A general Kirchhoff approximation for echo simulation in ultrasonic NDT
|
|
- David Williamson
- 6 years ago
- Views:
Transcription
1 A genera rchhoff approxmaton for echo smaton n trasonc NDT V. Dorva, S. Chaton, B. L, M. Darmon, S. Mahat (CEA, LIST) CEA, LIST, F-99 Gf-sr-Yvette, France
2 Pan A genera rchhoff approxmaton for echo smaton n trasonc NDT Introdcton. Genera rchhoff mode. fned rchhoff mode Concson
3 Introdcton Defect sponse mode n the Cva smaton patform Smaton method comptaton of emtted and receved feds wthot defects (penc method) convoton wth the defect response tted fed ceved fed Interacton Severa modes are avaabe to smate the nteracton wth dfferent defects rchhoff Vods, srfaces, cracs (specar) GTD Cracs (dffracton) SOV Sde dred hoes Modfed Born Sod ncsons 3
4 Introdcton Free srface rchhoff approxmaton «trasonc scatterng from smooth fat cracs: an eastodynamc rchhoff dffracton theory», 984 Dspacement on the srface of the faw rchhoff approxmaton: nfnte pane Tota fed= Incdent wave+ refected L wave + refected T wave Incdent L wave β fected T wave δ fe Appcaton of the Green theorem Integra on the faw srface p p x j x j x, x n j x d S Dffracted fed Dspacement Green s fncton x Faw srface rface Expresson of the dffracted fed as a fncton of srface dspacement A dffracton coeffcent can be obtaned by tang the far-fed mt Expresson of the dffracton coeffcent Exampe: L L coeffcent v L T BLL, sn sn A Lt cos sn vt vl Depends on ncdence and observaton anges ated to refecton coeffcents v A Ln Avec: A A Lt Ln R R LL LL v v v v L T L T cot tan R R LT LT 4
5 Introdcton Lmtatons of the free-srface rchhoff mode Propagaton of waves aong the defect not taen nto accont Case of sde dred hoes: a wave not taen nto accont by rchhoff crces the defect SOV mode (separaton of varabes) avaabe n Cva Free srface approxmaton Appcabe ony n cases where the srface can be consdered as free (cracs, bacwa echoes ) Extenson of the mode to nterfaces between any two materas Inaccraces n crac tp dffracton rchhoff s sed for specar echoes, GTD s sed for dffracton Deveopment of a mode that combnes rchhoff and GTD 5
6 Pan A genera rchhoff approxmaton for echo smaton n trasonc NDT Introdcton. Genera rchhoff mode. fned rchhoff mode Concson 6
7 Genera rchhoff mode Formasm Ad s recprocty theorem emtter defect S F recever S F Defect echo proportona to: ba 4P S F D D D: tted fed wth defect : ceved fed wthot defect nˆ ds rchhoff approxmaton apped on the defect srface Insonfed srface ocay approxmated by an nfnte pane Fed = tangent ncdent wave pane + refected L wave defect + refected T wave Fed assmed to be zero n the defect shadow Expresson of D and σ D on the defect srface 7
8 Genera rchhoff mode Pane wave approxmaton Expresson of the stress and dspacement on the defect srface Comptaton of the refected pane waves The dspacement can be expressed drecty D nc Tref The expresson of stress s factated by the pane wave decomposton j Cj x Hooe s aw for a pane wave D j nc nc Tref Tref Expresson of the scatterng coeffcent Coeff Tref Tref Tref C j nˆ j Stress wth defect Dspacement wth defect Expresson vad for any ncdent and scattered modes 8
9 Genera rchhoff mode For each probe poston For each mode (L/T, drect/refected ) Sampng of the nsonfed sde For each sampe pont Comptaton method Comptaton of emtted fed and receved fed (recprocty) sng the penc method Approxmaton by pane waves For the emtted fed: comptaton of the drectons and amptdes of the refected waves Comptatons of rchhoff coeffcents refector Smmaton over the srface + 9
10 Genera rchhoff mode Comparson wth prevos mode and expermenta rests The free srface mode cannot be sed for srface echoes: p p x j x j x, x n j x d S Free srface rchhoff: dspacement on the srface x Terme negected by the free srface mode The genera mode taes nto accont an addtonna contrbton ba 4 P S F v D nˆ v D nˆ Genera rchhoff: dspacement and stress on the srface ds 4mm 5mm Pate (STEEL) WATER Pate (STEEL) Experment Free srface rchhoff Rgd rchhoff Genera rchhoff Stee/Water 6 db 7.5 db -. db 7. db Water/Stee 5 db -3.3 db 6. db 5.9 db Srface echoes / reference echoes The genera rchhoff mode s appcabe to both echoes The genera rchhoff mode removes the need for two modes and can be sed n other cases (sod-sod for exampe)
11 Genera rchhoff mode Adaptaton to varos materas Lst of refected waves dependant on the propagaton medm In qds, se of a smpfed expresson eqvaent to: Coeff Pref Pref Pref C j nˆ j In sotropc sods: Coeff Tref Tref Tref C j nˆ j In ansotropc sods: Coeff q q qtref qtref qtref qtref qtref qtref C j nˆ j Drectons of refected waves dependant on the propagaton medm Amptdes of refected waves dependant on the propagaton and refectng medm
12 Pan A genera rchhoff approxmaton for echo smaton n trasonc NDT Introdcton. Genera rchhoff mode. fned rchhoff mode Concson
13 Pressre fned rchhoff mode Lmtaton de to approxmatons on edge.5 Exampe of a rgd haf-pane n a fd Exact rchhoff defect.5 Exact soton rchhoff x / norma ncdent wave θ=5 ; r = λ Oscatons on defect edges not modeed by rchhoff Lead to naccraces n tp dffracton Separaton of the specar and dffracted parts: A x nc G x, x' x' x n d ' Statonary pont (specar refecton) ower ntegraton mt contrbton (dffracton x =) A ( GO) A dff x x D A, e r r D A e / 4 tan tan 3
14 fned rchhoff mode Combnaton wth GTD mode refecton Geometrca Theory of Dffracton mode yeds accrate rests for crac tp dffracton dvergence for refected and transmtted waves Inc 3.5 GTD GTD( GO) D GTD, D GTD e, / 4 e r r cos cos 8 4 transmsson 7 Exact GTD 3 θ=5 ; r = λ defect 33 Prncpe of the refned rchhoff mode: rchhoff mode for the refected and transmtted part, GTD mode for the dffracted part RA A( spec) A D GTD A dff D A e A dff r r GTD dff Correcton of the rchhoff dffracton 4
15 fned rchhoff mode RA Improvement of the rchhoff mode A D GTD D A e r r D GTD - D rchoff nc = D GTD D rchoff dvergence of the GTD coeffcent canceed by the dvergence of rchhoff for a sem-nfnte pane = Inc zoom Fd-rgd (presented here) Improvement of the dffracton rests 4 Exact A 33 fned-a 3 Exact A fned-a Sod-vod Encoragng premnary rests: Improvement more sgnfcant 7 fd-rgd case 5
16 Pan A genera rchhoff approxmaton for echo smaton n trasonc NDT Introdcton. Genera rchhoff mode. fned rchhoff mode Concson 6
17 Concson Deveopment of a genera rchhoff mode Generc formasm Appcabe to nterfaces between any types of materas (fds, sotropc sods, ansotropc sods) Extends the appcaton doman of the rchhoff mode n Cva fnement of the rchhoff mode to mprove dffracton rests Coaboraton wth Approach vadated for the fd-rgd case (edge) Wor n progress: mpementaton of the sod-vod case (edge) Ftre wors: deveopments for other materas and geometres 7
LECTURE 21 Mohr s Method for Calculation of General Displacements. 1 The Reciprocal Theorem
V. DEMENKO MECHANICS OF MATERIALS 05 LECTURE Mohr s Method for Cacuaton of Genera Dspacements The Recproca Theorem The recproca theorem s one of the genera theorems of strength of materas. It foows drect
More information3. Stress-strain relationships of a composite layer
OM PO I O U P U N I V I Y O F W N ompostes ourse 8-9 Unversty of wente ng. &ech... tress-stran reatonshps of a composte ayer - Laurent Warnet & emo Aerman.. tress-stran reatonshps of a composte ayer Introducton
More informationIntroduction to Antennas & Arrays
Introducton to Antennas & Arrays Antenna transton regon (structure) between guded eaves (.e. coaxal cable) and free space waves. On transmsson, antenna accepts energy from TL and radates t nto space. J.D.
More informationNumerical Investigation of Power Tunability in Two-Section QD Superluminescent Diodes
Numerca Investgaton of Power Tunabty n Two-Secton QD Superumnescent Dodes Matta Rossett Paoo Bardea Ivo Montrosset POLITECNICO DI TORINO DELEN Summary 1. A smpfed mode for QD Super Lumnescent Dodes (SLD)
More informationECE 107: Electromagnetism
ECE 107: Electromagnetsm Set 8: Plane waves Instructor: Prof. Vtaly Lomakn Department of Electrcal and Computer Engneerng Unversty of Calforna, San Dego, CA 92093 1 Wave equaton Source-free lossless Maxwell
More information[WAVES] 1. Waves and wave forces. Definition of waves
1. Waves and forces Defnton of s In the smuatons on ong-crested s are consdered. The drecton of these s (μ) s defned as sketched beow n the goba co-ordnate sstem: North West East South The eevaton can
More informationSupplementary Material: Learning Structured Weight Uncertainty in Bayesian Neural Networks
Shengyang Sun, Changyou Chen, Lawrence Carn Suppementary Matera: Learnng Structured Weght Uncertanty n Bayesan Neura Networks Shengyang Sun Changyou Chen Lawrence Carn Tsnghua Unversty Duke Unversty Duke
More information22.51 Quantum Theory of Radiation Interactions
.51 Quantum Theory of Radaton Interactons Fna Exam - Soutons Tuesday December 15, 009 Probem 1 Harmonc oscator 0 ponts Consder an harmonc oscator descrbed by the Hamtonan H = ω(nˆ + ). Cacuate the evouton
More informationRemark: Positive work is done on an object when the point of application of the force moves in the direction of the force.
Unt 5 Work and Energy 5. Work and knetc energy 5. Work - energy theore 5.3 Potenta energy 5.4 Tota energy 5.5 Energy dagra o a ass-sprng syste 5.6 A genera study o the potenta energy curve 5. Work and
More information*B. Shankar Goud 1, M.N Rajashekar 2
IOSR Jorna of Mathematcs (IOSR-JM) e-iss: 78-578, p-iss: 39-765X. Vome, Isse 6 Ver. IV(ov. - Dec. 6), PP 55-64 www.osrornas.org Fnte Eement Method Appcaton of Effects on an Unsteady MHD Convectve Heat
More information16 Reflection and transmission, TE mode
16 Reflecton transmsson TE mode Last lecture we learned how to represent plane-tem waves propagatng n a drecton ˆ n terms of feld phasors such that η = Ẽ = E o e j r H = ˆ Ẽ η µ ɛ = ˆ = ω µɛ E o =0. Such
More informationLecture 3. Interaction of radiation with surfaces. Upcoming classes
Radaton transfer n envronmental scences Lecture 3. Interacton of radaton wth surfaces Upcomng classes When a ray of lght nteracts wth a surface several nteractons are possble: 1. It s absorbed. 2. It s
More informationTRANSFER MATRIX METHOD FOR FORCED VIBRATIONS OF BARS
U.P.B. Sc. B., Seres D, Vo. 7, Iss., ISSN 454-358 TRANSFER MATRIX METHOD FOR FORCED VIBRATIONS OF BARS Vaentn CEAUŞU, Andre CRAIFALEANU, Crstan DRAGOMIRESCU 3 Lcrarea prezntă metoda matrceor de transfer,
More informationPanel transmission measurements: the influence of the non plane wave nature of the incident field
Acoustcs 8 Pars Panel transmsson measurements: the nfluence of the non plane wave nature of the ncdent feld V. F Humphrey a J. Smth b a Insttute of Sound Vbraton, Unv. of Southampton, Unversty Road, Hghfeld,
More informationMEMBRANE ELEMENT WITH NORMAL ROTATIONS
9. MEMBRANE ELEMENT WITH NORMAL ROTATIONS Rotatons Mst Be Compatble Between Beam, Membrane and Shell Elements 9. INTRODUCTION { XE "Membrane Element" }The comple natre of most bldngs and other cvl engneerng
More informationStrain Energy in Linear Elastic Solids
Duke Unverst Department of Cv and Envronmenta Engneerng CEE 41L. Matr Structura Anass Fa, Henr P. Gavn Stran Energ n Lnear Eastc Sods Consder a force, F, apped gradua to a structure. Let D be the resutng
More informationMCM-based Uncertainty Evaluations practical aspects and critical issues
C-based Uncertanty Evalatons practcal aspects and crtcal sses H. Hatjea, B. van Dorp,. orel and P.H.J. Schellekens Endhoven Unversty of Technology Contents Introdcton Standard ncertanty bdget de wthot
More informationAE/ME 339. K. M. Isaac. 8/31/2004 topic4: Implicit method, Stability, ADI method. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept.
AE/ME 339 Comptatonal Fld Dynamcs (CFD) Comptatonal Fld Dynamcs (AE/ME 339) Implct form of dfference eqaton In the prevos explct method, the solton at tme level n,,n, depended only on the known vales of,
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationEstimation of homogenized elastic coefficients of pre-impregnated composite materials
Proceedngs of the nd IASME / WSEAS Internatonal Conference on Contnm Mechancs (CM'7) Portoroz Slovena Ma 5-7 7 34 Estmaton of homogenzed elastc coeffcents of pre-mpregnated composte materals HORATIU TEODORESCU
More informationReprint (R34) Accurate Transmission Measurements Of Translucent Materials. January 2008
Reprnt (R34) Accurate ransmsson Measurements Of ranslucent Materals January 2008 Gooch & Housego 4632 36 th Street, Orlando, FL 32811 el: 1 407 422 3171 Fax: 1 407 648 5412 Emal: sales@goochandhousego.com
More informationAtomic Scattering Factor for a Spherical Wave and the Near Field Effects in X-ray Fluorescence Holography
Atomc Scatterng Factor for a Spherca Wave and the Near Fed Effects n X-ray Fuorescence Hoography Janmng Ba Oak Rdge Natona Laboratory, Oak Rdge, TN 37831 Formua for cacuatng the atomc scatterng factor
More informationIntroduction to elastic wave equation. Salam Alnabulsi University of Calgary Department of Mathematics and Statistics October 15,2012
Introdcton to elastc wave eqaton Salam Alnabls Unversty of Calgary Department of Mathematcs and Statstcs October 15,01 Otlne Motvaton Elastc wave eqaton Eqaton of moton, Defntons and The lnear Stress-
More informationBAR & TRUSS FINITE ELEMENT. Direct Stiffness Method
BAR & TRUSS FINITE ELEMENT Drect Stness Method FINITE ELEMENT ANALYSIS AND APPLICATIONS INTRODUCTION TO FINITE ELEMENT METHOD What s the nte element method (FEM)? A technqe or obtanng approxmate soltons
More informationA DIMENSION-REDUCTION METHOD FOR STOCHASTIC ANALYSIS SECOND-MOMENT ANALYSIS
A DIMESIO-REDUCTIO METHOD FOR STOCHASTIC AALYSIS SECOD-MOMET AALYSIS S. Rahman Department of Mechanca Engneerng and Center for Computer-Aded Desgn The Unversty of Iowa Iowa Cty, IA 52245 June 2003 OUTLIE
More informationTraceability and uncertainty for phase measurements
Traceablty and ncertanty for phase measrements Karel Dražl Czech Metrology Insttte Abstract In recent tme the problems connected wth evalatng and expressng ncertanty n complex S-parameter measrements have
More informationDynamics of a Discrete Predator-Prey System with Beddington-DeAngelis Function Response
Apped Mathematcs 3 389-394 http://dxdoorg/46/am46 Pshed Onne Apr (http://wwwscrporg/jorna/am) Dynamcs of a Dscrete Predator-Prey System wth Beddngton-DeAnges Fncton Response Qn Fang Xaopng L * Mey Cao
More informationLecture 8: Reflection and Transmission of Waves. Normal incidence propagating waves. Normal incidence propagating waves
/8/5 Lecture 8: Reflecton and Transmsson of Waves Instructor: Dr. Gleb V. Tcheslavsk Contact: gleb@ee.lamar.edu Offce Hours: Room 3 Class web ste: www.ee.lamar.edu/gleb/e m/index.htm So far we have consdered
More informationEN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics
N40: ynamcs and Vbratons Homewor 7: Rgd Body Knematcs School of ngneerng Brown Unversty 1. In the fgure below, bar AB rotates counterclocwse at 4 rad/s. What are the angular veloctes of bars BC and C?.
More informationChapter 6. Rotations and Tensors
Vector Spaces n Physcs 8/6/5 Chapter 6. Rotatons and ensors here s a speca knd of near transformaton whch s used to transforms coordnates from one set of axes to another set of axes (wth the same orgn).
More informationThermodynamics II. Department of Chemical Engineering. Prof. Kim, Jong Hak
Thermodynamcs II Department o Chemca ngneerng ro. Km, Jong Hak .5 Fugacty & Fugacty Coecent : ure Speces µ > provdes undamenta crteron or phase equbrum not easy to appy to sove probem Lmtaton o gn (.9
More informationAmplification and Relaxation of Electron Spin Polarization in Semiconductor Devices
Amplfcaton and Relaxaton of Electron Spn Polarzaton n Semconductor Devces Yury V. Pershn and Vladmr Prvman Center for Quantum Devce Technology, Clarkson Unversty, Potsdam, New York 13699-570, USA Spn Relaxaton
More informationImplementation of the Matrix Method
Computatonal Photoncs, Prof. Thomas Pertsch, Abbe School of Photoncs, FSU Jena Computatonal Photoncs Semnar 0 Implementaton of the Matr Method calculaton of the transfer matr calculaton of reflecton and
More informationBoundaries, Near-field Optics
Boundares, Near-feld Optcs Fve boundary condtons at an nterface Fresnel Equatons : Transmsson and Reflecton Coeffcents Transmttance and Reflectance Brewster s condton a consequence of Impedance matchng
More informationTheoretical Analysis of Stress Distribution in Bonded Single Strap and Stiffened Joints
56 Theoretca Anayss of Stress Dstrbton n Bonded Snge Strap and Stffened Jonts Abstract In ths paper, dstrbton of peeng stress n two types of adhesvey-bonded jonts s nvestgated. The jonts are a snge strap
More informationUnsteady MHD Free Convective Flow Through Porous Media Past on Moving Vertical Plate with Variable Temperature and Viscous Dissipation
ISS 976 4 Avalable onlne at www.nternatonalejornals.com Internatonal ejornals Internatonal ejornal of Mathematcs and Engneerng (7) Vol. 8, Isse, pp Unstead MHD Free Convectve Flow Throgh Poros Meda Past
More information( ) + + REFLECTION FROM A METALLIC SURFACE
REFLECTION FROM A METALLIC SURFACE For a metallc medum the delectrc functon and the ndex of refracton are complex valued functons. Ths s also the case for semconductors and nsulators n certan frequency
More informationIX Mechanics of Rigid Bodies: Planar Motion
X Mechancs of Rd Bodes: Panar Moton Center of Mass of a Rd Bod Rotaton of a Rd Bod About a Fed As Moent of nerta Penduu, A Genera heore Concernn Anuar Moentu puse and Coson nvovn Rd Bodes. Rd bod: dea
More informationAsymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation
Nonl. Analyss and Dfferental Equatons, ol., 4, no., 5 - HIKARI Ltd, www.m-har.com http://dx.do.org/.988/nade.4.456 Asymptotcs of the Soluton of a Boundary alue Problem for One-Characterstc Dfferental Equaton
More informationAERODYNAMICS I LECTURE 6 AERODYNAMICS OF A WING FUNDAMENTALS OF THE LIFTING-LINE THEORY
LECTURE 6 AERODYNAMICS OF A WING FUNDAMENTALS OF THE LIFTING-LINE THEORY The Bot-Savart Law The velocty nduced by the sngular vortex lne wth the crculaton can be determned by means of the Bot- Savart formula
More informationFormal solvers of the RT equation
Formal solvers of the RT equaton Formal RT solvers Runge- Kutta (reference solver) Pskunov N.: 979, Master Thess Long characterstcs (Feautrer scheme) Cannon C.J.: 970, ApJ 6, 55 Short characterstcs (Hermtan
More informationUnified spin-wave theory for quantum spin systems with single-ion anisotropies
J. Phys. A: Math. Gen. 3 (999) 6687 674. Prnted n the UK PII: S35-447(99)67-8 Unfed spn-wave theory for quantum spn systems wth snge-on ansotropes Le Zhou and Yoshyuk Kawazoe Insttute for Materas Research,
More informationCourse Electron Microprobe Analysis
Course 12.141 Electron Mcroprobe Analyss THE ELECTROMAGNETIC SPECTRUM Electron Probe X-ray Mcro-Analyss A) quanttatve chemcal analyss of solds: Be to U 1 mcrometer resoluton up to 10 ppm B) hgh-resoluton
More informationScattering cross section (scattering width)
Scatterng cro ecton (catterng wdth) We aw n the begnnng how a catterng cro ecton defned for a fnte catterer n ter of the cattered power An nfnte cylnder, however, not a fnte object The feld radated by
More informationNumerical Study of the Momentumless Wake of an Axisymmetric Body
43rd AIAA Aerospace Scences Meetng and Exhbt 10-13 Janary 2005, Reno, Nevada AIAA 2005-1109 Nmerca Stdy of the Momentmess Wae of an Axsymmetrc Body Meng-Hang L * and Ana I. Srvente Unversty of Mchgan,
More informationPrinciples of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer
Prncples of Food and Boprocess Engneerng (FS 31) Solutons to Example Problems on Heat Transfer 1. We start wth Fourer s law of heat conducton: Q = k A ( T/ x) Rearrangng, we get: Q/A = k ( T/ x) Here,
More informationNegative Birefraction of Acoustic Waves in a Sonic Crystal
Negatve Brefracton of Acoustc Waves n a Sonc Crysta Mng-Hu Lu 1, Chao Zhang 1, Lang Feng 1, * Jun Zhao 1, Yan-Feng Chen 1, Y-We Mao 2, Jan Z 3, Yong-Yuan Zhu 1, Sh-Nng Zhu 1 and Na-Ben Mng 1 1 Natona Laboratory
More information829. An adaptive method for inertia force identification in cantilever under moving mass
89. An adaptve method for nerta force dentfcaton n cantlever under movng mass Qang Chen 1, Mnzhuo Wang, Hao Yan 3, Haonan Ye 4, Guola Yang 5 1,, 3, 4 Department of Control and System Engneerng, Nanng Unversty,
More informationGeneralized form of reflection coefficients in terms of impedance matrices of qp-qp and qp-qs waves in TI media
Generalzed form of reflecton coeffcents n terms of mpedance matrces of q-q and q-q waves n TI meda Feng Zhang and Xangyang L CNC Geophyscal KeyLab, Chna Unversty of etroleum, Bejng, Chna ummary Reflecton
More informationProblem Points Score Total 100
Physcs 450 Solutons of Sample Exam I Problem Ponts Score 1 8 15 3 17 4 0 5 0 Total 100 All wor must be shown n order to receve full credt. Wor must be legble and comprehensble wth answers clearly ndcated.
More informationA Hybrid Variational Iteration Method for Blasius Equation
Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method
More informationThe Study and Analysis of Neutron Activation with the Application of Gamma Ray Emission
Cumhuryet Ünverstes Fen Fakültes Fen Blmler Dergs (CFD), Clt:36, No: 3 Özel Sayı (2015) ISSN: 1300-1949 Cumhuryet Unversty Faculty of Scence Scence Journal (CSJ), Vol. 36, No: 3 Specal Issue (2015) ISSN:
More informationFirst looking at the scalar potential term, suppose that the displacement is given by u = φ. If one can find a scalar φ such that u = φ. u x.
7.4 Eastodynams 7.4. Propagaton of Wavs n East Sods Whn a strss wav travs throgh a matra, t ass matra parts to dspa by. It an b shown that any vtor an b wrttn n th form φ + ra (7.4. whr φ s a saar potnta
More informationBoundary Value Problems. Lecture Objectives. Ch. 27
Boundar Vaue Probes Ch. 7 Lecture Obectves o understand the dfference between an nta vaue and boundar vaue ODE o be abe to understand when and how to app the shootng ethod and FD ethod. o understand what
More informationIntroduction to Turbulence Modelling
Introdcton to Trblence Modellng 1 Nmercal methods 0 1 t Mathematcal descrpton p F Reslts For eample speed, pressre, temperatre Geometry Models for trblence, combston etc. Mathematcal descrpton of physcal
More informationImplementation of the Matrix Method
Computatonal Photoncs, Prof. Thomas Pertsch, Abbe School of Photoncs, FSU Jena Computatonal Photoncs Semnar 0 Implementaton of the Matr Method calculaton of the transfer matr calculaton of reflecton and
More informationC PLANE ELASTICITY PROBLEM FORMULATIONS
C M.. Tamn, CSMLab, UTM Corse Content: A ITRODUCTIO AD OVERVIEW mercal method and Compter-Aded Engneerng; Phscal problems; Mathematcal models; Fnte element method. B REVIEW OF -D FORMULATIOS Elements and
More informationIntroductory Optomechanical Engineering. 2) First order optics
Introductory Optomechancal Engneerng 2) Frst order optcs Moton of optcal elements affects the optcal performance? 1. by movng the mage 2. hgher order thngs (aberratons) The frst order effects are most
More informationECE Spring Prof. David R. Jackson ECE Dept. Notes 25
ECE 6345 Sprng 2015 Prof. Davd R. Jackson ECE Dept. Notes 25 1 Overvew In ths set of notes we use the spectral-doman method to fnd the nput mpedance of a rectangular patch antenna. Ths method uses the
More informationDigital Signal Processing
Dgtal Sgnal Processng Dscrete-tme System Analyss Manar Mohasen Offce: F8 Emal: manar.subh@ut.ac.r School of IT Engneerng Revew of Precedent Class Contnuous Sgnal The value of the sgnal s avalable over
More informationAPPROXIMATE ANALYSIS OF RIGID PLATE LOADING ON ELASTIC MULTI-LAYERED SYSTEMS
6th ICPT, Sapporo, Japan, July 008 APPROXIMATE ANALYSIS OF RIGID PLATE LOADING ON ELASTIC MULTI-LAYERED SYSTEMS James MAINA Prncpal Researcher, Transport and Infrastructure Engneerng, CSIR Bult Envronment
More informationIn this section is given an overview of the common elasticity models.
Secton 4.1 4.1 Elastc Solds In ths secton s gven an overvew of the common elastcty models. 4.1.1 The Lnear Elastc Sold The classcal Lnear Elastc model, or Hooean model, has the followng lnear relatonshp
More informationThermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)
hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
More informationTitle: Radiative transitions and spectral broadening
Lecture 6 Ttle: Radatve transtons and spectral broadenng Objectves The spectral lnes emtted by atomc vapors at moderate temperature and pressure show the wavelength spread around the central frequency.
More informationElectricity and Magnetism - Physics 121 Lecture 10 - Sources of Magnetic Fields (Currents) Y&F Chapter 28, Sec. 1-7
Electrcty and Magnetsm - Physcs 11 Lecture 10 - Sources of Magnetc Felds (Currents) Y&F Chapter 8, Sec. 1-7 Magnetc felds are due to currents The Bot-Savart Law Calculatng feld at the centers of current
More informationDeterministic and Monte Carlo Codes for Multiple Scattering Photon Transport
Determnstc and Monte Carlo Codes for Multple Scatterng Photon Transport Jorge E. Fernández 1 1 Laboratory of Montecuccolno DIENCA Alma Mater Studorum Unversty of Bologna Italy Isttuto Nazonale d Fsca Nucleare
More informationAccuracy-control techniques applied to stable transfer-matrix computations
PHYSICAL REVIEW E VOLUME 59, NUMBER 4 APRIL 1999 Accuracy-control technques appled to stable transfer-matrx computatons A. Mayer* and J.-P. Vgneron Laboratore de Physque du Solde, Facultés Unverstares
More informationEPR Paradox and the Physical Meaning of an Experiment in Quantum Mechanics. Vesselin C. Noninski
EPR Paradox and the Physcal Meanng of an Experment n Quantum Mechancs Vesseln C Nonnsk vesselnnonnsk@verzonnet Abstract It s shown that there s one purely determnstc outcome when measurement s made on
More informationFlow equations To simulate the flow, the Navier-Stokes system that includes continuity and momentum equations is solved
Smulaton of nose generaton and propagaton caused by the turbulent flow around bluff bodes Zamotn Krll e-mal: krart@gmal.com, cq: 958886 Summary Accurate predctons of nose generaton and spread n turbulent
More informationExact Solutions for Nonlinear D-S Equation by Two Known Sub-ODE Methods
Internatonal Conference on Compter Technology and Scence (ICCTS ) IPCSIT vol. 47 () () IACSIT Press, Sngapore DOI:.7763/IPCSIT..V47.64 Exact Soltons for Nonlnear D-S Eqaton by Two Known Sb-ODE Methods
More informationTHE COUPLED LES - SUBGRID STOCHASTIC ACCELERATION MODEL (LES-SSAM) OF A HIGH REYNOLDS NUMBER FLOWS
/2 THE COUPLED LES - SUBGRID STOCHASTIC ACCELERATION MODEL LES-SSAM OF A HIGH REYNOLDS NUMBER FLOWS Vladmr Sabel nov DEFA/EFCA ONERA, France In collaboraton wth: Anna Chtab CORIA, Unversté de Rouen, France
More informationLight diffraction by a subwavelength circular aperture
Early Vew publcaton on www.nterscence.wley.com ssue and page numbers not yet assgned; ctable usng Dgtal Object Identfer DOI) Laser Phys. Lett. 1 5 25) / DOI 1.12/lapl.2516 1 Abstract: Dffracton of normally
More informationLinear Approximation with Regularization and Moving Least Squares
Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...
More information3/31/ = 0. φi φi. Use 10 Linear elements to solve the equation. dx x dx THE PETROV-GALERKIN METHOD
THE PETROV-GAERKIN METHO Consder the Galern solton sng near elements of the modfed convecton-dffson eqaton α h d φ d φ + + = α s a parameter between and. If α =, we wll have the dscrete Galern form of
More informationSCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors.
SCALARS AND ECTORS All phscal uanttes n engneerng mechancs are measured usng ether scalars or vectors. Scalar. A scalar s an postve or negatve phscal uantt that can be completel specfed b ts magntude.
More informationNeural network-based athletics performance prediction optimization model applied research
Avaabe onne www.jocpr.com Journa of Chemca and Pharmaceutca Research, 04, 6(6):8-5 Research Artce ISSN : 0975-784 CODEN(USA) : JCPRC5 Neura networ-based athetcs performance predcton optmzaton mode apped
More informationGauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law
Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s
More informationˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m)
7.. = = 3 = 4 = 5. The electrc feld s constant everywhere between the plates. Ths s ndcated by the electrc feld vectors, whch are all the same length and n the same drecton. 7.5. Model: The dstances to
More informationNoise from structure borne sound sources mounted on lightweight receivers; progress report from CEN/TC126/WG7
Nose from structure borne sound sources mounted on lghtweght recevers; progress report from CENTC126WG7 Mchel Vllot CSTB (Center for Buldng Scence and Technology), France COST FP0702 workshop, Delft COST
More informationECON 351* -- Note 23: Tests for Coefficient Differences: Examples Introduction. Sample data: A random sample of 534 paid employees.
Model and Data ECON 35* -- NOTE 3 Tests for Coeffcent Dfferences: Examples. Introducton Sample data: A random sample of 534 pad employees. Varable defntons: W hourly wage rate of employee ; lnw the natural
More informationD hh ν. Four-body charm semileptonic decay. Jim Wiss University of Illinois
Four-body charm semeptonc decay Jm Wss Unversty of Inos D hh ν 1 1. ector domnance. Expected decay ntensty 3. SU(3) apped to D s φν 4. Anaytc forms for form factors 5. Non-parametrc form factors 6. Future
More informationPulse Coded Modulation
Pulse Coded Modulaton PCM (Pulse Coded Modulaton) s a voce codng technque defned by the ITU-T G.711 standard and t s used n dgtal telephony to encode the voce sgnal. The frst step n the analog to dgtal
More informationSUPPLEMENTARY INFORMATION
do: 0.08/nature09 I. Resonant absorpton of XUV pulses n Kr + usng the reduced densty matrx approach The quantum beats nvestgated n ths paper are the result of nterference between two exctaton paths of
More informationA boundary element method with analytical integration for deformation of inhomogeneous elastic materials
Journal of Physcs: Conference Seres PAPER OPEN ACCESS A boundary element method wth analytcal ntegraton for deformaton of nhomogeneous elastc materals To cte ths artcle: Moh. Ivan Azs et al 2018 J. Phys.:
More informationLab 2e Thermal System Response and Effective Heat Transfer Coefficient
58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),
More informationChapter 18, Part 1. Fundamentals of Atmospheric Modeling
Overhead Sldes for Chapter 18, Part 1 of Fundamentals of Atmospherc Modelng by Mark Z. Jacobson Department of Cvl & Envronmental Engneerng Stanford Unversty Stanford, CA 94305-4020 January 30, 2002 Types
More information6.3.4 Modified Euler s method of integration
6.3.4 Modfed Euler s method of ntegraton Before dscussng the applcaton of Euler s method for solvng the swng equatons, let us frst revew the basc Euler s method of numercal ntegraton. Let the general from
More informationInductance Calculation for Conductors of Arbitrary Shape
CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors
More informationComputational Electromagnetics in Antenna Analysis and Design
Computatonal Electromagnetcs n Antenna Analyss and Desgn Introducton It s rare for real-lfe EM problems to fall neatly nto a class that can be solved by the analytcal methods presented n the precedng lectures.
More informationPO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges
wth Modfed Suface-nomal Vectos fo RCS calculaton of Scattees wth Edges and Wedges N. Omak N. Omak, T.Shjo, and M. Ando Dep. of Electcal and Electonc Engneeng, Tokyo Insttute of Technology, Japan 1 Outlne.
More informationLecture 11. Transport in Membranes (1)
ecture 11. Transport n embranes (1) ass Transfer n embranes uk Fow qud Dffuson through ores Gas Dffuson through orous embranes Transport through onporous embranes - Souton-dffuson for qud mxtures - Souton-dffuson
More informationVEKTORANALYS GAUSS THEOREM STOKES THEOREM. and. Kursvecka 3. Kapitel 6 7 Sidor 51 82
VEKTORANAY Kursvecka 3 GAU THEOREM and TOKE THEOREM Kaptel 6 7 dor 51 82 TARGET PROBEM Do magnetc monopoles est? EECTRIC FIED MAGNETIC FIED N +? 1 TARGET PROBEM et s consder some EECTRIC CHARGE 2 - + +
More informationNested case-control and case-cohort studies
Outne: Nested case-contro and case-cohort studes Ørnuf Borgan Department of Mathematcs Unversty of Oso NORBIS course Unversty of Oso 4-8 December 217 1 Radaton and breast cancer data Nested case contro
More informationarxiv: v1 [physics.flu-dyn] 16 Sep 2013
Three-Dmensonal Smoothed Partcle Hydrodynamcs Method for Smulatng Free Surface Flows Rzal Dw Prayogo a,b, Chrstan Fredy Naa a a Faculty of Mathematcs and Natural Scences, Insttut Teknolog Bandung, Jl.
More informationMultiple-view geometry and 3D reconstruction
Mtpe-vew geometry and 3D reconstrcton Agsto Sart, Stefano baro Marco Marcon, Fabo Antonacc Dpartmento d Eettronca, Informazone e Bongegnera Potecnco d Mano Overvew More on two-vew geometry Projectve reconstrcton
More informationImplementation of the Matrix Method
Computatonal Photoncs, Summer Term 01, Abbe School of Photoncs, FSU Jena, Prof. Thomas Pertsch Computatonal Photoncs Semnar 03, 7 May 01 Implementaton of the Matr Method calculaton of the transfer matr
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationLecture Note 3. Eshelby s Inclusion II
ME340B Elastcty of Mcroscopc Structures Stanford Unversty Wnter 004 Lecture Note 3. Eshelby s Incluson II Chrs Wenberger and We Ca c All rghts reserved January 6, 004 Contents 1 Incluson energy n an nfnte
More informationEffect of Losses in a Layered Structure Containing DPS and DNG Media
PIERS ONLINE, VOL. 4, NO. 5, 8 546 Effect of Losses n a Layered Structure Contanng DPS and DNG Meda J. R. Canto, S. A. Matos, C. R. Pava, and A. M. Barbosa Insttuto de Telecomuncações and Department of
More information