Application of MS-Excel Solver to Non-linear Beam Analysis
|
|
- Jocelin Stephens
- 6 years ago
- Views:
Transcription
1 / Application of S-cl Solr to Non-linar Bam Analysis Toshimi Taki arch 4, 007 April 8, 007, R. A. ntroction Sprasht softwar in crrnt prsonal comptrs is high prformanc an th softwar has nogh fnctions for application to nginring prolms. lop a mtho to sol non-linar strctral prolms y optimization fnction Solr of S-cl.. S-cl Solr Th most poplar sprasht softwar, S-cl has an a-in tool call Solr which prforms nmrical optimization. Solr fins paramtrs to optimiz ojcti al with mltipl constraints. W can s Solr to sol strctral prolms applying principl of total potntial nrgy or principl of total complimntary nrgy.. qations Non-linar Bam lmnt Bam strctr is iscrtiz to lmnts as finit lmnt mtho (F). Thn, total potntial nrgy is calclat. Shap fnction is th sam as F formlation. This mans that th formlation is th sam as F, t w on t n to prform ariational opration. W jst n to calclat strain nrgy of ach am lmnt an sm p th strain nrgy for all th lmnts. Following formlation show strain nrgy of -imntional am lmnt. s () Bam lmnt Assm that proprtis of a am lmnt as follows. niform cross sction in a lmnt. Sction Ara, A, omnt of nrtia,, ngth, Yong s ols, As shown in figr, following symols ar s., y flction an rotation at Gri in lmnt coorinats for flction: (,, ), y flction an rotation at Gri in lmnt coorinats for flction: (,, ) (, ) -φ 0 y -φ y φ (, ) 0 Figr. Bam lmnt () Bning Dflction of lmnt, is prss as follows.
2 / c ) (, c, at 0,, c 0 at, c a, a Soling th qations, ( ) a, ( ) c, Strain nrgy for ning is prss as follows. ( ) ( ) 0 0 a a To calclat shar forc an ning momnt, s following am qations. Shar forc an ning momnt at Gri, (V, ) Shar forc an ning momnt at Gri, (V, ) qation of am: c V, V V, V () tnsion ngth aftr flction is prss as follows. ( ) ( ) ' tnsion is, ( ) ( ) Strain nrgy is, A
3 / To calclat ial forc at Gri, P an Gri, P, s following qations. P A P P, (4) Consiration of Gomtrical Non-linarity in Coorinat Systm aftr Dformation lmnt coorinat systm aftr flction is consir as shown in figr. lmnt fctions in lmnt coorinat systm aftr flction,, com zro an strain nrgy for ning of th lmnt is prss as follows. a, ' ' ' ', c ', 0 whr, ' φ, ' φ φ is angl twn lmnt coorinat aftr an for flction. Thn, strain nrgy for ning (gomtrical non-linarity is consir), is prss in th following qation. ( a a ) (5) Total Potntial nrgy Total potntial nrgy of th lmnt, total is prss as th following qation. total ( ) ( P Py z z) all lmnts all trnal forcs sing flctions an rotations at all gris as paramtrs, minimiz total potntial nrgy, total y Solr of S-cl, thn yo will ha th soltion. 4. ampl Prolm lastica Post-ckling flction of a simply spport am nr ial forc is analyz. This prolm is a typical gomtrically non-linar prolm known as lastica. Analytical soltion is aailal for lastica an th rslt of th prsnt mtho is compar with th analytical soltion. A am with niform cross sction is ii to 0 lmnts as shown in figr. A tmplat of S-cl to calclat total potntial nrgy was lop. Thn, th total potntial nrgy was minimiz y Solr.
4 4/ y, lmnt D oa , Gri D Figr. ol for lastica Figr shows flction shap for arios ial forcs. Figr 4 shows rlationship twn cntr flction an ial forc. Cntr flction an ial forc ar normaliz with am lngth, an ckling loa, P cr, rspctily. act analytical soltion is shown in th figr for comparison (rfrnc []) y/ / Figr. Dflction Shap
5 5/.. act Soltion Propos tho P/Pcr m/ Figr 4. Rlationship twn Cntr Dflction an Aial Forc 5. Othr Applications Th mtho introc in this papr can appli to following prolms in aircraft strctral analysis. lop th mtho 0 yars ago an ha appli to many prolms of actal aircraft strctral analysis. Trss (linar, or gomtrically non-linar) Bam an Ramn (linar, or gomtrically non-linar) Bolt Joint (linar) Bam Colmn (gomtrically non-linar) -imnsional lastic Prolms (linar, or gomtrically non-linar) Shar Fil Prolms (linar)
6 /. Conclsions Th mtho prsnt in this papr has following fatrs an pct that th mtho will wily s in th aircraft instry. Straight forwar mtho. Spcial tchniq an tios iation of qations ar not ncssary to sol non-linar prolms. No spcial programs ar rqir. Gnral prpos sprasht softwar is s. Applical to actal aircraft strctral analysis. sfl to cation of nrgy mtho. 7. Rfrncs [] C.. Dym an. H. Shams, Soli chanics, A Variational Approach
Potential energy of a structure. Vforce. joints j
Potntial nrgy of a strctr P y P x y x P y P x ij ij ij V K ( ) Vforc P V ij ij j j K ( ) P [ K] r Elastic Potntial nrgy of mmbr ij Potntial nrgy of applid forc at joint i i i i mmbrs joints j Find th st
More informationProper Orthogonal Decomposition for simulating the alongwind Equivalent Static Force of long-span bridges
Propr Orthogonal Dcomposition for simlating th alongwin Eqivalnt Static orc of long-span brigs Alssanra ior, Pitro Monaco Politcnico i Bari, Dpartmnt of ivil an Environmntal Enginring, a.fior@poliba.it,
More informationHydrogen Atom and One Electron Ions
Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial
More informationFinite Element Analysis
Finit Elmnt Analysis L4 D Shap Functions, an Gauss Quaratur FEA Formulation Dr. Wiong Wu EGR 54 Finit Elmnt Analysis Roamap for Dvlopmnt of FE Strong form: govrning DE an BCs EGR 54 Finit Elmnt Analysis
More informationMiddle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis
Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 4 Introduction to Finit Elmnt Analysis Chaptr 4 Trusss, Bams and Frams Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationDivision 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 informationa 1and x is any real number.
Calcls Nots Eponnts an Logarithms Eponntial Fnction: Has th form y a, whr a 0, a an is any ral nmbr. Graph y, Graph y ln y y Th Natral Bas (Elr s nmbr): An irrational nmbr, symboliz by th lttr, appars
More informationMechanical Properties
Mchanical Proprtis Elastic dformation Plastic dformation Fractur Mchanical Proprtis: Th Tnsion Tst s u P L s s y ΔL I II III For matrials proprtis, rplac load-dflction by strss-strain Enginring strss,
More informationImage Enhancement in the Spatial Domain
s=tr Eampl PR3.: Eponntials of th form -ar a a positi constant ar sfl for constrcting smooth gra-ll transformation fnctions. Constrct th transformation fnctions haing th gnral shaps shown in th following
More informationVSMN30 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 information10. 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 informationDynamic 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 informationDifferential Equations
UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs
More informationMultiple-Choice Test Introduction to Partial Differential Equations COMPLETE SOLUTION SET
Mltipl-Choic Tst Introdction to Partial Diffrntial Eqations COMPLETE SOLUTION SET 1. A partial diffrntial qation has (A on indpndnt variabl (B two or mor indpndnt variabls (C mor than on dpndnt variabl
More informationContent Skills Assessments Lessons. Identify, classify, and apply properties of negative and positive angles.
Tachr: CORE TRIGONOMETRY Yar: 2012-13 Cours: TRIGONOMETRY Month: All Months S p t m b r Angls Essntial Qustions Can I idntify draw ngativ positiv angls in stard position? Do I hav a working knowldg of
More informationy cos x = cos xdx = sin x + c y = tan x + c sec x But, y = 1 when x = 0 giving c = 1. y = tan x + sec x (A1) (C4) OR y cos x = sin x + 1 [8]
DIFF EQ - OPTION. Sol th iffrntial quation tan +, 0
More informationCOMPUTATATION OF INCOMPRESSIBLE TURBULENT BOUNDARY LAYER WITH FAVORABLE AND ADVERSE PRESSURE GRADIENT AT HIGH REYNOLDS NUMBERS UDC :532.
ACTA NIVERITATI ris: Mchanics Atomatic Control an Robotics Vol N o pp 7 - COMPTATATION O INCOMPREIBLE TRBLENT BONDARY LAYER WITH AVORABLE AND ADVERE PRERE GRADIENT AT HIGH REYNOLD NMBER DC 7: Miloš M Jovanović
More information3 2D Elastostatic Problems in Cartesian Coordinates
D lastostatic Problems in Cartesian Coordinates Two dimensional elastostatic problems are discssed in this Chapter, that is, static problems of either plane stress or plane strain. Cartesian coordinates
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 informationThomas Whitham Sixth Form
Thomas Whitham Sith Form Pur Mathmatics Cor rvision gui Pag Algbra Moulus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv blow th ais in th ais. f () f () f
More informationHomotopy 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 informationGabor window grid (900 samples) dual window (grid) dual window (quincunx) quincunx (800 samples)
alclating th dal Gabor window for gnral sampling sts Ptr Prinz Univrsitat Win, Institt f Mathmatik, U H A G Strdlhofgass 4 tl: ++43 / / 448 695 fax: ++43 / / 448 697 -mail: prinztychmatniviacat Abstract
More informationThomas Whitham Sixth Form
Thomas Whitham Sith Form Pur Mathmatics Unit C Algbra Trigonomtr Gomtr Calculus Vctor gomtr Pag Algbra Molus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv
More informationFEA Solution Procedure
EA Soltion Procedre (demonstrated with a -D bar element problem) EA Procedre for Static Analysis. Prepare the E model a. discretize (mesh) the strctre b. prescribe loads c. prescribe spports. Perform calclations
More informationBackground: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.
Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby
More informationThat 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 informationNotes on Differential Geometry
Nots from phz 6607, Spcial an Gnral Rlativity Univrsity of Floria, Fall 2004, Dtwilr Nots on Diffrntial Gomtry Ths nots ar not a substitut in any mannr for class lcturs. Plas lt m know if you fin rrors.
More informationSelf-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016
Ronald I. Frank 06 Adjoint https://n.wikipdia.org/wiki/adjoint In gnral thr is an oprator and a procss that dfin its adjoint *. It is thn slf-adjoint if *. Innr product spac https://n.wikipdia.org/wiki/innr_product_spac
More informationSME 3033 FINITE ELEMENT METHOD. Bending of Prismatic Beams (Initial notes designed by Dr. Nazri Kamsah)
Bnding of Prismatic Bams (Initia nots dsignd by Dr. Nazri Kamsah) St I-bams usd in a roof construction. 5- Gnra Loading Conditions For our anaysis, w wi considr thr typs of oading, as iustratd bow. Not:
More informationTotal Wave Function. e i. Wave function above sample is a plane wave: //incident beam
Total Wav Function Wav function abov sampl is a plan wav: r i kr //incidnt bam Wav function blow sampl is a collction of diffractd bams (and ): r i k r //transmittd bams k ks W nd to know th valus of th.
More informationThe Interlaminar Stress of Laminated Composite under Uniform Axial Deformation
Moling an umrical Simulation of Matrial Scinc, 23, 3, 49-6 http://x.oi.org/.4236/mnsms.23.327 Publish Onlin April 23 (http://www.scirp.org/journal/mnsms) 49 Th Intrlaminar Strss of Laminat Composit unr
More informationElectron energy in crystal potential
Elctron nry in crystal potntial r r p c mc mc mc Expand: r r r mc mc mc r r p c mc mc mc r pc m c mc p m m m m r E E m m m r p E m r nr nr whr: E V mc E m c Wav quation Hamiltonian: Tim-Indpndnt Schrodinr
More informationA Practical Fuzzy Logic Controller for the Path Tracking of Wheeled Mobile Robots
APPLICATION NOTES A Practical Fzzy Logic Controllr for th Path Tracking of Whld Mobil Robots By T.H. L, H.K. Lam, F.H.F. Lng, and P.K.S. Tam T his articl tackls th path-tracking problm of whld mobil robots
More information9 Kinetic Theory of Gases
Contnt 9 Kintic hory of Gass By Liw Sau oh 9. Ial gas quation 9. rssur of a gas 9. Molcular kintic nrgy 9.4 h r..s. sp of olculs 9.5 Dgrs of fro an law of quipartition of nrgy 9.6 Intrnal nrgy of an ial
More informationSIGNIFICANCE OF SMITH CHART IN ANTENNA TECHNOLOGY
SIGNIFICANCE OF SMITH CHART IN ANTENNA TECHNOLOGY P. Poornima¹, Santosh Kumar Jha² 1 Associat Profssor, 2 Profssor, ECE Dpt., Sphoorthy Enginring Collg Tlangana, Hyraba (Inia) ABSTRACT This papr prsnts
More informationIterative Learning Control for Periodic Systems using Model Predictive Methods with adaptive sampling rates
Prprints of th 19th Worl Congrss Th Intrnational Fration of Atomatic Control Cap Town, Soth Africa. Agst 4-9, 14 Itrativ Larning Control for Prioic Systms sing Mol Prictiv Mthos with aaptiv sampling rats
More informationvon Neumann-Wigner theorem: level s repulsion and degenerate eigenvalues.
von Numann-Wignr thorm: lvl s rpulsion an gnrat ignvalus. Yu.N.Dmkov an P.Kurasov Abstract. Spctral proprtis of Schröingr oprators with point intractions ar invstigat. Attntion is focus on th intrplay
More informationSurface wave in ZnO/SiO 2 /Si piezoelectric structure
Availabl onlin at www.scincdirct.com hysics hysics rocdia rocdia 2 (2009) (2008) 1385 1390 000 000 www.lsvir.com/locat/procdia www.lsvir.com/locat/xxx rocdings of th JMSM 2008 onfrnc Srfac wav in ZnO/SiO
More informationAS 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 informationPhys 402: Nonlinear Spectroscopy: SHG and Raman Scattering
Rquirmnts: Polariation of Elctromagntic Wavs Phys : Nonlinar Spctroscopy: SHG and Scattring Gnral considration of polariation How Polarirs work Rprsntation of Polariation: Jons Formalism Polariation of
More informationLinear 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 information22/ 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 information11/13/17. directed graphs. CS 220: Discrete Structures and their Applications. relations and directed graphs; transitive closure zybooks
dirctd graphs CS 220: Discrt Strctrs and thir Applications rlations and dirctd graphs; transiti closr zybooks 9.3-9.6 G=(V, E) rtics dgs dgs rtics/ nods Edg (, ) gos from rtx to rtx. in-dgr of a rtx: th
More informationY 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall
Staning Wav Intrfrnc btwn th incint & rflct wavs Staning wav A string with on n fix on a wall Incint: y, t) Y cos( t ) 1( Y 1 ( ) Y (St th incint wav s phas to b, i.., Y + ral & positiv.) Rflct: y, t)
More information08.06 Shooting Method for Ordinary Differential Equations
8.6 Shooting Method for Ordinary Differential Eqations After reading this chapter, yo shold be able to 1. learn the shooting method algorithm to solve bondary vale problems, and. apply shooting method
More informationNonlinear Bending of Strait Beams
Nonlinar Bnding of Strait Bams CONTENTS Th Eulr-Brnoulli bam thory Th Timoshnko bam thory Govrning Equations Wak Forms Finit lmnt modls Computr Implmntation: calculation of lmnt matrics Numrical ampls
More informationConstants and Conversions:
EXAM INFORMATION Radial Distribution Function: P 2 ( r) RDF( r) Br R( r ) 2, B is th normalization constant. Ordr of Orbital Enrgis: Homonuclar Diatomic Molculs * * * * g1s u1s g 2s u 2s u 2 p g 2 p g
More informationTMMI37, vt2, Lecture 8; Introductory 2-dimensional elastostatics; cont.
Lctr 8; ntrodctor 2-dimnsional lastostatics; cont. (modifid 23--3) ntrodctor 2-dimnsional lastostatics; cont. W will now contin or std of 2-dim. lastostatics, and focs on a somwhat mor adancd lmnt thn
More informationRecounting the Rationals
Rconting th Rationals Nil Calkin and Hrbrt S. Wilf pril, 000 It is wll known (indd, as Pal Erd}os might hav said, vry child knows) that th rationals ar contabl. Howvr, th standard prsntations of this fact
More information4.2 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 informationMA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c.
MA56 utorial Solutions Qustion a Intgrating fator is ln p p in gnral, multipl b p So b ln p p sin his kin is all a Brnoulli quation -- st Sin w fin Y, Y Y, Y Y p Qustion Dfin v / hn our quation is v μ
More information5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd
1. First you chck th domain of g x. For this function, x cannot qual zro. Thn w find th D domain of f g x D 3; D 3 0; x Q x x 1 3, x 0 2. Any cosin graph is going to b symmtric with th y-axis as long as
More informationMock Exam 2 Section A
Mock Eam Mock Eam Sction A. Rfrnc: HKDSE Math M Q ( + a) n n n n + C ( a) + C( a) + C ( a) + nn ( ) a nn ( )( n ) a + na + + + 6 na 6... () \ nn ( ) a n( n )( n ) a + 6... () 6 6 From (): a... () n Substituting
More informationMachine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005.
Intrnational Linar Collidr Machin Dtctor Intrfac Workshop: ILCSLAC, January 68, 2005. Prsntd by Brtt Parkr, BNLSMD Mssag: Tools ar now availabl to optimiz IR layout with compact suprconducting quadrupols
More informationAdvanced Control Techniques For Efficient And Robust Operation Of Advanced Life Support Systems
1ICES28 Advancd Control Tchniqs For Efficint And Robst Opration Of Advancd Lif Spport Systms Copyright 21 Socity of Atomotiv Enginrs, Inc. C.W. awlowski, A.M. Bll, S. Crawford Orbital Scincs Corporation
More information8 in in in
Exapl: Sisic Loads Givn: 8 in. noral wight (5 pc) CMU wall; Grad 60 stl; Tp S PCL ortar (spcial rinorcd wall); =000psi; roo orcs act at 7.in. ccntricit; S DS =., =.0. Rqird: Rinorcnt Soltion: Estiat aont
More informationSundials and Linear Algebra
Sundials and Linar Algbra M. Scot Swan July 2, 25 Most txts on crating sundials ar dirctd towards thos who ar solly intrstd in making and using sundials and usually assums minimal mathmatical background.
More information1 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 informationFinite 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 information3 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 informationLecture Notes: Finite Element Analysis, J.E. Akin, Rice University
9. TRUSS ANALYSIS... 1 9.1 PLANAR TRUSS... 1 9. SPACE TRUSS... 11 9.3 SUMMARY... 1 9.4 EXERCISES... 15 9. Trss analysis 9.1 Planar trss: The differential eqation for the eqilibrim of an elastic bar (above)
More informationCHAPTER 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 informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1
More informationA PROBABILISTIC FUZZY SET FOR UNCERTAINTIES- BASED MODELING IN LOGISTICS MANIPULATOR SYSTEM
A PROBABILISTIC FUZZY SET FOR UNCERTAINTIES BASED MODELING IN LOGISTICS MANIPULATOR SYSTEM YIHUA LI,,3 WENING HUANG Collg of Transportation and Logistics, Cntral Soth Univrsity of Forstry & Tchnology,
More informationFerroelectrics 342:73-82, 2006 Computational Modeling of Ferromagnetic Shape Memory Thin Films
Frrolctrics 4:7-8 6 Computational Modling of Frromagntic Shap Mmory Thin Films J. Liakhova M. Luskin and T. Zhang School of Mathmatics 6 Church St. SE Univrsity of Minnsota Minnapolis MN 55455 USA Email:
More informationInstantaneous 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 informationME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören
ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(
More informationRobot Formation Control in Leader-Follower Motion Using Direct Lyapunov Method
INTRNATIONA JOURNA O INTIGNT CONTRO AND SYSTMS VO. 0, NO. 3, SPTMBR 005, 44-50 Robot ormation Control in ar-ollowr Motion Using Dirct apunov Mtho Xiaohai I an Jizhong XIAO Abstract In this papr, w invstigat
More informationVII. Quantum Entanglement
VII. Quantum Entanglmnt Quantum ntanglmnt is a uniqu stat of quantum suprposition. It has bn studid mainly from a scintific intrst as an vidnc of quantum mchanics. Rcntly, it is also bing studid as a basic
More informationParameter Choice for International Linear Collider (ILC) *
005 ALCPG & ILC Workshops-Snowmass, U.S.A. Paramtr Choic for Intrnational Linar Collir (ILC) * J. Gao 1 Institut of igh Enrg Phsics, Chins Acam of Scincs, ijing 100049 In this papr a gnral procu to trmin
More informationRobust Digital Redesign of Continuous PID Controller for Power system Using Plant-Input-Mapping
Rcnt Avancs in lctrical nginring Robust Digital Rsign of Continuous PID Controllr for Powr systm Using Plant-Input-Mapping. Shabib, sam H. Ab-lham,. Magy Dpartmnt of lctrical Powr nginring, Faculty of
More informationThe 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 informationMulti-linear Systems and Invariant Theory. in the Context of Computer Vision and Graphics. Class 5: Self Calibration. CS329 Stanford University
Mlti-linar Systms and Invariant hory in th ontt of omtr Vision and Grahics lass 5: Slf alibration S39 Stanford Univrsity Amnon Shasha lass 5 Matrial W Will ovr oday h basic qations and conting argmnts
More informationText: WMM, Chapter 5. Sections , ,
Lcturs 6 - Continuous Probabilit Distributions Tt: WMM, Chaptr 5. Sctions 6.-6.4, 6.6-6.8, 7.-7. In th prvious sction, w introduc som of th common probabilit distribution functions (PDFs) for discrt sampl
More informationROBUST TRACKING CONTROL OF A QUADROTOR HELICOPTER WITHOUT VELOCITY MEASUREMENT
Annals of DAAAM for & Procings of th r ntrnational DAAAM Smposim Volm No. SSN 4-8 SBN 978--99-9-9 CDROM vrsion E. B. Katalinic Pblish b DAAAM ntrnational Vinna Astria EU Mak Harmon btwn Tchnolog an Natr
More informationClassical Magnetic Dipole
Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg
More informationDC-Link Stability Analysis for AC Drive System with Common DC-Bus
Jornal of Comptrs Vol. 8, No. 4, 7, pp. 48-56 doi:.3966/9955978846 DC-Link Stability Analysis for AC Driv Systm with Common DC-Bs Xiaoyan Wn Bijing Ky Laboratory of Robot Bionics and Fnction sarch, Bijing
More informationMAE4700/5700 Finite Element Analysis for Mechanical and Aerospace Design
MAE4700/5700 Finit Elmnt Analysis for Mchanical and Arospac Dsign Cornll Univrsity, Fall 2009 Nicholas Zabaras Matrials Procss Dsign and Control Laboratory Sibly School of Mchanical and Arospac Enginring
More informationChapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional
Chaptr 13 GMM for Linar Factor Modls in Discount Factor form GMM on th pricing rrors givs a crosssctional rgrssion h cas of xcss rturns Hors rac sting for charactristic sting for pricd factors: lambdas
More informationME 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 information4.4 Design of Sections for Flexure (Part III)
4.4 Dsign of Sctions for Flxur (Part ) This sction covrs th following topics. Choic of Sctions Dtrmination of Limiting Zon Post-tnsioning in Stags 4.4.1 Choic of Sctions Th typ of sction is slctd asd on
More informationReminder: Affine Transformations. Viewing and Projection. Shear Transformations. Transformation Matrices in OpenGL. Specification via Ratios
CSCI 420 Comptr Graphics Lctr 5 Viwing and Projction Jrnj Barbic Univrsity o Sothrn Caliornia Shar Transormation Camra Positioning Simpl Paralll Projctions Simpl Prspctiv Projctions [Angl, Ch. 5] Rmindr:
More informationUnfired 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 informationH Control Design for a Magnetostrictive Transducer
Control Dsign for a agntostrictiv Transdcr Jams Nalis and Ralph C. Smith Cntr for Rsarch in Scintific Comptation, North Carolina Stat Univrsity, Raligh, NC 27695 Abstract agntostrictiv transdcrs ar bcoming
More information5.80 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 informationEDM Implications for BSM Physics
EDM Implications for BSM Physics Kaori Fyto Univrsity of Massachstts, Amhrst K. Fyto, M. Ramsy-Msolf, T. Shn, PLB788(2019)52 J. d Vris, P. Drapr, K.Fyto, J. Kozaczk and D. Sthrland, 1809.10143 K. Fyto,
More informationOne-nucleon Transfers to Resonances
On-nclon Transfrs to Rsonancs INT, Sattl. March 6, 217 Ian Thompson Jtta schr, with TORUS collaboration: F. Nns, G. Arbanas & C. lstr This work was prformd ndr th aspics of th U.S. Dpartmnt of nrgy by
More informationFormal Methods for Deriving Element Equations
Formal Methods for Deriving Element Eqations And the importance of Shape Fnctions Formal Methods In previos lectres we obtained a bar element s stiffness eqations sing the Direct Method to obtain eact
More informationIntroduction to the quantum theory of matter and Schrödinger s equation
Introduction to th quantum thory of mattr and Schrödingr s quation Th quantum thory of mattr assums that mattr has two naturs: a particl natur and a wa natur. Th particl natur is dscribd by classical physics
More informationLet's start with the formulas. In fact for our purposes we need only the following three: d e e dx = (1.3)
. Diffrntiation Ms. M: So y = r /. And if yo dtrmin th rat of chang in this crv corrctly, I think yo'll b plasantly srprisd. Class: [chckls] Ms. M: Don't yo gt it, Bart? dy = r dr, or rdr, or rdrr. Har-d-har-har,
More informationDIFFERENTIAL EQUATION
MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous
More informationProblem 22: Journey to the Center of the Earth
Problm : Journy to th Cntr of th Earth Imagin that on drilld a hol with smooth sids straight through th ntr of th arth If th air is rmod from this tub (and it dosn t fill up with watr, liquid rok, or iron
More informationMECHANICS OF FRP SHEAR STRENGTHENING OF RC BEAMS
MECHANIC OF FRP HEAR TRENGTHENING OF RC BEAM G. Monti, F. antinlli an M. A. iotta Dipartimnto i Inggnria trttral Gotcnica, Univrsità i Roma a apina, Roma, Italy ABTRACT This papr prsnts th rslts o an primntal/analytical
More informationNTHU ESS5850 Micro System Design F. G. Tseng Fall/2016, 7-2, p1. Lecture 7-2 MOSIS/SCNA Design Example- Piezoresistive type Accelerometer II
F. G. Tsng Fall/016, 7-, p1 ctur 7- MOSIS/SCNA Dsign Exampl-!! Pizorsistivity Pizorsistiv typ Acclromtr II a Considr a conductiv lock of dimnsion a as shown in th figur. If a currnt is passd through th
More informationFEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك
FEM FOR HE RNSFER PROBLEMS 1 Fild problms Gnral orm o systm quations o D linar stady stat ild problms: For 1D problms: D D g Q y y (Hlmholtz quation) d D g Q d Fild problms Hat transr in D in h h ( D D
More informationEXST 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 informationThe van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012
Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor
More informationComputer Vision. Fourier Analysis. Computer Science Tripos Part II. Dr Christopher Town. Fourier Analysis. Fourier Analysis
Comptr Vision Comptr Scinc Tripos Part II Dr Christophr Town orir Analsis An imag can b rprsntd b a linar combination of basis fnctions: In th cas of 2D orir analsis: orir Analsis orir Analsis Th transform
More informationLogarithms. Secondary Mathematics 3 Page 164 Jordan School District
Logarithms Sondary Mathmatis Pag 6 Jordan Shool Distrit Unit Clustr 6 (F.LE. and F.BF.): Logarithms Clustr 6: Logarithms.6 For ponntial modls, prss as a arithm th solution to a and d ar numrs and th as
More informationAn Extensive Study of Approximating the Periodic. Solutions of the Prey Predator System
pplid athmatical Scincs Vol. 00 no. 5 5 - n xtnsiv Study of pproximating th Priodic Solutions of th Pry Prdator Systm D. Vnu Gopala Rao * ailing addrss: Plot No.59 Sctor-.V.P.Colony Visahapatnam 50 07
More information