Pseudo Inverse Approach for cold forging processes and its comparison with Adaptive Incremental Approach

Size: px
Start display at page:

Download "Pseudo Inverse Approach for cold forging processes and its comparison with Adaptive Incremental Approach"

Transcription

1 èm Congrès Français d Mécaniqu Bsançon, 9 août au sptmbr 11 Psudo Invrs Approach for cold forging procsss and its comparison with Adaptiv Incrmntal Approach F.J. MENG a, A.HALOUANI b, C. LABERGERE a, Y.M. LI b, B. ABBES b, P. LAFON a, Y.Q. GUO b a. Institut Charls Dlaunay LASMIS, Univrsité d Tchnologi d Troys b. Group d Rchrch n Scincs Pour l Ingéniur, Univrsité d Rims Champagn Ardnn Abstract : Numrical simulation for highly non-linar forming procss rquirs fficint numrical mthods. In an optimization loop, th calculation cost is vry larg, so it is important to choos a good numrical simulation tool to rduc it. In this papr, w propos to simulat a D axisymmtric forging procss of a whl by using a psudo invrs approach and an adaptiv incrmntal approach. Ths two mthods will b compard in trms of computation tim and prdictability on th form of rough forging. Th comparison of th rsults will show th fficincy and limitations of th Psudo Invrs Approach. Résumé : La simulation numériqu ds procédés d mis n form st un problèm fortmnt non-linéair qui nécssit ds méthods numériqus prformants. Ls coûts ds calculs, souvnt importants, rndnt difficil l utilisation d un outil d simulation numériqu dans un boucl d optimisation. Nous proposons dans c papir d simulr un procédé D axisymétriqu d forgag d un rou n utilisant un approch psudo invrs t un approch MEF adaptativ incrémntal. Cs dux approchs sront nsuit comparés n trms d tmps d calcul t prédictibilité sur la form ds bruts d forg. La comparaison avc l approch adaptiv incrémntal montr l'fficacité t ls limits d l Approch Psudo Invrs. Kywords : Mtal Forming Procsss, Numrical Simulation, Psudo Invrs Approach, Adaptiv Incrmntal Approach 1 Introduction In this papr, w propos to simulat a D axisymmtric forging procss of a whl by using a psudo invrs approach and an adaptiv incrmntal approach. Ths two mthods us diffrnt matrial bhaviour modls and numrical tchnologis. Th adaptiv incrmntal approach (A.I.A.) is th classical mthod for th simulation of mtal forming procsss. It givs good strain and strss stimation, but is tim consuming. A nw approach calld Psudo Invrs Approach (P.I.A.) was proposd by Batoz, Guo t al. [1] for th sht forming modlling, which kps th rapidity of th Invrs Approach but givs good strss stimation owing to th loading history considration. By comparing th rsults of th two mthods, it can b found that th P.I.A. mthod is vry fficint but lss accurat than th incrmntal approach. Mthodology of th two numrical approachs.1 Psudo invrs approach A simplifid mthod calld Invrs Approach (I.A.) has bn dvlopd for th axisymmtrical cold forging modlling. Th approach is basd on th knowldg of th final part shap. Two basic assumptions ar usd: th assumption of proportional loading givs an intgratd constitutiv law without considring th strain path and th plastic flow, and th assumption of tool-billt actions allows on to rplac th tool actions by nodal forcs without contact tratmnt [-3]. Ths two assumptions mak th I.A. calculation vry fast. This approach givs fairly good strain stimation but poor strss stimation. Th P.I.A., basd on th traditional I.A., is dvlopd to improv th strss stimation. Th main 1

2 èm Congrès Français d Mécaniqu Bsançon, 9 août au sptmbr 11 dvlopmnts in th P.I.A. can b rsumd as follows: - Som intrmdiats configurations, without contact tratmnt, ar gnratd for som givn punch positions to considr th dformation history. - For ach intrmdiat configuration, th strain incrmnt is calculatd by th invrs mthod btwn th prvious and actual configurations. - Th mshs at th last and actual stps ar indpndnt. So at th bginning of th actual stp, a transfr of th strain and strss filds should b carrid out btwn ths two mshs for plastic intgration schm. - An fficint mthod for plastic intgration calld Dirct Scalar Algorithm is dvlopd: th quations in function of unknown strss vctors ar transformd into th scalar quations using th notion of th quivalnt strss; thus th plastic multiplir can b dirctly obtaind without itrations [4]. Th P.I.A. is a good numrical tool for th prliminary prform dsign and optimization for th forging procsss..1.1 Larg strain calculation In th I.A., th calculation of larg strains is don in on stp by dirctly comparing th initial billt C and th final part C and using th logarithmic strains [-3]. Th sam calculation is kpt in th P.I.A. but btwn two succssiv configurations. For an axi-symmtric problm, it is mor convnint to dfin th strains in th local lmnt systm ( x,, z). Th movmnt of a matrial point btwn two succssiv configurations is xprssd by x x u whr x and x ar th initial and final position vctors, u is th displacmnt vctor in th local rfrnc. Thn th invrs dformation gradint tnsor is dfind as follows: x u x x Th invrs Cauchy-Grn lft tnsor in th local rfrnc is dfind by: 1 d x d x I d x F d x L (1) Th ignvalus ( λ, λ, λ ) logarithmic strains: m x x x x B F F d d d B d m 1 T 1 () of th tnsor B 1 m givs th thr principal longations, thn th thr larg ln i i i 1,,3 (3) Finally, ths larg strains ar transformd into th lmnt local rfrnc by: L L x cos sin 1 1 z sin cos 3 xz sin cos sin cos whr is th angl from th local rfrnc to th principal strain rfrnc. (4).1. Intrmdiat configurations and fild transfr Th basic ida of th P.I.A is to us svral intrmdiat configurations and to xcut an invrs calculation btwn two succssiv configurations considring th initial strains and strsss in th last stp. Ths intrmdiat configurations ar dtrmind gomtrically thn corrctd by som itrations of quilibrium. Lt s considr th P.I.A. in two stps (Figur 1). For th configuration C 1, th two mshs ar indpndnt: M 1 1 is th msh cratd thn corrctd at th nd of stp 1, M 1 is th msh obtaind at ach itration of th stp. A transfr of th strain and strss filds should b carrid out btwn ths two mshs on C Simplifid tool actions In th forging procss, th contact tratmnt is oftn unstabl and tim consuming. In th P.I.A., to avoid th

3 èm Congrès Français d Mécaniqu Bsançon, 9 août au sptmbr 11 contact tratmnt, th tool actions ar simply rprsntd by som xtrnal nodal forcs. At a nod, th valu of th rsultant forc is unknown; th dirction of this forc nf can b dtrmind by th friction con and th slid dirction: 1 n f n t (5) 1 whr n is th unit normal vctor on th contour, t th unit vctor of th nod slid displacmnt in th tangnt dirction of th contour, th friction cofficint. In th itration loop, th two intrnal forcs at ach nod k ar known. Th lmnt intrnal forc vctor in th local rfrnc is thn givn by: T int Wint u B rda u F (6) * * n A m n Thus th quilibrium condition allows calculating th unknown intnsity of th rsultant tool action forc F : k k k k k P n r F r F xt F int k k k (7) P n Z F xt Z int k k T whr n n n rprsnts th dirction of th rsultant forc at th nod k. r Z f Initial msh on C A.I. (stp 1) Configuration C 1 at stp 1 Configuration C 1 at stp Msh M 1 Transfr of th strain and strss filds A.I. (stp ) Msh M 1 1 Configuration C at stp Figur 1. Transfr of Filds btwn Two Indpndnt Mshs. FEM adaptiv incrmntal approach Nowadays, in mtal forming procsss th classical FE numrical simulation is usd to avoid xpnsiv xprimnts and many rsarch works hav bn mad using this powrful tool [5]. In th laboratory LASMIS of Univrsity of Tchnology of Troys, xtnsiv works ar don sinc tn yars. A spcific numrical mthodology packag basd on FEM has bn dvlopd to solv lasto- plastic problms with ductil damag in larg strains, such as th numrical simulation of mtal forming procsss. In ordr to avoid larg msh distortions and achiv proprly th solution convrgnc, th mshing and r-mshing procdur ar also includd [6-8]...1 Elasto-plastic constitutiv quations To build th matrial bhaviour modl, w should considr coupld multi-physics (plastic strains, hardning and damag) in th forging procss. W us an advancd constitutiv quations accounting for mixd nonlinar isotropic and kinmatic hardning strongly coupld with ductil isotropic damag. Th coupling btwn th ductil damag and th lasto- plastic constitutiv quations is formulatd in th framwork of th thrmodynamics of irrvrsibl procsss togthr with th Continuum Damag Mchanics (CDM) thory [6-8]. In our study, to simplify th problm and for comparison with th P.I.A., th kinmatic hardning is nglctd and only thr pairs of th intrnal stat variabls ar usd: (, ) for th plastic flow; (r, R) for isotropic hardning and (D, Y) for ductil damag. Whn th currnt configuration contains som ductil damag, th concpt of ffctiv variabls basd on th hypothsis of total nrgy quivalnc is usd. 3

4 èm Congrès Français d Mécaniqu Bsançon, 9 août au sptmbr 11 Accordingly, th fully coupld constitutiv quations ar summarizd as following. 1 D : R 1 D Qr Stat rlation 1 v I II III Y 9v (1 D ) E (Damag) (1 D ) E H 1 1 D Qr Evolution quation J R f y 1 D 1 D (Von Miss plasticity critria) Dp n T with n 1 r br 1 D s Y Y D S 1 D J 3 dv : dv 3 1 D J dv Whr Q is th isotopic hardning modulus; b is th non-linr cofficint; S, s, β and Y ar th matrial cofficints dscribing ductil damag volution; n th outward normal tnsor to th yild surfac f=; y th limit yild strss... Numrical aspct Th fully coupld thrmo-mchanical constitutiv quations prsntd abov hav bn implmntd into Abaqus/Explicit FE cod using th VUMAT usr subroutin. A dynamic xplicit rsolution procdur has bn usd in ordr to solv th quilibrium problm [6-8]. Du to th larg dformations of th matrial, th msh is rapidly distortd. To avoid ths distortions, th rmshing procdur must b adaptd. By using an adaptiv rmshing tchniqu, th msh is rfind in damagd zons and magnifid in inactiv zons. Th rmshing opration is indispnsibl for gomtrically and physically complicatd non-linar forming procss. 3 Numrical application In this papr, a D axisymmtric forging procss is prsntd and th final shap of th whl is shown in Figur. Bcaus of symmtry conditions, only a quartr of th axisymmtric part was modld. A st of boundary conditions of symmtry wr usd: th lowr horizontal plan is fixd and th uppr tool is translatd with a constant vlocity. Th total uppr punch travl quals to 6mm. Figur. Shap of th final billt Th matrial of th whl is aluminium whos mchanical proprtis ar dfind as follows: Young's modulus E = 73 (MPa), Poisson's ratio =.3, friction cofficint btwn th tool-billt µ=.5. Th matrial bhaviour modls usd by th two simulation mthods ar a littl diffrnt. For th 4

5 èm Congrès Français d Mécaniqu Bsançon, 9 août au sptmbr 11 P.1783 P.I.A., th Hollomon strss-strain curv is usd: 17.68( ) MPa. By FEM adaptiv incrmntal approach, an advancd lasto-plastic constitutiv quation is usd by implmnting VUMAT usr subroutin in th calculation and th paramtrs using ar y =71(MPa), Q=3(MPa), b=3, S=1, s=1, =5 and Y =. Hr w don t tak into account th influnc of tmpratur. Although th two mthods us diffrnt matrial bhaviour modl, th final strss-strain curv of th matrial is almost th sam. 3.1 Analysis of th numrical simulation rsults Distribution of th quivalnt plastic strain and quivalnt strss Figur 3 shows th distributions of th quivalnt plastic strain obtaind by th P.I.A. and FEM adaptiv incrmntal approach. For th P.I.A., th billt is mshd with 1371 axisymmtric triangl lmnts. For th mthod of th FEM adaptiv rmshing procdur, th billt is mshd with a quadrilatral lmnt CAX4R and th whol procss includs 5 rmshing stps. Th initial numbr of th lmnt is 344 and th final numbr of th lmnt incras to 163; th maximum msh siz is 3mm and th minimum msh siz is.9mm. With th dformation incrasing, th msh is rfind du to th larg strain. This adaptiv rmshing tchnology avoids th lmnt distortion during th larg dformation mtal-forming procss. In Figur 3, w also obsrv that th strain distributions of th two mthods ar vry similar to ach othr. Both th maximum and minimum valus ar situatd in th sam locations. Th maximum plastic quivalnt strains obtaind by th P.I.A. and incrmntal approach ar rspctivly.919 and.91. a. Psudo invrs approach b. FEM adaptiv incrmntal approach Figur 3. Equivalnt plastic strain obtaind by P.I.A. and A.I.A. a. Psudo invrs approach b. FEM adaptiv incrmntal approach Figur 4. Equivalnt strss obtaind by P.I.A. and A.I.A. 5

6 èm Congrès Français d Mécaniqu Bsançon, 9 août au sptmbr 11 Figur 4 shows th distributions of th quivalnt strss obtaind by th P.I.A. and adaptiv incrmntal approach. W not that th two strss distributions ar similar. Th maximum valus ar vry clos to ach othr (167.8 and MPa), but th minimum valus ar fairly diffrnt Comparison of th CPU tim Th incrmntal approach is widly usd for th forging procss modlling and it givs good strain and strss stimation. But compard to th Psudo Invrs Approach, th incrmntal approach is vry tim consuming. Th total CPU tim usd for th simulation of th whl is 145 s by th incrmntal approach but only 3 s by P.I.A. (78% of tim saving). In traditional Invrs Approach, two basic assumptions ar usd: th assumption of proportional loading (for cold forging) givs an intgratd constitutiv law without considring th strain path nithr th viscoplasticity, and th assumption of simplifid tool-billt actions allows on to rplac th tool actions by nodal forcs without contact tratmnt. Ths two assumptions mak th I.A. calculation vry fast. Th P.I.A. (or multi-stp invrs approach) basd on th I.A. kps th I.A. s high fficincy but givs good strss stimation owing to th loading history considration. In th FEM adaptiv rmshing mthod, an advancd lasto-plastic matrial bhaviour modl and th fac to fac contract condition ar usd, so th whol procss is tim consuming. 4 Conclusion By comparing with th rsults of th two diffrnt mtal forming simulation mthods, w can find that th rsults of Psudo Invrs Approach hav a good agrmnt with th rsults of classical adaptiv incrmntal approach and th psudo Invrs Approach is provd to b vry tim saving. So in th cas of th complicat tools shap or vry larg dformation mtal forming procss, th adaptiv incrmntal approach should b usd to gt accurat rsults; in th cas of th prliminary prform dsign and optimization for th forging procss modlling, th P.I.A. provs to b vry usful and highly fficint. Rfrncs [1] W.Gati, Y.Q. Guo, H. Nacur, J.L. Batoz, Approch psudo invrs pour stimation ds contraints dans ls piècs mboutis axisymétriqus, Rvu Europénn ds Elémnts Finis, Vol. 1, n 7-8, pp , 3. [] A. Halouani, Y.M. Li, B. Abbès, Y.Q. Guo. An Axisymmtric Invrs Approach for Cold Forging Modlling, Enginring Lttrs, Vol. 18, Issu 4, pp , 1. [3] A. Halouani, Y.M. Li, B. Abbès, Y.Q. Guo. Simulation of axi-symmtrical forging procss by Invrs Approach, Matrials Scinc Forum Vols (11) pp [4] Y.M. Li, B. Abbs, Y.Q. Guo. Two Efficint Algorithms of Plastic Intgration for sht Forming Modlling, ASME J. Manufacturing Scinc and Tchnology, Vol. 19, p , [5] M. Issa M., K. Saanouni, C. Labrgèr, A. Rassinux, Prdiction of srratd chip formation in orthogonal mtal cutting by advancd adaptiv D numrical mthodology., Int. J. Machining and Machinability of Matrial,Vol 9., Nos ¾, 11 [6] Labrgr C., Rassinux A., Saanouni K., D adaptiv msh mthodology for th simulation of mtal forming procsss with damag, DOI 1.17/s z, articl in Prss, 11 [7] Labrgr C., Lstriz P., Saanouni K. Numrical dsign of xtrusion procss using finit thrmolastoviscoplasticity with damag. Prdiction of chvron shapd cracks, Ky Enginring Matrials, Vol 44, pags 65-7, 1 [8] J. Mariag, K. Saanouni, P. Lstriz, A. Chrouat, Numrical simulation of ductil damag in mtal forming procsss. A simpl prdictiv modl. 1.thortical and numrical aspcts, Int. J. Form. Procss. 5 ( 4) ()

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA * 17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High

More information

AS 5850 Finite Element Analysis

AS 5850 Finite Element Analysis AS 5850 Finit Elmnt Analysis Two-Dimnsional Linar Elasticity Instructor Prof. IIT Madras Equations of Plan Elasticity - 1 displacmnt fild strain- displacmnt rlations (infinitsimal strain) in matrix form

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

More information

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology Bluchr Mchanical Enginring Procdings May 2014, vol. 1, num. 1 www.procdings.bluchr.com.br/vnto/10wccm TOPOLOGY DESIG OF STRUCTURE LOADED BY EARTHQUAKE P. Rosko 1 1 Cntr of Mchanics and Structural Dynamics,

More information

Finite Strain Elastic-Viscoplastic Model

Finite Strain Elastic-Viscoplastic Model Finit Strain Elastic-Viscoplastic Modl Pinksh Malhotra Mchanics of Solids,Brown Univrsity Introduction Th main goal of th projct is to modl finit strain rat-dpndnt plasticity using a modl compatibl for

More information

Instantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect

Instantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect Advancd Matrials sarch Onlin: -8-6 ISS: 66-8985, Vols. 34-36, pp 389-39 doi:.48/www.scintific.nt/am.34-36.389 rans ch Publications, Switzrland Instantanous Cutting Forc Modl in High-Spd Milling Procss

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

On the Hamiltonian of a Multi-Electron Atom

On the Hamiltonian of a Multi-Electron Atom On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula 7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting

More information

Finite Element Model of a Ferroelectric

Finite Element Model of a Ferroelectric Excrpt from th Procdings of th COMSOL Confrnc 200 Paris Finit Elmnt Modl of a Frrolctric A. Lópz, A. D Andrés and P. Ramos * GRIFO. Dpartamnto d Elctrónica, Univrsidad d Alcalá. Alcalá d Hnars. Madrid,

More information

Finite element discretization of Laplace and Poisson equations

Finite element discretization of Laplace and Poisson equations Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th

More information

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

Linear Non-Gaussian Structural Equation Models

Linear Non-Gaussian Structural Equation Models IMPS 8, Durham, NH Linar Non-Gaussian Structural Equation Modls Shohi Shimizu, Patrik Hoyr and Aapo Hyvarinn Osaka Univrsity, Japan Univrsity of Hlsinki, Finland Abstract Linar Structural Equation Modling

More information

4.2 Design of Sections for Flexure

4.2 Design of Sections for Flexure 4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

VSMN30 FINITA ELEMENTMETODEN - DUGGA

VSMN30 FINITA ELEMENTMETODEN - DUGGA VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

3-D SQCE Model and Its Application in Fracture Mechanics *

3-D SQCE Model and Its Application in Fracture Mechanics * 3-D SQCE Modl and Its Application in Fractur Mchanics * Zhichao Wang Sr. ad Enginr Applid Mchanics Dpt., Emrson Climat Tchnology, USA Tribikram Kundu - Profssor Enginring Mchanics Dpt.,Th Univrsity of

More information

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

More information

An adaptive Strategy for the Multi-scale Analysis of Plate and Shell Structures with Elasto-plastic Material Behaviour

An adaptive Strategy for the Multi-scale Analysis of Plate and Shell Structures with Elasto-plastic Material Behaviour TECHNISCHE MECHANIK, 36, 1-2, (2016), 142 154 submittd: Sptmbr 7, 2015 An adaptiv Stratgy for th Multi-scal Analysis of Plat and Shll Structurs with Elasto-plastic Matrial Bhaviour W Wagnr, F Gruttmann

More information

Direct Approach for Discrete Systems One-Dimensional Elements

Direct Approach for Discrete Systems One-Dimensional Elements CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME Introduction to Finit Elmnt Analysis Chaptr 5 Two-Dimnsional Formulation Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

ME469A Numerical Methods for Fluid Mechanics

ME469A Numerical Methods for Fluid Mechanics ME469A Numrical Mthods for Fluid Mchanics Handout #5 Gianluca Iaccarino Finit Volum Mthods Last tim w introducd th FV mthod as a discrtization tchniqu applid to th intgral form of th govrning quations

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

Finite Element Models for Steady Flows of Viscous Incompressible Fluids

Finite Element Models for Steady Flows of Viscous Incompressible Fluids Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

NONLINEAR ANALYSIS OF PLATE BENDING

NONLINEAR ANALYSIS OF PLATE BENDING NONLINEAR ANALYSIS OF PLATE BENDING CONTENTS Govrning Equations of th First-Ordr Shar Dformation thor (FSDT) Finit lmnt modls of FSDT Shar and mmbran locking Computr implmntation Strss calculation Numrical

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

High Energy Physics. Lecture 5 The Passage of Particles through Matter

High Energy Physics. Lecture 5 The Passage of Particles through Matter High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information

Une famille d algorithmes robustes pour l intégration de modèles de plasticité cristalline

Une famille d algorithmes robustes pour l intégration de modèles de plasticité cristalline Un famill d algorithms robusts pour l intégration d modèls d plasticité cristallin Andry Musinko, Nikolay Osipov, Gorgs Cailltaud Cntr ds Matriaux/Mins Paris, Paristch, CNRS UMR 7633, B.P. 87, 91003 Evry

More information

A New Approach to the Fatigue Life Prediction for Notched Components Under Multiaxial Cyclic Loading. Zhi-qiang TAO and De-guang SHANG *

A New Approach to the Fatigue Life Prediction for Notched Components Under Multiaxial Cyclic Loading. Zhi-qiang TAO and De-guang SHANG * 2017 2nd Intrnational Conrnc on Applid Mchanics, Elctronics and Mchatronics Enginring (AMEME 2017) ISBN: 978-1-60595-497-4 A Nw Approach to th Fatigu Li Prdiction or Notchd Componnts Undr Multiaxial Cyclic

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

THE ANALYSIS OF THE ITERATIONS PROCESS IN THE ELASTO-PLASTIC STRESS MODEL

THE ANALYSIS OF THE ITERATIONS PROCESS IN THE ELASTO-PLASTIC STRESS MODEL Plas cit this articl as: Joanna Wróbl, Adam Kulawik, Th analysis of th itrations procss in th lasto-plastic strss modl, Scintific Rsarch of th Institut of Mathmatics and Computr Scinc, 2012, Volum 11,

More information

ME311 Machine Design

ME311 Machine Design ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform

More information

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers: APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding

More information

Selective Mass Scaling (SMS)

Selective Mass Scaling (SMS) Slctiv Mass Scaling (SMS) Thory and Practic Thomas Borrvall Dynamor Nordic AB Octobr 20 LS DYNA information Contnt Background Is SMS nwsworthy? Thory and Implmntation Diffrnc btwn CMS and SMS Undr th hood

More information

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

More information

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):. Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions

More information

Scattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential

Scattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential Commun. Thor. Phys. 66 06 96 00 Vol. 66, No., August, 06 Scattring Stats of l-wav Schrödingr Equation with Modifid Rosn Mors Potntial Wn-Li Chn í,, Yan-Wi Shi á, and Gao-Fng Wi Ôô, Gnral Education Cntr,

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

3 Finite Element Parametric Geometry

3 Finite Element Parametric Geometry 3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,

More information

Higher-Order Discrete Calculus Methods

Higher-Order Discrete Calculus Methods Highr-Ordr Discrt Calculus Mthods J. Blair Prot V. Subramanian Ralistic Practical, Cost-ctiv, Physically Accurat Paralll, Moving Msh, Complx Gomtry, Slid 1 Contxt Discrt Calculus Mthods Finit Dirnc Mimtic

More information

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018 Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

More information

Symmetric centrosymmetric matrix vector multiplication

Symmetric centrosymmetric matrix vector multiplication Linar Algbra and its Applications 320 (2000) 193 198 www.lsvir.com/locat/laa Symmtric cntrosymmtric matrix vctor multiplication A. Mlman 1 Dpartmnt of Mathmatics, Univrsity of San Francisco, San Francisco,

More information

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions. Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind

More information

INC 693, 481 Dynamics System and Modelling: Linear Graph Modeling II Dr.-Ing. Sudchai Boonto Assistant Professor

INC 693, 481 Dynamics System and Modelling: Linear Graph Modeling II Dr.-Ing. Sudchai Boonto Assistant Professor INC 69, 48 Dynamics Systm and Modlling: Linar Graph Modling II Dr.-Ing. Sudchai Boonto Assistant Profssor Dpartmnt of Control Systm and Instrumntation Enginring King Mongkut s Unnivrsity of Tchnology Thonuri

More information

16. Electromagnetics and vector elements (draft, under construction)

16. Electromagnetics and vector elements (draft, under construction) 16. Elctromagntics (draft)... 1 16.1 Introduction... 1 16.2 Paramtric coordinats... 2 16.3 Edg Basd (Vctor) Finit Elmnts... 4 16.4 Whitny vctor lmnts... 5 16.5 Wak Form... 8 16.6 Vctor lmnt matrics...

More information

Chapter 2 BASIC EQUATIONS OF NONLINEAR CONSTITUTIVE MODELS

Chapter 2 BASIC EQUATIONS OF NONLINEAR CONSTITUTIVE MODELS Chaptr BASIC EQUATIONS OF NONLINEAR CONSTITUTIVE MODELS TYPES OF NONLINEAR CONSTITUTIVE MODELS Gomatrials ar charactrizd by nonlinar strss-strain bhavior and, oftn, by tim-dpndnt dformations. Th nonlinar

More information

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

An Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method

An Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method Amrican Journal of Applid Scincs 4 (1): 95-956, 7 ISSN 1546-939 7 Scinc Publications An Invstigation on th Effct of th Coupld and Uncoupld Formulation on Transint Spag by th Finit Elmnt Mthod 1 Ahad Ouria,

More information

2.5D Green s functions for transient heat transfer by conduction and convection

2.5D Green s functions for transient heat transfer by conduction and convection .5D Grn s functions for transint hat transfr by conduction and convction A. Tadu & N. Simõs Dpartmnt of Civil Enginring, Univrsity of Coimbra, Portugal Abstract This papr prsnts fundamntal solutions for

More information

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a 204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of

More information

3D ELECTRODE SHAPE CHANGE SIMULATION IN ELECTROPLATING

3D ELECTRODE SHAPE CHANGE SIMULATION IN ELECTROPLATING 3D ELECTRODE SHAPE CHANGE SIMULATION IN ELECTROPLATING MARIUS PURCAR 1, CALIN MUNTEANU, VASILE TOPA Ky words: Elctroplating, 3D modling, Elctrod shap chang, Potntial modl, Boundary lmnt mthod. This papr

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Unfired pressure vessels- Part 3: Design

Unfired pressure vessels- Part 3: Design Unfird prssur vssls- Part 3: Dsign Analysis prformd by: Analysis prformd by: Analysis vrsion: According to procdur: Calculation cas: Unfird prssur vssls EDMS Rfrnc: EF EN 13445-3 V1 Introduction: This

More information

Finite Element Analysis of Magneto-Superelastic Behavior of Shape Memory Alloy Composite Actuator

Finite Element Analysis of Magneto-Superelastic Behavior of Shape Memory Alloy Composite Actuator Procdings of th Intrnational MultiConfrnc of Enginrs and Computr cintists 28 Vol II IMEC 28, 19-21 March, 28, Hong Kong Finit Elmnt Analysis of Magnto-uprlastic Bhavior of hap Mmory Alloy Composit Actuator

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

COUPLED THERMOMECHANICAL BEHAVIOUR FOR METAL CASTING FE ANALYSIS

COUPLED THERMOMECHANICAL BEHAVIOUR FOR METAL CASTING FE ANALYSIS Int. Conf. on Computational Mthods for Coupld Problms in cinc and Enginring COUPLED PROBLEM 2005 M. Papadrakakis, E. Oñat and B. chrflr (Eds) CIMNE, Barclona, 2005 COUPLED THERMOMECHANICAL BEHAVIOUR FOR

More information

Keywords- Active vibration control, cantilever composite beam, Newmark-β method

Keywords- Active vibration control, cantilever composite beam, Newmark-β method Pratik K. Gandhi, J. R. Mvada / Intrnational Journal of Enginring Rsarch and Applications (IJERA) ISSN: 8-96 www.ijra.com Vol., Issu, May-Jun, pp.9-95 A Finit Elmnt Modl And Activ Vibration Control Of

More information

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea 2017 Watr Ractor Ful Prformanc Mting Sptmbr 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jju Jju Island, Kora Study of Ful Rod Bhavior with Missing Pllt Surfac Dfct Zhnhai Liu 1, Yi Zhou 1, Ping Chn 1, Yuanming

More information

Multi-scale Analysis of Void Closure for Heavy Ingot Hot Forging

Multi-scale Analysis of Void Closure for Heavy Ingot Hot Forging Modrn Applid Scinc; ol. 6, No. ; ISSN 9-844 E-ISSN 9-85 Publishd by Canadian Cntr of Scinc and Education Multi-scal Analysis of oid Closur for Havy Ingot Hot Forging Xiaoxun Zhang, Fang Ma, Kai Ma & Xia

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

Abstract Interpretation: concrete and abstract semantics

Abstract Interpretation: concrete and abstract semantics Abstract Intrprtation: concrt and abstract smantics Concrt smantics W considr a vry tiny languag that manags arithmtic oprations on intgrs valus. Th (concrt) smantics of th languags cab b dfind by th funzcion

More information

FINITE BEAM ELEMENT WITH PIEZOELECTRIC LAYERS AND FUNCTIONALLY GRADED MATERIAL OF CORE

FINITE BEAM ELEMENT WITH PIEZOELECTRIC LAYERS AND FUNCTIONALLY GRADED MATERIAL OF CORE ECCOMAS Congrss 20 II Europan Congrss on Computational Mthods in Applid Scincs and Enginring M. Papadrakakis,. Papadopoulos, G. Stfanou,. Plvris (ds.) Crt Island, Grc, 5 0 Jun 20 FINITE BEAM ELEMENT WITH

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

Analysis of potential flow around two-dimensional body by finite element method

Analysis of potential flow around two-dimensional body by finite element method Vol. 7(2), pp. 9-22, May, 2015 DOI: 10.5897/JMER2014.0342 rticl Numbr: 20E80053033 ISSN 2141 2383 Copyright 2015 uthor(s) rtain th copyright of this articl http://www.acadmicjournals.org/jmer Journal of

More information

INC 693, 481 Dynamics System and Modelling: The Language of Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Professor

INC 693, 481 Dynamics System and Modelling: The Language of Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Professor INC 693, 48 Dynamics Systm and Modlling: Th Languag o Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Prossor Dpartmnt o Control Systm and Instrumntation Enginring King Mongkut s Unnivrsity o Tchnology

More information

Topology Optimization of Suction Muffler for Noise Attenuation

Topology Optimization of Suction Muffler for Noise Attenuation Purdu Univrsity Purdu -Pubs Intrnational Comprssor Enginring Confrnc School of Mchanical Enginring 2012 Topology Optimization of Suction Mufflr for Nois Attnuation Jin Woo L jinwool@ajou.ac.kr Dong Wook

More information

Contemporary, atomic, nuclear, and particle physics

Contemporary, atomic, nuclear, and particle physics Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE507 - Plasma Physics and Applications Lctur 7 Prof. Jorg Rocca and Dr. Frnando Tomasl Dpartmnt of Elctrical and Computr Enginring Collisional and radiativ procsss All particls in a plasma intract with

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

An Efficiency Substructure Method for Nonlinear SSI Analysis of Large-scale Concrete Structures in Time Domain on the ANSYS Platform

An Efficiency Substructure Method for Nonlinear SSI Analysis of Large-scale Concrete Structures in Time Domain on the ANSYS Platform An Efficincy Substructur Mthod for Nonlinar SSI Analysis of Larg-scal Concrt Structurs in Tim Domain on th ANSYS Platform J. B. Li, X. Q. Yin, G. Lin School of Civil and Hydraulic Enginring, Dalian Univrsity

More information

Fixed-Point Harmonic-Balanced Method for Nonlinear Eddy Current Problems

Fixed-Point Harmonic-Balanced Method for Nonlinear Eddy Current Problems Intrnational Journal of Enrgy and Powr Enginring 206; 5(-): 37-4 Publishd onlin Octobr 4, 205 (http://www.scincpublishinggroup.com/j/ijp) doi: 0.648/j.ijp.s.2060500.5 ISSN: 2326-957X (Print); ISSN: 2326-960X

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark. . (a) Eithr y = or ( 0, ) (b) Whn =, y = ( 0 + ) = 0 = 0 ( + ) = 0 ( )( ) = 0 Eithr = (for possibly abov) or = A 3. Not If th candidat blivs that = 0 solvs to = 0 or givs an tra solution of = 0, thn withhold

More information

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt

More information

Section 11.6: Directional Derivatives and the Gradient Vector

Section 11.6: Directional Derivatives and the Gradient Vector Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th

More information