Available online at ScienceDirect. Procedia Engineering 153 (2016 )

Size: px
Start display at page:

Download "Available online at ScienceDirect. Procedia Engineering 153 (2016 )"

Transcription

1 Avalable onlne a ScenceDrec Proceda Engneerng 5 (6 ) XXV Polsh Russan Slova Semnar Theorecal Foundaon of Cvl Engneerng Vbraon of embedded foundaon a mul-layered base ang no accoun non-lnear and rheologcal properes of sols Ter-Marrsyan Z.G. a, Ter-Marrsyan A.Z. a *, Sobolev E.S. a a Moscow Sae Unversy of Cvl Engneerng (Naonal Research Unversy), 6 Yaroslavsoye Shosse, Moscow, 97, Russa Absrac Calculaon scheme of sold mul-layered base of he embedded foundaon s offered for descrpon of sysem vbraon foundaon s a mul-layered base. I s shown ha n hs case consderaon of apparen mass of he sold mul-layered base, as well as foundaon sde surface frcon leads o non-perodcal (non-harmonc) damped vbraon of he foundaon. Dfferen conac models ncludng elasc, non-lnear and rheologcal ones wh regard o srenghenng hroughou he me are consdered as for calculaon for soluon of problem of sysem vbraon. I s shown ha consderaon of sol srenghenng and sde surface frcon of he embedded foundaon grealy nfluence he nensy of vbraon dampng hroughou he me. 6 Publshed The Auhors. by Elsever Publshed Ld. by Ths Elsever s an open Ld. access arcle under he CC BY-NC-ND lcense Peer-revew (hp://creavecommons.org/lcenses/by-nc-nd/4./). under responsbly of he organng commee of he XXV Polsh Russan Slova Semnar Theorecal Foundaon Peer-revew under of Cvl responsbly Engneerng. of he organng commee of he XXV Polsh Russan Slova Semnar Theorecal Foundaon of Cvl Engneerng. Keywords: vbraons, base, sol, rheologcal properes, nonlneary.. Inroducon I s nown ha when desgnng he foundaon for machne and equpmen wh dynamc loads, ground base s consdered as a massless and s characered by sffness coeffcen K, Kx and. Such a smplfed model of he base, nown as Wnler model, enables us o smplfy consderably he soluon of dfferenal equaons of foundaon vbraon a compressble base regardless o vscous ressance [, 4, 5, ]. * Correspondng auhor. Tel.: E-mal address: gc-mgsu@mal.ru Publshed by Elsever Ld. Ths s an open access arcle under he CC BY-NC-ND lcense (hp://creavecommons.org/lcenses/by-nc-nd/4./). Peer-revew under responsbly of he organng commee of he XXV Polsh Russan Slova Semnar Theorecal Foundaon of Cvl Engneerng. do:.6/j.proeng.6.8.7

2 748 Z.G. Ter-Marrsyan e al. / Proceda Engneerng 5 ( 6 ) One uses he models whch ae no accoun dampng properes of he sol, ncludng Kelvn-Vog model and Maxwell model when s necessary o accoun non-elasc ressance of he base []. Ths paper presens he problem of vbraon of he embedded foundaon a he sold (neral) mul-layered base ang no accoun vscous properes of base sols and sde surface frcon [8, 9]. Frs aemps o accoun he apparen mass of base sols are made by E. Ressner, hen by O.Ya.Sheher []. One consdered he problem of forced vbraons of he round plae a he elasc sold semspace nfluenced by harmonc dsurbng force. Accoun of neral forces of base sols resuls n he fac ha vbraon amplude does no urn no nfny anywhere ha s here s no resonance, provded ha he ncrease n Posson s rao leads o he ncrease of energy emsson from vbrang foundaon o he sol, consequenly, he dampng of sysem vbraons. Besdes, accoun of nera of base sols resuls n aperodc foundaon vbraon ha s here s no vbraon moon of he foundaon. In hs respec, neral properes of base sols nfluence more he foundaons of low hegh and large se han he foundaons of hgh hegh and relavely small base square. The models wh he apparen mass are currenly used for soluon of praccal problems wh dfferen mehods ncludng s seng o he sol volume conaned n he acve deformaon area of he base. When calculang wde foundaons, dynamc load s consdered o be ransferred o he ground base as a load-bearng pos, concal (rapeodal) sold mass and semspace.. Vbraon of embedded massve foundaon a he mul-layered sold vsco-elasc base I s nown [, 7] ha n case of neral base, he dynamc equlbrum of he foundaon wh one degree of freedom under he nfluence of vbraon power can be expressed wh he equaon: m F sn( ) = p sn( ω) (), where s a vercal dsplacemen; m s a foundaon mass; F s a sde surface frcon force. The equaon sysem of ype (5) mus be solved n case of sold mul-layered base wh several degrees of freedom. The number of equaons mus concde wh he number of degrees of freedom of hs sysem. Reacve and neral forces, as well as sde surface frcon force of foundaon and sol appear n case of vbraon of he embedded foundaon a he sol sold mul-layered base. These forces can consderably nfluence he characer of foundaon vbraon, ncludng amplude and vbraon frequency, exclude resonance possbly and enable he accumulaon of foundaon resdual selemen and nclnaon. The problem of vbraon on elasc and neral unform base s consdered n paper [] ncludng he approxmae calculaon scheme where he dynamc load s consdered o be ransferred o: exclusvely load-bearng prsmac sol pos; load-bearng sold mass n he form of fne (rapeodal) sold mass and semspace. One also nows he approxmae calculaon scheme where base nera s aen no accoun by way of jonng of acve one sol mass o foundaon mass. All hese calculaon schemes lead o decrease of vbraon amplude and exclude resonance. Ths paper offers he approxmae calculaon scheme of vbraon of he embedded foundaon a sold mullayered base wh regard o sde surface frcon of foundaon and sol, as well as elasc and vscous sol properes. Sol base s shown as sold layers of fne hcness joned by elasc and elasc and vscous elemens. In hs case, each layer wh mass m wll vbrae ndvdually and, consequenly, here wll be a sysem wh mulple degree of freedom equal o he number of layers (fg. ). Soluon of sffness coeffcen of each layer, s mass m and mean value of sac load p, as well as sress dsrbuon angle of sascal load are defned for mahemacal descrpon of vbraon of such a sysem. The las n he frs approxmaon can be defned on he bass of dampng sress coeffcen under he foundaon of he cenral axs by ables [] dependng on foundaon ype n plan (recangle, square, crcle). There s dependence beween he dsrbuon angle and sress dampng coeffcen as follows: b( α ) an λ =, () α Z a

3 Z.G. Ter-Marrsyan e al. / Proceda Engneerng 5 ( 6 ) FOUNDATION where b and l are he breadh and he lengh of he recangular foundaon, respecvely; Z a s he lower bound of he compressble foundaon hcness defned from he condon p =,5 g [6, 7]. Thus, for example, for recangular foundaon wh breadh b = m, and lengh l = 8m a he deph = m, he value maes =.46. Then an =.58,. Havng he values, one can defne he dmensons of he -h layer n plan, ha s b = b l an, where h s he hcness of he -h layer. Values p and can be defned by formulas: bl b p = p ; p = ; S S p β h = ; () E where E s he module of lnear deformaon of he -h layer; S s of he selemen of he -h layer; ν β =,8. (4) ν where s a coeffcen of Posson s rao of he -h layer. Le s consder he smples suaon. Imagne he vbraon calculaon scheme of he sysem foundaon s a valuable base wh hree degrees of freedom consderng ha he foundaon wh mass m co-operaes wh valuable wo-layered base wh mass m and m, whch cener of gravy s on one hrd of he hegh of layers h and h (fg. ). In hs case, here s a possbly of only vercal dsplacemen of he foundaon. If n he frs approxmaon one does no accoun energy absorpon, hen he dfferenal equaon of forced vbraons of such a sysem can be represened as follows:

4 75 Z.G. Ter-Marrsyan e al. / Proceda Engneerng 5 ( 6 ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) sn sn = = = m m p F m ω. (5) Fg.. Vbraon calculaon scheme of he sysem foundaon s a valuable wo-layered base wh hree degrees of freedom where,, are vercal dsplacemens of he foundaon and ceners of gravy of he frs and he second layers of he foundaon, respecvely; m, m, m are he masses of foundaon, he frs and he second layers of ground bases, respecvely; s a sffness coeffcen of he base, where ( ) ( ) = ; s a vscous ressance coeffcen of sols, where ( ) ( ) = ; F s a sde surface frcon force of he foundaon. Equaon soluon (5) can be obaned by numercal mehod wh he help of sofware MahCAD. The resuls of he soluon are shown n fg. ang no accoun sol srenghenng, ha s a e β =, e α = and a foundaon mass m=8 ons, dameer 8 m under nfluence of dsurbng mpulse force P()=p, a layer hcness h =h =5m. FOUNDATION

5 Z.G. Ter-Marrsyan e al. / Proceda Engneerng 5 ( 6 ) Vercal dsplacemen(m) () () ().5.5 Fg.. Curves of vbraons of he sysem foundaon s a wo-layered base wh hree layers of freedom ploed based on equaon soluon (5) wh he help of sofware MahCAD ang no accoun srenghenng and frcon of sols by sde surface of he embedded foundaon; foundaon ( ), frs layer ( ) and second layer ( ) Tme(s) I s apparen n case of absence of harmonc vbraon and foundaon resdual selemen. Ths problem s solved also n elasc approach boh n soluon (5) and sofware PLAXIS. Benchmarng of hese soluons (fgures 4, 5, 6) demonsraes ha here s a sasfacory convergence. Consequenly, he proposed calculaon model (fg. ) can be used for calculaon of vbraon sysem foundaon s a mul-layered valuable base wh he help of sofware MahCAD. 5 Vercal dsplacemen(m) () () () Tme(s) Fg. 4. Curves of vbraons of he sysem foundaon s a wo-layered base wh hree layers of freedom ploed based on soluon (5) wh he help of sofware MahCAD ang no accoun he elasc sol model; foundaon ( ), frs layer ( ) and second layer ( )

6 75 Z.G. Ter-Marrsyan e al. / Proceda Engneerng 5 ( 6 ) Vercal dsplacemen[m] 5e- -5e- -. Pon A Pon B Tme[s] Pon C Fg. 5. Curves of vbraons of foundaon (Pon A), ceners of he frs (Pon B) and he second (Pon C) layers of sols ang no accoun elasc properes of foundaon sols ploed based on he resuls of numercal calculaon of plane problem n sofware PLAXIS Vercal dsplacemen [m] -5e- -. Pon A -.5 Pon B Tme [s] Pon C Fg. 6. Curves of vbraons of foundaon (Pon A), ceners of he frs (Pon B) and he second (Pon C) layers ang no accoun elasc and plasc properes of foundaon sols ploed based on he resuls of numercal calculaon of plane problem n sofware PLAXIS. Conclusons. The proposed calculaon scheme (fg. ) wh adequae accuracy descrbes he vbraon of he embedded foundaon a sold mul-layered base.. The examples of problems soluons on vbraon of he sysem foundaon s a base on he ground of he proposed calculaon scheme of he sold mul-layered base wh several degrees of freedom and her comparson wh he resuls of numercal problem soluon n sofware PLAXIS showed her sasfacory convergence.. Accoun of wegh of base sols and sde surface frcon of he embedded foundaon n he proposed model (fg. ) has consderable nfluence on he characerscs of foundaon vbraon ncludng amplude and accumulaon of foundaon resdual selemen.

7 Z.G. Ter-Marrsyan e al. / Proceda Engneerng 5 ( 6 ) Acnowledgemens Ths wor was fnancally suppored by he Mnsry of Russan Educaon (sae as #4/4; # /K). References [] E.A.Vonesensy Sol Dynamc Insably. Moscow: Edoral, 999. page 64 [] Yu.K. Zaresy, V.N. Lombardo Sascs and Dynamcs of Sol Dams. Moscow: Energoaomda, 98. page 56 [] N.D. Krasnov Dynamc Properes of Sols and Mehods of her Deermnaon. Lenngrad: Sroyda, 97. page 9 [4] E. Rausch Machne Foundaons. Moscow: Sroyda, 965. page 48 [5] O.A. Savnov Modern Consrucons of Machne Foundaons and her Calculaons. Moscow: Sroyda, 979. page 79 [6] SP... Foundaons of Buldngs and Srucures. Revsed edon SNP..-8* Moscow: Mnsry of Regonal Developmen of Russa,. page 6 [7] SP 6... Foundaons for Machnes wh Dynamc Loads. Revsed edon SNP Moscow: Mnsry of Regonal Developmen of Russa, page 66 [8] L.R. Savnser Sesmc Ressance of Basemens and Foundaons. Moscow: ASB,. page 447 [9] Z.G. Ter-Marrsyan Sol Mechancs. Moscow: ASB, 9. page 55 [] Sol Mechancs, Basemens and Foundaons / S.B. Uchov, V.V. Semenov, V.V. Znamenovsy, Z.G. Ter-Marrsyan, S.N. Chernyshev eded by S.B. Uchov rd edon. Moscow: Vysshaya Shola, 4. page 566 [] O.Ya. Sheher Dynamc Calculaon of Ples Jon by Rgd Foundaon Frame on Top // Collecon of Wors of he Research Esablshmen of Foundaons and Basemens, No.. Moscow: 948. pages 4-5 [] M. Nova Sae of he Ar n Analyss and Desgn of Machne Foundaons // Sol-Srucure Ineracon pages 55-67

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Journal of Appled Mahemacs and Compuaonal Mechancs 3, (), 45-5 HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Sansław Kukla, Urszula Sedlecka Insue of Mahemacs,

More information

First-order piecewise-linear dynamic circuits

First-order piecewise-linear dynamic circuits Frs-order pecewse-lnear dynamc crcus. Fndng he soluon We wll sudy rs-order dynamc crcus composed o a nonlnear resse one-por, ermnaed eher by a lnear capacor or a lnear nducor (see Fg.. Nonlnear resse one-por

More information

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy Arcle Inernaonal Journal of Modern Mahemacal Scences, 4, (): - Inernaonal Journal of Modern Mahemacal Scences Journal homepage: www.modernscenfcpress.com/journals/jmms.aspx ISSN: 66-86X Florda, USA Approxmae

More information

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems Swss Federal Insue of Page 1 The Fne Elemen Mehod for he Analyss of Non-Lnear and Dynamc Sysems Prof. Dr. Mchael Havbro Faber Dr. Nebojsa Mojslovc Swss Federal Insue of ETH Zurch, Swzerland Mehod of Fne

More information

On One Analytic Method of. Constructing Program Controls

On One Analytic Method of. Constructing Program Controls Appled Mahemacal Scences, Vol. 9, 05, no. 8, 409-407 HIKARI Ld, www.m-hkar.com hp://dx.do.org/0.988/ams.05.54349 On One Analyc Mehod of Consrucng Program Conrols A. N. Kvko, S. V. Chsyakov and Yu. E. Balyna

More information

Gear System Time-varying Reliability Analysis Based on Elastomer Dynamics

Gear System Time-varying Reliability Analysis Based on Elastomer Dynamics A publcaon of CHEMICAL ENGINEERING TRANSACTIONS VOL. 33, 013 Gues Edors: Enrco Zo, Pero Barald Copyrgh 013, AIDIC Servz S.r.l., ISBN 978-88-95608-4-; ISSN 1974-9791 The Ialan Assocaon of Chemcal Engneerng

More information

ELASTIC MODULUS ESTIMATION OF CHOPPED CARBON FIBER TAPE REINFORCED THERMOPLASTICS USING THE MONTE CARLO SIMULATION

ELASTIC MODULUS ESTIMATION OF CHOPPED CARBON FIBER TAPE REINFORCED THERMOPLASTICS USING THE MONTE CARLO SIMULATION THE 19 TH INTERNATIONAL ONFERENE ON OMPOSITE MATERIALS ELASTI MODULUS ESTIMATION OF HOPPED ARBON FIBER TAPE REINFORED THERMOPLASTIS USING THE MONTE ARLO SIMULATION Y. Sao 1*, J. Takahash 1, T. Masuo 1,

More information

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION S19 A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION by Xaojun YANG a,b, Yugu YANG a*, Carlo CATTANI c, and Mngzheng ZHU b a Sae Key Laboraory for Geomechancs and Deep Underground Engneerng, Chna Unversy

More information

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS R&RATA # Vol.) 8, March FURTHER AALYSIS OF COFIDECE ITERVALS FOR LARGE CLIET/SERVER COMPUTER ETWORKS Vyacheslav Abramov School of Mahemacal Scences, Monash Unversy, Buldng 8, Level 4, Clayon Campus, Wellngon

More information

Dynamic Model of the Axially Moving Viscoelastic Belt System with Tensioner Pulley Yanqi Liu1, a, Hongyu Wang2, b, Dongxing Cao3, c, Xiaoling Gai1, d

Dynamic Model of the Axially Moving Viscoelastic Belt System with Tensioner Pulley Yanqi Liu1, a, Hongyu Wang2, b, Dongxing Cao3, c, Xiaoling Gai1, d Inernaonal Indsral Informacs and Comper Engneerng Conference (IIICEC 5) Dynamc Model of he Aally Movng Vscoelasc Bel Sysem wh Tensoner Plley Yanq L, a, Hongy Wang, b, Dongng Cao, c, Xaolng Ga, d Bejng

More information

Behavioral Study of Finite Beam Resting on Elastic Foundation and Subjected to Travelling Distributed Masses

Behavioral Study of Finite Beam Resting on Elastic Foundation and Subjected to Travelling Distributed Masses 3 Behavoral Sudy of Fne Beam Resng on Elasc Foundaon and Subeced o Travellng Dsrbued Masses Absrac The classcal problem of he response characerscs of unform srucural member resng on elasc subgrade and

More information

Response of MDOF systems

Response of MDOF systems Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss

More information

Anisotropic Behaviors and Its Application on Sheet Metal Stamping Processes

Anisotropic Behaviors and Its Application on Sheet Metal Stamping Processes Ansoropc Behavors and Is Applcaon on Shee Meal Sampng Processes Welong Hu ETA-Engneerng Technology Assocaes, Inc. 33 E. Maple oad, Sue 00 Troy, MI 48083 USA 48-79-300 whu@ea.com Jeanne He ETA-Engneerng

More information

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim Korean J. Mah. 19 (2011), No. 3, pp. 263 272 GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS Youngwoo Ahn and Kae Km Absrac. In he paper [1], an explc correspondence beween ceran

More information

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5 TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres

More information

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs.

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs. Handou # 6 (MEEN 67) Numercal Inegraon o Fnd Tme Response of SDOF mechancal sysem Sae Space Mehod The EOM for a lnear sysem s M X DX K X F() () X X X X V wh nal condons, a 0 0 ; 0 Defne he followng varables,

More information

VEHICLE DYNAMIC MODELING & SIMULATION: COMPARING A FINITE- ELEMENT SOLUTION TO A MULTI-BODY DYNAMIC SOLUTION

VEHICLE DYNAMIC MODELING & SIMULATION: COMPARING A FINITE- ELEMENT SOLUTION TO A MULTI-BODY DYNAMIC SOLUTION 21 NDIA GROUND VEHICLE SYSTEMS ENGINEERING AND TECHNOLOGY SYMPOSIUM MODELING & SIMULATION, TESTING AND VALIDATION (MSTV) MINI-SYMPOSIUM AUGUST 17-19 DEARBORN, MICHIGAN VEHICLE DYNAMIC MODELING & SIMULATION:

More information

Implementation of Quantized State Systems in MATLAB/Simulink

Implementation of Quantized State Systems in MATLAB/Simulink SNE T ECHNICAL N OTE Implemenaon of Quanzed Sae Sysems n MATLAB/Smulnk Parck Grabher, Mahas Rößler 2*, Bernhard Henzl 3 Ins. of Analyss and Scenfc Compung, Venna Unversy of Technology, Wedner Haupsraße

More information

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.3. COMPATIBILITY EQUATIONS Connuum Mechancs Course (MMC) - ETSECCPB - UPC Overvew Compably Condons Compably Equaons of a Poenal Vecor Feld Compably Condons for Infnesmal Srans Inegraon of he Infnesmal

More information

Structure Analysis and Optimization for Compacting System of Asphalt Paver

Structure Analysis and Optimization for Compacting System of Asphalt Paver Send Orders for Reprns o reprns@benhamscence.ae 86 The Open Mechancal Engneerng Journal, 05, 9, 86-9 Open Access Srucure Analyss and Opmzaon for Compacng Sysem of Asphal Paver Sun Jan * Mechancal and Elecronc

More information

Deformation Calculating of Electromagnetic Launcher s Rail Subjected to Logarithmic Magnetic Pressure

Deformation Calculating of Electromagnetic Launcher s Rail Subjected to Logarithmic Magnetic Pressure Deformaon Calculang of Elecromagnec auncher s al Subjeced o ogarhmc Magnec Pressure Wen u (Correspondng auhor) & Mn School of Scences, Yanshan Unversy, Qnhuangdao 664, Chna Xangzhong Ba School of Cvl Engneerng

More information

2/20/2013. EE 101 Midterm 2 Review

2/20/2013. EE 101 Midterm 2 Review //3 EE Mderm eew //3 Volage-mplfer Model The npu ressance s he equalen ressance see when lookng no he npu ermnals of he amplfer. o s he oupu ressance. I causes he oupu olage o decrease as he load ressance

More information

Relative controllability of nonlinear systems with delays in control

Relative controllability of nonlinear systems with delays in control Relave conrollably o nonlnear sysems wh delays n conrol Jerzy Klamka Insue o Conrol Engneerng, Slesan Techncal Unversy, 44- Glwce, Poland. phone/ax : 48 32 37227, {jklamka}@a.polsl.glwce.pl Keywor: Conrollably.

More information

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he

More information

New M-Estimator Objective Function. in Simultaneous Equations Model. (A Comparative Study)

New M-Estimator Objective Function. in Simultaneous Equations Model. (A Comparative Study) Inernaonal Mahemacal Forum, Vol. 8, 3, no., 7 - HIKARI Ld, www.m-hkar.com hp://dx.do.org/.988/mf.3.3488 New M-Esmaor Objecve Funcon n Smulaneous Equaons Model (A Comparave Sudy) Ahmed H. Youssef Professor

More information

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () we define the interaction representation by the unitary transformation () = () Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger

More information

Robustness Experiments with Two Variance Components

Robustness Experiments with Two Variance Components Naonal Insue of Sandards and Technology (NIST) Informaon Technology Laboraory (ITL) Sascal Engneerng Dvson (SED) Robusness Expermens wh Two Varance Componens by Ana Ivelsse Avlés avles@ns.gov Conference

More information

Attribute Reduction Algorithm Based on Discernibility Matrix with Algebraic Method GAO Jing1,a, Ma Hui1, Han Zhidong2,b

Attribute Reduction Algorithm Based on Discernibility Matrix with Algebraic Method GAO Jing1,a, Ma Hui1, Han Zhidong2,b Inernaonal Indusral Informacs and Compuer Engneerng Conference (IIICEC 05) Arbue educon Algorhm Based on Dscernbly Marx wh Algebrac Mehod GAO Jng,a, Ma Hu, Han Zhdong,b Informaon School, Capal Unversy

More information

Chapter 2 Linear dynamic analysis of a structural system

Chapter 2 Linear dynamic analysis of a structural system Chaper Lnear dynamc analyss of a srucural sysem. Dynamc equlbrum he dynamc equlbrum analyss of a srucure s he mos general case ha can be suded as akes no accoun all he forces acng on. When he exernal loads

More information

Variants of Pegasos. December 11, 2009

Variants of Pegasos. December 11, 2009 Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on

More information

Chapters 2 Kinematics. Position, Distance, Displacement

Chapters 2 Kinematics. Position, Distance, Displacement Chapers Knemacs Poson, Dsance, Dsplacemen Mechancs: Knemacs and Dynamcs. Knemacs deals wh moon, bu s no concerned wh he cause o moon. Dynamcs deals wh he relaonshp beween orce and moon. The word dsplacemen

More information

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!) i+1,q - [(! ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL The frs hng o es n wo-way ANOVA: Is here neracon? "No neracon" means: The man effecs model would f. Ths n urn means: In he neracon plo (wh A on he horzonal

More information

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria IOSR Journal of Mahemacs (IOSR-JM e-issn: 78-578, p-issn: 9-765X. Volume 0, Issue 4 Ver. IV (Jul-Aug. 04, PP 40-44 Mulple SolonSoluons for a (+-dmensonalhroa-sasuma shallow waer wave equaon UsngPanlevé-Bӓclund

More information

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model BGC1: Survval and even hsory analyss Oslo, March-May 212 Monday May 7h and Tuesday May 8h The addve regresson model Ørnulf Borgan Deparmen of Mahemacs Unversy of Oslo Oulne of program: Recapulaon Counng

More information

FTCS Solution to the Heat Equation

FTCS Solution to the Heat Equation FTCS Soluon o he Hea Equaon ME 448/548 Noes Gerald Reckenwald Porland Sae Unversy Deparmen of Mechancal Engneerng gerry@pdxedu ME 448/548: FTCS Soluon o he Hea Equaon Overvew Use he forward fne d erence

More information

ID-1193 STUDY ON IMPACT BEHAVIOR OF COMPOSITES USING THE FINITE ELEMENT METHOD INTRODUCTION

ID-1193 STUDY ON IMPACT BEHAVIOR OF COMPOSITES USING THE FINITE ELEMENT METHOD INTRODUCTION ID-1193 STUDY ON IMPACT BEHAVIOR OF COMPOSITES USING THE FINITE ELEMENT METHOD Volne Ta and Jonas de Carvalho Deparmen of Mechancal Engneerng, S. Carlos Engneerng School, Unversy of S. Paulo, Brazl SUMMARY:

More information

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany Herarchcal Markov Normal Mxure models wh Applcaons o Fnancal Asse Reurns Appendx: Proofs of Theorems and Condonal Poseror Dsrbuons John Geweke a and Gann Amsano b a Deparmens of Economcs and Sascs, Unversy

More information

5th International Conference on Advanced Design and Manufacturing Engineering (ICADME 2015)

5th International Conference on Advanced Design and Manufacturing Engineering (ICADME 2015) 5h Inernaonal onference on Advanced Desgn and Manufacurng Engneerng (IADME 5 The Falure Rae Expermenal Sudy of Specal N Machne Tool hunshan He, a, *, La Pan,b and Bng Hu 3,c,,3 ollege of Mechancal and

More information

Comb Filters. Comb Filters

Comb Filters. Comb Filters The smple flers dscussed so far are characered eher by a sngle passband and/or a sngle sopband There are applcaons where flers wh mulple passbands and sopbands are requred Thecomb fler s an example of

More information

Sampling Procedure of the Sum of two Binary Markov Process Realizations

Sampling Procedure of the Sum of two Binary Markov Process Realizations Samplng Procedure of he Sum of wo Bnary Markov Process Realzaons YURY GORITSKIY Dep. of Mahemacal Modelng of Moscow Power Insue (Techncal Unversy), Moscow, RUSSIA, E-mal: gorsky@yandex.ru VLADIMIR KAZAKOV

More information

Comparison of Differences between Power Means 1

Comparison of Differences between Power Means 1 In. Journal of Mah. Analyss, Vol. 7, 203, no., 5-55 Comparson of Dfferences beween Power Means Chang-An Tan, Guanghua Sh and Fe Zuo College of Mahemacs and Informaon Scence Henan Normal Unversy, 453007,

More information

Single-loop System Reliability-Based Design & Topology Optimization (SRBDO/SRBTO): A Matrix-based System Reliability (MSR) Method

Single-loop System Reliability-Based Design & Topology Optimization (SRBDO/SRBTO): A Matrix-based System Reliability (MSR) Method 10 h US Naonal Congress on Compuaonal Mechancs Columbus, Oho 16-19, 2009 Sngle-loop Sysem Relably-Based Desgn & Topology Opmzaon (SRBDO/SRBTO): A Marx-based Sysem Relably (MSR) Mehod Tam Nguyen, Junho

More information

Cubic Bezier Homotopy Function for Solving Exponential Equations

Cubic Bezier Homotopy Function for Solving Exponential Equations Penerb Journal of Advanced Research n Compung and Applcaons ISSN (onlne: 46-97 Vol. 4, No.. Pages -8, 6 omoopy Funcon for Solvng Eponenal Equaons S. S. Raml *,,. Mohamad Nor,a, N. S. Saharzan,b and M.

More information

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β SARAJEVO JOURNAL OF MATHEMATICS Vol.3 (15) (2007), 137 143 SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β M. A. K. BAIG AND RAYEES AHMAD DAR Absrac. In hs paper, we propose

More information

Available online at ScienceDirect. Procedia CIRP 56 (2016 )

Available online at   ScienceDirect. Procedia CIRP 56 (2016 ) Avalable onlne a www.scencedrec.com ScenceDrec Proceda CIRP 56 (6 ) 8 87 9h Inernaonal Conference on Dgal Enerprse Technology- DET6 Inellgen Manufacurng n he Knowledge Economy Era Revson of bearng faul

More information

Comprehensive Integrated Simulation and Optimization of LPP for EUV Lithography Devices

Comprehensive Integrated Simulation and Optimization of LPP for EUV Lithography Devices Comprehense Inegraed Smulaon and Opmaon of LPP for EUV Lhograph Deces A. Hassanen V. Su V. Moroo T. Su B. Rce (Inel) Fourh Inernaonal EUVL Smposum San Dego CA Noember 7-9 2005 Argonne Naonal Laboraor Offce

More information

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s Ordnary Dfferenal Equaons n Neuroscence wh Malab eamples. Am - Gan undersandng of how o se up and solve ODE s Am Undersand how o se up an solve a smple eample of he Hebb rule n D Our goal a end of class

More information

Motion in Two Dimensions

Motion in Two Dimensions Phys 1 Chaper 4 Moon n Two Dmensons adzyubenko@csub.edu hp://www.csub.edu/~adzyubenko 005, 014 A. Dzyubenko 004 Brooks/Cole 1 Dsplacemen as a Vecor The poson of an objec s descrbed by s poson ecor, r The

More information

Numerical Definition of Indicators of the Development of Creeping Oil Layer on Values of Change of an Well Production

Numerical Definition of Indicators of the Development of Creeping Oil Layer on Values of Change of an Well Production Inernaonal Journal of Theorecal and Appled Mahemacs 7; 3(5: 67-73 hp://www.scencepublshnggroup.com//am do:.648/.am.735.3 ISSN: 575-57 (Prn; ISSN: 575-58 (Onlne Numercal Defnon of Indcaors of he Developmen

More information

Lecture 9: Dynamic Properties

Lecture 9: Dynamic Properties Shor Course on Molecular Dynamcs Smulaon Lecure 9: Dynamc Properes Professor A. Marn Purdue Unversy Hgh Level Course Oulne 1. MD Bascs. Poenal Energy Funcons 3. Inegraon Algorhms 4. Temperaure Conrol 5.

More information

Kelvin Viscoelasticity and Lagrange Multipliers Applied to the Simulation of Nonlinear Structural Vibration Control

Kelvin Viscoelasticity and Lagrange Multipliers Applied to the Simulation of Nonlinear Structural Vibration Control 964 Kelvn Vscoelascy and Lagrange Mulplers Appled o he Smulaon of Nonlnear Srucural Vbraon Conrol Absrac Ths sudy proposes a new pure numercal way o model mass / sprng / damper devces o conrol he vbraon

More information

Introduction to. Computer Animation

Introduction to. Computer Animation Inroducon o 1 Movaon Anmaon from anma (la.) = soul, spr, breah of lfe Brng mages o lfe! Examples Characer anmaon (humans, anmals) Secondary moon (har, cloh) Physcal world (rgd bodes, waer, fre) 2 2 Anmaon

More information

TSS = SST + SSE An orthogonal partition of the total SS

TSS = SST + SSE An orthogonal partition of the total SS ANOVA: Topc 4. Orhogonal conrass [ST&D p. 183] H 0 : µ 1 = µ =... = µ H 1 : The mean of a leas one reamen group s dfferen To es hs hypohess, a basc ANOVA allocaes he varaon among reamen means (SST) equally

More information

Scattering at an Interface: Oblique Incidence

Scattering at an Interface: Oblique Incidence Course Insrucor Dr. Raymond C. Rumpf Offce: A 337 Phone: (915) 747 6958 E Mal: rcrumpf@uep.edu EE 4347 Appled Elecromagnecs Topc 3g Scaerng a an Inerface: Oblque Incdence Scaerng These Oblque noes may

More information

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading Onlne Supplemen for Dynamc Mul-Technology Producon-Invenory Problem wh Emssons Tradng by We Zhang Zhongsheng Hua Yu Xa and Baofeng Huo Proof of Lemma For any ( qr ) Θ s easy o verfy ha he lnear programmng

More information

Bernoulli process with 282 ky periodicity is detected in the R-N reversals of the earth s magnetic field

Bernoulli process with 282 ky periodicity is detected in the R-N reversals of the earth s magnetic field Submed o: Suden Essay Awards n Magnecs Bernoull process wh 8 ky perodcy s deeced n he R-N reversals of he earh s magnec feld Jozsef Gara Deparmen of Earh Scences Florda Inernaonal Unversy Unversy Park,

More information

Let s treat the problem of the response of a system to an applied external force. Again,

Let s treat the problem of the response of a system to an applied external force. Again, Page 33 QUANTUM LNEAR RESPONSE FUNCTON Le s rea he problem of he response of a sysem o an appled exernal force. Agan, H() H f () A H + V () Exernal agen acng on nernal varable Hamlonan for equlbrum sysem

More information

This document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore.

This document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore. Ths documen s downloaded from DR-NTU, Nanyang Technologcal Unversy Lbrary, Sngapore. Tle A smplfed verb machng algorhm for word paron n vsual speech processng( Acceped verson ) Auhor(s) Foo, Say We; Yong,

More information

PHYS 1443 Section 001 Lecture #4

PHYS 1443 Section 001 Lecture #4 PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law

More information

Density Matrix Description of NMR BCMB/CHEM 8190

Density Matrix Description of NMR BCMB/CHEM 8190 Densy Marx Descrpon of NMR BCMBCHEM 89 Operaors n Marx Noaon If we say wh one bass se, properes vary only because of changes n he coeffcens weghng each bass se funcon x = h< Ix > - hs s how we calculae

More information

Solution in semi infinite diffusion couples (error function analysis)

Solution in semi infinite diffusion couples (error function analysis) Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of

More information

EVALUATION OF FORCE COEFFICIENTS FOR A 2-D ANGLE SECTION USING REALIZABLE k-ε TURBULENCE MODEL

EVALUATION OF FORCE COEFFICIENTS FOR A 2-D ANGLE SECTION USING REALIZABLE k-ε TURBULENCE MODEL The Sevenh Asa-Pacfc Conference on Wnd Engneerng, November 8-, 009, Tape, Tawan EVALUATION OF FORCE COEFFICIENTS FOR A -D ANGLE SECTION USING REALIZABLE k-ε TURBULENCE MODEL S. Chra Ganapah, P. Harkrshna,

More information

Notes on the stability of dynamic systems and the use of Eigen Values.

Notes on the stability of dynamic systems and the use of Eigen Values. Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon

More information

Density Matrix Description of NMR BCMB/CHEM 8190

Density Matrix Description of NMR BCMB/CHEM 8190 Densy Marx Descrpon of NMR BCMBCHEM 89 Operaors n Marx Noaon Alernae approach o second order specra: ask abou x magnezaon nsead of energes and ranson probables. If we say wh one bass se, properes vary

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Lnear Response Theory: The connecon beween QFT and expermens 3.1. Basc conceps and deas Q: ow do we measure he conducvy of a meal? A: we frs nroduce a weak elecrc feld E, and hen measure

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ

More information

e-journal Reliability: Theory& Applications No 2 (Vol.2) Vyacheslav Abramov

e-journal Reliability: Theory& Applications No 2 (Vol.2) Vyacheslav Abramov June 7 e-ournal Relably: Theory& Applcaons No (Vol. CONFIDENCE INTERVALS ASSOCIATED WITH PERFORMANCE ANALYSIS OF SYMMETRIC LARGE CLOSED CLIENT/SERVER COMPUTER NETWORKS Absrac Vyacheslav Abramov School

More information

Survival Analysis and Reliability. A Note on the Mean Residual Life Function of a Parallel System

Survival Analysis and Reliability. A Note on the Mean Residual Life Function of a Parallel System Communcaons n Sascs Theory and Mehods, 34: 475 484, 2005 Copyrgh Taylor & Francs, Inc. ISSN: 0361-0926 prn/1532-415x onlne DOI: 10.1081/STA-200047430 Survval Analyss and Relably A Noe on he Mean Resdual

More information

Analysis And Evaluation of Econometric Time Series Models: Dynamic Transfer Function Approach

Analysis And Evaluation of Econometric Time Series Models: Dynamic Transfer Function Approach 1 Appeared n Proceedng of he 62 h Annual Sesson of he SLAAS (2006) pp 96. Analyss And Evaluaon of Economerc Tme Seres Models: Dynamc Transfer Funcon Approach T.M.J.A.COORAY Deparmen of Mahemacs Unversy

More information

Physical Simulation Using FEM, Modal Analysis and the Dynamic Equilibrium Equation

Physical Simulation Using FEM, Modal Analysis and the Dynamic Equilibrium Equation Physcal Smulaon Usng FEM, Modal Analyss and he Dynamc Equlbrum Equaon Paríca C. T. Gonçalves, Raquel R. Pnho, João Manuel R. S. Tavares Opcs and Expermenal Mechancs Laboraory - LOME, Mechancal Engneerng

More information

Shear Stress-Slip Model for Steel-CFRP Single-Lap Joints under Thermal Loading

Shear Stress-Slip Model for Steel-CFRP Single-Lap Joints under Thermal Loading Shear Sress-Slp Model for Seel-CFRP Sngle-Lap Jons under Thermal Loadng *Ank Agarwal 1), Eha Hamed 2) and Sephen J Foser 3) 1), 2), 3) Cenre for Infrasrucure Engneerng and Safey, School of Cvl and Envronmenal

More information

Numerical simulation of a solar chimney power plant in the southern region of Iran

Numerical simulation of a solar chimney power plant in the southern region of Iran Energy Equp. Sys./ Vol. 5/No.4/December 2017/ 431-437 Energy Equpmen and Sysems hp://energyequpsys.u.ac.r www.energyequpsys.com Numercal smulaon of a solar chmney power plan n he souhern regon of Iran

More information

Bandlimited channel. Intersymbol interference (ISI) This non-ideal communication channel is also called dispersive channel

Bandlimited channel. Intersymbol interference (ISI) This non-ideal communication channel is also called dispersive channel Inersymol nererence ISI ISI s a sgnal-dependen orm o nererence ha arses ecause o devaons n he requency response o a channel rom he deal channel. Example: Bandlmed channel Tme Doman Bandlmed channel Frequency

More information

12d Model. Civil and Surveying Software. Drainage Analysis Module Detention/Retention Basins. Owen Thornton BE (Mech), 12d Model Programmer

12d Model. Civil and Surveying Software. Drainage Analysis Module Detention/Retention Basins. Owen Thornton BE (Mech), 12d Model Programmer d Model Cvl and Surveyng Soware Dranage Analyss Module Deenon/Reenon Basns Owen Thornon BE (Mech), d Model Programmer owen.hornon@d.com 4 January 007 Revsed: 04 Aprl 007 9 February 008 (8Cp) Ths documen

More information

On computing differential transform of nonlinear non-autonomous functions and its applications

On computing differential transform of nonlinear non-autonomous functions and its applications On compung dfferenal ransform of nonlnear non-auonomous funcons and s applcaons Essam. R. El-Zahar, and Abdelhalm Ebad Deparmen of Mahemacs, Faculy of Scences and Humanes, Prnce Saam Bn Abdulazz Unversy,

More information

Chapter Lagrangian Interpolation

Chapter Lagrangian Interpolation Chaper 5.4 agrangan Inerpolaon Afer readng hs chaper you should be able o:. dere agrangan mehod of nerpolaon. sole problems usng agrangan mehod of nerpolaon and. use agrangan nerpolans o fnd deraes and

More information

LARGE SCALE THERMAL-SOLID COUPLING ANALYSIS USING INEXACT BALANCING DOMAIN DECOMPOSITION

LARGE SCALE THERMAL-SOLID COUPLING ANALYSIS USING INEXACT BALANCING DOMAIN DECOMPOSITION RAC Unversy Journal, vol. VI, no. & 2, 200, pp. -7 LARGE SCALE THERMAL-SOLID COUPLING ANALYSIS USING INEXACT ALANCING DOMAIN DECOMPOSITION Abul Mukd Mohammad Mukaddes Deparmen of Indusral and Producon

More information

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005 Dynamc Team Decson Theory EECS 558 Proec Shruvandana Sharma and Davd Shuman December 0, 005 Oulne Inroducon o Team Decson Theory Decomposon of he Dynamc Team Decson Problem Equvalence of Sac and Dynamc

More information

Robust and Accurate Cancer Classification with Gene Expression Profiling

Robust and Accurate Cancer Classification with Gene Expression Profiling Robus and Accurae Cancer Classfcaon wh Gene Expresson Proflng (Compuaonal ysems Bology, 2005) Auhor: Hafeng L, Keshu Zhang, ao Jang Oulne Background LDA (lnear dscrmnan analyss) and small sample sze problem

More information

Different kind of oscillation

Different kind of oscillation PhO 98 Theorecal Qeson.Elecrcy Problem (8 pons) Deren knd o oscllaon e s consder he elecrc crc n he gre, or whch mh, mh, nf, nf and kω. The swch K beng closed he crc s copled wh a sorce o alernang crren.

More information

APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC CORRECTION

APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC CORRECTION THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY Seres A OF THE ROMANIAN ACADEMY Volume 6 Number /5 pp 8 86 APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC

More information

NATIONAL UNIVERSITY OF SINGAPORE PC5202 ADVANCED STATISTICAL MECHANICS. (Semester II: AY ) Time Allowed: 2 Hours

NATIONAL UNIVERSITY OF SINGAPORE PC5202 ADVANCED STATISTICAL MECHANICS. (Semester II: AY ) Time Allowed: 2 Hours NATONAL UNVERSTY OF SNGAPORE PC5 ADVANCED STATSTCAL MECHANCS (Semeser : AY 1-13) Tme Allowed: Hours NSTRUCTONS TO CANDDATES 1. Ths examnaon paper conans 5 quesons and comprses 4 prned pages.. Answer all

More information

Fuzzy Set Theory in Modeling Uncertainty Data. via Interpolation Rational Bezier Surface Function

Fuzzy Set Theory in Modeling Uncertainty Data. via Interpolation Rational Bezier Surface Function Appled Mahemacal Scences, Vol. 7, 013, no. 45, 9 38 HIKARI Ld, www.m-hkar.com Fuzzy Se Theory n Modelng Uncerany Daa va Inerpolaon Raonal Bezer Surface Funcon Rozam Zakara Deparmen of Mahemacs, Faculy

More information

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes. umercal negraon of he dffuson equaon (I) Fne dfference mehod. Spaal screaon. Inernal nodes. R L V For hermal conducon le s dscree he spaal doman no small fne spans, =,,: Balance of parcles for an nernal

More information

Increasing the Probablility of Timely and Correct Message Delivery in Road Side Unit Based Vehicular Communcation

Increasing the Probablility of Timely and Correct Message Delivery in Road Side Unit Based Vehicular Communcation Halmsad Unversy For he Developmen of Organsaons Producs and Qualy of Lfe. Increasng he Probablly of Tmely and Correc Message Delvery n Road Sde Un Based Vehcular Communcaon Magnus Jonsson Krsna Kuner and

More information

. The geometric multiplicity is dim[ker( λi. number of linearly independent eigenvectors associated with this eigenvalue.

. The geometric multiplicity is dim[ker( λi. number of linearly independent eigenvectors associated with this eigenvalue. Lnear Algebra Lecure # Noes We connue wh he dscusson of egenvalues, egenvecors, and dagonalzably of marces We wan o know, n parcular wha condons wll assure ha a marx can be dagonalzed and wha he obsrucons

More information

RELATIONSHIP BETWEEN VOLATILITY AND TRADING VOLUME: THE CASE OF HSI STOCK RETURNS DATA

RELATIONSHIP BETWEEN VOLATILITY AND TRADING VOLUME: THE CASE OF HSI STOCK RETURNS DATA RELATIONSHIP BETWEEN VOLATILITY AND TRADING VOLUME: THE CASE OF HSI STOCK RETURNS DATA Mchaela Chocholaá Unversy of Economcs Braslava, Slovaka Inroducon (1) one of he characersc feaures of sock reurns

More information

Investigation of Sway, Roll and Yaw Motions of a Ship with Forward Speed: Numerical modeling for flared up conditions

Investigation of Sway, Roll and Yaw Motions of a Ship with Forward Speed: Numerical modeling for flared up conditions h Inernaonal onference on Hgh Performance Marne Vehcles 8- November usrala Invesgaon of Sway Roll and Yaw Moons of a Shp wh Forward Speed: Numercal modelng for flared up condons S.K. Das Inernaonal Insue

More information

Transient Numerical of Piston Wind in Subway Station. Haitao Bao

Transient Numerical of Piston Wind in Subway Station. Haitao Bao Appled Mechancs and Maerals Submed: 2014-07-20 ISSN: 1662-7482, Vols. 644-650, pp 467-470 Acceped: 2014-07-21 do:10.4028/www.scenfc.ne/amm.644-650.467 Onlne: 2014-09-22 2014 Trans Tech Publcaons, Swzerland

More information

TEMPERATURE-DEPENDENT VISCOELASTIC PROPERTIES OF UNIDIRECTIONAL COMPOSITE MATERIALS

TEMPERATURE-DEPENDENT VISCOELASTIC PROPERTIES OF UNIDIRECTIONAL COMPOSITE MATERIALS 6 INERNAIONAL CONFERENCE ON COMPOSIE MAERIALS EMPERAURE-DEPENDEN VISCOELASIC PROPERIES OF UNIDIRECIONAL COMPOSIE MAERIALS Shuan Lu, Fengzh Wang Deparmen of Engneerng Mechancs, Sae Key Laboraory of Srucural

More information

. The geometric multiplicity is dim[ker( λi. A )], i.e. the number of linearly independent eigenvectors associated with this eigenvalue.

. The geometric multiplicity is dim[ker( λi. A )], i.e. the number of linearly independent eigenvectors associated with this eigenvalue. Mah E-b Lecure #0 Noes We connue wh he dscusson of egenvalues, egenvecors, and dagonalzably of marces We wan o know, n parcular wha condons wll assure ha a marx can be dagonalzed and wha he obsrucons are

More information

National Exams December 2015 NOTES: 04-BS-13, Biology. 3 hours duration

National Exams December 2015 NOTES: 04-BS-13, Biology. 3 hours duration Naonal Exams December 205 04-BS-3 Bology 3 hours duraon NOTES: f doub exss as o he nerpreaon of any queson he canddae s urged o subm wh he answer paper a clear saemen of any assumpons made 2 Ths s a CLOSED

More information

Tools for Analysis of Accelerated Life and Degradation Test Data

Tools for Analysis of Accelerated Life and Degradation Test Data Acceleraed Sress Tesng and Relably Tools for Analyss of Acceleraed Lfe and Degradaon Tes Daa Presened by: Reuel Smh Unversy of Maryland College Park smhrc@umd.edu Sepember-5-6 Sepember 28-30 206, Pensacola

More information

2.1 Constitutive Theory

2.1 Constitutive Theory Secon.. Consuve Theory.. Consuve Equaons Governng Equaons The equaons governng he behavour of maerals are (n he spaal form) dρ v & ρ + ρdv v = + ρ = Conservaon of Mass (..a) d x σ j dv dvσ + b = ρ v& +

More information

A new concept for the contact at the interface of steel-concrete composite beams

A new concept for the contact at the interface of steel-concrete composite beams A new concep for he conac a he nerface of seel-concree compose beams Samy Guezoul, Anas Alhasaw To ce hs verson: Samy Guezoul, Anas Alhasaw. A new concep for he conac a he nerface of seelconcree compose

More information

EXPERIMENTAL VALIDATION OF A MULTIBODY DYNAMICS MODEL OF THE SUSPENSION SYSTEM OF A TRACKED VEHICLE

EXPERIMENTAL VALIDATION OF A MULTIBODY DYNAMICS MODEL OF THE SUSPENSION SYSTEM OF A TRACKED VEHICLE NDIA GROUND VEHICLE SYSTEMS ENGINEERING AND TECHNOLOGY SYMPOSIUM MODELING & SIMULATION, TESTING AND VALIDATION (MSTV) MINI-SYMPOSIUM AUGUST 9- DEARBORN, MICHIGAN EXPERIMENTAL VALIDATION OF A MULTIBODY

More information

LATTICE TOWER DYNAMIC PERFORMANCE UNDER HUMAN INDUCED DYNAMIC LOADING

LATTICE TOWER DYNAMIC PERFORMANCE UNDER HUMAN INDUCED DYNAMIC LOADING Inernaonal RASD Conference 0 h -3 July 03 Psa 3 LATTICE TOWER DYNAMIC PERFORMANCE UNDER HUMAN INDUCED DYNAMIC LOADING L. Gale *, I. Radnsh Deparmen of Srucural Engneerng Rga Techncal Unversy Azenes sr.

More information

Dynamics Analysis and Modeling of Rubber Belt in Large Mine Belt Conveyors

Dynamics Analysis and Modeling of Rubber Belt in Large Mine Belt Conveyors Sensors & Transducers Vol. 8 Issue 0 Ocober 04 pp. 0-8 Sensors & Transducers 04 by IFSA Publshng S. L. hp://www.sensorsporal.com Dynamcs Analyss and Modelng of Rubber Bel n Large Mne Bel Conveyors Gao

More information

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 9 h INTERNATIONAL CONGRESS ON ACOUSTICS MADRID -7 SEPTEMBER 7 SOUND INSULATION CHARACTERISTICS OF A MICROPERFORATED PANEL ITH A SUBDIVIDED AIR LAYER PACS:.55.T Toyoda Masahro ; Daj Takahash B Kyoo Unv.

More information

Chapter 6: AC Circuits

Chapter 6: AC Circuits Chaper 6: AC Crcus Chaper 6: Oulne Phasors and he AC Seady Sae AC Crcus A sable, lnear crcu operang n he seady sae wh snusodal excaon (.e., snusodal seady sae. Complee response forced response naural response.

More information