u 1 Figure 1 3D Solid Finite Elements
|
|
- Roxanne Fox
- 5 years ago
- Views:
Transcription
1 Sold Elemets he Fte Elemet Lbrary of the MIDAS Famly Programs cludes the follog Sold Elemets: - ode tetrahedro, -ode petahedro, ad -ode hexahedro sho Fg.. he fte elemet formulato of all elemet types s based o the soparametrc procedure (the elemet geometry ad dsplacemets are terpolated the same ay). Z Y X u u u u u u u u u u u u u u u u u u Fgure D Sold Fte Elemets he odal degrees of freedom (DOF s) are llustrated Fg.. he elemet geometry ad dsplacemet feld are defed terms of odal coordated ad DOF s by the follog fuctos: here u,, = dsplacemets drecto of global X, Y, Z axes, respectely, at th ode x, y, z = x, yz, coordates at x= f(,, ) x u = f(,, ) u = = y = f(,, ) y = f(,, ) u= fq = = z = f(,, ) z = f(,, ) = = th ode
2 f (, ), = terpolato fucto related to system of the elemet th arables,, + ),, = atural coordates of the th ode of the elemet = umber of odes elemet he odal terpolato fuctos f (,, ) are of the follog form: th ode ad defed the atural coordate ( +, +, ad For -ode tetrahedro elemet f ( + ) for =,, = ( + )( ) for= ( + )( )( ) for =, ( ) For -ode petahedro (edge) elemet f (,, ) ( + )( + ) for =, = ( + )( + )( + ) for =,,, For -ode hexahedro (brck) elemet f,, = for =,,,..., ( ) ( )( )( )
3 No, the stras at ay pot th elemet doma are expressed terms of odal dsplacemets as, u 0 0 x x 0 0 ε x y y ε y 0 0 u ε z z z = = ε γ u = du = dfq = Bq xy + 0 γ y x y x yz γ zx + 0 z y z y u + 0 x z z x here B = stra-dsplacemet matrx q = ector of odal dsplacemets he, the stress-stra relato become, σ = Dε = DBq here, D s the elastcty matrx defg mechacal propertes of the materal. For a lear sotropc materal D matrx takes the follog form: ν ν ν ν ν ν E ν 0 0 D = ( + ν)( ν ) ν Sym. 0 ν hch E = Youg modulus ν = Posso s rato
4 Accordgly, the stffess matrx ad force ectors for a typcal soparametrc D sold elemet are defed by the follog tegrals: K = B DB V dv p b = f bdω Ω here K V = stffess matrx = olume of the elemet p = B Dε dω 0 0 Ω A = surface area of the elemet p b = odal force ector due to dstrbuted body forces b p0 = odal force ector due to tal stra ε 0 Ω = rage of the tegrato So far e hae demostrated the stadard soparametrc formulato procedure, hch s detcal for all D solds elemets. It should be oted the -ode tetrahedro ad -ode edge elemets preseted here are fact the degeerated forms of the -ode hexahedro (brck). Formulato of these elemets by collapsg the -ode hexahedra allos ealuatg the aboe tegrals for all types of D sold elemets by use of the same stadard D umercal tegrato procedure, based o the Gauss-Legedre quadrature. hus the umercal tegrato formulas used for D elemets are: here: W l m = j= k= (,, ) (,, ) (,, ) K WW W B DB J = j k k k k k k k l m b = j k k k k k = j= k= (,, ) (,, ) (,, ) p WW W f b J k k l m 0 = WW jwk k k ε0 k k k k = j= k= (,, ) (,, ) (,, ) p B D J = eghtg factor of -th tegrato pot,, = atural coordates of -th tegrato pot (, j, k) J = determat of the Jacoba matrx l, m, = umber of tegrato pots drecto of,, ad, respectely. he approprate order of umercal tegrato ad correspodg locatos of tegrato pots used the D sold elemets are sho able bello.
5 able Gauss-Legedre Itegrato for D Sold Elemets Itegrato order Locato of tegrato pots 9 0 Here t should be oted that the compatble -ode hexahedro elemet based o stadard soparametrc formulato does ot produce accurate results may cases for both dsplacemets ad stresses. I order to mproe the performace of ths elemet are added so called the compatble dsplacemets modes. akg to accout the compatble modes, the dsplacemet feld s defed as, here, P, P, P u = f(,, ) u + αp + αp+ αp = = f(,, ) + αp + αp+ αp = = f(,, ) + αp + αp+ α9p = are the extra shape fuctos related to the compatble modes expressed as, ( ) ( ) ( ) P,, =, P,, = ad P,, = ad α ( =,,,...,9) are so called odeless extra DOF s. Note that the extra shape fuctos permt a parabolc deformato alog the elemet edge ad mproe the elemet stffess performace. Here t should be oted that the fal stffess matrx s obtaed by statc codesato of the
6 compatble modes the same ay as case of -ode quadrlateral D plae elemet.
Analysis of von Kármán plates using a BEM formulation
Boudary Elemets ad Other Mesh Reducto Methods XXIX 213 Aalyss of vo Kármá plates usg a BEM formulato L. Wademam & W. S. Vetur São Carlos School of Egeerg, Uversty of São Paulo, Brazl Abstract Ths work
More informationInstituto Tecnológico de Aeronáutica FINITE ELEMENTS I. Class notes AE-245
Isttto Tecológco de Aeroátca FIITE ELEETS I Class otes AE-45 Isttto Tecológco de Aeroátca 8. Beams ad Plates AE-45 Isttto Tecológco de Aeroátca BEAS AD PLATES Itrodcto Eler-Beroll beam model ad Krcoff
More informationChapter 2 - Free Vibration of Multi-Degree-of-Freedom Systems - II
CEE49b Chapter - Free Vbrato of Mult-Degree-of-Freedom Systems - II We ca obta a approxmate soluto to the fudametal atural frequecy through a approxmate formula developed usg eergy prcples by Lord Raylegh
More informationMMJ 1113 FINITE ELEMENT METHOD Introduction to PART I
MMJ FINITE EEMENT METHOD Cotut requremets Assume that the fuctos appearg uder the tegral the elemet equatos cota up to (r) th order To esure covergece N must satsf Compatblt requremet the fuctos must have
More informationANALYTICAL SOLUTION FOR NONLINEAR BENDING OF FG PLATES BY A LAYERWISE THEORY
6 TH ITERATIOAL COFERECE O COMPOSITE MATERIALS AALYTICAL SOLUTIO FOR OLIEAR BEDIG OF FG PLATES BY A LAYERWISE THEORY M. Taha*, S.M. Mrababaee** *Departmet of Mechacal Egeerg, Ferdows Uversty of Mashhad,
More informationNumerical Integration of Arbitrary Functions over a Convex and Non Convex Polygonal Domain by Eight Noded Linear Quadrilateral Finite Element Method
Australa Joural of Basc ad Appled Sceces, 10(16) ovember 016, Pages: 104-110 AUSTRALIA JOURAL OF BASI AD APPLIED SIEES ISS:1991-8178 EISS: 309-8414 Joural home page: www.abasweb.com umercal Itegrato of
More informationNumerical investigation on the failure mechanisms of. particulate composite material under a various loading
Fal report Numercal vestgato o the falure mechasms of partculate composte materal uder a varous loadg codtos usg a damage costtutve model P.I.: Hrosh Okada, Ph.D., Assocate Professor Address: Departmet
More informationSmoothed Finite Element Method
Smooted Fte Elemet Metod K.Y. DA ad G.R. LU, 2 Sgapore-MT Allace (SMA), E4-04-0, 4 Egeerg Drve, Sgapore, 7576 2 eter for Advaced omputatos Egeerg Scece (AES), Departmet of Mecacal Egeerg, Natoal Uversty
More informationThe hypersingular boundary element method revisited
Boudary Elemets ad Other Mesh Reducto Methods XXXVII 7 The hypersgular boudary elemet method revsted N. A. Dumot Cvl Egeerg Departmet, Potfcal Catholc Uversty of Ro de Jaero, Brazl Abstract Ths s the sequel
More informationAhmed Elgamal. MDOF Systems & Modal Analysis
DOF Systems & odal Aalyss odal Aalyss (hese otes cover sectos from Ch. 0, Dyamcs of Structures, Al Chopra, Pretce Hall, 995). Refereces Dyamcs of Structures, Al K. Chopra, Pretce Hall, New Jersey, ISBN
More informationA NEW FINITE ELEMENT CONSIDERING SHEAR LAG
Bullet of the raslvaa Uversty of Braşov CIBv 204 Vol. 7 (56) Specal Issue No. - 204 A NEW FINIE EEMEN CONSIDERING SHEAR AG A. PROIC M. VOJNIC PURCAR D. UIC Abstract: A ew model of descrbg the shear lag
More informationCS5620 Intro to Computer Graphics
CS56 Itro to Computer Graphcs Geometrc Modelg art II Geometrc Modelg II hyscal Sples Curve desg pre-computers Cubc Sples Stadard sple put set of pots { } =, No dervatves specfed as put Iterpolate by cubc
More informationTHE NEW OPTIMALITY CRITERIA FOR STRUCTURAL DESIGN WITH CONSTRAINING ELASTIC DISPLACEMENTS (NON-COMPOSITE FORWARD SWEPT WING WITHOUT DIVERGENCE)
8 TH INTRNATIONAL CONGRSS OF TH ARONAUTICAL SCINCS TH NW OPTIMALITY CRITRIA FOR STRUCTURAL DSIGN WITH CONSTRAINING LASTIC DISPLACMNTS (NON-COMPOSIT FORWARD SWPT WING WITHOUT DIVRGNC) Alexader I Dal, Samara
More informationComparison of Analytical and Numerical Results in Modal Analysis of Multispan Continuous Beams with LS-DYNA
th Iteratoal S-N Users oferece Smulato Techology omparso of alytcal ad Numercal Results Modal alyss of Multspa otuous eams wth S-N bht Mahapatra ad vk hatteree etral Mechacal Egeerg Research Isttute, urgapur
More informationMethodology of design of wind turbine tower structures
3 rd Jot Iteratal Coferece O Rome/Italy Methodology of desg of wd turbe tower structures Avelo Alves Flho Lcol Sadao Mazaka Cha Abstract he preset work aalyzes the methodology of desg of wd turbe tower
More informationL5 Polynomial / Spline Curves
L5 Polyomal / Sple Curves Cotets Coc sectos Polyomal Curves Hermte Curves Bezer Curves B-Sples No-Uform Ratoal B-Sples (NURBS) Mapulato ad Represetato of Curves Types of Curve Equatos Implct: Descrbe a
More information( q Modal Analysis. Eigenvectors = Mode Shapes? Eigenproblem (cont) = x x 2 u 2. u 1. x 1 (4.55) vector and M and K are matrices.
4.3 - Modal Aalyss Physcal coordates are ot always the easest to work Egevectors provde a coveet trasformato to modal coordates Modal coordates are lear combato of physcal coordates Say we have physcal
More informationEPM RT HYBRID FINITE ELEMENT METHOD APPLIED TO THE ANALYSIS OF FREE VIBRATION OF SPHERICAL SHELL
EPM T 03-0 HYBID FINITE ELEMENT METHOD APPLIED TO THE ANALYSIS OF FEE VIBATION OF SPHEICAL SHELL M. Meaa, A.A. Laks Départemet de Gée mécaque École Polytechque de Motréal Avrl 03 EPM-T-03-0 HYBID FINITE
More informationDivision of Materials Science, Graduate School of Science and Engineering, Saitama University, Saitama, Japan
CHECKERBOARD PROBLEM TO TOPOLOGY OPTIMIZATIO OF COTIUUM STRUCTURES Ju-ch Koga, Jro Koga ad Shu Homma Dvso of Materals Scece, Graduate School of Scece ad Egeerg, Satama Uversty, Satama, 338-8570 Japa Keywords:
More informationA Method for Damping Estimation Based On Least Square Fit
Amerca Joural of Egeerg Research (AJER) 5 Amerca Joural of Egeerg Research (AJER) e-issn: 3-847 p-issn : 3-936 Volume-4, Issue-7, pp-5-9 www.ajer.org Research Paper Ope Access A Method for Dampg Estmato
More informationDIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS
DIFFERENTIAL GEOMETRIC APPROACH TO HAMILTONIAN MECHANICS Course Project: Classcal Mechacs (PHY 40) Suja Dabholkar (Y430) Sul Yeshwath (Y444). Itroducto Hamltoa mechacs s geometry phase space. It deals
More informationApplication of Legendre Bernstein basis transformations to degree elevation and degree reduction
Computer Aded Geometrc Desg 9 79 78 www.elsever.com/locate/cagd Applcato of Legedre Berste bass trasformatos to degree elevato ad degree reducto Byug-Gook Lee a Yubeom Park b Jaechl Yoo c a Dvso of Iteret
More informationStochastic Finite Element Based on Stochastic Linearization for Stochastic Nonlinear Ordinary Differential Equations with Random coefficients
Proc. of the 5th WSEAS It. Cof. o No-Lear Aalyss, No-Lear Systems ad Chaos, Bucharest, Romaa, October 6-8, 6 Stochastc Fte Elemet Based o Stochastc Learzato for Stochastc Nolear Ordary Dfferetal Equatos
More informationCS475 Parallel Programming
CS475 Parallel Programmg Deretato ad Itegrato Wm Bohm Colorado State Uversty Ecept as otherwse oted, the cotet o ths presetato s lcesed uder the Creatve Commos Attrbuto.5 lcese. Pheomea Physcs: heat, low,
More informationAN EULER-MC LAURIN FORMULA FOR INFINITE DIMENSIONAL SPACES
AN EULER-MC LAURIN FORMULA FOR INFINITE DIMENSIONAL SPACES Jose Javer Garca Moreta Graduate Studet of Physcs ( Sold State ) at UPV/EHU Address: P.O 6 890 Portugalete, Vzcaya (Spa) Phoe: (00) 3 685 77 16
More informationDerivation of 3-Point Block Method Formula for Solving First Order Stiff Ordinary Differential Equations
Dervato of -Pot Block Method Formula for Solvg Frst Order Stff Ordary Dfferetal Equatos Kharul Hamd Kharul Auar, Kharl Iskadar Othma, Zara Bb Ibrahm Abstract Dervato of pot block method formula wth costat
More informationLecture 07: Poles and Zeros
Lecture 07: Poles ad Zeros Defto of poles ad zeros The trasfer fucto provdes a bass for determg mportat system respose characterstcs wthout solvg the complete dfferetal equato. As defed, the trasfer fucto
More informationBezier curve and its application
, 49-55 Receved: 2014-11-12 Accepted: 2015-02-06 Ole publshed: 2015-11-16 DOI: http://dx.do.org/10.15414/meraa.2015.01.02.49-55 Orgal paper Bezer curve ad ts applcato Duša Páleš, Jozef Rédl Slovak Uversty
More informationα1 α2 Simplex and Rectangle Elements Multi-index Notation of polynomials of degree Definition: The set P k will be the set of all functions:
Smplex ad Rectagle Elemets Mult-dex Notato = (,..., ), o-egatve tegers = = β = ( β,..., β ) the + β = ( + β,..., + β ) + x = x x x x = x x β β + D = D = D D x x x β β Defto: The set P of polyomals of degree
More informationHarley Flanders Differential Forms with Applications to the Physical Sciences. Dover, 1989 (1962) Contents FOREWORD
Harley Fladers Dfferetal Forms wth Applcatos to the Physcal Sceces FORWORD Dover, 989 (962) Cotets PRFAC TO TH DOVR DITION PRFAC TO TH FIRST DITION.. xteror Dfferetal Forms.2. Comparso wth Tesors 2.. The
More informationThe numerical tool for a posteriori detection of boundary layers in hp-adaptive analysis
The umercal tool for a posteror detecto of boudary layers hp-adaptve aalyss ukasz Mazo ad Grzegorz Zbosk, Faculty of Techcal Sceces, Uversty of Warma ad Mazury ul.oczapowskego ; -79 Olszty, Polad e-mal:
More information1 Lyapunov Stability Theory
Lyapuov Stablty heory I ths secto we cosder proofs of stablty of equlbra of autoomous systems. hs s stadard theory for olear systems, ad oe of the most mportat tools the aalyss of olear systems. It may
More informationCHAPTER VI Statistical Analysis of Experimental Data
Chapter VI Statstcal Aalyss of Expermetal Data CHAPTER VI Statstcal Aalyss of Expermetal Data Measuremets do ot lead to a uque value. Ths s a result of the multtude of errors (maly radom errors) that ca
More informationThe solution of Euler-Bernoulli beams using variational derivative method
Scetfc Research ad Essays Vol. 5(9), pp. 9-4, 4 May Avalable ole at http://www.academcjourals.org/sre ISSN 99-48 Academc Jourals Full egth Research Paper The soluto of Euler-Beroull beams usg varatoal
More informationIntegral Equation Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, Xin Wang and Karen Veroy
Itroducto to Smulato - Lecture 22 Itegral Equato ethods Jacob Whte Thaks to Deepak Ramaswamy, chal Rewesk, X Wag ad Kare Veroy Outle Itegral Equato ethods Exteror versus teror problems Start wth usg pot
More informationA NEW FINITE ELEMENT CONSIDERING SHEAR LAG
INERNAIONA SCIENIFIC CONFERENCE CIBV 204 7-8 November 204, Braşov A NEW FINIE EEMEN CONSIDERING SHEAR AG A. PROIC M. VOJNIC PURCAR D. UIC Abstract: A ew model of descrbg the shear lag pheomeo composte
More informationAn Adaptive Meshless Method for Modeling Large Mechanical Deformation and Contacts
2007 IEEE Iteratoal Coferece o Robotcs ad Automato Roma, Italy, 0-4 Aprl 2007 WeD7. A Adaptve Meshless Method for Modelg Large Mechacal Deformato ad Cotacts Qag L ad Kok-Meg Lee*, Fellow, IEEE Abstract-
More informationA MLPG Meshless Method for Numerical Simulaton of Unsteady Incompressible Flows
Joural of Appled Flud Mechacs, Vol. x, No. x, pp. x-x, 00x. Avalable ole at www.afmole.et, ISSN 735-3645. A MLPG Meshless Method for Numercal Smulato of Usteady Icompressble Flows Ira Saeedpaah Assstat
More informationON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS
ON THE MOTION OF PLANAR BARS SYSTEMS WITH CLEARANCES IN JOINTS Şl uv dr g Ja-Crsta GRIGORE, Uverstatea d Pteşt, strtîrgu dvale Nr Prof uv dr g Ncolae PANDREA, Uverstatea d Pteşt, strtîrgu dvale Nr Cof
More informationOPTIMIZATION FORMULATION FOR NONLINEAR STRUCTURAL ANALYSIS
INTERNATIONAL JOURNAL OF OPTIMIZATION IN CIVIL ENGINEERING It. J. Optm. Cvl Eg., 2017; 7(1):109-127 Dowloaded from joce.ust.ac.r at 7:24 IRDT o Saturday July 7th 2018 OPTIMIZATION FORMULATION FOR NONLINEAR
More informationB-spline curves. 1. Properties of the B-spline curve. control of the curve shape as opposed to global control by using a special set of blending
B-sple crve Copyrght@, YZU Optmal Desg Laboratory. All rghts reserved. Last pdated: Yeh-Lag Hs (--9). ote: Ths s the corse materal for ME Geometrc modelg ad compter graphcs, Ya Ze Uversty. art of ths materal
More informationModeling and analysis of waves in a heat conducting thermo-elastic plate of elliptical shape
589 Modelg ad aalyss of waves a heat coductg thermo-elastc plate of ellptcal shape Abstract Wave propagato heat coductg thermo elastc plate of ellptcal cross-secto s studed usg the Fourer expaso collocato
More informationENGI 4421 Joint Probability Distributions Page Joint Probability Distributions [Navidi sections 2.5 and 2.6; Devore sections
ENGI 441 Jot Probablty Dstrbutos Page 7-01 Jot Probablty Dstrbutos [Navd sectos.5 ad.6; Devore sectos 5.1-5.] The jot probablty mass fucto of two dscrete radom quattes, s, P ad p x y x y The margal probablty
More informationPRACTICAL CONSIDERATIONS IN HUMAN-INDUCED VIBRATION
PRACTICAL CONSIDERATIONS IN HUMAN-INDUCED VIBRATION Bars Erkus, 4 March 007 Itroducto Ths docuet provdes a revew of fudaetal cocepts structural dyacs ad soe applcatos hua-duced vbrato aalyss ad tgato of
More informationTHREE-DIMENSIONAL POROELASTIC SIMULATION OF HYDRAULIC AND NATURAL FRACTURES USING THE DISPLACEMENT DISCONTINUITY METHOD
PROCEEDINGS, Thrty-Fourth Workshop o Geothermal Reservor Egeerg Staford Uversty, Staford, Calfora, February 9-11, 9 SGP-TR-187 THREE-DIMENSIONAL POROELASTIC SIMULATION OF HYDRAULIC AND NATURAL FRACTURES
More information2. Independence and Bernoulli Trials
. Ideedece ad Beroull Trals Ideedece: Evets ad B are deedet f B B. - It s easy to show that, B deedet mles, B;, B are all deedet ars. For examle, ad so that B or B B B B B φ,.e., ad B are deedet evets.,
More information( ) = ( ) ( ) Chapter 13 Asymptotic Theory and Stochastic Regressors. Stochastic regressors model
Chapter 3 Asmptotc Theor ad Stochastc Regressors The ature of eplaator varable s assumed to be o-stochastc or fed repeated samples a regresso aalss Such a assumpto s approprate for those epermets whch
More informationCOMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL
Sebasta Starz COMPROMISE HYPERSPHERE FOR STOCHASTIC DOMINANCE MODEL Abstract The am of the work s to preset a method of rakg a fte set of dscrete radom varables. The proposed method s based o two approaches:
More informationUpdated frequency domain analysis in LS-DYNA
Updated frequecy doma aalyss LS-DYNA Yu Huag, Zhe Cu Lvermore Software Techology Corporato 1 Overvew A seres of frequecy doma features have bee mplemeted to LS-DYNA sce verso 971 R6. These features ca
More informationONE GENERALIZED INEQUALITY FOR CONVEX FUNCTIONS ON THE TRIANGLE
Joural of Pure ad Appled Mathematcs: Advaces ad Applcatos Volume 4 Number 205 Pages 77-87 Avalable at http://scetfcadvaces.co. DOI: http://.do.org/0.8642/jpamaa_7002534 ONE GENERALIZED INEQUALITY FOR CONVEX
More informationLaw of Large Numbers
Toss a co tmes. Law of Large Numbers Suppose 0 f f th th toss came up H toss came up T s are Beroull radom varables wth p ½ ad E( ) ½. The proporto of heads s. Itutvely approaches ½ as. week 2 Markov s
More informationUPPER BOUND LIMIT ANALYSIS OF SOIL SLOPE STABILITY BASED ON RPIM MESHLESS METHOD
he 5th Cross-strat Coferece o Structural ad Geotechcal Egeerg (SGE-5) Hog Kog, Cha, 13-15 July 011 UPPER BOUND LM ANALYSS OF SOL SLOPE SABLY BASED ON RPM MESHLESS MEHOD F.. Lu 1, J. D. Zhao 1, Y. F. Fa,
More informationSpecial Instructions / Useful Data
JAM 6 Set of all real umbers P A..d. B, p Posso Specal Istructos / Useful Data x,, :,,, x x Probablty of a evet A Idepedetly ad detcally dstrbuted Bomal dstrbuto wth parameters ad p Posso dstrbuto wth
More informationCohesive zone models towards a robust implementation of irreversible behaviour
Cohesve zoe models towards a robust mplemetato of rreversble behavour Reé Kregtg rd February 5 MT5. Supervso: dr.r. O. va der Slus (Phlps Appled Techloges) dr.r. R.H.J. Peerlgs prof.dr.r. M.G.D. Geers
More informationCAD-based approach for identification of elasto-static parameters of robotic manipulators
A. Klmchk, A. Pashkevch, D. Chablat, CAD-based approach for detfcato of elasto-statc parameters of robotc mapulators 1 CAD-based approach for detfcato of elasto-statc parameters of robotc mapulators Alexadr
More informationLecture Notes Types of economic variables
Lecture Notes 3 1. Types of ecoomc varables () Cotuous varable takes o a cotuum the sample space, such as all pots o a le or all real umbers Example: GDP, Polluto cocetrato, etc. () Dscrete varables fte
More informationGLOBAL PROBABILISTIC SEISMIC CAPACITY ANALYSIS OF STRUCTURES THROUGH STOCHASTIC PUSHOVER ANALYSIS
The 4 th World oferece o Earthquae Egeerg October -7, 008, Beg, ha GLOBAL PROBABILISTI SEISMI APAITY ANALYSIS OF STRUTURES THROUGH STOHASTI PUSHOVER ANALYSIS Xao-Hu Yu, Da-Gag Lu, Peg-Ya Sog 3, Guag-Yua
More informationInvestigating Cellular Automata
Researcher: Taylor Dupuy Advsor: Aaro Wootto Semester: Fall 4 Ivestgatg Cellular Automata A Overvew of Cellular Automata: Cellular Automata are smple computer programs that geerate rows of black ad whte
More informationA Review on Attempts towards CAD/CAE Integration Using Macroelements
Computatoal Research (3): 6-84, 3 DOI:.389/cr.3.3 http://www.hrpub.org A Revew o Attempts towards CAD/CAE Itegrato Usg Macroelemets Chrstopher Provatds Natoal Techcal Uversty of Athes, Greece *Correspodg
More informationEngineering Vibration 1. Introduction
Egeerg Vbrato. Itroducto he study of the moto of physcal systems resultg from the appled forces s referred to as dyamcs. Oe type of dyamcs of physcal systems s vbrato, whch the system oscllates about certa
More information4 Inner Product Spaces
11.MH1 LINEAR ALGEBRA Summary Notes 4 Ier Product Spaces Ier product s the abstracto to geeral vector spaces of the famlar dea of the scalar product of two vectors or 3. I what follows, keep these key
More informationd dt d d dt dt Also recall that by Taylor series, / 2 (enables use of sin instead of cos-see p.27 of A&F) dsin
Learzato of the Swg Equato We wll cover sectos.5.-.6 ad begg of Secto 3.3 these otes. 1. Sgle mache-fte bus case Cosder a sgle mache coected to a fte bus, as show Fg. 1 below. E y1 V=1./_ Fg. 1 The admttace
More informationDynamic Analysis of Axially Beam on Visco - Elastic Foundation with Elastic Supports under Moving Load
Dyamc Aalyss of Axally Beam o Vsco - Elastc Foudato wth Elastc Supports uder Movg oad Saeed Mohammadzadeh, Seyed Al Mosayeb * Abstract: For dyamc aalyses of ralway track structures, the algorthm of soluto
More informationSTK3100 and STK4100 Autumn 2018
SK3 ad SK4 Autum 8 Geeralzed lear models Part III Covers the followg materal from chaters 4 ad 5: Cofdece tervals by vertg tests Cosder a model wth a sgle arameter β We may obta a ( α% cofdece terval for
More informationTESTS BASED ON MAXIMUM LIKELIHOOD
ESE 5 Toy E. Smth. The Basc Example. TESTS BASED ON MAXIMUM LIKELIHOOD To llustrate the propertes of maxmum lkelhood estmates ad tests, we cosder the smplest possble case of estmatg the mea of the ormal
More informationExtreme Value Theory: An Introduction
(correcto d Extreme Value Theory: A Itroducto by Laures de Haa ad Aa Ferrera Wth ths webpage the authors ted to form the readers of errors or mstakes foud the book after publcato. We also gve extesos for
More information2C09 Design for seismic and climate changes
2C09 Desg for sesmc ad clmate chages Lecture 08: Sesmc aalyss of elastc MDOF systems Aurel Strata, Poltehca Uversty of Tmsoara 06/04/2017 Europea Erasmus Mudus Master Course Sustaable Costructos uder atural
More informationThird handout: On the Gini Index
Thrd hadout: O the dex Corrado, a tala statstca, proposed (, 9, 96) to measure absolute equalt va the mea dfferece whch s defed as ( / ) where refers to the total umber of dvduals socet. Assume that. The
More informationChapter 4 Multiple Random Variables
Revew o BST 63: Statstcal Theory I Ku Zhag, /0/008 Revew for Chapter 4-5 Notes: Although all deftos ad theorems troduced our lectures ad ths ote are mportat ad you should be famlar wth, but I put those
More informationCubic Nonpolynomial Spline Approach to the Solution of a Second Order Two-Point Boundary Value Problem
Joural of Amerca Scece ;6( Cubc Nopolyomal Sple Approach to the Soluto of a Secod Order Two-Pot Boudary Value Problem W.K. Zahra, F.A. Abd El-Salam, A.A. El-Sabbagh ad Z.A. ZAk * Departmet of Egeerg athematcs
More informationManipulator Dynamics. Amirkabir University of Technology Computer Engineering & Information Technology Department
Mapulator Dyamcs mrkabr Uversty of echology omputer Egeerg formato echology Departmet troducto obot arm dyamcs deals wth the mathematcal formulatos of the equatos of robot arm moto. hey are useful as:
More informationThe Application of hybrid BEM/FEM methods to solve Electrical Impedance Tomography s forward problem for the human head
The Applcato of hybrd / methods to solve Electrcal Impedace Tomography s forward problem for the huma head S.R. Arrdge, R.H. ayford, L. Horesh ad J. Skora March, Abstract The forward problem Electrcal
More informationNonlinear frequency response analysis of structural vibrations
Comput Mech mauscrpt No. (wll be serted by the edtor) Nolear frequecy respose aalyss of structural vbratos O. Weeger U. Wever B. Smeo Receved: date / Accepted: date Abstract I ths paper we preset a method
More informationTransactions, SMiRT-23 Manchester, United Kingdom - August 10-14, 2015 Division V, Paper ID 703
Trasactos, SMRT-23 Machester, Uted Kgdom - August 10-14, 2015 Dvso V, Paper ID 703 SOIL-STRUCTURE INTERACTION UNDER STATIC LOADS ACCOUNTING FOR THE EFFECT OF ADJACENT BUILDINGS: DEFINITION AND USE OF A
More informationStress Wave propagation in Electro-Magneto-Elastic plate of arbitrary cross-sections
Iteratoal Joural of Scetfc & Egeerg Research Volume 3, Issue 8, August-1 1 ISSN 9-5518 Stress Wave propagato Electro-Mageto-Elastc plate of arbtrary cross-sectos P. Pousamy Departmet of Mathematcs Govermet
More informationModule 7: Probability and Statistics
Lecture 4: Goodess of ft tests. Itroducto Module 7: Probablty ad Statstcs I the prevous two lectures, the cocepts, steps ad applcatos of Hypotheses testg were dscussed. Hypotheses testg may be used to
More informationDEVELOPMENT OF FLUID-SEDIMENT-SEABED INTERACTION MODEL AND ITS APPLICATION. Tomoaki Nakamura 1 and Norimi Mizutani 1
DEVELOPMENT OF FLUID-SEDIMENT-SEABED INTERACTION MODEL AND ITS APPLICATION Tomoak Nakamura 1 ad Norm Mzuta 1 To provde a computatoal framework for smulatg flud-sedmet-seabed teractos, a three-dmesoal coupled
More informationPhysics 114 Exam 2 Fall Name:
Physcs 114 Exam Fall 015 Name: For gradg purposes (do ot wrte here): Questo 1. 1... 3. 3. Problem Aswer each of the followg questos. Pots for each questo are dcated red. Uless otherwse dcated, the amout
More informationThe number of observed cases The number of parameters. ith case of the dichotomous dependent variable. the ith case of the jth parameter
LOGISTIC REGRESSION Notato Model Logstc regresso regresses a dchotomous depedet varable o a set of depedet varables. Several methods are mplemeted for selectg the depedet varables. The followg otato s
More informationAn Expansion of the Derivation of the Spline Smoothing Theory Alan Kaylor Cline
A Epaso of the Derato of the Sple Smoothg heory Ala Kaylor Cle he classc paper "Smoothg by Sple Fctos", Nmersche Mathematk 0, 77-83 967) by Chrsta Resch showed that atral cbc sples were the soltos to a
More informationFREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM
Joural of Appled Matematcs ad Computatoal Mecacs 04, 3(4), 7-34 FREQUENCY ANALYSIS OF A DOUBLE-WALLED NANOTUBES SYSTEM Ata Cekot, Stasław Kukla Isttute of Matematcs, Czestocowa Uversty of Tecology Częstocowa,
More informationA Method for Determining the Number of Dependent Constraints Using Transformation Parameters of Coordinate Systems Korganbay Sholanov1, a*
Iteratoal Coferece o Mechacs, Materals ad Structural Egeerg (ICMMSE 206) A Method for Determg the Number of Depedet Costrats Usg Trasformato Parameters of Coordate Systems Korgabay Sholaov, a* Karagada
More informationSeismic Soil-Structure Interaction Including Non-Synchronous Motion Effects for Structures with Torsional Eccentricities
Sesmc Sol-Structure Iteracto Icludg No-Sychroous Moto Effects for Structures wth Torsoal Eccetrctes a M. Ghocel, Ph.. Advaced Computatoal Software Ic., New York, USA dgho@aol.com ABSTRACT The paper addresses
More informationSTK3100 and STK4100 Autumn 2017
SK3 ad SK4 Autum 7 Geeralzed lear models Part III Covers the followg materal from chaters 4 ad 5: Sectos 4..5, 4.3.5, 4.3.6, 4.4., 4.4., ad 4.4.3 Sectos 5.., 5.., ad 5.5. Ørulf Borga Deartmet of Mathematcs
More informationFunctions of Random Variables
Fuctos of Radom Varables Chapter Fve Fuctos of Radom Varables 5. Itroducto A geeral egeerg aalyss model s show Fg. 5.. The model output (respose) cotas the performaces of a system or product, such as weght,
More informationLecture 12 APPROXIMATION OF FIRST ORDER DERIVATIVES
FDM: Appromato of Frst Order Dervatves Lecture APPROXIMATION OF FIRST ORDER DERIVATIVES. INTRODUCTION Covectve term coservato equatos volve frst order dervatves. The smplest possble approach for dscretzato
More information13. Parametric and Non-Parametric Uncertainties, Radial Basis Functions and Neural Network Approximations
Lecture 7 3. Parametrc ad No-Parametrc Ucertates, Radal Bass Fuctos ad Neural Network Approxmatos he parameter estmato algorthms descrbed prevous sectos were based o the assumpto that the system ucertates
More informationUnit 9. The Tangent Bundle
Ut 9. The Taget Budle ========================================================================================== ---------- The taget sace of a submafold of R, detfcato of taget vectors wth dervatos at
More informationBuckling Analysis of Polar Orthotropic Circular and Annular Plates of Uniform and Linearly Varying Thickness with Different Edge Conditions
Joural of Sold Mechacs Vol., No. (00 pp. 56-67 Bucklg Aalyss of Polar Orthotropc Crcular ad Aular Plates of Uform ad Learly Varyg Thckess wth Dfferet Edge Codtos F. Farhata,*, A. Golshah Mechacal Egeerg
More informationCH E 374 Computational Methods in Engineering Fall 2007
CH E 7 Computatoal Methods Egeerg Fall 007 Sample Soluto 5. The data o the varato of the rato of stagato pressure to statc pressure (r ) wth Mach umber ( M ) for the flow through a duct are as follows:
More informationC-1: Aerodynamics of Airfoils 1 C-2: Aerodynamics of Airfoils 2 C-3: Panel Methods C-4: Thin Airfoil Theory
ROAD MAP... AE301 Aerodyamcs I UNIT C: 2-D Arfols C-1: Aerodyamcs of Arfols 1 C-2: Aerodyamcs of Arfols 2 C-3: Pael Methods C-4: Th Arfol Theory AE301 Aerodyamcs I Ut C-3: Lst of Subects Problem Solutos?
More informationHUYGENS S ENVELOPING-WAVE PRINCIPLE
CONTRIBUTION TO THE THEORY OF HUYGENS S ENVELOPING-WAVE PRINCIPLE BY J. VAN MIEGHEM TRANSLATED BY D. H. DELPHENICH BRUSSELS PALAIS DES ACADEMIES RUE DUCAL, 96 TABLE OF CONTENTS INTRODUCTION FIRST CHAPTER
More informationOverview of the weighting constants and the points where we evaluate the function for The Gaussian quadrature Project two
Overvew of the weghtg costats ad the pots where we evaluate the fucto for The Gaussa quadrature Project two By Ashraf Marzouk ChE 505 Fall 005 Departmet of Mechacal Egeerg Uversty of Teessee Koxvlle, TN
More informationThe conformations of linear polymers
The coformatos of lear polymers Marc R. Roussel Departmet of Chemstry ad Bochemstry Uversty of Lethbrdge February 19, 9 Polymer scece s a rch source of problems appled statstcs ad statstcal mechacs. I
More informationGeneral Method for Calculating Chemical Equilibrium Composition
AE 6766/Setzma Sprg 004 Geeral Metod for Calculatg Cemcal Equlbrum Composto For gve tal codtos (e.g., for gve reactats, coose te speces to be cluded te products. As a example, for combusto of ydroge wt
More informationReflection of Plane Waves from a Free Surface of an Initially Stressed Transversely Isotropic Dissipative Medium
ppled Mathematcs 0 9- do:0.6/am.0.956 Publshed Ole September 0 (http://www.scrp.org/joural/am) Reflecto of Plae Waves from a Free Surface of a Itally Stressed Trasversely Isotropc Dsspatve Medum bstract
More informationGENERALIZATIONS OF CEVA S THEOREM AND APPLICATIONS
GENERLIZTIONS OF CEV S THEOREM ND PPLICTIONS Floret Smaradache Uversty of New Mexco 200 College Road Gallup, NM 87301, US E-mal: smarad@um.edu I these paragraphs oe presets three geeralzatos of the famous
More informationLinear Regression Linear Regression with Shrinkage. Some slides are due to Tommi Jaakkola, MIT AI Lab
Lear Regresso Lear Regresso th Shrkage Some sldes are due to Tomm Jaakkola, MIT AI Lab Itroducto The goal of regresso s to make quattatve real valued predctos o the bass of a vector of features or attrbutes.
More information4. Standard Regression Model and Spatial Dependence Tests
4. Stadard Regresso Model ad Spatal Depedece Tests Stadard regresso aalss fals the presece of spatal effects. I case of spatal depedeces ad/or spatal heterogeet a stadard regresso model wll be msspecfed.
More informationON THE LOGARITHMIC INTEGRAL
Hacettepe Joural of Mathematcs ad Statstcs Volume 39(3) (21), 393 41 ON THE LOGARITHMIC INTEGRAL Bra Fsher ad Bljaa Jolevska-Tueska Receved 29:9 :29 : Accepted 2 :3 :21 Abstract The logarthmc tegral l(x)
More information