Dalles. Introduction à l élasticité. Structures en béton II. Dr O. Burdet. ENAC Section de génie civil IS-BETON Laboratoire de construction en béton

Size: px
Start display at page:

Download "Dalles. Introduction à l élasticité. Structures en béton II. Dr O. Burdet. ENAC Section de génie civil IS-BETON Laboratoire de construction en béton"

Transcription

1 Dalles Introduction à l élasticité

2 Le gauchissement : près de l appui Fig. 7.35

3 Le gauchissement: bande de champ Fig. 7.35

4 Le gauchissement : visualisation Fig. 7.35

5 On pourrait éviter la torsion Fig. 7.37

6 Dalles Théorie de l élasticité

7 Equation différentielle des dalles Etablie par Lagrange Hpothèses de base: Dalles élancées (l/h > 5) Dalles isotropes homogènes Pas de déformation du feuillet moen dans son plan Les sections planes restent planes Les contraintes normales sont négligées Fig. 7.5

8 Elément infinitésimal de dalle d d Fig. 7.6

9 Equilibre d un élément de dalle d m d v d m d z v d m d d q( m d dm ) d m d ( m dm ) d ( m dm ) d ( m dm ) d ( v dv ) d ( m dm ) d ( v dv ) d Fig. 7.6

10 m Equilibre autour de m v = 0 v d z m d m d Fig. 7.6 m m d m m d v v d

11 Equilibre autour de m d z m v d m v = 0 m Fig. 7.6 m m d v v d m m d

12 Equilibre vertical z = 0 q v v Fig. 7.6 v d d v v v d d v v

13 Equilibre d un élément infinitésimal de dalle = 0 v m m = 0 v m m = 0 q v v Fig. 7.6 q m m m = Eq. 7.

14 Déformation d un élément de dalle Etablie par Lagrange Hpothèses de base: Dalles élancées (l/h > 5) Dalles isotropes homogènes Pas de déformation du feuillet moen dans son plan Les sections planes restent planes Les contraintes normales sont négligées Fig. 7.5

15 Déformation dans un plan parallèle au feuillet moen γ = γ γ Fig. 7.7 = u v

16 Répartition des contraintes σ = σ h,ma / z Fig. 7.8

17 Moments en fonction de la déformée m w w = B ν w w m = B ν m = B ( 1 ν ) w avec B = 3 E h 1 ν ( 1 ) Eq. 7.9

18 Equation de Lagrange (1811) w w w q = B Eq. 7.10

19 Grille de poutres sans torsion w w = q B Fig. 7.37

20 Conditions de bord w w w = q B Tab Tpe de condition cinématique statique (déplacements connus) (efforts connus) appui simple w = 0 m = 0 encastrement total w = 0, w n = 0 encastrement élastique w = 0 w n proportionnel à m m proportionnel à w n bord libre m = 0, r = 0

21 Résolution de l équation de Lagrange w(,) = m n a mn sin mπ a sin nπ b w (, ) qa 1 αm tanhαm = π D m coshα m= 135,,,... m cosh α b m α m coshα m αm sinh b b sin mπ a avec α m mπb = a a b On peut le faire avec Ecel! b Fig. 7.11

22 Moments dalle rectangulaire Diagramme Distribution transversale des moments m à = M qa Distribution Diagramme des moments m à = a/ a a/ 0 a/ a 3a/ a 3a a Distribution Diagramme des moments m à = M qa b = a b = a b = 1.5 Diagramme a Distribution transversale des moments m à = a/ b = 3 a b = a Fig. 7.1

23 Isolignes des déformations

24 Vue 3D des déformations

25 Vue 3D des déformations

26 Isolignes des moments m

27 Isolignes des moments m

28 Isolignes des moments de torsion m

29 Moments élastiques (ν = 0.17)

30 Soulèvement des coins a) coins libres de se soulever b) coins ancrés Fig. 7.1

31 Efforts dans les coins Fig. 7.15

32 Torsion pure dans les coins de dalles A R a a m - m réaction répartie r m - m a A a) moments dans l'angle d'une dalle simplement appuée et ancrée b) moments dans l'angle d'une dalle sur quatre colonnes Fig. 7.17

33 Réactions d appui Fig. 7.13

34 Dalle encastrée sur son pourtour Fig. 7.18

35 Etat de contraintes dans un coin σ α d dz τ α ds dz α dz z τ d dz τ d dz σ d dz σ d dz d d Fig. 7.19

36 Moments principau m T m m m m 1 m m α m Figs. 7.0 et 7.1

37 Trajectoires des moments principau

38 Comparaison dalle-poutre (1) Dalle Poutre h h b z w z w w(, ) w()

39 Comparaison dalle-poutre () m m m B w h w ν = B w w ν = = m = B ( 1 ν ) w b h M = B B = EI I = M M 0 = 0 d w d bh 1 3

40 Comparaison dalle-poutre (3) h h b w w w = q B w = q B 3 3 EI h bh B = I = B = EI I = 1 ν 1 1

Non uniform warping for composite beams. Theory and numerical applications

Non uniform warping for composite beams. Theory and numerical applications 19 ème Congrès Français de Mécanique Marseille, 24-28 août 29 Non uniform warping for composite beams. Theor and numerical applications R. EL FATMI, N. GHAZOUANI Laboratoire de Génit Civil, Ecole Nationale

More information

Flow energy harvesting with piezoelectric plates

Flow energy harvesting with piezoelectric plates Flow energy harvesting with piezoelectric plates Olivier Doaré IMSIA, ENSTA Paristech LMT 9 mars 2017 Sébastien Michelin, LadHyX Miguel Pineirua, IMSIA Yifan Xia, IMSIA, LadHyX 1 La piézoélectricité Déplacement

More information

ASYMPTOTIC BEHAVIOR OF STRUCTURES MADE OF CURVED RODS

ASYMPTOTIC BEHAVIOR OF STRUCTURES MADE OF CURVED RODS ASYMPTOTIC BEHAVIOR OF STRUCTURES MADE OF CURVED RODS G. GRISO Abstract. In this paper we study the asymptotic behavior of a structure made of curved rods of thickness when 0. This study is carried on

More information

Analytical Method for Calculating the Reduction in Strength Due to Shear Lag Effect in Tension Member Connections Dominique Bauer

Analytical Method for Calculating the Reduction in Strength Due to Shear Lag Effect in Tension Member Connections Dominique Bauer Analytical Method for Calculating the Reduction in Strength Due to Shear ag Effect in ension Member Connections Dominique Bauer SSEF Architecture and Engineering Educators Meeting 2008 February 29 - March

More information

Mesurer des déplacements ET des contraintes par correlation mécanique d images

Mesurer des déplacements ET des contraintes par correlation mécanique d images Mesurer des déplacements ET des contraintes par correlation mécanique d images J. RÉTHORÉ a, A. LEYGUE a, M. CORET a, L. STAINIER a, E. VERRON a a. Institut de Recherche en Génie Civil et Mécanique (GeM)

More information

Dynamic response of a beam on a frequencyindependent damped elastic foundation to moving load

Dynamic response of a beam on a frequencyindependent damped elastic foundation to moving load 60 Dynamic response of a beam on a frequencyindependent damped elastic foundation to moving load Seong-Min Kim and Jose M. Roesset Abstract: The dynamic displacement response of an infinitely long beam

More information

( ) 2 ( kg) ( 9.80 m/s 2

( ) 2 ( kg) ( 9.80 m/s 2 Chapitre 1 Charges et champs électriques [9 au 1 mai] DEVOIR : 1.78, 1.84, 1.56, 1.90, 1.71 1.1. Charge électrique et structure de la matière À lire rapidement. Concepts déjà familiers. 1.. Conducteurs,

More information

Restauration de bassins sédimentaires avec gocad. J-L. Rudkiewicz, M. Guiton, J-F. Lecomte, I. Moretti, S. Brocheray, M-C.

Restauration de bassins sédimentaires avec gocad. J-L. Rudkiewicz, M. Guiton, J-F. Lecomte, I. Moretti, S. Brocheray, M-C. Restauration de bassins sédimentaires avec gocad Kine3D J-L. Rudkiewicz, M. Guiton, J-F. Lecomte, I. Moretti, S. Brocheray, M-C. Cacas, (IFP) Février 2009 23 février 2009 Summary Principles of geological

More information

Unit 13 Review of Simple Beam Theory

Unit 13 Review of Simple Beam Theory MIT - 16.0 Fall, 00 Unit 13 Review of Simple Beam Theory Readings: Review Unified Engineering notes on Beam Theory BMP 3.8, 3.9, 3.10 T & G 10-15 Paul A. Lagace, Ph.D. Professor of Aeronautics & Astronautics

More information

Dynamic simulation of the formation of granular media and study of their properties

Dynamic simulation of the formation of granular media and study of their properties 8 ème Congrès Français de Mécanique Grenoble, 7-3 août 7 Dynamic simulation of the formation of granular media and study of their properties V. Mourzenko (), J.-F. Thovert () & P.M. Adler () () Laboratoire

More information

F.M. Gelagoti *1, P.P. Lekkakis 1, R.S. Kourkoulis 1 and G. Gazetas 1 1 PREFACE

F.M. Gelagoti *1, P.P. Lekkakis 1, R.S. Kourkoulis 1 and G. Gazetas 1 1 PREFACE Proceedings of the XVI ECSMGE ISBN 978--7277-667-8 The authors and ICE Publishing: All rights reserved, 25 doi:68/ecsmge.6678 Estimation of elastic and non-linear stiffness coefficients for suction caisson

More information

Solutions to Practice Test 3

Solutions to Practice Test 3 Solutions to Practice Test 3. (a) Find the equation for the plane containing the points (,, ), (, 2, ), and (,, 3). (b) Find the area of the triangle with vertices (,, ), (, 2, ), and (,, 3). Answer: (a)

More information

SSNL141 beams multifibre and multimatériaux

SSNL141 beams multifibre and multimatériaux Titre : SSNL141 - poutres multifibres et multimatériaux Date : 04/04/2013 Page : 1/7 SSNL141 beams multifibre and multimatériaux Abstract: The purpose of this test is to validate the use of multimatériaux

More information

Numerical modelling of elastic-plastic deformation at crack tips in composite material under stress wave loading

Numerical modelling of elastic-plastic deformation at crack tips in composite material under stress wave loading JOURNAL DE PHYSIQUE IV Colloque C8, supplément au Journal de Physique III, Volume 4, septembre 1994 C8-53 Numerical modelling of elastic-plastic deformation at crack tips in composite material under stress

More information

Nonlinear free transverse vibration of n*p-dof

Nonlinear free transverse vibration of n*p-dof Nonlinear free transverse vibration of n*p-dof K. LATRACH a, Z. BEIDOURI a, R. BOUKSOUR a, R. BENAMAR b a. Laboratoire de Mécanique Productique & Génie Industriel (LMPGI), Université Hassan II Ain Chock,

More information

Modélisation & simulation de la génération de champs magnetiques par des écoulements de métaux liquides. Wietze Herreman

Modélisation & simulation de la génération de champs magnetiques par des écoulements de métaux liquides. Wietze Herreman Modélisation & simulation de la génération de champs magnetiques par des écoulements de métaux liquides Wietze Herreman 19ième Colloque Alain Bouyssy!!"#$%&'()*+(,#-*.#*+( )/01+"2(!!!!!!! Origine des champs

More information

La question posée (en français, avec des mots justes ; pour un calcul, l'objectif doit être clairement écrit formellement)

La question posée (en français, avec des mots justes ; pour un calcul, l'objectif doit être clairement écrit formellement) Exercise : You have to make one ton of mayonnaise sauce using 95 % oil, 2.5 % egg yolk, 2.5 % vinegar. What is the minimum energy that you have to spend? Calculation for mayonnaise Hervé 4th October 2013

More information

Expression of Dirichlet boundary conditions in terms of the strain tensor in linearized elasticity

Expression of Dirichlet boundary conditions in terms of the strain tensor in linearized elasticity Expression of Dirichlet boundary conditions in terms of the strain tensor in linearized elasticity Philippe Ciarlet a, Cristinel Mardare b a Department of Mathematics, City University of Hong Kong, 83

More information

SSNV199 Cracking of a beam DCB with cohesive models

SSNV199 Cracking of a beam DCB with cohesive models Titre : SSNV199 - Fissuration d une poutre DCB avec des mo[...] Date : 05/09/2012 Page : 1/12 SSNV199 Cracking of a beam DCB with cohesive models Summarized: This test makes it possible to model the propagation

More information

SSNL141 - P multifibre and multimatériaux goatskin bottles

SSNL141 - P multifibre and multimatériaux goatskin bottles Titre : SSNL141 - Poutres multifibres et multimatériaux Date : 17/07/2014 Page : 1/7 SSNL141 - P multifibre and multimatériaux goatskin bottles Summary: The objective this test is to validate the use of

More information

Apprentissage automatique Méthodes à noyaux - motivation

Apprentissage automatique Méthodes à noyaux - motivation Apprentissage automatique Méthodes à noyaux - motivation MODÉLISATION NON-LINÉAIRE prédicteur non-linéaire On a vu plusieurs algorithmes qui produisent des modèles linéaires (régression ou classification)

More information

Apprentissage automatique Machine à vecteurs de support - motivation

Apprentissage automatique Machine à vecteurs de support - motivation Apprentissage automatique Machine à vecteurs de support - motivation RÉGRESSION À NOYAU régression à noyau Algorithme de régression à noyau entraînement : prédiction : a = (K + λi N ) 1 t. y(x) =k(x) T

More information

Elasticité de surface. P. Muller and A. Saul Surf. Sci Rep. 54, 157 (2004).

Elasticité de surface. P. Muller and A. Saul Surf. Sci Rep. 54, 157 (2004). Elasticité de surface P. Muller and A. Saul Surf. Sci Rep. 54, 157 (2004). The concept I Physical origin Definition Applications Surface stress and crystallographic parameter of small crystals Surface

More information

Φ B. , into the page. 2π ln(b/a).

Φ B. , into the page. 2π ln(b/a). Chapitre 29 Induction électromagnétique [13 au 15 juin] DEVOIR : 29.8; 29.20; 29.22; 29.30; 29.36 29.1. Expériences d'induction Il n est pas nécessaire de lire cette section. Ce qu il faut retenir de la

More information

La molécule d'adn vue comme une poutre élastique : application aux expériences de pinces magnétiques

La molécule d'adn vue comme une poutre élastique : application aux expériences de pinces magnétiques La molécule d'adn vue comme une poutre élastique : application aux expériences de pinces magnétiques joint work with: Sébastien Neukirch CNRS & UPMC Univ Paris 6 Institut Jean le Rond d Alembert Michael

More information

Boundary-value Problems in Rectangular Coordinates

Boundary-value Problems in Rectangular Coordinates Boundary-value Problems in Rectangular Coordinates 2009 Outline Separation of Variables: Heat Equation on a Slab Separation of Variables: Vibrating String Separation of Variables: Laplace Equation Review

More information

Ecoulements turbulents des eaux peu profondes Turbulent flows in shallow water

Ecoulements turbulents des eaux peu profondes Turbulent flows in shallow water Ecoulements turbulents des eaux peu profondes Turbulent flows in shallow water SERGEY GAVRILYUK a, HENRI GOUIN b a. Université d Aix-Marseille & C.N.R.S. U.M.R. 6595, IUSTI, Project SMASH, 5 rue E. Fermi,

More information

NORME INTERNATIONALE INTERNATIONAL STANDARD

NORME INTERNATIONALE INTERNATIONAL STANDARD NORME INTERNATIONALE INTERNATIONAL STANDARD CEI IEC 60027-1 1992 AMENDEMENT 1 AMENDMENT 1 1997-05 Amendement 1 Symboles littéraux à utiliser en électrotechnique Partie 1: Généralités Amendment 1 Letter

More information

Determining the asphalt mastercurve from free-free resonant testing on cylindrical samples

Determining the asphalt mastercurve from free-free resonant testing on cylindrical samples Determining the asphalt mastercurve from free-free resonant testing on cylindrical samples Nils RYDEN Engineering Geology, Faculty of Engineering, Lund University, Sweden Abstract There is a need to develop

More information

Time-varying cascade model for flow forecasting

Time-varying cascade model for flow forecasting Hydrological forecasting - Prévisions hydrologiques (Proceedings of the Oxford Symposium, April 1980; Actes du Colloque d'oxford, avril 1980): IAHS-AISH Publ. no. 129. Time-varying cascade model for flow

More information

Numerical solution of the Monge-Ampère equation by a Newton s algorithm

Numerical solution of the Monge-Ampère equation by a Newton s algorithm Numerical solution of the Monge-Ampère equation by a Newton s algorithm Grégoire Loeper a, Francesca Rapetti b a Département de Mathématiques, Ecole Polytechnique Fédérale de Lausanne, 1015 Lausanne, CH

More information

Poisson s ratio effect of slope stability calculations

Poisson s ratio effect of slope stability calculations Poisson s ratio effect of slope stability calculations Murray Fredlund, & Robert Thode SoilVision Systems Ltd., Saskatoon, SK, Canada ABSTRACT This paper presents the results of a study on the effect of

More information

Cartesian closed 2-categories and rewriting

Cartesian closed 2-categories and rewriting Cartesian closed 2-categories and rewriting Aurore Alcolei A brief presentation of Tom Hirschowitz s paper, Cartesian closed 2-categories and permutation equivalence in higher-order rewriting June 7, 2014

More information

Dynamics of cold dark matter. Michael Joyce

Dynamics of cold dark matter. Michael Joyce Dynamics of cold dark matter Michael Joyce Dynamics of cold dark matter Michael Joyce Dynamics of cold dark matter Michael Joyce My hidden past * Current physical theory of the fundamental interactions

More information

Introduction 1. Partie II : Cosmologie

Introduction 1. Partie II : Cosmologie Introduction 1 Partie II : Cosmologie Introduction 2 Only 5% of universe is ordinary matter! For the first time in human history we believe we have an inventory of the constituents of the universe. Rapid

More information

Chaotic gas bubble oscillations in a viscoelastic fluid

Chaotic gas bubble oscillations in a viscoelastic fluid Chaotic gas bubble oscillations in a viscoelastic fluid Javier Jimenez-Fernandez Dp to. Ingenieria Energetica y Fluidomecdnica, E.T.S.I. Industriales, 28006 Madrid, Spain Abstract Regular and chaotic radial

More information

The thin plate theory assumes the following deformational kinematics:

The thin plate theory assumes the following deformational kinematics: MEG6007 (Fall, 2017) - Solutions of Homework # 8 (ue on Tuesay, 29 November 2017) 8.0 Variational Derivation of Thin Plate Theory The thin plate theory assumes the following eformational kinematics: u

More information

Stokes-Darcy coupling for periodically curved interfaces

Stokes-Darcy coupling for periodically curved interfaces Stokes-Darcy coupling for periodically curved interfaces Sören Dobberschütz sdobber@nano.ku.dk February 21, 2014 Abstract We investigate the boundary condition between a free fluid and a porous medium,

More information

Numerical analysis for an interpretation of the pressuremeter test in cohesive soil

Numerical analysis for an interpretation of the pressuremeter test in cohesive soil Numerical analysis for an interpretation of the pressuremeter test in cohesive soil J. Monnet Joseph Fourier University L3S-R Domaine Universitaire, BP n 53, 3841, Grenoble, Cedex 9, France jmonnet@ujf-grenoble.fr

More information

ANNALES SCIENTIFIQUES L ÉCOLE NORMALE SUPÉRIEURE. Cluster ensembles, quantization and the dilogarithm. Vladimir V. FOCK & Alexander B.

ANNALES SCIENTIFIQUES L ÉCOLE NORMALE SUPÉRIEURE. Cluster ensembles, quantization and the dilogarithm. Vladimir V. FOCK & Alexander B. ISSN 0012-9593 ASENAH quatrième série - tome 42 fascicule 6 novembre-décembre 2009 ANNALES SCIENTIFIQUES de L ÉCOLE NORMALE SUPÉRIEURE Vladimir V. FOCK & Alexander B. GONCHAROV Cluster ensembles, quantization

More information

SSLL104 - Predeformations in a straight beam

SSLL104 - Predeformations in a straight beam Titre : SSLL104 - Déformations initiales dans une poutre d[...] Date : 07/08/2012 Page : 1/6 SSLL104 - Predeformations in a straight beam Summarized: This test validates the taking into account of predeformations

More information

Inelastic scattering of 30 Mev polarized protons from 112Cd

Inelastic scattering of 30 Mev polarized protons from 112Cd Inelastic scattering of 30 Mev polarized protons from 112Cd R. De Swiniarski, G. Bagieu, DinhLien Pham, M. Massaad, J.Y. Grossiord, A. Guichard To cite this version: R. De Swiniarski, G. Bagieu, DinhLien

More information

A generalization of the classical Cesàro Volterra path integral formula

A generalization of the classical Cesàro Volterra path integral formula C. R. Acad. Sci. Paris, Ser. I 347 (2009) 577 582 Mathematical Problems in Mechanics A generalization of the classical Cesàro Volterra path integral formula Philippe G. Ciarlet a, Liliana Gratie a, Cristinel

More information

Interslice force functions for computing active and passive earth force

Interslice force functions for computing active and passive earth force 1015 Interslice force functions for computing active and passive earth force Noshin Zakerzadeh, D.G. Fredlund, and D.E. Pufahl Abstract: Recent methods to calculate the lateral earth force on a retaining

More information

Mathematical Methods and its Applications (Solution of assignment-12) Solution 1 From the definition of Fourier transforms, we have.

Mathematical Methods and its Applications (Solution of assignment-12) Solution 1 From the definition of Fourier transforms, we have. For 2 weeks course only Mathematical Methods and its Applications (Solution of assignment-2 Solution From the definition of Fourier transforms, we have F e at2 e at2 e it dt e at2 +(it/a dt ( setting (

More information

Electrodynamics PHY712. Lecture 4 Electrostatic potentials and fields. Reference: Chap. 1 & 2 in J. D. Jackson s textbook.

Electrodynamics PHY712. Lecture 4 Electrostatic potentials and fields. Reference: Chap. 1 & 2 in J. D. Jackson s textbook. Electrodynamics PHY712 Lecture 4 Electrostatic potentials and fields Reference: Chap. 1 & 2 in J. D. Jackson s textbook. 1. Complete proof of Green s Theorem 2. Proof of mean value theorem for electrostatic

More information

Approximate expressions for the ageing coefficient and the relaxation function in the viscoelastic analysis of concrete structures

Approximate expressions for the ageing coefficient and the relaxation function in the viscoelastic analysis of concrete structures Materials and Structures/Matériaux et Constructions, Vol. 29, April 1996, pp 131-140 Approximate expressions for the ageing coefficient and the relaxation function in the viscoelastic analysis of concrete

More information

Principal Stress Ratios and Their Infuence on the Compressibility of Soils

Principal Stress Ratios and Their Infuence on the Compressibility of Soils Principal Stress Ratios and Their Infuence on the Compressibility of Soils Les Rapports des contraintes principales et leur influence sur la compressibilité des sols > N. JAN BU, Technical University of

More information

DETERMINING HIGH VOLTAGE CABLE CONDUCTOR TEMPERATURES. Guy Van der Veken. Euromold, Belgium. INVESTIGATIONS. INTRODUCTION.

DETERMINING HIGH VOLTAGE CABLE CONDUCTOR TEMPERATURES. Guy Van der Veken. Euromold, Belgium. INVESTIGATIONS. INTRODUCTION. DETERMINING HIGH VOLTAGE CABLE CONDUCTOR TEMPERATURES. Guy Van der Veken. Euromold, Belgium. INTRODUCTION. INVESTIGATIONS. Type tests on MV cable accessories are described in CENELEC HD68 and HD69 documents.

More information

Outils de Recherche Opérationnelle en Génie MTH Astuce de modélisation en Programmation Linéaire

Outils de Recherche Opérationnelle en Génie MTH Astuce de modélisation en Programmation Linéaire Outils de Recherche Opérationnelle en Génie MTH 8414 Astuce de modélisation en Programmation Linéaire Résumé Les problèmes ne se présentent pas toujours sous une forme qui soit naturellement linéaire.

More information

DESIGN AND ANALYSIS OF CAM MECHANISM WITH TRANSLATING FOLLOWER HAVING DOUBLE ROLLERS. Jung-Fa Hsieh

DESIGN AND ANALYSIS OF CAM MECHANISM WITH TRANSLATING FOLLOWER HAVING DOUBLE ROLLERS. Jung-Fa Hsieh DESIGN AND ANALYSIS OF CAM MECHANISM WITH TRANSLATING FOLLOWER HAVING DOUBLE ROLLERS Jung-Fa Hsieh Far East University Department of Mechanical Engineering Tainan, 74448, Taiwan E-mail: seznof@cc.feu.edu.tw

More information

Some consequences of the analytical theory of the ferromagnetic hysteresis

Some consequences of the analytical theory of the ferromagnetic hysteresis Some consequences of the analytical theory of the ferromagnetic hysteresis G. Biorci, D. Pescetti To cite this version: G. Biorci, D. Pescetti. Some consequences of the analytical theory of the ferromagnetic

More information

MAE 82 Engineering Mathematics

MAE 82 Engineering Mathematics Class otes : First Order Differential Equation on Linear AE 8 Engineering athematics Universe on Linear umerical Linearization on Linear Special Cases Analtical o General Solution Linear Analtical General

More information

TOLERABLE HAZARD RATE FOR FUNCTION WITH INDEPENDENT SAFETY BARRIER ACTING AS FAILURE DETECTION AND NEGATION MECHANISM

TOLERABLE HAZARD RATE FOR FUNCTION WITH INDEPENDENT SAFETY BARRIER ACTING AS FAILURE DETECTION AND NEGATION MECHANISM e Congrès de maîtrise des risques et de sûreté de fonctionnement - Saint-Malo -3 octobre 6 TOLERABLE HAZARD RATE FOR FUNCTION WITH INDEPENDENT SAFETY BARRIER ACTING AS FAILURE DETECTION AND NEGATION MECHANISM

More information

Quasi-invariant measures on the path space of a diffusion

Quasi-invariant measures on the path space of a diffusion Quasi-invariant measures on the path space of a diffusion Denis Bell 1 Department of Mathematics, University of North Florida, 4567 St. Johns Bluff Road South, Jacksonville, FL 32224, U. S. A. email: dbell@unf.edu,

More information

Strength properties of reinforced porous medium

Strength properties of reinforced porous medium ème Congrès Français de Mécanique Bordeaux, 6 au 30 août 03 Strength properties of reinforced porous medium Z. He a, L. Dormieux a, D. Kondo b a. E.N.P.C, Institut Navier, 77455 Marne-la-Vallee, France

More information

Non-uniform consolidation around vertical drains installed in soft ground Consolidation non-uniforme autour de drains verticaux dans un sol faible

Non-uniform consolidation around vertical drains installed in soft ground Consolidation non-uniforme autour de drains verticaux dans un sol faible Non-uniform consolidation around vertical drains installed in soft ground Consolidation non-uniforme autour de drains verticaux dans un sol faible I.C. Pyrah, I.G.N. Smith & D. Hull Napier University,

More information

Meningitis Weekly Bulletin

Meningitis Weekly Bulletin Meningitis Weekly Bulletin Inter country Support Team - West Africa Semaine/Week 40-43 October 2018 Bulletin Hebdomadaire de retro-information sur la méningite cérébrospinale Weekly feedback bulletin on

More information

ME FINITE ELEMENT ANALYSIS FORMULAS

ME FINITE ELEMENT ANALYSIS FORMULAS ME 2353 - FINITE ELEMENT ANALYSIS FORMULAS UNIT I FINITE ELEMENT FORMULATION OF BOUNDARY VALUE PROBLEMS 01. Global Equation for Force Vector, {F} = [K] {u} {F} = Global Force Vector [K] = Global Stiffness

More information

LE JOURNAL DE PHYSIQUE - LETTRES

LE JOURNAL DE PHYSIQUE - LETTRES Les The Tome 46 No 6 15 MARS 1985 LE JOURNAL DE PHYSIQUE - LETTRES J. Physique Lett. 46 (1985) L-217 - L-222 15 MARS 1985, : L-217 Classification Physics Abstracts 75.50K Random free energies in spin glasses

More information

Spectral element schemes for the. Korteweg-de Vries and Saint-Venant equations

Spectral element schemes for the. Korteweg-de Vries and Saint-Venant equations Spectral element schemes for the Korteweg-de Vries and Saint-Venant equations R. PASQUETTI a a. Université Côte d Azur, CNRS, Inria, LJAD, France, richard.pasquetti@unice.fr... Résumé : Les sytèmes hyperboliques

More information

A note on top-k lists: average distance between two top-k lists

A note on top-k lists: average distance between two top-k lists A note on top-k lists: average distance between two top-k lists Antoine Rolland Univ Lyon, laboratoire ERIC, université Lyon, 69676 BRON, antoine.rolland@univ-lyon.fr Résumé. Ce papier présente un complément

More information

FORCES DUE TO DIFFRACTION OF SOUND WAVE ON SMALL-DIAMETER CYLINDRICAL PARTICLES

FORCES DUE TO DIFFRACTION OF SOUND WAVE ON SMALL-DIAMETER CYLINDRICAL PARTICLES FORCES DUE TO DIFFRACTION OF SOUND WAVE ON SMALL-DIAMETER CYLINDRICAL PARTICLES H. Czyz, T. Gudra To cite this version: H. Czyz, T. Gudra. FORCES DUE TO DIFFRACTION OF SOUND WAVE ON SMALL- DIAMETER CYLINDRICAL

More information

Consider an elastic spring as shown in the Fig.2.4. When the spring is slowly

Consider an elastic spring as shown in the Fig.2.4. When the spring is slowly .3 Strain Energy Consider an elastic spring as shown in the Fig..4. When the spring is slowly pulled, it deflects by a small amount u 1. When the load is removed from the spring, it goes back to the original

More information

Soil Mechanics Permeability of Soils and Seepage page 1 CHAPITRE 9. PERMEABILITY OF SOILS AND SEEPAGE...1

Soil Mechanics Permeability of Soils and Seepage page 1 CHAPITRE 9. PERMEABILITY OF SOILS AND SEEPAGE...1 Soil Mechanics Permeability of Soils and Seepage page 1 Contents of this chapter : CHAPITRE 9. PERMEABILITY OF SOILS AND SEEPAGE...1 9.1 INTRODUCTION...1 9.2 DARCY S LAW...1 9.2.1 DEFINITION OF HEAD...1

More information

APPROXIMATE EXPRESSION OF THE "THREE HALVES LAW" FOR A BOUNDED CATHODE IN A UNIFORM FIELD

APPROXIMATE EXPRESSION OF THE THREE HALVES LAW FOR A BOUNDED CATHODE IN A UNIFORM FIELD A translation from Atomic Energy of Canada Limited APPROXIMATE EXPRESSION OF THE "THREE HALVES LAW" FOR A BOUNDED CATHODE IN A UNIFORM FIELD (INTRODUCED BY ACADEMICIAN N.N. SEMENOV 3 JULY 1952) by I.I.

More information

Random variables. Florence Perronnin. Univ. Grenoble Alpes, LIG, Inria. September 28, 2018

Random variables. Florence Perronnin. Univ. Grenoble Alpes, LIG, Inria. September 28, 2018 Random variables Florence Perronnin Univ. Grenoble Alpes, LIG, Inria September 28, 2018 Florence Perronnin (UGA) Random variables September 28, 2018 1 / 42 Variables aléatoires Outline 1 Variables aléatoires

More information

arxiv:cs/ v1 [cs.dm] 21 Apr 2005

arxiv:cs/ v1 [cs.dm] 21 Apr 2005 arxiv:cs/0504090v1 [cs.dm] 21 Apr 2005 Abstract Discrete Morse Theory for free chain complexes Théorie de Morse pour des complexes de chaines libres Dmitry N. Kozlov Eidgenössische Technische Hochschule,

More information

3 2 6 Solve the initial value problem u ( t) 3. a- If A has eigenvalues λ =, λ = 1 and corresponding eigenvectors 1

3 2 6 Solve the initial value problem u ( t) 3. a- If A has eigenvalues λ =, λ = 1 and corresponding eigenvectors 1 Math Problem a- If A has eigenvalues λ =, λ = 1 and corresponding eigenvectors 1 3 6 Solve the initial value problem u ( t) = Au( t) with u (0) =. 3 1 u 1 =, u 1 3 = b- True or false and why 1. if A is

More information

Divergence theorems in path space II: degenerate diffusions

Divergence theorems in path space II: degenerate diffusions Divergence theorems in path space II: degenerate diffusions Denis Bell 1 Department of Mathematics, University of North Florida, 4567 St. Johns Bluff Road South, Jacksonville, FL 32224, U. S. A. email:

More information

12. MHD Approximation.

12. MHD Approximation. Phys780: Plasma Physics Lecture 12. MHD approximation. 1 12. MHD Approximation. ([3], p. 169-183) The kinetic equation for the distribution function f( v, r, t) provides the most complete and universal

More information

DESIGN AND ANALYSIS OF CAM MECHANISM WITH NEGATIVE RADIUS ROLLER-FOLLOWER. Jung-Fa Hsieh

DESIGN AND ANALYSIS OF CAM MECHANISM WITH NEGATIVE RADIUS ROLLER-FOLLOWER. Jung-Fa Hsieh DESIGN AND ANALYSIS OF CAM MECHANISM WITH NEGATIVE RADIUS ROLLER-FOLLOWER Jung-Fa Hsieh Department of Mechanical Engineering, Far East University, Tainan, Taiwan E-mail: seznof@cc.feu.edu.tw Received July

More information

Drop impingement on a deep liquid surface: study of a crater s sinking dynamics

Drop impingement on a deep liquid surface: study of a crater s sinking dynamics C. R. Mecanique 331 (2003) 61 67 Drop impingement on a deep liquid surface: study of a crater s sinking dynamics Impact d une goutte sur une surface liquide profonde : étude de la dynamique d enfoncement

More information

3 The Friedmann-Robertson-Walker metric

3 The Friedmann-Robertson-Walker metric 3 The Friedmann-Robertson-Walker metric 3.1 Three dimensions The most general isotropic and homogeneous metric in three dimensions is similar to the two dimensional result of eq. (43): ( ) dr ds 2 = a

More information

A note on the moving hyperplane method

A note on the moving hyperplane method 001-Luminy conference on Quasilinear Elliptic and Parabolic Equations and Systems, Electronic Journal of Differential Equations, Conference 08, 00, pp 1 6. http://ejde.math.swt.edu or http://ejde.math.unt.edu

More information

the transverse beam of light follows a diagonal path because of addition of light and the

the transverse beam of light follows a diagonal path because of addition of light and the Alternative explanation for the Michelson-Morley experiment Daquan Gao 3929 Stonyrun Drive,Louisville KY 40220 USA daquangao@hotmail.com Abstract: The famous Michelson-Morley experiment has been reanalyzed

More information

Aircraft Structures for engineering students Fourth Edition Solutions Manual T. H. G. Megson

Aircraft Structures for engineering students Fourth Edition Solutions Manual T. H. G. Megson Aircraft Structures for engineering students Fourth Edition Solutions Manual T. H. G. Megson This page intentionally left blank Solutions Manual Solutions to Chapter 1 Problems S.1.1 The principal stresses

More information

11.4. Differentiating ProductsandQuotients. Introduction. Prerequisites. Learning Outcomes

11.4. Differentiating ProductsandQuotients. Introduction. Prerequisites. Learning Outcomes Differentiating ProductsandQuotients 11.4 Introduction We have seen, in the first three Sections, how standard functions like n, e a, sin a, cos a, ln a may be differentiated. In this Section we see how

More information

SSNS106 Damage of a reinforced concrete plate under requests varied with model GLRC_DM

SSNS106 Damage of a reinforced concrete plate under requests varied with model GLRC_DM Titre : SSNS106 - Endommagement d une plaque plane sous so[...] Date : 01/03/2013 Page : 1/67 SSNS106 Damage of a reinforced concrete plate under requests varied with model GLRC_DM Summarized: This test

More information

Extending Zagier s Theorem on Continued Fractions and Class Numbers

Extending Zagier s Theorem on Continued Fractions and Class Numbers Extending Zagier s Theorem on Continued Fractions and Class Numbers Colin Weir University of Calgary Joint work with R. K. Guy, M. Bauer, M. Wanless West Coast Number Theory December 2012 The Story of

More information

The piston problem in hyperelasticity with the stored energy in separable form

The piston problem in hyperelasticity with the stored energy in separable form The piston problem in hyperelasticity with the stored energy in separable form Serge Ndanou Nicolas Favrie Sergey Gavrilyuk To cite this version: Serge Ndanou Nicolas Favrie Sergey Gavrilyuk. The piston

More information

The First Fundamental Form

The First Fundamental Form The First Fundamental Form Outline 1. Bilinear Forms Let V be a vector space. A bilinear form on V is a function V V R that is linear in each variable separately. That is,, is bilinear if αu + β v, w αu,

More information

Exercise sheet n Compute the eigenvalues and the eigenvectors of the following matrices. C =

Exercise sheet n Compute the eigenvalues and the eigenvectors of the following matrices. C = L2 - UE MAT334 Exercise sheet n 7 Eigenvalues and eigenvectors 1. Compute the eigenvalues and the eigenvectors of the following matrices. 1 1 1 2 3 4 4 1 4 B = 1 1 1 1 1 1 1 1 1 C = Which of the previous

More information

Vector-Valued Functions

Vector-Valued Functions Vector-Valued Functions 1 Parametric curves 8 ' 1 6 1 4 8 1 6 4 1 ' 4 6 8 Figure 1: Which curve is a graph of a function? 1 4 6 8 1 8 1 6 4 1 ' 4 6 8 Figure : A graph of a function: = f() 8 ' 1 6 4 1 1

More information

INFLUENCE OF INITIAL STATE OF STRESS AND AMPLITUDE OF DISPLACEMENT ON THE CYLIC BEEHAVIOUR OF INTERFACE

INFLUENCE OF INITIAL STATE OF STRESS AND AMPLITUDE OF DISPLACEMENT ON THE CYLIC BEEHAVIOUR OF INTERFACE 57ième CONGRÈS CANADIEN DE GÉOTECHNIQUE 5ième CONGRÈS CONJOINT SCG/AIH-CNN 57TH CANADIAN GEOTECHNICAL CONFERENCE 5TH JOINT CGS/IAH-CNC CONFERENCE INFLUENCE OF INITIAL STATE OF STRESS AND AMPLITUDE OF DISPLACEMENT

More information

Equidistant curve coordinate system. Morio Kikuchi

Equidistant curve coordinate system. Morio Kikuchi Equidistant curve coordinate system Morio Kiuchi Abstract: An isometry is realized between Poincaré dis of which radius is not limited to 1 and upper half-plane. Poincaré metrics are the same in both regions

More information

The p-adic Jacquet-Langlands correspondence and a question of Serre

The p-adic Jacquet-Langlands correspondence and a question of Serre The p-adic Jacquet-Langlands correspondence and a question of Serre Sean Howe University of Chicago CNTA 2016, 2016-06-24 Outline Serre s mod p Jacquet-Langlands A p-adic Jacquet-Langlands Proof (highlights)

More information

Analysis of the quality of suspended sediment data

Analysis of the quality of suspended sediment data Sediment Budgets (Proceedings of the Porto Alegre Symposium, December 1988). IAHS Publ. no. 174, 1988. Analysis of the quality of suspended sediment data F. R. SEMMELMANN & A. E. LANNA Institute of Hydraulic

More information

CHAPTER 5. Beam Theory

CHAPTER 5. Beam Theory CHPTER 5. Beam Theory SangJoon Shin School of Mechanical and erospace Engineering Seoul National University ctive eroelasticity and Rotorcraft Lab. 5. The Euler-Bernoulli assumptions One of its dimensions

More information

Experimental studies on low-rise structural walls

Experimental studies on low-rise structural walls Materials and Structures/Matériaux et Constructions, Vol. 31, August-September 1998, pp 465-472 Experimental studies on low-rise structural walls Y. L. Mo 1 and J. Y. Kuo 2 1) Professor, Dept. of Civil

More information

Math 265 (Butler) Practice Midterm III B (Solutions)

Math 265 (Butler) Practice Midterm III B (Solutions) Math 265 (Butler) Practice Midterm III B (Solutions). Set up (but do not evaluate) an integral for the surface area of the surface f(x, y) x 2 y y over the region x, y 4. We have that the surface are is

More information

Waves in plasma. Denis Gialis

Waves in plasma. Denis Gialis Waves in plasma Denis Gialis This is a short introduction on waves in a non-relativistic plasma. We will consider a plasma of electrons and protons which is fully ionized, nonrelativistic and homogeneous.

More information

Solving the torsion problem for isotropic matrial with a rectangular cross section using the FEM and FVM methods with triangular elements

Solving the torsion problem for isotropic matrial with a rectangular cross section using the FEM and FVM methods with triangular elements Solving the torsion problem for isotropic matrial with a rectangular cross section using the FEM and FVM methods with triangular elements Nasser M. Abbasi. June 0, 04 Contents Introduction. Problem setup...................................

More information

The coercive force and rotational hysteresis of elongated ferromagnetic particles

The coercive force and rotational hysteresis of elongated ferromagnetic particles The coercive force and rotational hysteresis of elongated ferromagnetic particles S. Shtrikman, D. Treves To cite this version: S. Shtrikman, D. Treves. The coercive force and rotational hysteresis of

More information

1. De Sitter Space. (b) Show that the line element for a positively curved FRW model (k = +1) with only vacuum energy (P = ) is

1. De Sitter Space. (b) Show that the line element for a positively curved FRW model (k = +1) with only vacuum energy (P = ) is 1. De Sitter Space (a) Show in the context of expanding FRW models that if the combination +3P is always positive, then there was a Big Bang singularity in the past. [A sketch of a(t) vs.t may be helpful.]

More information

Final Exam Ship Structures Page 1 MEMORIAL UNIVERSITY OF NEWFOUNDLAND. Engineering Ship Structures

Final Exam Ship Structures Page 1 MEMORIAL UNIVERSITY OF NEWFOUNDLAND. Engineering Ship Structures Final Exam - 53 - Ship Structures - 16 Page 1 MEMORIA UNIVERSITY OF NEWFOUNDAND Faculty of Engineering and Applied Science Engineering 53 - Ship Structures FINA EXAMINATION SONS Date: Wednesday April 13,

More information

5.7 Differential Equations: Separation of Variables Calculus

5.7 Differential Equations: Separation of Variables Calculus 5.7 DIFFERENTIAL EQUATIONS: SEPARATION OF VARIABLES In the last section we discussed the method of separation of variables to solve a differential equation. In this section we have 4 basic goals. (1) Verif

More information

The interaction of normal fault ruptures and shallow foundations: (failles normale et fondations) Centrifuge modelling. Contents

The interaction of normal fault ruptures and shallow foundations: (failles normale et fondations) Centrifuge modelling. Contents The interaction of normal fault ruptures and shallow foundations: (failles normale et fondations) Centrifuge modelling Fraser Bransby, Ala a El Nahas, Shuichi Nagaoka, Michael Davies The University of

More information

Physics 235 Chapter 7. Chapter 7 Hamilton's Principle - Lagrangian and Hamiltonian Dynamics

Physics 235 Chapter 7. Chapter 7 Hamilton's Principle - Lagrangian and Hamiltonian Dynamics Chapter 7 Hamilton's Principle - Lagrangian and Hamiltonian Dynamics Many interesting physics systems describe systems of particles on which many forces are acting. Some of these forces are immediately

More information

David Izabel. To cite this version: HAL Id: hal

David Izabel. To cite this version: HAL Id: hal Taking into account the rigidity of space-time in general relativity - Understanding by a simple analogy based on the concepts of the strength of materials David Izabel To cite this version: David Izabel.

More information