Simulation Study on Characteristics of the Vortex Structure in Human Mouth-throat Model in Cyclic Respiratory Pattern

Size: px
Start display at page:

Download "Simulation Study on Characteristics of the Vortex Structure in Human Mouth-throat Model in Cyclic Respiratory Pattern"

Transcription

1 Avalable onlne at Energy Proceda 17 (2012 ) Internatonal Conference on Future Electrcal Power and Energy Systems Smulaton Study on Characterstcs of the Vortex Structure n Human Mouth-throat Model n Cyclc Respratory Pattern SUN Dong,XU Xn-X*,ZHAO Xu-Guo,Tan Shu-Ln,L Fu-Sheng Insttute of Medcal Equpment, Academy of Mltary Medcne Scences; Natonal Bologcal Protecton Engneerng Center, Tann Abstract The research on vortex structure and vortex evoluton n human upper respratory tract can deepen understandng of the characterstcs of the arflow n human upper respratory tract and plays a very mportant role n analyzng the dffuson, transton and deposton patterns of aerosol n human upper respratory tract. Large eddy smulaton was used to smulate the vortex structure and vortex movement n human mouth-throat model n cyclc respratory pattern, and the vortex structure and vortex evoluton n mouth-throat model was dscussed. The results show that et formatons n pharynx and laryngeal lead to two vortcty growth regons at cyclc nhalaton flow, flat vortex appeared n the throat, a curved vortex lke the trachea wall appeared n the anteror wall of trachea, and nearly symmetrc reverse vortex pars appeared n the trachea; a vortex lke 3 appeared n the posteror wall of the throat, two curved vortexes lke eyebrow appeared n the posteror wall of the pharynx Publshed by by Elsever Ltd. Ltd. Selecton and/or and/or peer-revew under under responsblty of Hanan of [name Unversty. organzer] Open access under CC BY-NC-ND lcense. Key wordscyclc respratory patternmouth-throat model vortex structure vortex evolutonlarge eddy smulaton 1.Introducton The arflow n human mouth-throat leads to the generaton of varous scales vortexes and the cyclc varaton of pressure and sharng stress, whch wll affect the dffuson and deposton of aerosol. Wth the effects of respratory mode and geometrcal characterstcs of respratory tract, a transton from lamnar flow to turbulence occurs n respratory tract. In ths transton, complex arflow movements appears, such as the vortex structure [1], the flow separaton [2] and the second flow [3], whch wll result n the dfferent dstrbuton of pressure [4] and sharng stress. In fact, ths process of transton also occurs n the dffuson of aerosol, whch essentally presented as the affectons of the vortex structures and the cyclc varaton of pressure and sharng stress on the dffuson of aerosol. Recent years, prelmnary studes on vortex flow have been conducted by many scholars, the whole moton state of vortex flow [256] has been analyzed, and that the structure of Publshed by Elsever Ltd. Selecton and/or peer-revew under responsblty of Hanan Unversty. Open access under CC BY-NC-ND lcense. do: /.egypro

2 SUN Dong et al. / Energy Proceda 17 ( 2012 ) human upper respratory tract and the respratory flow cause vortex flow has been proved [7]. However, there are few systematc studes on vortex structure and vortex evoluton n human upper respratory tract, whch has restrcted the understandng of arflow movement characterstc n human upper respratory tract. In ths paper, large eddy smulaton was used to smulate precse flow feld n human mouth-throat model n the condtons of the low ntensve cyclc respratory patterns. The process of vortex evoluton n human mouth-throat model was studed and the characterstcs of vortex structure n mouth-throat model at dfferent tme were dscussed. 2.Geometrcal model and mathematcal model 2.1. Geometrcal model As shown n Fg.1, an dealzed mouth-throat model geometry that s developed at Aerosol Research Laboratory of Alberta (ARLA) conssts of oral cavty, pharynx, larynx and trachea. The szes of the model are smlar to those gven by Aerosol Research Laboratory of Alberta (ARLA) [8] and Stapleton K.W [9]. 2.2.Governng equatons of the gas phase Fg. 1 Human mouth-throat model The large eddy smulaton used n the paper s a transton between drect numercal smulatons and theoretcal model smulatons. It has a great potental n engneerng applcaton and fundamental research, and s a present research focus on flud numercal smulaton. The governng equatons [10] of large eddy smulaton s obtaned from the N-S flterng equatons, and t s tensor expresson can be descrbed as: u 0 x u uu 1 p 2 u t x x x Where,, 1,2, 3, and,, u and p are flow densty, knetc molecular vscosty, large scale part of flow velocty and pressure, respectvely. And the Sub-grd scale stress : uu uu. Large eddy smulaton wth Smagornsky sub-grd scale model was used n the present work, and sub-grd scale stress can be descrbed as the followng:

3 1788 SUN Dong et al. / Energy Proceda 17 ( 2012 ) T S kk 3 Where s Kronecker symbol, and stran rate tensor S can be defned as: S u x Sub-grd eddy vscosty T can be descrbed as: ( ) Where u x 2 T C s S 2S S, and the Smagornsky constant C s =0.1 was adopted n ths paper. S 2.3.Numercal smulaton In the smulaton for flow feld n human mouth-throat model under the condtons of the low ntensve cyclc respratory patterns, the respratory flow changes accordng to the sne wave functon, as s shown n the Fg.2. The breathng ntensty Q=30L/mn, the respratory frequency s 15 cycle/mn. The assocated boundary condtons nclude unform velocty prescrbed at the mouth nlet and zero pressure at the outlets. Meanwhle, the arway condut s assumed to be smooth and rgd. The effects of arway condut flexblty were not consdered, and the no-slp boundary condton was adopted n the present analyss. 8 tme ponts (T 1 ~T 8 ) n a cycle were analyzed as the smulaton result, where T 1 =0.2 st 2 =0.5sT 3 =1s T 4 =1.5sT 5 =2.2sT 6 =2.5sT 7 =3sT 8 =3.5s, as s shown n the Fg Model valdaton Fg. 2 the change of respratory flow n cyclc respratory patterns The experment research was performed wth the Partcle mage velocmetry (PIV) technque and nspraton flows were examned under steady flow condtons wth the breathng ntensty Q=30L/mn. Comparson of averaged velocty magntude s performed between PIV measurement and large eddy smulaton result to verfy the accuracy of the numercal smulaton results. As the Fg.3 shows, the comparson of averaged velocty magntude between the expermental results [11] of the larynx and the numercal results has been dsplayed. The results show that the numercal smulaton data are n reasonable agreement wth expermental measurements, whch verfes that the large eddy smulaton methods are accurate and reasonable.

4 SUN Dong et al. / Energy Proceda 17 ( 2012 ) B A Fg.3 Comparson of arflow patterns between expermental results (A) and large eddy smulaton results (B) of the larynx 3.Results and dscusson 3.1.Evoluton of vortex structure n mouth -throat model n cyclc respratory pattern The vortcty dstrbuton contours n symmetrcal vertcal plane of human mouth-throat model and the so-surface of vortcy at dfferent tme were dsplayed respectvely n Fg.4 and Fg.5, and the evoluton process of vortex structure n human mouth-throat model n cyclc respratory pattern was revealed. In nspratory acceleraton phase, the arflow entered nto oral cavty through mouth, then arrved pharynx. Due to the sectonal area of pharynx decreased rapdly, the frst et generated n pharynx and two vortcty growth regons formed on the anteror and posteror wall of pharynx. When the arflow arrved larynx, the second et generated n larynx owng to the lmtaton of the secton of glotts, and a vortcty growth regon formed n the glotts. Wth the passage of tme, the vortcty of pharynx and glotts ncreased rapdly, the vortex structure moved to downstream of the arflow, and the core of vortex n the trachea was gradually nearng the anteror wall of trachea. At t=1s, the vortcty dstrbuton n human mouth-throat model present a knd of fully developed stuaton, and the vortcty n every part reached ts maxmum. As s shown n Fg.5, n nspratory acceleraton phase, the vortcty developed from pharynx and larynx, and a curved vortex lke the trachea wall appeared n the model. From the pcture at 1.5s, t can be drown that the vortcty decreased gradually n nspraton deceleraton phase, and the dstrbuton of vortcy at the fnshed tme approached to that at the ntal tme. a b c d e f Fg.4 The vortcty dstrbuton contours n symmetrcal vertcal plane of human mouth-throat model at dfferent tmeat=0.2s bt=1sct=1.5sdt=2.2set=3sft=3.5s

5 1790 SUN Dong et al. / Energy Proceda 17 ( 2012 ) Characterstcs of vortex structure n mouth-throat model at T=1s In Fg.6, the vortcty dstrbuton n dfferent cross sectons of the human mouth-throat model at t=1s were dsplayed. From the cross-sectons of A-A, t can be seen that as the arflow entered nto pharynx, the vortcty n boundary layer ncreased and a stuaton of hgher external and lower nternal vortcty was formed. As the arflow arrved cross-sectons of B-B, a et generated n pharynx and the vortex flow separated. Meanwhle, a flat vortex wth hgher central vortcty appeared n the throat. When the arflow got to glotts, a complex vortex structure of hgher vortcty on posteror wall and lower vortcty n the center generated owng to the lmtaton of the secton of glotts, as s shown n the cross-secton C-C. Due to the drecton of et fow s to the anteror wall of trachea, a phenomenon that vortcty extended to the anteror wall of trachea formed, and a curved vortex lke the trachea wall appeared n the anteror wall of trachea, as s shown n the cross-secton E-E. At the same tme, nearly symmetrc reverse vortex pars appeared n the trachea, whch was smlar to the kdney vortex and reverse kdney vortex appeared n the et flow of transverse vortex flow, as s shown n the cross-secton E-E and F-F. a b c d e f Fg.5 The so-surface of vortcy n human mouth-throat model at dfferent tmeat=0.2sbt=1sct=1.5sdt=2.2s et=3sft=3.5s 3.3.Characterstcs of vortex structure n mouth-throat model at T=3s In Fg.7, the vortcty dstrbuton n dfferent cross sectons of the human mouth-throat model at t=3s were dsplayed. From the cross-sectons of E-E and F-F, t can be seen that as the arflow entered nto trachea, the vortcty n boundary layer ncreased and a stuaton of hgher external and lower nternal vortcty was formed. As the arflow arrved cross-sectons of D-D, a et generated n glotts and two vortcty growth regons formed on the anteror and posteror wall of larynx. Due to the drecton of et fow s to the posteror wall of larynx, the vortcty extended to the posteror wall of larynx. A complex vortex structure of hgher vortcty on posteror wall and lower vortcty on anteror wall generated, and a vortex lke 3 appeared n the posteror wall of the throat, as s shown n cross-sectons of C-C. When the arflow reached pharynx, the second et generated n pharynx and two vortcty growth regons formed on the anteror and posteror wall of pharynx. Then, two curved vortexes lke eyebrow appeared n the posteror wall of the pharynx, as s shown n cross-sectons of B-B. After the flow reached mouth, the vortcty dspersed and varous scales of vortexes generated, as s shown n cross-sectons of A-A.

6 SUN Dong et al. / Energy Proceda 17 ( 2012 ) A-A Fg. 6 Vortcty dstrbuton n dfferent cross sectons of the human mouth-throat model at t=1s A-A Fg. 7 Vortcty dstrbuton n dfferent cross sectons of the human mouth-throat model at t=3s 4.Conclusons Large eddy smulaton was used to smulate the vortex structure and vortex movement n human mouth-throat model n the condtons of the low ntensve cyclc respratory patterns wth the breathng ntensty Q=30 L/mn and the vortex structure and vortex evoluton n mouth-throat model were dscussed. The followng concluson can be drawn: In nspratory acceleraton phase, two et formatons n pharynx and laryngeal lead to two vortcty growth regons at cyclc nhalaton flow. Wth the passage of tme, the vortcty of pharynx and glotts ncreased rapdly, the vortex structure moved to downstream of the arflow, and the core of vortex n the trachea was gradually nearng the anteror wall of trachea. In nspraton deceleraton phase, the vortcty decreased gradually and the dstrbuton of vortcy at the fnshed tme approached to that at the ntal tme. In expratory acceleraton phase, two et formatons n pharynx and glotts lead to two vortcty growth regons. Wth the passage of tme, the vortex structure moved to downstream of the arflow, the maxmum appeared on the posteror wall of pharynx. In expraton deceleraton phase, the vortcty decreased gradually and the dstrbuton of vortcy at the fnshed tme approached to that at the ntal tme. At t=1s, the vortcty dstrbuton n human mouth-throat model present a knd of fully developed stuaton. A flat vortex appeared n the pharynx, and a curved vortex lke the trachea

7 1792 SUN Dong et al. / Energy Proceda 17 ( 2012 ) wall appeared n the anteror wall of trachea. A nearly symmetrc reverse vortex pars appeared n the trachea, whch was smlar to the kdney vortex and reverse kdney vortex appeared n the et flow of transverse vortex flow. At t=1s, the vortcty dstrbuton n human mouth-throat model present a knd of fully developed stuaton. A vortex lke 3 appeared n the posteror wall of the throat, two curved vortexes lke eyebrow appeared n the posteror wall of the pharynx. After the flow reached mouth, the vortcty dspersed and varous scales of vortexes generated. References [1] Martn ANagelsJohn ECaterLarge eddy smulaton of hgh frequency oscllatng flow n an asymmetrc branchng arway model[j]medcal Engneerng & Physcs200931(9): [2] Klenstreuer C, Zhang ZArflow and partcle transport n the human respratory system[j]annual Revew of Flud Mechancs, 2010, [3] Luo HYLu YModelng the bfurcatng flow n a CT-scanned human lung arway[j]journal of Bomechancs2008, 41(12) [4] Goutham M, Shanmugam M, Mha M, et alvaldaton of computatonal flud dynamcs methodology used for human upper arway flow smulatons[j]journal of Bomechancs, 2009, (42) [5] Xu Xnx,, Lu YaunSmulaton study on characterstcs of the transent arflow movement n human arway at cyclc nhalaton flow[j]chnese Journal of Bomedcal Engneerng [6] Nazrdoust KAsgharan BUnsteady-state arflow and partcle deposton n a three-generaton human lung geometry y[j]inhalaton Toxcology200820(6) [7] Wolfgang AWallTmon RFlud-structure nteracton n lower arways of CT-based lung geometres[j]internatonal Journal for Numercal Methods n Fluds,2008,57(5) [8] Grgc BFnlay WHHeenan AFRegonal aerosol deposton and flow measurements n an dealzed mouth and throat[j]aerosol Scence [9] Stapleton KWGuentsch EHosknson MKet alon the sutablty of k-turbulence modelng for aerosol deposton n the mouth and throat: a comparson wth experment[j]aerosol Scence200031(6) [10] Zhang ZhaoshunCu GuxangXu ChunxaoTheory and Applcaton for Large Eddy Smulaton of turbulent flow [M]BengTsnghua Unversty [11] Zhao XuguoXu XnxTan Shuln et alpiv experment of steady flow wthn the human upper respratory tract [J] Journal of Experments n Flud Mechancs,

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate

(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 information

A Hybrid Variational Iteration Method for Blasius Equation

A Hybrid Variational Iteration Method for Blasius Equation Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method

More information

A Numerical Study of Heat Transfer and Fluid Flow past Single Tube

A 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 information

A large scale tsunami run-up simulation and numerical evaluation of fluid force during tsunami by using a particle method

A large scale tsunami run-up simulation and numerical evaluation of fluid force during tsunami by using a particle method A large scale tsunam run-up smulaton and numercal evaluaton of flud force durng tsunam by usng a partcle method *Mtsuteru Asa 1), Shoch Tanabe 2) and Masaharu Isshk 3) 1), 2) Department of Cvl Engneerng,

More information

Numerical analysis on the agglomeration behavior of fine particles in plane jet

Numerical analysis on the agglomeration behavior of fine particles in plane jet Numercal analyss on the agglomeraton behavor of fne partcles n plane et Mn Guo 1, a, Ja L 2, Xn Su 1 and Gurong Yang 1 1 Tann Academy of Envronmental Scences, Tann, 300191, Chna; 2 The Fourth Research

More information

Numerical Simulation of Lid-Driven Cavity Flow Using the Lattice Boltzmann Method

Numerical Simulation of Lid-Driven Cavity Flow Using the Lattice Boltzmann Method Proceedngs of the 3th WSEAS Internatonal Conference on APPLIED MATHEMATICS (MATH'8) Numercal Smulaton of Ld-Drven Cavty Flow Usng the Lattce Boltzmann Method M.A. MUSSA, S. ABDULLAH *, C.S. NOR AZWADI

More information

Investigation of a New Monte Carlo Method for the Transitional Gas Flow

Investigation of a New Monte Carlo Method for the Transitional Gas Flow Investgaton of a New Monte Carlo Method for the Transtonal Gas Flow X. Luo and Chr. Day Karlsruhe Insttute of Technology(KIT) Insttute for Techncal Physcs 7602 Karlsruhe Germany Abstract. The Drect Smulaton

More information

Turbulent Flow. Turbulent Flow

Turbulent 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 information

FEATURES OF TURBULENT TRANSPORT OF MOMENTUM AND HEAT IN STABLY STRATIFIED BOUNDARY LAYERS AND THEIR REPRODUCTION IN ATMOSPHERIC MESOSCALE MODELS

FEATURES OF TURBULENT TRANSPORT OF MOMENTUM AND HEAT IN STABLY STRATIFIED BOUNDARY LAYERS AND THEIR REPRODUCTION IN ATMOSPHERIC MESOSCALE MODELS C I T E S 009_ Krasnoyarsk 009 FEATURES OF TURBULENT TRANSPORT OF MOMENTUM AND HEAT IN STABLY STRATIFIED BOUNDARY LAYERS AND THEIR REPRODUCTION IN ATMOSPHERIC MESOSCALE MODELS A. F. Kurbatsky Insttute

More information

Numerical Heat and Mass Transfer

Numerical 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 information

IC Engine Flow Simulation using KIVA code and A Modified Reynolds Stress Turbulence Model

IC Engine Flow Simulation using KIVA code and A Modified Reynolds Stress Turbulence Model IC Engne Flow Smulaton usng KIVA code and A Modfed Reynolds Stress Turbulence Model Satpreet Nanda and S.L. Yang Mechancal Engneerng-Engneerng Mechancs Department Mchgan Technologcal Unversty Houghton,

More information

FORCED CONVECTION HEAT TRANSFER FROM A RECTANGULAR CYLINDER: EFFECT OF ASPECT RATIO

FORCED CONVECTION HEAT TRANSFER FROM A RECTANGULAR CYLINDER: EFFECT OF ASPECT RATIO ISTP-,, PRAGUE TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA FORCED CONVECTION HEAT TRANSFER FROM A RECTANGULAR CYLINDER: EFFECT OF ASPECT RATIO Mohammad Rahnama*, Seyed-Mad Hasheman*, Mousa Farhad**

More information

A New Evolutionary Computation Based Approach for Learning Bayesian Network

A New Evolutionary Computation Based Approach for Learning Bayesian Network Avalable onlne at www.scencedrect.com Proceda Engneerng 15 (2011) 4026 4030 Advanced n Control Engneerng and Informaton Scence A New Evolutonary Computaton Based Approach for Learnng Bayesan Network Yungang

More information

PERMEABILITY-POROSITY RELATIONSHIP ASSESSMENT BY 2-D NUMERICAL SIMULATIONS

PERMEABILITY-POROSITY RELATIONSHIP ASSESSMENT BY 2-D NUMERICAL SIMULATIONS ISTP-16, 005, PRAGUE 16 TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA PERMEABILITY-POROSITY RELATIONSHIP ASSESSMENT BY -D NUMERICAL SIMULATIONS J. Pnela*, S. Kruz*, A. F. Mguel* +, A. H. Res*, M. Aydn**

More information

STUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS

STUDY 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 information

Tensor Smooth Length for SPH Modelling of High Speed Impact

Tensor Smooth Length for SPH Modelling of High Speed Impact Tensor Smooth Length for SPH Modellng of Hgh Speed Impact Roman Cherepanov and Alexander Gerasmov Insttute of Appled mathematcs and mechancs, Tomsk State Unversty 634050, Lenna av. 36, Tomsk, Russa RCherepanov82@gmal.com,Ger@npmm.tsu.ru

More information

CFD VALIDATION OF STRATIFIED TWO-PHASE FLOWS IN A HORIZONTAL CHANNEL

CFD VALIDATION OF STRATIFIED TWO-PHASE FLOWS IN A HORIZONTAL CHANNEL CFD VALIDATION OF STRATIFIED TWO-PHASE FLOWS IN A HORIZONTAL CHANNEL 1. Introducton Chrstophe Vallée and Thomas Höhne In dfferent scenaros of small break Loss of Coolant Accdent (SB-LOCA), stratfed twophase

More information

High resolution entropy stable scheme for shallow water equations

High resolution entropy stable scheme for shallow water equations Internatonal Symposum on Computers & Informatcs (ISCI 05) Hgh resoluton entropy stable scheme for shallow water equatons Xaohan Cheng,a, Yufeng Ne,b, Department of Appled Mathematcs, Northwestern Polytechncal

More information

Application of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems

Application 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 information

Numerical Analysis of Heat Transfer and Pressure Drop in a Channel Equipped with Triangular Bodies in Side-By-Side Arrangement

Numerical Analysis of Heat Transfer and Pressure Drop in a Channel Equipped with Triangular Bodies in Side-By-Side Arrangement mercal Analyss of Heat Transfer and Pressure Drop n a Channel Equpped wth Trangular Bodes n Sde-By-Sde Arrangement E. Manay Department of Mechancal Engneerng, Faculty of Engneerng, Bayburt Unversty, Bayburt,

More information

Computational Modelling of the Unbalanced Magnetic Pull by Finite Element Method

Computational Modelling of the Unbalanced Magnetic Pull by Finite Element Method Avalable onlne at www.scencedrect.com Proceda Engneerng 48 (2012 ) 83 89 MMaMS 2012 Computatonal Modellng of the Unbalanced Magnetc Pull by Fnte Element Method Martn Donát a * a Brno Unversty of Technology,

More information

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

COMPARISON 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 information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE 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 information

Numerical Studies on Flow Features past a Backward Facing Sharp Edge Step Introducing Hybrid RANS-LES

Numerical Studies on Flow Features past a Backward Facing Sharp Edge Step Introducing Hybrid RANS-LES ISSN NO : 49-7455 Numercal Studes on Flow Features past a Backward Facng Sharp Edge Step Introducng Hybrd RANS-LES Abstract Dr. Nrmal Kumar Kund Assocate Professor, Department of Producton Engneerng Veer

More information

Numerical simulation of flow past circular duct

Numerical simulation of flow past circular duct Water Scence and Engneerng, 010, 3(): 08-16 do:10.388/.ssn.1674-370.010.0.009 http://.aterournal.cn e-mal: se008@vp.163.com Numercal smulaton of flo past crcular duct Ze-gao YIN* 1, Xan-e Cao 1, Hong-da

More information

A numerical study on the shell-side turbulent heat transfer enhancement of shell-and-tube heat exchanger with trefoilhole

A numerical study on the shell-side turbulent heat transfer enhancement of shell-and-tube heat exchanger with trefoilhole Avalable onlne at www.scencedrect.com ScenceDrect Energy Proceda 75 (2015 ) 3174 3179 The 7 th Internatonal Conference on Appled Energy ICAE2015 A numercal study on the shell-sde turbulent heat transfer

More information

The Analysis of Convection Experiment

The Analysis of Convection Experiment Internatonal Conference on Appled Scence and Engneerng Innovaton (ASEI 5) The Analyss of Convecton Experment Zlong Zhang School of North Chna Electrc Power Unversty, Baodng 7, Chna 469567@qq.com Keywords:

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE 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 information

Perfect Fluid Cosmological Model in the Frame Work Lyra s Manifold

Perfect 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 information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC 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 information

A NEW FILTERED DYNAMIC SUBGRID-SCALE MODEL FOR LARGE EDDY SIMULATION OF INDOOR AIRFLOW

A NEW FILTERED DYNAMIC SUBGRID-SCALE MODEL FOR LARGE EDDY SIMULATION OF INDOOR AIRFLOW A NEW FILTERED DYNAMIC SUBGRID-SCALE MODEL FOR LARGE EDDY SIMULATION OF INDOOR AIRFLOW We Zhang and Qngyan Chen Buldng Technology Program Massachusetts Insttute of Technology 77 Mass. Ave., Cambrdge, MA

More information

THE NEAR-WALL INFLUENCE ON THE FLOW AROUND A SINGLE SQUARE CYLINDER.

THE NEAR-WALL INFLUENCE ON THE FLOW AROUND A SINGLE SQUARE CYLINDER. THE NEAR-WALL INFLUENCE ON THE FLOW AROUND A SINGLE SQUARE CYLINDER. Campregher, Rubens Faculty of Mechancal Engneerng, FEMEC Federal Unversty of Uberlânda, UFU 38400-902 Uberlânda - Brazl campregher@mecanca.ufu.br

More information

Introduction to Computational Fluid Dynamics

Introduction 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 information

CFPD Simulation of Radioactive Particle Deposition in Lungs

CFPD Simulation of Radioactive Particle Deposition in Lungs CFPD Smulaton of Radoactve Partcle Deposton n Lungs Ayhan Ylmazer*, Ceml Kocar, Ismal Sercan Özer, Cem Gündüzalp *Hacettepe Unversty, Eng. Fac., Nuclear Eng. Dept., 06800, Beytepe, Ankara, Turkey ylmazer@hacettepe.edu.tr,

More information

Turbulent Flow in Curved Square Duct: Prediction of Fluid flow and Heat transfer Characteristics

Turbulent Flow in Curved Square Duct: Prediction of Fluid flow and Heat transfer Characteristics Internatonal Research Journal of Engneerng and Technology (IRJET) e-issn: 2395-56 Volume: 4 Issue: 7 July -217 www.ret.net p-issn: 2395-72 Turbulent Flow n Curved Square Duct: Predcton of Flud flow and

More information

2 MODELS A typcal hgh-sded artculated lorry, whch was nvestgated extensvely by Baker and hs colleagues n wnd tunnels and later used n the dynamc analy

2 MODELS A typcal hgh-sded artculated lorry, whch was nvestgated extensvely by Baker and hs colleagues n wnd tunnels and later used n the dynamc analy The Seventh Internatonal Colloquum on Bluff Body Aerodynamcs and Applcatons (BBAA7) Shangha, Chna; September 2-6, 2012 Determnaton of aerodynamc characterstcs of a vehcle mmerged n the wake of brdge tower

More information

Effect of loading frequency on the settlement of granular layer

Effect of loading frequency on the settlement of granular layer Effect of loadng frequency on the settlement of granular layer Akko KONO Ralway Techncal Research Insttute, Japan Takash Matsushma Tsukuba Unversty, Japan ABSTRACT: Cyclc loadng tests were performed both

More information

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI 2017 2nd Internatonal Conference on Electrcal and Electroncs: echnques and Applcatons (EEA 2017) ISBN: 978-1-60595-416-5 Study on Actve Mcro-vbraton Isolaton System wth Lnear Motor Actuator Gong-yu PAN,

More information

Simulation and experiment of the effect of clearance of impeller wear-rings on the performance of centrifugal pump

Simulation and experiment of the effect of clearance of impeller wear-rings on the performance of centrifugal pump IOP Conference Seres: Earth and Envronmental Scence Smulaton and experment of the effect of clearance of mpeller wear-rngs on the performance of centrfugal pump To cte ths artcle: S X Chen et al 01 IOP

More information

GeoSteamNet: 2. STEAM FLOW SIMULATION IN A PIPELINE

GeoSteamNet: 2. STEAM FLOW SIMULATION IN A PIPELINE PROCEEDINGS, Thrty-Ffth Workshop on Geothermal Reservor Engneerng Stanford Unversty, Stanford, Calforna, February 1-3, 010 SGP-TR-188 GeoSteamNet:. STEAM FLOW SIMULATION IN A PIPELINE Mahendra P. Verma

More information

Irregular vibrations in multi-mass discrete-continuous systems torsionally deformed

Irregular 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 information

Comparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy

Comparative 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 information

The unsteady flow characteristic research on the initial period flow of micro channel

The unsteady flow characteristic research on the initial period flow of micro channel Avalable onlne www.ocpr.com Journal of Chemcal and Pharmaceutcal Research, 2014, 6(6):2020-2024 Research Artcle ISSN : 0975-7384 CODEN(USA) : JCPRC5 The unsteady flow characterstc research on the ntal

More information

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS

NON-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 information

One-sided finite-difference approximations suitable for use with Richardson extrapolation

One-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 information

Computational investigation of the external excitation frequency effect on liquid sloshing phenomenon

Computational investigation of the external excitation frequency effect on liquid sloshing phenomenon Computatonal nvestgaton of the external exctaton frequency effect on lqud sloshng phenomenon Abdallah Bouabd *, Zed Drss, Laboratory of Electro-Mechanc Systems (LASEM) Natonal School of Engneers of Sfax

More information

Lattice Boltzmann simulation of nucleate boiling in micro-pillar structured surface

Lattice Boltzmann simulation of nucleate boiling in micro-pillar structured surface Proceedngs of the Asan Conference on Thermal Scences 017, 1st ACTS March 6-30, 017, Jeju Island, Korea ACTS-P00545 Lattce Boltzmann smulaton of nucleate bolng n mcro-pllar structured surface Png Zhou,

More information

Simulation of Flow Pattern in Open Channels with Sudden Expansions

Simulation of Flow Pattern in Open Channels with Sudden Expansions Research Journal of Appled Scences, Engneerng and Technology 4(19): 3852-3857, 2012 ISSN: 2040-7467 Maxwell Scentfc Organzaton, 2012 Submtted: May 11, 2012 Accepted: June 01, 2012 Publshed: October 01,

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, 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 information

CHAPTER 14 GENERAL PERTURBATION THEORY

CHAPTER 14 GENERAL PERTURBATION THEORY CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves

More information

Computational Fluid Dynamics. Smoothed Particle Hydrodynamics. Simulations. Smoothing Kernels and Basis of SPH

Computational Fluid Dynamics. Smoothed Particle Hydrodynamics. Simulations. Smoothing Kernels and Basis of SPH Computatonal Flud Dynamcs If you want to learn a bt more of the math behnd flud dynamcs, read my prevous post about the Naver- Stokes equatons and Newtonan fluds. The equatons derved n the post are the

More information

Turbulence and its Modelling

Turbulence 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 information

Consideration of 2D Unsteady Boundary Layer Over Oscillating Flat Plate

Consideration 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

The Study of Teaching-learning-based Optimization Algorithm

The Study of Teaching-learning-based Optimization Algorithm Advanced Scence and Technology Letters Vol. (AST 06), pp.05- http://dx.do.org/0.57/astl.06. The Study of Teachng-learnng-based Optmzaton Algorthm u Sun, Yan fu, Lele Kong, Haolang Q,, Helongang Insttute

More information

Study on Effect of Different Porosity on Thermally Driven Heat Transfer in a Centrifugal Force Field

Study on Effect of Different Porosity on Thermally Driven Heat Transfer in a Centrifugal Force Field 5th Internatonal Conference on Cvl Engneerng and Transportaton (ICCET 015) Study on Effect of Dfferent Porosty on Thermally Drven Heat Transfer n a Centrfugal Force Feld 1 Xa Je1,a*, Chang Ha-png,b, and

More information

A NUMERICAL COMPARISON OF LANGRANGE AND KANE S METHODS OF AN ARM SEGMENT

A 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 information

A Cartesian-grid integrated-rbf method for viscoelastic flows

A Cartesian-grid integrated-rbf method for viscoelastic flows Home Search Collectons Journals About Contact us My IOPscence A Cartesan-grd ntegrated-rbf method for vscoelastc flows Ths artcle has been downloaded from IOPscence. Please scroll down to see the full

More information

Brownian-Dynamics Simulation of Colloidal Suspensions with Kob-Andersen Type Lennard-Jones Potentials 1

Brownian-Dynamics Simulation of Colloidal Suspensions with Kob-Andersen Type Lennard-Jones Potentials 1 Brownan-Dynamcs Smulaton of Collodal Suspensons wth Kob-Andersen Type Lennard-Jones Potentals 1 Yuto KIMURA 2 and Mcho TOKUYAMA 3 Summary Extensve Brownan-dynamcs smulatons of bnary collodal suspenton

More information

NUMERICAL SIMULATION OF FLOW OVER STEPPED SPILLWAYS

NUMERICAL SIMULATION OF FLOW OVER STEPPED SPILLWAYS ISSN: 345-3109 RCEE Research n Cvl and Envronmental Engneerng www.rcee.com Research n Cvl and Envronmental Engneerng 014 (04) 190-198 NUMERICAL SIMULATION OF FLOW OVER STEPPED SPILLWAYS Rasoul Daneshfaraz

More information

Numerical study of the effect of wedge angle of a wedge-shaped body in a channel using lattice Boltzmann method

Numerical study of the effect of wedge angle of a wedge-shaped body in a channel using lattice Boltzmann method Avalable onlne at www.scencedrect.com Proceda Engneerng 56 (2013 ) 232 238 5 th BSME Internatonal Conference on Thermal Engneerng Numercal study of the effect of wedge angle of a wedge-shaped body n a

More information

Flow Induced Vibration

Flow Induced Vibration Flow Induced Vbraton Project Progress Report Date: 16 th November, 2005 Submtted by Subhrajt Bhattacharya Roll no.: 02ME101 Done under the gudance of Prof. Anrvan Dasgupta Department of Mechancal Engneerng,

More information

Analysis of Unsteady Aerodynamics of a Car Model with Radiator in Dynamic Pitching Motion using LS-DYNA

Analysis of Unsteady Aerodynamics of a Car Model with Radiator in Dynamic Pitching Motion using LS-DYNA Analyss of Unsteady Aerodynamcs of a Car Model wth Radator n Dynamc Ptchng Moton usng LS-DYNA Yusuke Nakae 1, Jro Takamtsu 1, Hrosh Tanaka 1, Tsuyosh Yasuk 1 1 Toyota Motor Corporaton 1 Introducton Recently,

More information

Simulation of Turbulent Flow Using FEM

Simulation of Turbulent Flow Using FEM Internatonal Journal of Engneerng and Technology Volume 2 No. 8, August, 2012 Smulaton of Turbulent Flow Usng FEM Sabah Tamm College of Computng, AlGhurar Unversty, Duba, Unted Arab Emrates. ABSTRACT An

More information

The Tangential Force Distribution on Inner Cylinder of Power Law Fluid Flowing in Eccentric Annuli with the Inner Cylinder Reciprocating Axially

The 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

STATIC ANALYSIS OF TWO-LAYERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION

STATIC 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 information

NUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST

NUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST Appled Computer Scence, vol. 13, no. 4, pp. 56 64 do: 10.23743/acs-2017-29 Submtted: 2017-10-30 Revsed: 2017-11-15 Accepted: 2017-12-06 Abaqus Fnte Elements, Plane Stress, Orthotropc Materal Bartosz KAWECKI

More information

Various Speed Ratios of Two-Sided Lid-Driven Cavity Flow using Lattice Boltzmann Method

Various Speed Ratios of Two-Sided Lid-Driven Cavity Flow using Lattice Boltzmann Method Penerbt and Thermal Scences ISSN (onlne): 2289-7879 Varous Speed Ratos of Two-Sded Ld-Drven Cavty Flow usng Lattce Boltzmann Method Nor Azwad Che Sdk *,a and St Asyah Razal b Department of Thermo-Fluds,

More information

Understanding Electrophoretic Displays: Transient Current Characteristics of Dispersed Charges in a Non-Polar Medium

Understanding Electrophoretic Displays: Transient Current Characteristics of Dispersed Charges in a Non-Polar Medium Understandng Electrophoretc Dsplays: Transent Current Characterstcs of Dspersed Charges n a Non-Polar Medum Yoocharn Jeon, Pavel Kornlovtch, Patrca Beck, Zhang-Ln Zhou, Rchard Henze, Tm Koch HP Laboratores

More information

Module 1 : The equation of continuity. Lecture 1: Equation of Continuity

Module 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 information

The Order Relation and Trace Inequalities for. Hermitian Operators

The 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 information

Amplification and Relaxation of Electron Spin Polarization in Semiconductor Devices

Amplification and Relaxation of Electron Spin Polarization in Semiconductor Devices Amplfcaton and Relaxaton of Electron Spn Polarzaton n Semconductor Devces Yury V. Pershn and Vladmr Prvman Center for Quantum Devce Technology, Clarkson Unversty, Potsdam, New York 13699-570, USA Spn Relaxaton

More information

CHAPTER 7 ENERGY BALANCES SYSTEM SYSTEM. * What is energy? * Forms of Energy. - Kinetic energy (KE) - Potential energy (PE) PE = mgz

CHAPTER 7 ENERGY BALANCES SYSTEM SYSTEM. * What is energy? * Forms of Energy. - Kinetic energy (KE) - Potential energy (PE) PE = mgz SYSTM CHAPTR 7 NRGY BALANCS 1 7.1-7. SYSTM nergy & 1st Law of Thermodynamcs * What s energy? * Forms of nergy - Knetc energy (K) K 1 mv - Potental energy (P) P mgz - Internal energy (U) * Total nergy,

More information

Three-Phase Distillation in Packed Towers: Short-Cut Modelling and Parameter Tuning

Three-Phase Distillation in Packed Towers: Short-Cut Modelling and Parameter Tuning European Symposum on Computer Arded Aded Process Engneerng 15 L. Pugjaner and A. Espuña (Edtors) 2005 Elsever Scence B.V. All rghts reserved. Three-Phase Dstllaton n Packed Towers: Short-Cut Modellng and

More information

Uniqueness of Weak Solutions to the 3D Ginzburg- Landau Model for Superconductivity

Uniqueness of Weak Solutions to the 3D Ginzburg- Landau Model for Superconductivity Int. Journal of Math. Analyss, Vol. 6, 212, no. 22, 195-114 Unqueness of Weak Solutons to the 3D Gnzburg- Landau Model for Superconductvty Jshan Fan Department of Appled Mathematcs Nanjng Forestry Unversty

More information

A Comparative Investigation into Aerodynamic Performances of Two Set Finned Bodies with Circular and Non Circular Cross Sections

A Comparative Investigation into Aerodynamic Performances of Two Set Finned Bodies with Circular and Non Circular Cross Sections A Comparatve Investgaton nto Aerodynamc Performances of Two Set Fnned Bodes wth Crcular and Non Crcular Cross Sectons MAHMOUD MANI and SHADI MAHJOOB Aerospace Engneerng Department Amrkabr Unversty of Technology

More information

arxiv: v1 [physics.flu-dyn] 16 Sep 2013

arxiv: 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 information

NUMERICAL ANALYSIS OF TURBULENT FLOW WITH HEAT TRANSFER IN A SQUARE DUCT WITH 45 DEGREE RIBS

NUMERICAL ANALYSIS OF TURBULENT FLOW WITH HEAT TRANSFER IN A SQUARE DUCT WITH 45 DEGREE RIBS Proceedngs of IONE19 19th Internatonal onference on Nuclear Engneerng May 16-19, 011, hba, Japan IONE19-43147 NUMERIAL ANALYSIS OF TURBULENT FLOW WITH HEAT TRANSFER IN A SQUARE DUT WITH 45 DEGREE RIBS

More information

Field computation with finite element method applied for diagnosis eccentricity fault in induction machine

Field computation with finite element method applied for diagnosis eccentricity fault in induction machine Proceedngs of the Internatonal Conference on Recent Advances n Electrcal Systems, Tunsa, 216 Feld computaton wth fnte element method appled for dagnoss eccentrcty fault n nducton machne Moufd Mohammed,

More information

A Solution of the Harry-Dym Equation Using Lattice-Boltzmannn and a Solitary Wave Methods

A Solution of the Harry-Dym Equation Using Lattice-Boltzmannn and a Solitary Wave Methods Appled Mathematcal Scences, Vol. 11, 2017, no. 52, 2579-2586 HIKARI Ltd, www.m-hkar.com https://do.org/10.12988/ams.2017.79280 A Soluton of the Harry-Dym Equaton Usng Lattce-Boltzmannn and a Soltary Wave

More information

Wavelet chaotic neural networks and their application to continuous function optimization

Wavelet chaotic neural networks and their application to continuous function optimization Vol., No.3, 04-09 (009) do:0.436/ns.009.307 Natural Scence Wavelet chaotc neural networks and ther applcaton to contnuous functon optmzaton Ja-Ha Zhang, Yao-Qun Xu College of Electrcal and Automatc Engneerng,

More information

STUDY OF A THREE-AXIS PIEZORESISTIVE ACCELEROMETER WITH UNIFORM AXIAL SENSITIVITIES

STUDY OF A THREE-AXIS PIEZORESISTIVE ACCELEROMETER WITH UNIFORM AXIAL SENSITIVITIES STUDY OF A THREE-AXIS PIEZORESISTIVE ACCELEROMETER WITH UNIFORM AXIAL SENSITIVITIES Abdelkader Benchou, PhD Canddate Nasreddne Benmoussa, PhD Kherreddne Ghaffour, PhD Unversty of Tlemcen/Unt of Materals

More information

PHYS 705: Classical Mechanics. Newtonian Mechanics

PHYS 705: Classical Mechanics. Newtonian Mechanics 1 PHYS 705: Classcal Mechancs Newtonan Mechancs Quck Revew of Newtonan Mechancs Basc Descrpton: -An dealzed pont partcle or a system of pont partcles n an nertal reference frame [Rgd bodes (ch. 5 later)]

More information

NUMERICAL SIMULATION OF 3D TURBULENT FLOW STRUCTURES AROUND AN ATTRACTING GROIN WITH LOCAL SCOUR

NUMERICAL SIMULATION OF 3D TURBULENT FLOW STRUCTURES AROUND AN ATTRACTING GROIN WITH LOCAL SCOUR NUMERICAL SIMULATION OF 3D TURBULENT FLOW STRUCTURES AROUND AN ATTRACTING GROIN WITH LOCAL SCOUR ICHIRO KIMURA Department of Cvl and Envronmental Engneerng, Matsue Natonal College of Technology 4-4 Nsh-kuma,

More information

Computation of drag and flow noise along wavy wall in turbulent flow

Computation of drag and flow noise along wavy wall in turbulent flow roceedngs of 0 th Internatonal Congress on Acoustcs, ICA 010 3-7 August 010, ydney, Australa Computaton of drag and flow nose along wavy wall n turbulent flow Huaxn Zhang (1), Kunyu Meng (1) and Yongln

More information

Research & Reviews: Journal of Engineering and Technology

Research & Reviews: Journal of Engineering and Technology Research & Revews: Journal of Engneerng and Technology Case Study to Smulate Convectve Flows and Heat Transfer n Arcondtoned Spaces Hussen JA 1 *, Mazlan AW 1 and Hasanen MH 2 1 Department of Mechancal

More information

SIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME. Abstract

SIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME. Abstract SIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME PACS REFERENCE: 43.20.Mv Andreas Wlde Fraunhofer Insttut für Integrerte Schaltungen, Außenstelle EAS Zeunerstr.

More information

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE

CHAPTER 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 information

3-D Numerical computations of turbulence in a partially vegetated shallow channel

3-D Numerical computations of turbulence in a partially vegetated shallow channel Rver Flow 010 - Dttrch, Koll, Aberle & Gesenhaner (eds) - 010 Bundesanstalt für Wasserbau ISBN 978-3-93930-00-7 3-D Numercal computatons of turbulence n a partally vegetated shallow channel D. Soulots

More information

EXPERIMENTAL STUDY OF NEAR WALL TURBULENCE USING PIV

EXPERIMENTAL STUDY OF NEAR WALL TURBULENCE USING PIV EUROMECH 411 Rouen, 9-31 May EXPERIMENTAL STUDY OF NEAR WALL TURBULENCE USING PIV J. Carler, J. M. Foucaut and M. Stanslas LML URA 1441, Bv Paul Langevn, Cté Scentfque, 59655 Vlleneuve d'ascq Cedex, France

More information

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM

DETERMINATION 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 information

Physics 181. Particle Systems

Physics 181. Particle Systems Physcs 181 Partcle Systems Overvew In these notes we dscuss the varables approprate to the descrpton of systems of partcles, ther defntons, ther relatons, and ther conservatons laws. We consder a system

More information

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force.

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force. The fundamental prncples of classcal mechancs were lad down by Galleo and Newton n the 16th and 17th centures. In 1686, Newton wrote the Prncpa where he gave us three laws of moton, one law of gravty,

More information

Flow equations To simulate the flow, the Navier-Stokes system that includes continuity and momentum equations is solved

Flow equations To simulate the flow, the Navier-Stokes system that includes continuity and momentum equations is solved Smulaton of nose generaton and propagaton caused by the turbulent flow around bluff bodes Zamotn Krll e-mal: krart@gmal.com, cq: 958886 Summary Accurate predctons of nose generaton and spread n turbulent

More information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information Thrd Chnese-German Jont Symposum on Coastal and Ocean Engneerng Natonal Cheng Kung Unversty, Tanan November 8-16, 2006 Modal Stran Energy Decomposton Method for Damage Detecton of an Offshore Structure

More information

Survey of applications of discrete vortex method in civil engineering

Survey of applications of discrete vortex method in civil engineering Budownctwo Archtektura 5 (2009) 29-38 Survey of applcatons of dscrete vortex method n cvl engneerng Tomasz Nowck Lubln Unversty of Technology, Faculty of Cvl Engneerng and Archtecture, Department of Structural

More information

Large Scale Electrostatic Precipitator

Large Scale Electrostatic Precipitator 11th Internatonal Conference on Electrostatc Precptaton 164 4BStudy and Applcaton of Numercal Calculaton Method for Gas Flow Dstrbuton of Large Scale Electrostatc Precptator DANG Xaoqng, HU Hongsheng,

More information

Mathematical Preparations

Mathematical 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 information

Susceptibility and Inverted Hysteresis Loop of Prussian Blue Analogs with Orthorhombic Structure

Susceptibility and Inverted Hysteresis Loop of Prussian Blue Analogs with Orthorhombic Structure Commun. Theor. Phys. 58 (202) 772 776 Vol. 58, No. 5, November 5, 202 Susceptblty and Inverted Hysteress Loop of Prussan Blue Analogs wth Orthorhombc Structure GUO An-Bang (ÁËǑ) and JIANG We ( å) School

More information

Simulation for Pedestrian Dynamics by Real-Coded Cellular Automata (RCA)

Simulation for Pedestrian Dynamics by Real-Coded Cellular Automata (RCA) Smulaton for Pedestran Dynamcs by Real-Coded Cellular Automata (RCA) Kazuhro Yamamoto 1*, Satosh Kokubo 1, Katsuhro Nshnar 2 1 Dep. Mechancal Scence and Engneerng, Nagoya Unversty, Japan * kazuhro@mech.nagoya-u.ac.jp

More information

Modeling of Dynamic Systems

Modeling of Dynamic Systems Modelng of Dynamc Systems Ref: Control System Engneerng Norman Nse : Chapters & 3 Chapter objectves : Revew the Laplace transform Learn how to fnd a mathematcal model, called a transfer functon Learn how

More information