Interactive Simulation of Elasto-Plastic Materials using the Finite Element Method
|
|
- Daisy Carr
- 5 years ago
- Views:
Transcription
1 Otline Interctie Simltion of Elsto-Plstic Mterils sing the Finite Element Method Moie Mtthis Müller Seminr Wintersemester FEM s. Mss-Spring he Mtri StticDnmic Deformtion Continm Mechnics nd FEM Strin nd Stress ensors Continos PDE s FEM Discretition Plsticit Plstic Strin Updte Rles Frctre Principl Stresses Crck Compttion Mss-Spring s. FEM Pros nd Cons of FEM. Discretition of n object into mss points. Representtion of forces beteen mss points ith springs. Compttion of the dnmics. Discretition of n object into s tetrhedr. Discretition of continos energ eqtions into lgebric eqtions for forces cting t ertices. Compttion of the dnmics Pros: o indiidl spring constnts needed onl knon mteril prmeters Eν o inersion problems inerted tetrhedr prodce forces Stress nd strin tensors llo frctre nd plsticit simltions deformble mss-spring sstem deformble FEM sstem Cons: Pre-compte stiffness mtri Store stiffness mtri per edge Store originl nd ctl positions of ertices
2 Otline One-dimensionl Spring FEM s. Mss-Spring he Mtri StticDnmic Deformtion Continm Mechnics nd FEM Strin nd Stress ensors Continos PDE s FEM Discretition Plsticit Plstic Strin Updte Rles Frctre Principl Stresses Crck Compttion f f k 5 hree-dimensionl Object 6 hree-dimensionl Object Finite Element Mesh 9 tetrhedr 9 ertices 9 79 dof.... n n n f f f f... fn f fel K Mti K Rnn fn fn fel F Fnction F : Rn Rn 7 8
3 Sttic Deformtion Dnmic Deformtion fet fel K K- fet M C K f et Copled sstem of n liner ODEs Eplicit integrtion: o soler needed Implicit integrtion: Liner soler per time step Sole liner sstem Conjgte Grdients fet fel F F-fet M C F f et f Copled sstem of n non-liner ODEs Eplicit integrtion: o soler needed Implicit integrtion: Linerie t eer time step: K dfd Sole non-liner sstem eton-rphson - generlied eton-method 9 Otline Continos Elsticit -d FEM s. Mss-Spring he Mtri StticDnmic Deformtion Continm Mechnics nd FEM Strin nd Stress ensors Continos PDE s FEM Discretition Plsticit Plstic Strin Updte Rles Frctre Principl Stresses Crck Compttion fn l stress [m] orml-spnnng l fn E ll strin [] Dehnng Elsticit Yong s Modls [m] Metl: ~ m Soft mteril: ~6 m
4 Continos Elsticit -d Deformtion: Continos -d ector field : R R Defined ithin ndeformed object Liner -d Strin norml strin in - direction: d d d d d- d d sher strin: d d d d- d d 5 Liner -d Strin Liner strin tensor: Smmetric mtri 6 ector: 6 on-liner -d Strin Green-Sint-Vennt strin tensor: rnsformtion e se: : Use cobin of trnsformtion: I Green Interprettion:
5 -d Stress Constittie Reltion isotropic Stress is force per oriented re: df df d d df n d n n f n he stress tensor is smmetric mtri 6 ector: Hooke s l: ν c E ν c E E c G ν ν ν ν c G G G Onl to sclr prmeters: E: Yong s modls ν: Poisson rtio 7 8 Ptting it ll together Energ Formltion Gien e cn compte strin nd stress E t eer point ithin the object. Energ U is sclr U t point is gien b displcement force : U elstic E Find sch tht corresponding stresses re in blnce ith eternl forces f eerhere ithin object: f Strong formltion f Copled sstem of prtil differentil eqtions! f he totl Energ of the deformed bod: U bod bod E f dv Gien f E e cn compte U bod for n Find sch tht U bod is minimm δu 9 5
6 6 Otline FEM s. Mss-Spring he Mtri StticDnmic Deformtion Continm Mechnics nd FEM Strin nd Stress ensors Continos PDE s FEM Discretition Plsticit Plstic Strin Updte Rles Frctre Principl Stresses Crck Compttion Finite Element Formltion So fr e looked for continos field o e look for.. n t fied loctions:.. n nd interpolte ith fied bsis fnctions: Σ i i φ i i i φ i Liner Displcement etrhedron nknons.. eqtions i i i re ribles i i i re gien nmbers Displcements he displcement fnction cn be epressed s mtri of bsis fnctions H times ector of displcements: H à
7 Strin Stress nd Energ Liner displcements ield constnt strin: Stress s fnction of the displcements: H à B à Mtri B R 6 is constnt independent of B depends on the originl geometr of the tetrhedron onl E EB à Energ s fnction of the displcements: U E dv à B EB dv à à B EB dv à à [ V B EB ] à à K à 5 6 Mtri ssembl of s U bod à K à Forces re the derities of the energ ith respect to the degrees of freedom: U bod à K à f Single : f f f f f f K e he mtri K R is the stiffness mtri of the! K B EB dv V B EB Entire bod: f.. f n.. n 7 8 7
8 Implementtion Otline f.. f n K.. n K is sprse block t ij describes ho j inflences f i eer erte stores djcenc list of -mtri erte-reference pirs FEM s. Mss-Spring he Mtri StticDnmic Deformtion Continm Mechnics nd FEM Strin nd Stress ensors Continos PDE s FEM Discretition Plsticit Plstic Strin Updte Rles Frctre Principl Stresses Crck Compttion 9 Plstic Strin Plstic Updte Rles n is nder strin û de to displcements û: û [ ] B û Initilition plstic : Updte rle eer time step: plstic stores strin in stte rible: plstic he elstic strin tht cses internl forces is no: Compte û B û from ctl displcements Compte elstic û - plstic if elstic > ield then plstic plstic creep elstic if plstic > m then plstic plstic m plstic elstic û - plstic û o internl forces re present hen û plstic Might be for û! plstic elstic before fter 6 dimensionl 8
9 Implementtion Otline Since B û the displcements tht correpsond to the plstic strin re: û plstic B - plstic nd the correpsonding forces re: f plstic KB - plstic [B EB] B - plstic B E plstic dd plstic forces to eternl forces FEM s. Mss-Spring he Mtri StticDnmic Deformtion Continm Mechnics nd FEM Strin nd Stress ensors Continos PDE s FEM Discretition Plsticit Plstic Strin Updte Rles Frctre Principl Stresses Crck Compttion Frctre criterion Principl Stresses Brek if internl elstic force eeeds threshold stress is tensor the force.r.t. norml n is: he stress tensor is smmetric there is rottion mtri R sch tht df n d n p R p R p Find n m sch tht dfd is miml! n m is direction of miml tensile stress the digonl entries re the eigenles of the colmns of R re the corresponing eigenectors there is ls rotted coordinte sstem here is digonl! 5 6 9
10 Principl Stresses Crck compttion p for ll s: compte miml tensile stress p m p p the p re the principl etreml stresses find miml eigenle of corresponding eigenector is the direction of miml stress 7 8 Crck compttion Crck compttion for ll s: compte miml tensile stress p m if p m eceeds ield stress for ll s: compte miml tensile stress p m if p m eceeds ield stress select erte crck tip rndom p m p m 9
11 Crck compttion Crck compttion for ll s: compte miml tensile stress p m if p m eceeds ield stress select erte crck tip rndom set plne α norml p m to throgh p m α for ll s: compte miml tensile stress p m if p m eceeds ield stress select erte crck tip rndom set plne α norml p m to throgh α mrk tetrs.r.t. α p m - - Crck compttion he End for ll s: compte miml tensile stress p m if p m eceeds ield stress select erte crck tip rndom set plne α norml p m to throgh α mrk tetrs.r.t. α split erte p m hnk o for or ttention! - -
Weighted Residual Methods
Weighted Resil Methods Formltion of FEM Model Direct Method Formltion of FEM Model Vritionl Method Weighted Resils Severl pproches cn e sed to trnsform the phsicl formltion of prolem to its finite element
More informationPlate Theory. Section 11: PLATE BENDING ELEMENTS
Section : PLATE BENDING ELEMENTS Plte Theor A plte is structurl element hose mid surfce lies in flt plne. The dimension in the direction norml to the plne is referred to s the thickness of the plte. A
More informationChapter 4 FEM in the Analysis of a Four Bar Mechanism
Chpter FEM in the nlysis of For r Mechnism he finite element method (FEM) is powerfl nmericl techniqe tht ses vritionl nd interpoltion methods for modeling nd solving bondry vle problem. he method is lso
More informationConcept of Stress at a Point
Washkeic College of Engineering Section : STRONG FORMULATION Concept of Stress at a Point Consider a point ithin an arbitraril loaded deformable bod Define Normal Stress Shear Stress lim A Fn A lim A FS
More informationPlate Theory. Section 13: PLATE BENDING ELEMENTS
Section : PLATE BENDING ELEENTS Wshkeic College of Engineering Plte Theor A plte is structurl element hose mid surfce lies in flt plne. The dimension in the direction norml to the plne is referred to s
More informationWhy symmetry? Symmetry is often argued from the requirement that the strain energy must be positive. (e.g. Generalized 3-D Hooke s law)
Why symmetry? Symmetry is oten rgued rom the requirement tht the strin energy must be positie. (e.g. Generlized -D Hooke s lw) One o the derities o energy principles is the Betti- Mxwell reciprocity theorem.
More information4. Classical lamination theory
O POSI TES GROUP U I V ERSIT Y OF T W ET E omposites orse 8-9 Uniersit o Tente Eng. & Tech. 4. 4. lssicl lmintion theor - Lrent Wrnet & Remo ermn. 4. lssicl lmintion theor 4.. Introction hpter n ocse on
More informationEquations of Motion. Figure 1.1.1: a differential element under the action of surface and body forces
Equtions of Motion In Prt I, lnce of forces nd moments cting on n component ws enforced in order to ensure tht the component ws in equilirium. Here, llownce is mde for stresses which vr continuousl throughout
More informationA - INTRODUCTION AND OVERVIEW
MMJ5 COMPUTATIONAL METHOD IN SOLID MECHANICS A - INTRODUCTION AND OVERVIEW INTRODUCTION AND OVERVIEW M.N. Tmin, CSMLb, UTM MMJ5 COMPUTATIONAL METHOD IN SOLID MECHANICS Course Content: A INTRODUCTION AND
More informationI. Backgrounds and preliminaries
I. Bckgrounds nd preliminries 1.1 Vector 1.2 Mtri nd Liner lger 1.3 Function nd Differentition 1.4 Bsis of mechnics nd Sttics 1.5 Unit nd Dimension 1.6 Bem heor -1- 1.1 Vector -2- Definition of vector
More informationINTERFACE DESIGN OF CORD-RUBBER COMPOSITES
8 TH INTENATIONAL CONFEENCE ON COMPOSITE MATEIALS INTEFACE DESIGN OF COD-UBBE COMPOSITES Z. Xie*, H. Du, Y. Weng, X. Li Ntionl Ke Lbortor of Science nd Technolog on Advnced Composites in Specil Environment,
More informationThe Algebra (al-jabr) of Matrices
Section : Mtri lgebr nd Clculus Wshkewicz College of Engineering he lgebr (l-jbr) of Mtrices lgebr s brnch of mthemtics is much broder thn elementry lgebr ll of us studied in our high school dys. In sense
More information1 Bending of a beam with a rectangular section
1 Bending of bem with rectngulr section x3 Episseur b M x 2 x x 1 2h M Figure 1 : Geometry of the bem nd pplied lod The bem in figure 1 hs rectngur section (thickness 2h, width b. The pplied lod is pure
More informationElectromagnetics P5-1. 1) Physical quantities in EM could be scalar (charge, current, energy) or vector (EM fields).
Electromgnetics 5- Lesson 5 Vector nlsis Introduction ) hsicl quntities in EM could be sclr (chrge current energ) or ector (EM fields) ) Specifing ector in -D spce requires three numbers depending on the
More information6.5 Plate Problems in Rectangular Coordinates
6.5 lte rolems in Rectngulr Coordintes In this section numer of importnt plte prolems ill e emined ug Crte coordintes. 6.5. Uniform ressure producing Bending in One irection Consider first the cse of plte
More informationGeneralizations of the Basic Functional
3 Generliztions of the Bsic Functionl 3 1 Chpter 3: GENERALIZATIONS OF THE BASIC FUNCTIONAL TABLE OF CONTENTS Pge 3.1 Functionls with Higher Order Derivtives.......... 3 3 3.2 Severl Dependent Vribles...............
More informationINTRODUCTION TO LINEAR ALGEBRA
ME Applied Mthemtics for Mechnicl Engineers INTRODUCTION TO INEAR AGEBRA Mtrices nd Vectors Prof. Dr. Bülent E. Pltin Spring Sections & / ME Applied Mthemtics for Mechnicl Engineers INTRODUCTION TO INEAR
More information1/31/ :33 PM. Chapter 11. Kinematics of Particles. Mohammad Suliman Abuhaiba,Ph.D., P.E.
1/31/18 1:33 PM Chpter 11 Kinemtics of Prticles 1 1/31/18 1:33 PM First Em Sturdy 1//18 3 1/31/18 1:33 PM Introduction Mechnics Mechnics = science which describes nd predicts conditions of rest or motion
More informationStatically indeterminate examples - axial loaded members, rod in torsion, members in bending
Elsticity nd Plsticity Stticlly indeterminte exmples - xil loded memers, rod in torsion, memers in ending Deprtment of Structurl Mechnics Fculty of Civil Engineering, VSB - Technicl University Ostrv 1
More informationIntroduction to Finite Elements in Engineering. Tirupathi R. Chandrupatla Rowan University Glassboro, New Jersey
Introduction to Finite Elements in Engineering Tirupthi R. Chndruptl Rown Universit Glssboro, New Jerse Ashok D. Belegundu The Pennslvni Stte Universit Universit Prk, Pennslvni Solutions Mnul Prentice
More information2/2/ :36 AM. Chapter 11. Kinematics of Particles. Mohammad Suliman Abuhaiba,Ph.D., P.E.
//16 1:36 AM Chpter 11 Kinemtics of Prticles 1 //16 1:36 AM First Em Wednesdy 4//16 3 //16 1:36 AM Introduction Mechnics Mechnics = science which describes nd predicts the conditions of rest or motion
More informationMECHANICS OF SOLIDS. MM-504 & MM 505 (Option-A 1
MECHANICS OF SOLIDS M.A./M.Sc. Mthemtics (Finl) MM-504 & MM 505 (Option-A ) Directorte of Distnce Eduction Mhrshi Dynnd University ROHTAK 4 00 Copyright 004, Mhrshi Dynnd University, ROHTAK All Rights
More informationChapter 6 Polarization and Crystal Optics
EE 485, Winter 4, Lih Y. Lin Chpter 6 Polriztion nd Crstl Optics - Polriztion Time course of the direction of E ( r, t - Polriztion ffects: mount of light reflected t mteril interfces. bsorption in some
More information1. Solve Problem 1.3-3(c) 2. Solve Problem 2.2-2(b)
. Sole Problem.-(c). Sole Problem.-(b). A two dimensional trss shown in the figre is made of alminm with Yong s modls E = 8 GPa and failre stress Y = 5 MPa. Determine the minimm cross-sectional area of
More information2/20/ :21 AM. Chapter 11. Kinematics of Particles. Mohammad Suliman Abuhaiba,Ph.D., P.E.
//15 11:1 M Chpter 11 Kinemtics of Prticles 1 //15 11:1 M Introduction Mechnics Mechnics = science which describes nd predicts the conditions of rest or motion of bodies under the ction of forces It is
More informationMath 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008
Mth 520 Finl Exm Topic Outline Sections 1 3 (Xio/Dums/Liw) Spring 2008 The finl exm will be held on Tuesdy, My 13, 2-5pm in 117 McMilln Wht will be covered The finl exm will cover the mteril from ll of
More information13.4 Work done by Constant Forces
13.4 Work done by Constnt Forces We will begin our discussion of the concept of work by nlyzing the motion of n object in one dimension cted on by constnt forces. Let s consider the following exmple: push
More informationMidterm Examination Wed Oct Please initial the statement below to show that you have read it
EN10: Continuum Mechnics Midterm Exmintion Wed Oct 6 016 School of Engineering Brown University NAME: Generl Instructions No collbortion of ny kind is permitted on this exmintion. You my bring double sided
More informationStress distribution in elastic isotropic semi-space with concentrated vertical force
Bulgrin Chemicl Communictions Volume Specil Issue pp. 4 9 Stress distribution in elstic isotropic semi-spce with concentrted verticl force L. B. Petrov Deprtment of Mechnics Todor Kbleshkov Universit of
More informationElementary Linear Algebra
Elementry Liner Algebr Anton & Rorres, 9 th Edition Lectre Set Chpter : Vectors in -Spce nd -Spce Chpter Content Introdction to Vectors (Geometric Norm of Vector; Vector Arithmetic Dot Prodct; Projections
More informationIntroduction to Finite Element Method
Introduction to Finite Element Method Introductory Course on Multiphysics Modelling TOMASZ G. ZIELIŃSKI bluebox.ippt.pn.pl/ tzielins/ Tble of Contents 1 Introduction 1 1.1 Motivtion nd generl concepts.............
More informationIntroduction to Finite Elements in Engineering. Tirupathi R. Chandrupatla Rowan University Glassboro, New Jersey
Introduction to Finite lements in ngineering Tirupthi R. Chndruptl Rown Universit Glssboro, New Jerse Ashok D. Belegundu The Pennslvni Stte Universit Universit Prk, Pennslvni Solutions Mnul Prentice Hll,
More informationR. I. Badran Solid State Physics
I Bdrn Solid Stte Physics Crystl vibrtions nd the clssicl theory: The ssmption will be mde to consider tht the men eqilibrim position of ech ion is t Brvis lttice site The ions oscillte bot this men position
More informationPlates on elastic foundation
Pltes on elstic foundtion Circulr elstic plte, xil-symmetric lod, Winkler soil (fter Timoshenko & Woinowsky-Krieger (1959) - Chpter 8) Prepred by Enzo Mrtinelli Drft version ( April 016) Introduction Winkler
More informationChapter 1: Differential Form of Basic Equations
MEG 74 Energ and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hghes College of Engineering Universit of Nevada Las Vegas TBE B- (7)
More informationColumns and Stability
ARCH 331 Note Set 1. Su01n Columns nd Stilit Nottion: A = nme or re A36 = designtion o steel grde = nme or width C = smol or compression C c = column slenderness clssiiction constnt or steel column design
More informationMEG 741 Energy and Variational Methods in Mechanics I
MEG 74 Energ and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hghes College of Engineering Universit of Nevada Las Vegas TBE B- (7)
More informationMultiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution
Multiple Integrls eview of Single Integrls eding Trim 7.1 eview Appliction of Integrls: Are 7. eview Appliction of Integrls: Volumes 7.3 eview Appliction of Integrls: Lengths of Curves Assignment web pge
More informationSUPPLEMENTARY INFORMATION
DOI:.38/NMAT343 Hybrid Elstic olids Yun Li, Ying Wu, Ping heng, Zho-Qing Zhng* Deprtment of Physics, Hong Kong University of cience nd Technology Cler Wter By, Kowloon, Hong Kong, Chin E-mil: phzzhng@ust.hk
More informationA finite thin circular beam element for out-of-plane vibration analysis of curved beams
Journl of Mechnicl Science nd echnology (009) 196~1405 Journl of Mechnicl Science nd echnology www.springerlink.com/content/178-494x DOI 10.1007/s106-008-11- A finite thin circulr bem element for out-of-plne
More informationROTATION IN 3D WORLD RIGID BODY MOTION
OTATION IN 3D WOLD IGID BODY MOTION igid Bod Motion Simultion igid bod motion Eqution of motion ff mmvv NN ddiiωω/dddd Angulr velocit Integrtion of rottion nd it s eression is necessr. Simultion nd Eression
More informationMultiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution
Multiple Integrls eview of Single Integrls eding Trim 7.1 eview Appliction of Integrls: Are 7. eview Appliction of Integrls: olumes 7.3 eview Appliction of Integrls: Lengths of Curves Assignment web pge
More informationReference. Vector Analysis Chapter 2
Reference Vector nlsis Chpter Sttic Electric Fields (3 Weeks) Chpter 3.3 Coulomb s Lw Chpter 3.4 Guss s Lw nd pplictions Chpter 3.5 Electric Potentil Chpter 3.6 Mteril Medi in Sttic Electric Field Chpter
More informationElement Morphing 17 1
17 Element Morphing 17 1 Chpter 17: ELEMENT MORPHING TABLE OF CONTENTS Pge 17.1 Introduction..................... 17 3 17. Plte in Plne Stress.................. 17 4 17.3 Source Element 1: 4-Node Rectngulr
More informationDesign and Testing of Coils for Pulsed Electromagnetic Forming
Design nd Testing of Coils for Pulsed Electromgnetic Forming. Golovshchenko, N. Bessonov, R. Dvies Ford Reserch & Advnced Engineering, Derborn, UA University of Michign-Derborn, Derborn, UA Pcific Northwest
More informationProblem set 5: Solutions Math 207B, Winter r(x)u(x)v(x) dx.
Problem set 5: Soltions Mth 7B, Winter 6. Sppose tht p : [, b] R is continosly differentible fnction sch tht p >, nd q, r : [, b] R re continos fnctions sch tht r >, q. Define weighted inner prodct on
More informationUNIVERSITY OF BOLTON SCHOOL OF ENGINEERING B.ENG (HONS) ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATION SEMESTER /2018
ENG005 B.ENG (HONS) ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATION SEMESTER 1-017/018 MODULE NO: EEE4001 Dte: 19Jnury 018 Time:.00 4.00 INSTRUCTIONS TO CANDIDATES: There re SIX questions. Answer ANY
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES Introduction In rigid body kinemtics, e use the reltionships governing the displcement, velocity nd ccelertion, but must lso ccount for the rottionl motion of the body. Description
More informationDYNAMIC EARTH PRESSURE SIMULATION BY SINGLE DEGREE OF FREEDOM SYSTEM
13 th World Conference on Erthque Engineering Vncouver, B.C., Cnd August 1-6, 2004 per No. 2663 DYNAMIC EARTH RESSURE SIMULATION BY SINGLE DEGREE OF FREEDOM SYSTEM Arsln GHAHRAMANI 1, Seyyed Ahmd ANVAR
More informationOptimizing LTS-Simulation Algorithm
Optimizing LTS-ltion Algorithm MEMICS 09 Lkáš Holík 1, Jiří Šimáček 1,2 emil: {holik,isimcek}@fit.tbr.cz, simcek@img.fr 1 FIT BUT, Božetěcho 2, 61266 Brno, Czech Repblic 2 VERIMAG, UJF, 2.. de Vignte,
More informationWorksheet #2 Math 285 Name: 1. Solve the following systems of linear equations. The prove that the solutions forms a subspace of
Worsheet # th Nme:. Sole the folloing sstems of liner equtions. he proe tht the solutions forms suspe of ) ). Find the neessr nd suffiient onditions of ll onstnts for the eistene of solution to the sstem:.
More informationSIMULATION OF DYNAMIC RESPONSE OF SATURATED SANDS USING MODIFIED DSC MODEL
th World Conference on Erthqke Engineering Vncover, B.C., Cnd Agst -6, 4 Pper No. 8 SIMULATION OF DYNAMIC RESPONSE OF SATURATED SANDS USING MODIFIED DSC MODEL Soo-il KIM, Je-soon CHOI, Ken-bo PARK, Kyng-bm
More informationWe are looking for ways to compute the integral of a function f(x), f(x)dx.
INTEGRATION TECHNIQUES Introdction We re looking for wys to compte the integrl of fnction f(x), f(x)dx. To pt it simply, wht we need to do is find fnction F (x) sch tht F (x) = f(x). Then if the integrl
More informationEigen Values and Eigen Vectors of a given matrix
Engineering Mthemtics 0 SUBJECT NAME SUBJECT CODE MATERIAL NAME MATERIAL CODE : Engineering Mthemtics I : 80/MA : Prolem Mteril : JM08AM00 (Scn the ove QR code for the direct downlod of this mteril) Nme
More information2 Stress, Strain, Piezoresistivity, and Piezoelectricity
2 Stress, Strin, Piezoresistivity, nd Piezoelectricity 2.1 STRAIN TENSOR Strin in crystls is creted by deformtion nd is defined s reltive lttice displcement. For simplicity, we use 2D lttice model in Fig.
More informationExtended tan-cot method for the solitons solutions to the (3+1)-dimensional Kadomtsev-Petviashvili equation
Interntionl Jornl of Mthemticl Anlysis nd Applictions ; (): 9-9 Plished online Mrch, (http://www.scit.org/jornl/ijm) Extended tn-cot method for the solitons soltions to the (+)-dimensionl Kdomtsev-Petvishvili
More information1.1. Linear Constant Coefficient Equations. Remark: A differential equation is an equation
1 1.1. Liner Constnt Coefficient Equtions Section Objective(s): Overview of Differentil Equtions. Liner Differentil Equtions. Solving Liner Differentil Equtions. The Initil Vlue Problem. 1.1.1. Overview
More informationComputer Graphics (CS 4731) Lecture 7: Linear Algebra for Graphics (Points, Scalars, Vectors)
Computer Grphics (CS 4731) Lecture 7: Liner Alger for Grphics (Points, Sclrs, Vectors) Prof Emmnuel Agu Computer Science Dept. Worcester Poltechnic Institute (WPI) Annoncements Project 1 due net Tuesd,
More informationKinematic Waves. These are waves which result from the conservation equation. t + I = 0. (2)
Introduction Kinemtic Wves These re wves which result from the conservtion eqution E t + I = 0 (1) where E represents sclr density field nd I, its outer flux. The one-dimensionl form of (1) is E t + I
More informationSolution Manual. for. Fracture Mechanics. C.T. Sun and Z.-H. Jin
Solution Mnul for Frcture Mechnics by C.T. Sun nd Z.-H. Jin Chpter rob.: ) 4 No lod is crried by rt nd rt 4. There is no strin energy stored in them. Constnt Force Boundry Condition The totl strin energy
More informationSimple Harmonic Motion I Sem
Simple Hrmonic Motion I Sem Sllus: Differentil eqution of liner SHM. Energ of prticle, potentil energ nd kinetic energ (derivtion), Composition of two rectngulr SHM s hving sme periods, Lissjous figures.
More informationThomas Whitham Sixth Form
Thoms Whithm Sith Form Pure Mthemtics Unit C Alger Trigonometry Geometry Clculus Vectors Trigonometry Compound ngle formule sin sin cos cos Pge A B sin Acos B cos Asin B A B sin Acos B cos Asin B A B cos
More information(uv) = u v + uv, (1) u vdx + b [uv] b a = u vdx + u v dx. (8) u vds =
Integrtion by prts Integrting the both sides of yields (uv) u v + uv, (1) or b (uv) dx b u vdx + b uv dx, (2) or b [uv] b u vdx + Eqution (4) is the 1-D formul for integrtion by prts. Eqution (4) cn be
More informationChapter 2. Vectors. 2.1 Vectors Scalars and Vectors
Chpter 2 Vectors 2.1 Vectors 2.1.1 Sclrs nd Vectors A vector is quntity hving both mgnitude nd direction. Emples of vector quntities re velocity, force nd position. One cn represent vector in n-dimensionl
More informationMatrix Eigenvalues and Eigenvectors September 13, 2017
Mtri Eigenvlues nd Eigenvectors September, 7 Mtri Eigenvlues nd Eigenvectors Lrry Cretto Mechnicl Engineering 5A Seminr in Engineering Anlysis September, 7 Outline Review lst lecture Definition of eigenvlues
More informationES.182A Topic 30 Notes Jeremy Orloff
ES82A opic 3 Notes Jerem Orloff 3 Non-independent vribles: chin rule Recll the chin rule: If w = f, ; nd = r, t, = r, t then = + r t r t r t = + t t t r nfortuntel, sometimes there re more complicted reltions
More informationCounting intersections of spirals on a torus
Counting intersections of spirls on torus 1 The problem Consider unit squre with opposite sides identified. For emple, if we leve the centre of the squre trveling long line of slope 2 (s shown in the first
More informationANALYSIS OF STRUCTURES
Mech_Eng 36 Stress Anlsis Anlsis of Structures ANAYSIS OF STRUCTURES Sridhr Krishnswm 8-1 Mech_Eng 36 Stress Anlsis Anlsis of Structures 8.1 ANAYSIS OF STRUCTURES: At this point, we hve developed n understnding
More informationPlane curvilinear motion is the motion of a particle along a curved path which lies in a single plane.
Plne curiliner motion is the motion of prticle long cured pth which lies in single plne. Before the description of plne curiliner motion in n specific set of coordintes, we will use ector nlsis to describe
More informationPhysics 319 Classical Mechanics. G. A. Krafft Old Dominion University Jefferson Lab Lecture 2
Physics 319 Clssicl Mechnics G. A. Krfft Old Dominion University Jefferson Lb Lecture Undergrdute Clssicl Mechnics Spring 017 Sclr Vector or Dot Product Tkes two vectors s inputs nd yields number (sclr)
More informationSession Trimester 2. Module Code: MATH08001 MATHEMATICS FOR DESIGN
School of Science & Sport Pisley Cmpus Session 05-6 Trimester Module Code: MATH0800 MATHEMATICS FOR DESIGN Dte: 0 th My 06 Time: 0.00.00 Instructions to Cndidtes:. Answer ALL questions in Section A. Section
More informationFULL MECHANICS SOLUTION
FULL MECHANICS SOLUION. m 3 3 3 f For long the tngentil direction m 3g cos 3 sin 3 f N m 3g sin 3 cos3 from soling 3. ( N 4) ( N 8) N gsin 3. = ut + t = ut g sin cos t u t = gsin cos = 4 5 5 = s] 3 4 o
More informationy b y y sx 2 y 2 z CHANGE OF VARIABLES IN MULTIPLE INTEGRALS
ECION.8 CHANGE OF VAIABLE IN MULIPLE INEGAL 73 CA tive -is psses throgh the point where the prime meridin (the meridin throgh Greenwich, Englnd) intersects the eqtor. hen the ltitde of P is nd the longitde
More informationDistributed Forces: Centroids and Centers of Gravity
Distriuted Forces: Centroids nd Centers of Grvit Introduction Center of Grvit of D Bod Centroids nd First Moments of Ares nd Lines Centroids of Common Shpes of Ares Centroids of Common Shpes of Lines Composite
More informationDETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING MOMENT INTERACTION AT MICROSCALE
Determintion RevAdvMterSci of mechnicl 0(009) -7 properties of nnostructures with complex crystl lttice using DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING
More informationINTRODUCTION. The three general approaches to the solution of kinetics problems are:
INTRODUCTION According to Newton s lw, prticle will ccelerte when it is subjected to unblnced forces. Kinetics is the study of the reltions between unblnced forces nd the resulting chnges in motion. The
More informationPoint Lattices: Bravais Lattices
Physics for Solid Stte Applictions Februry 18, 2004 Lecture 7: Periodic Structures (cont.) Outline Review 2D & 3D Periodic Crystl Structures: Mthemtics X-Ry Diffrction: Observing Reciprocl Spce Point Lttices:
More informationDYNAMIC CONTACT PROBLEM OF ROLLING ELASTIC WHEELS
DYNMIC CONTCT PROBLEM OF ROLLING ELSTIC WHEELS Dénes Tkács nd Gábor Stépán Deprtment of pplied Mechnics Budpest Uniersity of Technology nd Economics Budpest, H-151, Hungry BSTRCT: The lterl ibrtion of
More informationKirchhoff and Mindlin Plates
Kirchhoff nd Mindlin Pltes A plte significntly longer in two directions compred with the third, nd it crries lod perpendiculr to tht plne. The theory for pltes cn be regrded s n extension of bem theory,
More informationSolution Set 2. y z. + j. u + j
Soltion Set 2. Review of Div, Grd nd Crl. Prove:. () ( A) =, where A is ny three dimensionl vector field. i j k ( Az A = y z = i A A y A z y A ) ( y A + j z z A ) ( z Ay + k A ) y ( A) = ( Az y A ) y +
More informationPHYSICS 211 MIDTERM I 21 April 2004
PHYSICS MIDERM I April 004 Exm is closed book, closed notes. Use only your formul sheet. Write ll work nd nswers in exm booklets. he bcks of pges will not be grded unless you so request on the front of
More informationPlane curvilinear motion is the motion of a particle along a curved path which lies in a single plane.
Plne curiliner motion is the motion of prticle long cured pth which lies in single plne. Before the description of plne curiliner motion in n specific set of coordintes, we will use ector nlsis to describe
More information4 The dynamical FRW universe
4 The dynmicl FRW universe 4.1 The Einstein equtions Einstein s equtions G µν = T µν (7) relte the expnsion rte (t) to energy distribution in the universe. On the left hnd side is the Einstein tensor which
More informationJob No. Sheet 1 of 8 Rev B. Made by IR Date Aug Checked by FH/NB Date Oct Revised by MEB Date April 2006
Job o. Sheet 1 of 8 Rev B 10, Route de Limours -78471 St Rémy Lès Chevreuse Cedex rnce Tel : 33 (0)1 30 85 5 00 x : 33 (0)1 30 5 75 38 CLCULTO SHEET Stinless Steel Vloristion Project Design Exmple 5 Welded
More informationMAC-solutions of the nonexistent solutions of mathematical physics
Proceedings of the 4th WSEAS Interntionl Conference on Finite Differences - Finite Elements - Finite Volumes - Boundry Elements MAC-solutions of the nonexistent solutions of mthemticl physics IGO NEYGEBAUE
More informationChapter 1 VECTOR ALGEBRA
Chpter 1 VECTOR LGEBR INTRODUCTION: Electromgnetics (EM) m be regrded s the stud of the interctions between electric chrges t rest nd in motion. Electromgnetics is brnch of phsics or electricl engineering
More informationExplain shortly the meaning of the following eight words in relation to shells structures.
Delft University of Technology Fculty of Civil Engineering nd Geosciences Structurl Mechnics Section Write your nme nd study number t the top right-hnd of your work. Exm CIE4143 Shell Anlysis Tuesdy 15
More informationANALYSIS OF MECHANICAL PROPERTIES OF COMPOSITE SANDWICH PANELS WITH FILLERS
ANALYSIS OF MECHANICAL PROPERTIES OF COMPOSITE SANDWICH PANELS WITH FILLERS A. N. Anoshkin *, V. Yu. Zuiko, A.V.Glezmn Perm Ntionl Reserch Polytechnic University, 29, Komsomolski Ave., Perm, 614990, Russi
More informationTest , 8.2, 8.4 (density only), 8.5 (work only), 9.1, 9.2 and 9.3 related test 1 material and material from prior classes
Test 2 8., 8.2, 8.4 (density only), 8.5 (work only), 9., 9.2 nd 9.3 relted test mteril nd mteril from prior clsses Locl to Globl Perspectives Anlyze smll pieces to understnd the big picture. Exmples: numericl
More informationEducational version : Bolt Specification. Initial clamping force F = N Number of bolts n = 4 Demand factor k = 50 %
Euctionl version rogrm MDESIG Moule version 11.0 Dte 1.11.2007 roj. r Bolt Specifiction Input t Bolt Specifiction Initil clmping force F 10000 umer of olts n 4 Demn fctor k 50 % Constnt epenent on the
More informationMEG 741 Energy and Variational Methods in Mechanics I
ME 7 Energy n rition Methos in Mechnics I Brenn J. O ooe, Ph.D. Associte Professor of Mechnic Engineering Hor R. Hghes Coege of Engineering Uniersity of e Ls egs BE B- (7) 895-885 j@me.n.e Chter : Strctr
More informationChapter 3. Vector Spaces
3.4 Liner Trnsformtions 1 Chpter 3. Vector Spces 3.4 Liner Trnsformtions Note. We hve lredy studied liner trnsformtions from R n into R m. Now we look t liner trnsformtions from one generl vector spce
More informationProblems for HW X. C. Gwinn. November 30, 2009
Problems for HW X C. Gwinn November 30, 2009 These problems will not be grded. 1 HWX Problem 1 Suppose thn n object is composed of liner dielectric mteril, with constnt reltive permittivity ɛ r. The object
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGI OIES Introduction In rigid body kinemtics, e use the reltionships governing the displcement, velocity nd ccelertion, but must lso ccount for the rottionl motion of the body. escription
More informationTopic 1 Notes Jeremy Orloff
Topic 1 Notes Jerem Orloff 1 Introduction to differentil equtions 1.1 Gols 1. Know the definition of differentil eqution. 2. Know our first nd second most importnt equtions nd their solutions. 3. Be ble
More informationFinal Technical Report. STTR Grant No: FA C Software for the Design and Certification of Unitized Airframe Components
Engineering Softwre Reserch & Development, Inc. 111 West Port Plz, Suite 825 St. Louis, MO 63146 Finl Technicl Report STTR Grnt No: FA9550-05-C-0128 Softwre for the Design nd Certifiction of Unitized Airfrme
More informationLinear Strain Triangle and other types of 2D elements. By S. Ziaei Rad
Linear Strain Triangle and other tpes o D elements B S. Ziaei Rad Linear Strain Triangle (LST or T6 This element is also called qadratic trianglar element. Qadratic Trianglar Element Linear Strain Triangle
More informationPavel Rytí. November 22, 2011 Discrete Math Seminar - Simon Fraser University
Geometric representtions of liner codes Pvel Rytí Deprtment of Applied Mthemtics Chrles University in Prgue Advisor: Mrtin Loebl November, 011 Discrete Mth Seminr - Simon Frser University Bckground Liner
More informationConducting Ellipsoid and Circular Disk
1 Problem Conducting Ellipsoid nd Circulr Disk Kirk T. McDonld Joseph Henry Lbortories, Princeton University, Princeton, NJ 08544 (September 1, 00) Show tht the surfce chrge density σ on conducting ellipsoid,
More informationYear 12 Mathematics Extension 2 HSC Trial Examination 2014
Yer Mthemtics Etension HSC Tril Emintion 04 Generl Instructions. Reding time 5 minutes Working time hours Write using blck or blue pen. Blck pen is preferred. Bord-pproved clcultors my be used A tble of
More information