallel porous plates for Couette flow under pressure gradient and Hall current Sādhanā Vol. 4, Par, Febrar 5, pp. 83 97. c Indian Academ of Sciences Hea ransfer beeen o parallel poros plaes for Coee flo nder pressre gradien and Hall crren HAZEM A ATTIA,WABBAS, MOSTAFA A M ABDEEN

More information

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen

More information

Atmospheric Dynamics 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35

Atmospheric Dynamics 11:670:324. Class Time: Tuesdays and Fridays 9:15-10:35 Amospheric Dnamics 11:67:324 Class ime: esdas and Fridas 9:15-1:35 Insrcors: Dr. Anhon J. Broccoli (ENR 229 broccoli@ensci.rgers.ed 848-932-5749 Dr. Benjamin Linner (ENR 25 linner@ensci.rgers.ed 848-932-5731

More information

MHD And Thermal Radiation Effects On Linearly Accelerated Isothermal Vertical Plate With Chemical Reaction Of First Order

MHD And Thermal Radiation Effects On Linearly Accelerated Isothermal Vertical Plate With Chemical Reaction Of First Order ISSN: 19-875 Inernaional Jornal of Innovaive Research in Science Engineering and echnology (An ISO 97: 7 erified Organizaion) Vol. Isse 1 December 1 MHD And hermal Radiaion Effecs On Linearly Acceleraed

More information

ME 425: Aerodynamics

ME 425: Aerodynamics ME 45: Aerodnamics Dr. A.B.M. Toiqe Hasan Proessor Deparmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET, Dhaka Lecre-7 Fndamenals so Aerodnamics oiqehasan.be.ac.bd oiqehasan@me.be.ac.bd

More information

ME 425: Aerodynamics

ME 425: Aerodynamics 3/4/18 ME 45: Aerodnamics Dr. A.B.M. Toiqe Hasan Proessor Deparmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET Dhaka Lecre-6 3/4/18 Fndamenals so Aerodnamics eacher.be.ac.bd/oiqehasan/

More information

Free Convective Flow of a Visco-Elastic Fluid Bounded By an Oscillating Porous Flat Plate in Slip Flow Regime

Free Convective Flow of a Visco-Elastic Fluid Bounded By an Oscillating Porous Flat Plate in Slip Flow Regime IOSR Jornal of ahemaics (IOSR-J) e-issn: 78-578 p-issn: 9-765X. olme Isse er. (ar - pr. 5) PP 9-5 www.iosrjornals.or Free onvecive Flow of a isco-elasic Flid Bonded B an Oscillain Poros Fla Plae in Slip

More information

CSE-4303/CSE-5365 Computer Graphics Fall 1996 Take home Test

CSE-4303/CSE-5365 Computer Graphics Fall 1996 Take home Test Comper Graphics roblem #1) A bi-cbic parameric srface is defined by Hermie geomery in he direcion of parameer. In he direcion, he geomery ecor is defined by a poin @0, a poin @0.5, a angen ecor @1 and

More information

CSE 5365 Computer Graphics. Take Home Test #1

CSE 5365 Computer Graphics. Take Home Test #1 CSE 5365 Comper Graphics Take Home Tes #1 Fall/1996 Tae-Hoon Kim roblem #1) A bi-cbic parameric srface is defined by Hermie geomery in he direcion of parameer. In he direcion, he geomery ecor is defined

More information

Unsteady laminar flow of visco-elastic fluid of second order type between two parallel plates

Unsteady laminar flow of visco-elastic fluid of second order type between two parallel plates Indian Jornal of Engineering & Maerials Sciences Vol., Febrary 5, pp. 5-57 Unseady laminar flow of visco-elasic flid of second order ype beween wo parallel plaes Ch V Ramana Mrhy & S B Klkarni Deparmen

More information

INTERMEDIATE FLUID MECHANICS

INTERMEDIATE FLUID MECHANICS INTERMEDIATE FLID MECHANICS Lecre 1: Inrodcion Benoi Cshman-Roisin Thaer School of Engineering Darmoh College Definiion of a Flid As opposed o a solid a flid is a sbsance ha canno resis a shear force iho

More information

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples In. J. Conemp. Mah. Sciences, Vol. 6, 011, no. 46, 83-90 A Direc Mehod for Solving Nonlinear PDEs and New Eac Solions for Some Eamples Ameina S. Nseir Jordan Universiy of Science and Technology Deparmen

More information

Learning from a Golf Ball

Learning from a Golf Ball Session 1566 Learning from a Golf Ball Alireza Mohammadzadeh Padnos School of Engineering Grand Valley Sae Uniersiy Oeriew Projecile moion of objecs, in he absence of air fricion, is sdied in dynamics

More information

Heat and Mass Transfer on the Unsteady MHD Flow of Chemically Reacting Micropolar Fluid with Radiation and Joule Heating

Heat and Mass Transfer on the Unsteady MHD Flow of Chemically Reacting Micropolar Fluid with Radiation and Joule Heating Inernaional Jornal of heoreical and Alied Mahemaics 7; (): - h://.scienceblishinggro.com//iam doi:.68/.iam.7. Hea and Mass ransfer on he nsead MHD Flo of hemicall Reacing Microolar Flid ih Radiaion and

More information

Computers and Mathematics with Applications

Computers and Mathematics with Applications Compers and Mahemaics wih Applicaions 59 (00) 80 809 Conens liss available a ScienceDirec Compers and Mahemaics wih Applicaions jornal homepage: www.elsevier.com/locae/camwa Solving fracional bondary vale

More information

Study on convection improvement of standard vacuum tube

Study on convection improvement of standard vacuum tube IOP Conference Series: Earh and Enironmenal Science PAPER OPEN ACCESS Sd on conecion improemen of sandard acm be To cie his aricle: J H He e al 017 IOP Conf. Ser.: Earh Eniron. Sci. 93 0100 View he aricle

More information

Numerical Solution and Exponential Decay to Von Kármán System with Frictional Damping

Numerical Solution and Exponential Decay to Von Kármán System with Frictional Damping Appl. Mah. Inf. Sci. 8, No. 4, 575-58 (4) 575 Applied Mahemaics & Informaion Sciences An Inernaional Jornal hp://d.doi.org/.785/amis/84 Nmerical Solion and Eponenial Deca o Von Kármán Ssem wih Fricional

More information

THE DARBOUX TRIHEDRONS OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE. Emin Özyilmaz

THE DARBOUX TRIHEDRONS OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE. Emin Özyilmaz Mahemaical and Compaional Applicaions, Vol. 9, o., pp. 7-8, 04 THE DARBOUX TRIHEDROS OF REULAR CURVES O A REULAR TIME-LIKE SURFACE Emin Özyilmaz Deparmen of Mahemaics, Facly of Science, Ee Uniersiy, TR-500

More information

Chapter 6 Momentum Transfer in an External Laminar Boundary Layer

Chapter 6 Momentum Transfer in an External Laminar Boundary Layer 6. Similarit Soltions Chapter 6 Momentm Transfer in an Eternal Laminar Bondar Laer Consider a laminar incompressible bondar laer with constant properties. Assme the flow is stead and two-dimensional aligned

More information

Unsteady MHD Second Grade Fluids Flow in a Porous Medium with Ramped Wall Temperature

Unsteady MHD Second Grade Fluids Flow in a Porous Medium with Ramped Wall Temperature Unsead MHD Second Grade Fluids Flow in a Porous Medium wih Ramped Wall Temperaure ZULKHIBRI ISMAIL Universii Malasia Pahang Facul of Indusrial Sciences & Technolog Lebuh Raa Tun Razak 6300 Kuanan Pahang

More information

Viscous Dissipation and Heat Absorption effect on Natural Convection Flow with Uniform Surface Temperature along a Vertical Wavy Surface

Viscous Dissipation and Heat Absorption effect on Natural Convection Flow with Uniform Surface Temperature along a Vertical Wavy Surface Aailable at htt://am.ed/aam Al. Al. Math. ISSN: 93-966 Alications and Alied Mathematics: An International Jornal (AAM) Secial Isse No. (Ma 6),. 8 8th International Mathematics Conference, March,, IUB Cams,

More information

CFD Modelling of Indoor Air Quality and Thermal Comfort

CFD Modelling of Indoor Air Quality and Thermal Comfort Proceedings of he nd IASME / WSEAS Inernaional Conference on Coninm Mechanics (CM'07), Pororo, Sloenia, Ma 5-7, 007 CFD Modelling of Indoor Air Qali and Thermal Comfor LÁSZLÓ KAJTÁR ANITA LEITNER Dearmen

More information

Numerical Modeling of the Effect of Fine Water Mist on the Small Scale Flame Spreading Over Solid Combustibles

Numerical Modeling of the Effect of Fine Water Mist on the Small Scale Flame Spreading Over Solid Combustibles Nmerical Modeling of he Effec of Fine Waer Mis on he Small Scale Flame Spreading Oer Solid Combsibles A.I. KARPOV 1, V. NOVOZHILOV, V.K. BULGAKOV 3, and A.A. GALAT 1 1 eparmen of Comper Science Komsomolsk-on-Amr

More information

Dynamic Response of Inclined Isotropic Elastic Damped Rectangular Mindlin Plate resting on Pasternak Foundation under a Moving Load

Dynamic Response of Inclined Isotropic Elastic Damped Rectangular Mindlin Plate resting on Pasternak Foundation under a Moving Load Proceedings of he Inernaional MliConference of Engineers and Comper Scieniss 016 Vol II, IMECS 016, March 16-18, 016, Hong Kong Dnamic Response of Inclined Isoropic Elasic Damped Recanglar Mindlin Plae

More information

U. S. Rajput and Gaurav Kumar

U. S. Rajput and Gaurav Kumar MATEMATIKA, 2018, Volume 34, Number 2, 433 443 c Penerbi UTM Press. All righs reserved Effec of Hall Curren on Unseady Magneo Hydrodynamic Flow Pas an Exponenially Acceleraed Inclined Plae wih Variable

More information

Scalar Conservation Laws

Scalar Conservation Laws MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )

More information

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method Available a hp://pva.ed/aa Appl. Appl. Mah. ISSN: 93-9466 Special Isse No. (Ags ) pp. 8 93 Applicaions Applied Maheaics: An Inernaional Jornal (AAM) Eac soliary-wave Special Solions for he Nonlinear Dispersive

More information

And the solution to the PDE problem must be of the form Π 1

And the solution to the PDE problem must be of the form Π 1 5. Self-Similar Soluions b Dimensional Analsis Consider he diffusion problem from las secion, wih poinwise release (Ref: Bluman & Cole, 2.3): c = D 2 c x + Q 0δ(x)δ() 2 c(x,0) = 0, c(±,) = 0 Iniial release

More information

PROJECTS WITH APPLICATIONS OF DIFFERENTIAL EQUATIONS AND MATLAB

PROJECTS WITH APPLICATIONS OF DIFFERENTIAL EQUATIONS AND MATLAB PROJECTS WITH APPLICATIONS OF DIFFERENTIAL EQUATIONS AND MATLAB David Szrley Francis Marion Universiy Deparmen of Mahemaics PO Box 1547 Florence, SC 95 dszrley@fmarion.ed I. INTRODUCTION Differenial eqaions

More information

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as Proceedings of he rd IMT-GT Regional Conference on Mahemaics Saisics and Applicaions Universii Sains Malaysia ANALYSIS ON () + () () = G( ( ) ()) Jessada Tanhanch School of Mahemaics Insie of Science Sranaree

More information

Predator-Prey Models with Diffusion and Time Delay

Predator-Prey Models with Diffusion and Time Delay Predaor-Prey Models wih Diffsion and Time Delay Irina Kozloa 1, Manmohan Singh 1 and Alan Eason 1,2 1 School of Mahemaical Sciences, Swinbrne Uniersiy of Technology, Hawhorn, Vicoria, Asralia. 2 Presen

More information

VISUALIZED DEVELOPMENT OF ONSET FLOW BETWEEN TWO ROTATING CYLINDERS

VISUALIZED DEVELOPMENT OF ONSET FLOW BETWEEN TWO ROTATING CYLINDERS ISFV14-14 h Inernaional Symposim on Flo Visalizaion Jne 1-4, 1, EXCO Daeg, Korea VISUALIZED DEVELOPMENT OF ONSET FLOW BETWEEN TWO ROTATING CYLINDERS Takashi Waanabe.*, Yorinob Toya**, Shohei Fjisaa* *Gradae

More information

UNSTEADY PARALLEL FLOW OF AN ELASTO-VISCO-HYPOPLASTIC FLUID BETWEEN TWO INFINITE PARALLEL PLATES

UNSTEADY PARALLEL FLOW OF AN ELASTO-VISCO-HYPOPLASTIC FLUID BETWEEN TWO INFINITE PARALLEL PLATES World Conference on Earhqake Engineering UNSEADY PARALLEL FLOW OF AN ELASO-VISCO-HYPOPLASIC FLUID BEWEEN WO INFINIE PARALLEL PLAES 1 C. Fang 1 and C.H. Lee Assisan Professor, Dep. of Civil Engineering,

More information

THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES

THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES Kragujevac J. Sci. 3 () 7-4. UDC 53.5:536. 4 THE EFFECT OF SUCTION AND INJECTION ON UNSTEADY COUETTE FLOW WITH VARIABLE PROPERTIES Hazem A. Aia Dep. of Mahemaics, College of Science,King Saud Universiy

More information

Riemann Function and Methods of Group Analysis

Riemann Function and Methods of Group Analysis American Research Jornal of Mahemaics Original Aricle ISSN 378-74X Volme Isse 3 5 Riemann Fncion and Mehods of Grop Analsis Akimov Andre Chernov Igor Abdllina Rfina 3 4533 Serliamak Rssia Lenina sree 47A

More information

Huazhong Tang 1 and Gerald Warnecke Introduction ANOTEON(2K + 1)-POINT CONSERVATIVE MONOTONE SCHEMES

Huazhong Tang 1 and Gerald Warnecke Introduction ANOTEON(2K + 1)-POINT CONSERVATIVE MONOTONE SCHEMES ESAIM: MAN Vol. 38, N o, 4, pp. 345 357 DOI:.5/man:46 ESAIM: Mahemaical Modelling and Nmerical Analysis ANOTEON(K + )-POINT CONSERVATIVE MONOTONE SCHEMES Hazhong Tang and Gerald Warnecke Absrac. Firs order

More information

Miscellanea Miscellanea

Miscellanea Miscellanea Miscellanea Miscellanea Miscellanea Miscellanea Miscellanea CENRAL EUROPEAN REVIEW OF ECONOMICS & FINANCE Vol., No. (4) pp. -6 bigniew Śleszński USING BORDERED MARICES FOR DURBIN WASON D SAISIC EVALUAION

More information

INSTABILITY REGIONS DUE TO INTERNAL DAMPING ON ROTORS IN WOUNDING-SHAFT

INSTABILITY REGIONS DUE TO INTERNAL DAMPING ON ROTORS IN WOUNDING-SHAFT NSTABTY RGONS DU TO NTRNA DAMPNG ON ROTORS N WOUNDNG-SHAFT José C. Pereira and Márcio. Silveira Deparameno de ngenharia Mecânica Universidade Federal de Sana Caarina Caixa Posal 476 - Camps Universiário

More information

International Journal "Information Theories & Applications" Vol.10

International Journal Information Theories & Applications Vol.10 44 Inernaional Jornal "Informaion eories & Applicaions" Vol. [7] R.A.Jonson (994 iller & Frend s Probabili and Saisics for Engineers5 ediion Prenice Hall New Jerse 763. [8] J.Carroll ( Hman - Comper Ineracion

More information

Study of MHD Oblique Stagnation Point Assisting Flow on Vertical Plate with Uniform Surface Heat Flux

Study of MHD Oblique Stagnation Point Assisting Flow on Vertical Plate with Uniform Surface Heat Flux World Academ of Science Engineering and echnolog International Jornal of Mechanical and Mechatronics Engineering Vol:5 No: 011 Std of MHD Obliqe Stagnation Point Assisting Flow on Vertical Plate with Uniform

More information

Method of Moment Area Equations

Method of Moment Area Equations Noe proided b JRR Page-1 Noe proided b JRR Page- Inrodcion ehod of omen rea qaions Perform deformaion analsis of flere-dominaed srcres eams Frames asic ssmpions (on.) No aial deformaion (aiall rigid members)

More information

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum.

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum. Inegraion of he equaion of moion wih respec o ime raher han displacemen leads o he equaions of impulse and momenum. These equaions greal faciliae he soluion of man problems in which he applied forces ac

More information

N. Sandeep 1 and V. Sugunamma 2

N. Sandeep 1 and V. Sugunamma 2 Journal of Applied Fluid Mechanics, Vol. 7, No., pp. 75-86, 4. Available online a www.jafmonline.ne, ISSN 735-357, EISSN 735-3645. Radiaion and Inclined Magneic Field Effecs on Unseady Hydromagneic Free

More information

3D Coordinate Systems. 3D Geometric Transformation Chapt. 5 in FVD, Chapt. 11 in Hearn & Baker. Right-handed coordinate system:

3D Coordinate Systems. 3D Geometric Transformation Chapt. 5 in FVD, Chapt. 11 in Hearn & Baker. Right-handed coordinate system: 3D Geomeric ransformaion Chap. 5 in FVD, Chap. in Hearn & Baker 3D Coordinae Ssems Righ-handed coordinae ssem: Lef-handed coordinae ssem: 2 Reminder: Vecor rodc U V UV VU sin ˆ V nu V U V U ˆ ˆ ˆ 3D oin

More information

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics

More information

Kinematics in two dimensions

Kinematics in two dimensions Lecure 5 Phsics I 9.18.13 Kinemaics in wo dimensions Course websie: hp://facul.uml.edu/andri_danlo/teaching/phsicsi Lecure Capure: hp://echo36.uml.edu/danlo13/phsics1fall.hml 95.141, Fall 13, Lecure 5

More information

Hall Effects on Rayleigh-Stokes Problem for Heated Second Grade Fluid

Hall Effects on Rayleigh-Stokes Problem for Heated Second Grade Fluid Proceedings of he Pakisan Academy of Sciences 49 (3):193 198 (1) Copyrigh Pakisan Academy of Sciences ISSN: 377-969 Pakisan Academy of Sciences Original Aricle Hall Effecs on Rayleigh-Sokes Problem for

More information

ELEMENTS OF ACOUSTIC WAVES IN POROUS MEDIA

ELEMENTS OF ACOUSTIC WAVES IN POROUS MEDIA ELEMENTS OF ACOSTIC WAVES IN POROS MEDIA By George F FREIHA niversiy of Balamand (Spervised y Dr Elie HNEIN) niversié de Valenciennes e d Haina Camrésis (Spervised y Dr Berrand NONGAILLARD & Dr George

More information

Chapter 12: Velocity, acceleration, and forces

Chapter 12: Velocity, acceleration, and forces To Feel a Force Chaper Spring, Chaper : A. Saes of moion For moion on or near he surface of he earh, i is naural o measure moion wih respec o objecs fixed o he earh. The 4 hr. roaion of he earh has a measurable

More information

THERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM

THERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM Telfh Inernaional Waer Technology Conference, IWTC1 008, Alexandria, Egyp 1069 THERMOPHORESIS PARTICLE DEPOSITION ON FLAT SURFACES DUE TO FLUID FLOW IN DARCY-FORCHHEIMER POROUS MEDIUM Rebhi A. Damseh 1

More information

Modelling Traffic Flow with Constant Speed using the Galerkin Finite Element Method

Modelling Traffic Flow with Constant Speed using the Galerkin Finite Element Method Proceedings of he World Congress on Engineering 29 Vol II WCE 29, Jly - 3, 29, London, U.K. Modelling Traffic Flow wih Consan Speed sing he Galerin Finie Elemen Mehod Wesley Celemans, Magd A. Wahab, Kr

More information

PH2130 Mathematical Methods Lab 3. z x

PH2130 Mathematical Methods Lab 3. z x PH130 Mahemaical Mehods Lab 3 This scrip shold keep yo bsy for he ne wo weeks. Yo shold aim o creae a idy and well-srcred Mahemaica Noebook. Do inclde plenifl annoaions o show ha yo know wha yo are doing,

More information

DESIGN OF TENSION MEMBERS

DESIGN OF TENSION MEMBERS CHAPTER Srcral Seel Design LRFD Mehod DESIGN OF TENSION MEMBERS Third Ediion A. J. Clark School of Engineering Deparmen of Civil and Environmenal Engineering Par II Srcral Seel Design and Analysis 4 FALL

More information

Elementary Differential Equations and Boundary Value Problems

Elementary Differential Equations and Boundary Value Problems Elemenar Differenial Equaions and Boundar Value Problems Boce. & DiPrima 9 h Ediion Chaper 1: Inroducion 1006003 คณ ตศาสตร ว ศวกรรม 3 สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา 1/2555 ผศ.ดร.อร ญญา ผศ.ดร.สมศ

More information

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation Inernaional Jornal of Basic & Applied Sciences IJBAS-IJENS Vol:9 No: A Comparison Among Homoopy Perrbaion Mehod And The Decomposiion Mehod Wih The Variaional Ieraion Mehod For Dispersive Eqaion Hasan BULUT*

More information

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions Proceedings of he World Congress on Engineering and Compuer Science 23 Vol I WCECS 23, 23-25 Ocober, 23, San Francisco, USA Homoopy Perurbaion Mehod for Solving Some Iniial Boundary Value Problems wih

More information

Solution of Integro-Differential Equations by Using ELzaki Transform

Solution of Integro-Differential Equations by Using ELzaki Transform Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform

More information

ATMS 310 The Vorticity Equation. The Vorticity Equation describes the factors that can alter the magnitude of the absolute vorticity with time.

ATMS 310 The Vorticity Equation. The Vorticity Equation describes the factors that can alter the magnitude of the absolute vorticity with time. ATMS 30 The Vorici Eqaion The Vorici Eqaion describes he acors ha can aler he magnide o he absole orici ih ime. Vorici Eqaion in Caresian Coordinaes The (,,,) orm is deried rom he rimiie horional eqaions

More information

Incompressible Viscoelastic Flow of a Generalised Oldroyed-B Fluid through Porous Medium between Two Infinite Parallel Plates in a Rotating System

Incompressible Viscoelastic Flow of a Generalised Oldroyed-B Fluid through Porous Medium between Two Infinite Parallel Plates in a Rotating System International Jornal of Compter Applications (97 8887) Volme 79 No., October Incompressible Viscoelastic Flow of a Generalised Oldroed-B Flid throgh Poros Medim between Two Infinite Parallel Plates in

More information

Conservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations

Conservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations Indian Jornal of Science and Technology Vol 8( 78 84 Janary 05 ISSN (Prin : 0974-84 ISSN (Online : 0974-545 DOI : 0.7485/ijs/05/8i/47809 Conseraion Laws and Hamilonian Symmeries of Whiham-Broer-Kap Eqaions

More information

Homotopy Perturbation Method for Solving Linear Boundary Value Problems

Homotopy Perturbation Method for Solving Linear Boundary Value Problems International Jornal of Crrent Engineering and Technolog E-ISSN 2277 4106, P-ISSN 2347 5161 2016 INPRESSCO, All Rights Reserved Available at http://inpressco.com/categor/ijcet Research Article Homotop

More information

Research on Eddy Air-Curtain Dust Controlled Flow Field in Hard Rock Mechanized Driving Face

Research on Eddy Air-Curtain Dust Controlled Flow Field in Hard Rock Mechanized Driving Face JOURNAL OF NETWORKS, VOL. 8, NO., FEBRUARY 013 453 Research on Edd Air-Crain Ds Conrolled Flo Field in Hard Roc Mechanied Driing Face Wei-min Cheng 1,, Wen Nie 1,, Gang Zho 1, 1,, Jn-lei Yang 1. College

More information

The Application of Optimal Homotopy Asymptotic Method for One-Dimensional Heat and Advection- Diffusion Equations

The Application of Optimal Homotopy Asymptotic Method for One-Dimensional Heat and Advection- Diffusion Equations Inf. Sci. Le., No., 57-61 13) 57 Informaion Sciences Leers An Inernaional Journal hp://d.doi.org/1.1785/isl/ The Applicaion of Opimal Homoopy Asympoic Mehod for One-Dimensional Hea and Advecion- Diffusion

More information

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation Hea (iffusion) Equaion erivaion of iffusion Equaion The fundamenal mass balance equaion is I P O L A ( 1 ) where: I inpus P producion O oupus L losses A accumulaion Assume ha no chemical is produced or

More information

A.G. VIJAYA KUMAR, 2. M. SUDHEER BABU, 3. S.V.K. VARMA

A.G. VIJAYA KUMAR, 2. M. SUDHEER BABU, 3. S.V.K. VARMA ..G. VIJY KUMR,. M. SUDHEER BBU, 3. S.V.K. VRM EFFECTS OF RDITION BSORPTION ND CHEMICL RECTION ON UNSTEDY MHD FREE CONVECTION FLOW PST N IMPULSIVELY STRTED INFINITE VERTICL PLTE THROUGH POROUS MEDIUM.

More information

On the numerical simulation of population dynamics with density-dependent migrations and the Allee effects

On the numerical simulation of population dynamics with density-dependent migrations and the Allee effects 7 Inernaional Symposim on Nonlinear Dynamics (7 ISND) IOP Pblishing Jornal of Physics: Conference Series 96 (8) 8 doi:88/74-6596/96//8 On he nmerical simlaion of poplaion dynamics wih densiy-dependen migraions

More information

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.7. PLANE LINEAR ELASTICITY. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.7. PLANE LINEAR ELASTICITY Coninuum Mechanics Course (MMC) - ETSECCPB - UPC Overview Plane Linear Elasici Theor Plane Sress Simplifing Hpohesis Srain Field Consiuive Equaion Displacemen Field The Linear

More information

Multiple-relaxation-time lattice Boltzmann modeling of. incompressible flows in porous media

Multiple-relaxation-time lattice Boltzmann modeling of. incompressible flows in porous media Muliple-relaaion-ime laice Bolzmann modeling of incompressible flows in porous media Qing Liu, Ya-Ling He* Ke Laboraor of Thermo-Fluid Science and Engineering of MOE, School of Energ and Power Engineering,

More information

The Research of Active Disturbance Rejection Control on Shunt Hybrid Active Power Filter

The Research of Active Disturbance Rejection Control on Shunt Hybrid Active Power Filter Available online a www.sciencedirec.com Procedia Engineering 29 (2) 456 46 2 Inernaional Workshop on Informaion and Elecronics Engineering (IWIEE) The Research of Acive Disrbance Rejecion Conrol on Shn

More information

An investigation of MHD Flows of Nanofluid over. an oscillating surface with Joule Heating

An investigation of MHD Flows of Nanofluid over. an oscillating surface with Joule Heating Jornal of Alied ahemaics & Bioiormaics, vol.7, no., 7, 7-48 ISSN: 79-66 (rin, 79-6939 (online Scienress Ld, 7 An invesigaion of HD Flows of Nanoflid over an oscillaing srface wih Jole Heaing B.. Namai,

More information

Transient Laminar MHD Free Convective Flow past a Vertical Cone with Non-Uniform Surface Heat Flux

Transient Laminar MHD Free Convective Flow past a Vertical Cone with Non-Uniform Surface Heat Flux Nonlinear Analysis: Modelling and Conrol, 29, Vol. 4, No. 4, 489 53 Transien Laminar MHD Free Convecive Flow pas a Verical Cone wih Non-Uniform Surface Hea Flux Bapuji Pullepu, A. J. Chamkha 2 Deparmen

More information

CHAPTER 6: FIRST-ORDER CIRCUITS

CHAPTER 6: FIRST-ORDER CIRCUITS EEE5: CI CUI T THEOY CHAPTE 6: FIST-ODE CICUITS 6. Inroducion This chaper considers L and C circuis. Applying he Kirshoff s law o C and L circuis produces differenial equaions. The differenial equaions

More information

Kinematics in two Dimensions

Kinematics in two Dimensions Lecure 5 Chaper 4 Phsics I Kinemaics in wo Dimensions Course websie: hp://facul.uml.edu/andri_danlo/teachin/phsicsi PHYS.141 Lecure 5 Danlo Deparmen of Phsics and Applied Phsics Toda we are oin o discuss:

More information

SIMULATION OF MODEL PREDICTIVE CONTROL OF SEMI-BATCH REACTOR. David Samek*, Lubomir Macku**

SIMULATION OF MODEL PREDICTIVE CONTROL OF SEMI-BATCH REACTOR. David Samek*, Lubomir Macku** SIMULATIO OF MODEL PREDICTIVE COTROL OF SEMI-BATCH REACTOR David Samek*, Lbomir Mack** *Tomas Baa Universi in Zlin, Facl of Technolog, Deparmen of Prodcion Engineering **Tomas Baa Universi in Zlin, Facl

More information

Experimental Study and Three-Dimensional Numerical Flow Simulation in a Centrifugal Pump when Handling Viscous Fluids

Experimental Study and Three-Dimensional Numerical Flow Simulation in a Centrifugal Pump when Handling Viscous Fluids IUST Inernaional Jornal o Engineering Science, Vol. 17, No.3-, 6, Page 53-6 Experimenal Sdy and Three-Dimensional Nmerical Flo Simlaion in a Cenrigal Pmp hen andling Viscos Flids Donloaded rom ijiepr.is.ac.ir

More information

Math 2214 Solution Test 1 B Spring 2016

Math 2214 Solution Test 1 B Spring 2016 Mah 14 Soluion Te 1 B Spring 016 Problem 1: Ue eparaion of ariable o ole he Iniial alue DE Soluion (14p) e =, (0) = 0 d = e e d e d = o = ln e d uing u-du b leing u = e 1 e = + where C = for he iniial

More information

Asymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice

Asymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice Asympoic Solion of he Ani-Plane Problem for a Two-Dimensional Laice N.I. Aleksandrova N.A. Chinakal Insie of Mining, Siberian Branch, Rssian Academy of Sciences, Krasnyi pr. 91, Novosibirsk, 6391 Rssia,

More information

SIMULATION OF TURBULENT FLOW AND HEAT TRANSFER OVER A BACKWARD-FACING STEP WITH RIBS TURBULATORS

SIMULATION OF TURBULENT FLOW AND HEAT TRANSFER OVER A BACKWARD-FACING STEP WITH RIBS TURBULATORS THERMAL SCIENCE, Year 011, Vol. 15, No. 1, pp. 45-55 45 SIMULATION OF TURBULENT FLOW AND HEAT TRANSFER OVER A BACKWARD-FACING STEP WITH RIBS TURBULATORS b Khdheer S. MUSHATET Mechanical Engineering Department,

More information

Modelisation and Simulation of Heat and Mass Transfers during Solar Drying of Sewage Sludge with Introduction of Real Climatic Conditions

Modelisation and Simulation of Heat and Mass Transfers during Solar Drying of Sewage Sludge with Introduction of Real Climatic Conditions Jornal o Alied Flid Mechanics, Vol., No.,. 65-659, 7. Aailable online a www.jamonline.ne, ISSN 735-357, EISSN 735-3645. DOI:.8869/acadb.jam.73.39.6854 Modelisaion and Simlaion o Hea and Mass ransers dring

More information

A numerical solution of the NS equations based on the mean value theorem with applications to aerothermodynamics

A numerical solution of the NS equations based on the mean value theorem with applications to aerothermodynamics Adanced Compaional Mehod in Hea ranfer IX 97 A nmerical olion of he NS eqaion baed on he mean ale heorem wih applicaion o aerohermodnamic F. Fergon & G. Elamin Deparmen of Mechanical Engineering, Norh

More information

HYPOTHESIS TESTING. four steps. 1. State the hypothesis. 2. Set the criterion for rejecting. 3. Compute the test statistics. 4. Interpret the results.

HYPOTHESIS TESTING. four steps. 1. State the hypothesis. 2. Set the criterion for rejecting. 3. Compute the test statistics. 4. Interpret the results. Inrodcion o Saisics in Psychology PSY Professor Greg Francis Lecre 23 Hypohesis esing for correlaions Is here a correlaion beween homework and exam grades? for seps. Sae he hypohesis. 2. Se he crierion

More information

Numerical investigation of natural convection of air in vertical divergent channels

Numerical investigation of natural convection of air in vertical divergent channels Adanced Comptational Methods in Heat ransfer X 13 Nmerical inestigation of natral conection of air in ertical diergent channels O. Manca, S. Nardini, D. Ricci & S. ambrrino Dipartimento di Ingegneria Aerospaziale

More information

International Journal of Innovative Research in Science, Engineering and Technology. (An ISO 3297: 2007 Certified Organization)

International Journal of Innovative Research in Science, Engineering and Technology. (An ISO 3297: 2007 Certified Organization) ISSN(Online): 39-8753 ISSN (Prin): 347-67 Inernaional Journal of Innovaive Research in Science, (An ISO 397: 7 Cerified Organizaion) Vol. 6, Issue 9, Sepember 7 Effecs of Non-ineger Order Time Fracional

More information

Numerical Simulation of Reaction-Diffusion Systems of Turing Pattern Formation

Numerical Simulation of Reaction-Diffusion Systems of Turing Pattern Formation Inernaional Jornal of Modern Nonlinear Theory and Applicaion 15 4 15-5 Pblished Online Deceber 15 in SciRes. hp://www.scirp.org/ornal/ina hp://dx.doi.org/1.436/ina.15.416 Nerical Silaion of Reacion-Diffsion

More information

CORRELATION EQUATIONS: FORCED AND FREE CONVECTION

CORRELATION EQUATIONS: FORCED AND FREE CONVECTION CHAPER 0 0. Inroducion CORREAION EQUAIONS: FORCED AND FREE CONECION A ey facor in convecion is e ea e ea ransfer coefficien. Insead of deermining we deermine e ssel number, wic a dimensionless ea ransfer

More information

Magnetohydrodynamic Flow and Heat Transfer of Two Immiscible Fluids through a Horizontal Channel

Magnetohydrodynamic Flow and Heat Transfer of Two Immiscible Fluids through a Horizontal Channel Research Article Internional Jornal of Crrent Engineering Technolog ISSN 77-46 3 INPRESSCO. All Rights Reserved. Available http://inpressco.com/cegor/ijcet Magnetohdrodnamic Flow He Transfer of Two Immiscible

More information

The Effects of Radiation on Free Convection Flow with Ramped Wall Temperature in Brinkman Type Fluid

The Effects of Radiation on Free Convection Flow with Ramped Wall Temperature in Brinkman Type Fluid Jurnal Teknologi Full paper The Effecs of Radiaion on Free Convecion Flow wih Ramped Wall Temperaure in Brinkman Tpe Fluid Muhamad Najib Zakaria a Abid Hussanan a Ilas Khan a Sharidan Shafie a* a Deparmen

More information

The role of the error function in three-dimensional singularly perturbed convection-diffusion problems with discontinuous data

The role of the error function in three-dimensional singularly perturbed convection-diffusion problems with discontinuous data The role of he error funcion in hree-dimensional singularl perurbed convecion-diffusion problems wih disconinuous daa José Luis López García, Eser Pérez Sinusía Depo. de Maemáica e Informáica, U. Pública

More information

ME 3560 Fluid Mechanics

ME 3560 Fluid Mechanics ME3560 Flid Mechanics Fall 08 ME 3560 Flid Mechanics Analsis of Flid Flo Analsis of Flid Flo ME3560 Flid Mechanics Fall 08 6. Flid Elemen Kinemaics In geneal a flid paicle can ndego anslaion, linea defomaion

More information

THE FOURIER-YANG INTEGRAL TRANSFORM FOR SOLVING THE 1-D HEAT DIFFUSION EQUATION. Jian-Guo ZHANG a,b *

THE FOURIER-YANG INTEGRAL TRANSFORM FOR SOLVING THE 1-D HEAT DIFFUSION EQUATION. Jian-Guo ZHANG a,b * Zhang, J.-G., e al.: The Fourier-Yang Inegral Transform for Solving he -D... THERMAL SCIENCE: Year 07, Vol., Suppl., pp. S63-S69 S63 THE FOURIER-YANG INTEGRAL TRANSFORM FOR SOLVING THE -D HEAT DIFFUSION

More information

The Numerical Simulation of Enhanced Heat Transfer Tubes

The Numerical Simulation of Enhanced Heat Transfer Tubes Aailable online at.sciencedirect.com Phsics Procedia 4 (01 70 79 01 International Conference on Applied Phsics and Indstrial Engineering The Nmerical Simlation of Enhanced Heat Transfer Tbes Li Xiaoan,

More information

Srednicki Chapter 20

Srednicki Chapter 20 Srednicki Chaper QFT Problems & Solions. George Ocober 4, Srednicki.. Verify eqaion.7. Using eqaion.7,., and he fac ha m = in his limi, or ask is o evalae his inegral:! x x x dx dx dx x sx + x + x + x

More information

Detecting Movement SINA 07/08

Detecting Movement SINA 07/08 Deecing Moemen How do we perceie moemen? This is no a simple qesion becase we are neer saionar obserers (ees and head moe An imporan isse is how we discriminae he moion of he eernal world from he moion

More information

ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt

ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt a 1/α s)ds < Indian J. pre appl. Mah., 396): 491-507, December 2008 c Prined in India. ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS SAID R. GRACE 1, RAVI P. AGARWAL 2 AND MUSTAFA

More information

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations Applied Mahemaics Leers 5 (0) 058 065 Conens liss available a SciVerse ScienceDirec Applied Mahemaics Leers jornal homepage: www.elsevier.com/locae/aml Oscillaion resls for forh-order nonlinear dynamic

More information

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z.

Mat 267 Engineering Calculus III Updated on 04/30/ x 4y 4z 8x 16y / 4 0. x y z x y. 4x 4y 4z 24x 16y 8z. Ma 67 Engineering Calcls III Updaed on 04/0/0 r. Firoz Tes solion:. a) Find he cener and radis of he sphere 4 4 4z 8 6 0 z ( ) ( ) z / 4 The cener is a (, -, 0), and radis b) Find he cener and radis of

More information