SSNP110 - Crack of edge in a rectangular plate finished in elastoplasticity

Similar documents
HSNV140 - Thermoplasticity with restoration of work hardening: test of blocked dilatometry

Code_Aster. SDLV123 - Computation of G elastodynamic in infinite medium for a plane crack finite length

Code_Aster. SSNP161 Biaxial tests of Kupfer

SSNP102 - Rate of energy restitution for a plate notched in elastoplasticity: approaches Summarized

SSNV221 Hydrostatic test with a behavior DRUCK_PRAGER linear and parabolic

HPLP100 - Calculation of the rate of refund of the energy of a plate fissured in thermoelasticity

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

HPLP300 - Plate with Young modulus function of the temperature

SDLV121 - Wave planes shearing in an elastic column

SSNA109 - Tensile test with the model VISC_CIN2_CHAB

SSNV199 Cracking of a beam DCB with cohesive models

Code_Aster. HSNV120 - Tension hyper elastic of a bar under thermal loading

ZZZZ120 - Calculation of an assembly pin-attaches

Code_Aster. SDNL113 - Piping in the shape of quadrant (tests ELSA) under seismic loading

Code_Aster. SDNV114 Simulation of benchmark SAFE - T5 veil out of reinforced concrete

Code_Aster. SSNV160 - Hydrostatic test with the law CAM_CLAY

Code_Aster. HSNV129 - Test of compression-dilation for study of the coupling thermics-cracking

Code_Aster. Law of behavior BETON_REGLE_PR

Version default Titre : Opérateur CALC_G Date : 07/12/2017 Page : 1/21 Responsable : GÉNIAUT Samuel Clé : U Révision : 73174f7ae6ec

SSNV231 Sphere digs under internal pressure in great deformations

Fracture mechanics. code_aster, salome_meca course material GNU FDL licence (

Example-3. Title. Description. Cylindrical Hole in an Infinite Mohr-Coulomb Medium

Code_Aster. SSNV235 - Influence of the temperature in the evolution of the creep of the laws of behavior KIT_RGI and BETON_BURGER

SSNV137 - Cable of prestressed in a Summarized concrete straight beam

SDNV114 Simulation of benchmark SAFE - T5 veil

SDLS505 - Buckling of a cylindrical envelope under external pressure

Non-linear and time-dependent material models in Mentat & MARC. Tutorial with Background and Exercises

SSNV235 - Law of behavior KIT_RGI : Influence of the temperature in the evolution of creep

Finite Element Simulation of the Liquid Silicon Oriented Crystallization in a Graphite Mold

Stresses Analysis of Petroleum Pipe Finite Element under Internal Pressure

Coupled CFD-FE-Analysis for the Exhaust Manifold of a Diesel Engine

Using MATLAB and. Abaqus. Finite Element Analysis. Introduction to. Amar Khennane. Taylor & Francis Croup. Taylor & Francis Croup,

Models of Bordet and Rice and Tracey

EFFECT OF STRAIN HARDENING ON ELASTIC-PLASTIC CONTACT BEHAVIOUR OF A SPHERE AGAINST A RIGID FLAT A FINITE ELEMENT STUDY

Seismic Response Analysis of Structure Supported by Piles Subjected to Very Large Earthquake Based on 3D-FEM

Code_Aster. A finite element of cable-pulley

Computational models of diamond anvil cell compression

University of Sheffield The development of finite elements for 3D structural analysis in fire

3-D Finite Element Analysis of Instrumented Indentation of Transversely Isotropic Materials

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading

MECHANICAL TESTING METHODS CONCERNING THE STRESS ANALYSIS FOR A VEHICLE WHEEL RIM

1 Introduction. Abstract

TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK

Constitutive models: Incremental plasticity Drücker s postulate

Practice Final Examination. Please initial the statement below to show that you have read it

Code_Aster. SSLS135 - Reinforcement of a square tank according to the method of Capra and Maury

Code_Aster. SDLL14 - Modes of vibration of an elbow of thin piping

Finite Element Method in Geotechnical Engineering

SSLL104 - Predeformations in a straight beam

SSNL141 - P multifibre and multimatériaux goatskin bottles

Prediction of the bilinear stress-strain curve of engineering material by nanoindentation test

Elastic-Plastic Fracture Mechanics. Professor S. Suresh

Code_Aster. Reaction of the steel subjected to corrosion

Experimental and theoretical characterization of Li 2 TiO 3 and Li 4 SiO 4 pebbles

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC.

Nonlinear Finite Element Modeling of Nano- Indentation Group Members: Shuaifang Zhang, Kangning Su. ME 563: Nonlinear Finite Element Analysis.

ANALYSIS AND SIMULATION OF AN AIRPLANE SEAT DURING VERTICAL IMPACTS

Shock Wave Propagation due to Methane-Air Mixture Explosion and Effect on a Concrete Enclosure

HSNV122 - Thermoplasticity and metallurgy in large deformations in simple tension

Module I: Two-dimensional linear elasticity. application notes and tutorial. Problems

6 Examples of pneumatic structures and material models for membranes

ELASTOPLASTIC STEEL BEAM BENDING ANALYSIS BY USING ABAQUS

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

Effect of Plasticity on Residual Stresses Obtained by the Incremental Hole-drilling Method with 3D FEM Modelling

Procedure for Performing Stress Analysis by Means of Finite Element Method (FEM)

Finite Element Analysis Prof. Dr. B. N. Rao Department of Civil Engineering Indian Institute of Technology, Madras. Module - 01 Lecture - 11

Lecture 8. Stress Strain in Multi-dimension

ENGN 2290: Plasticity Computational plasticity in Abaqus

USER S MANUAL 1D Seismic Site Response Analysis Example University of California: San Diego August 30, 2017

A PAPER ON DESIGN AND ANALYSIS OF PRESSURE VESSEL

Ultimate shear strength of FPSO stiffened panels after supply vessel collision

An example solution of a panel in the elastic-plastic regime

A FINITE ELEMENT STUDY OF ELASTIC-PLASTIC HEMISPHERICAL CONTACT BEHAVIOR AGAINST A RIGID FLAT UNDER VARYING MODULUS OF ELASTICITY AND SPHERE RADIUS

DISPENSA FEM in MSC. Nastran

Modelling the behaviour of plastics for design under impact

FEA A Guide to Good Practice. What to expect when you re expecting FEA A guide to good practice

Content. Department of Mathematics University of Oslo

SSNL141 beams multifibre and multimatériaux

A Finite Element Study of Elastic-Plastic Hemispherical Contact Behavior against a Rigid Flat under Varying Modulus of Elasticity and Sphere Radius

Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground

Transactions on Modelling and Simulation vol 9, 1995 WIT Press, ISSN X

EMEA. Liudmila Feoktistova Engineer Atomenergoproekt

elastoplastic contact problems D. Martin and M.H. Aliabadi Wessex Institute of Technology, Ashurst Lodge, Ashurst, Southampton, SO40 7AA, UK

The Finite Element Method II

Deterministic and stochastic investigation of welded, high strength steel T joint

Effect of Strain Hardening on Unloading of a Deformable Sphere Loaded against a Rigid Flat A Finite Element Study

ALGORITHM FOR NON-PROPORTIONAL LOADING IN SEQUENTIALLY LINEAR ANALYSIS

Module 10: Free Vibration of an Undampened 1D Cantilever Beam

FINITE ELEMENT ANALYSIS OF TAPERED COMPOSITE PLATE GIRDER WITH A NON-LINEAR VARYING WEB DEPTH

Shock wave speed and stress-strain relation of aluminium honeycombs under dynamic compression

Stress and Displacement Analysis of a Rectangular Plate with Central Elliptical Hole

NUMERICAL SIMULATION OF FLANGE-BOLT INTERACTION IN WIND TUBRINE TOWER CONNECTIONS

Deflections and Strains in Cracked Shafts due to Rotating Loads: A Numerical and Experimental Analysis

ULTIMATE STRENGTH OF SQUARE PLATE WITH RECTANGULAR OPENING UNDER AXIAL COMPRESSION

ANALYTICAL PENDULUM METHOD USED TO PREDICT THE ROLLOVER BEHAVIOR OF A BODY STRUCTURE

6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and

Numerical Solutions of 2-D Linear Elastostatic Problems by Network Method

MODELING OF CONCRETE MATERIALS AND STRUCTURES. Kaspar Willam. Uniaxial Model: Strain-Driven Format of Elastoplasticity

MITOCW MITRES2_002S10nonlinear_lec15_300k-mp4

PSEUDO ELASTIC ANALYSIS OF MATERIAL NON-LINEAR PROBLEMS USING ELEMENT FREE GALERKIN METHOD

Transcription:

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 1/14 SSNP110 - Crack of edge in a rectangular plate finished in elastoplasticity Summary: This test is a CAS-test in nonlinear breaking process. One considers a rectangular plate finished, fissured and subjected to a loading of traction. The law of behavior used is an elastoplastic law of Von Mises. This CAS-test understands five modelings in 2D : modelings A and B, in plane constraints, aim at studying the influence of the taking into account or not of the terms of second order of the deformations ( DEFORMATION = PETIT' or GREEN in the operator STAT_NON_LINE ) on the calculation of the rate of refund of energy G ; modelings C and D, in plane constraints, aim at testing method X-FEM (crack nonwith a grid) in nonlinear elasticity and elastoplasticity for calculation of the field of displacement; modeling E, in plane deformations, validates the calculation of G for the various methods of definition of the curve of work hardening.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 2/14 1 Problem of reference 1.1 Geometry C L B Uy= With has W Uy=- there X D Length Width Depth of crack L=50mm W =16 mm a=6 mm 1.2 Properties of material The material is elastoplastic of type Von Mises. For modelings A with D, there is no work hardening. For modeling E, various laws of work hardening are compared (linear work hardening or power). The properties of material are the following ones: Young modulus Poisson's ratio Yield stress Module of work hardening E=2,060110 5 MPa =0.3 y =808,34 MPa H =0 (modeling A with D) or H =6,867 10 4 MPa (modeling E) 1.3 Boundary conditions and loading For modelings A, B and E, the model is limited to half of the structure, the plan of the vertical crack being a symmetry plane. For modelings C and D, the totality of the structure is represented. Boundary conditions Vertical displacement UX =0 at the point B Horizontal displacement UY =0 in the ligament AB (condition of symmetry for modelings A, B and E) Loading Horizontal displacement imposed on the segment CD : UY =

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 3/14 2 Reference solution Pas de reference solution. This is a test of not-regression.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 4/14 3 Modeling A 3.1 Characteristics of modeling It is about a calculation in elastoplasticity under the assumption of small displacements, in plane constraints. 3.2 Characteristics of the grid Grid, built with an automatic procedure gibi, consists of 400 quadratic elements (1000 nodes). Tori are defined in bottom of crack in order to improve the precision of calculation in breaking process, cf [Figure 3.2-a] below. The ray of the largest torus is of 1,5 mm. Figure 3.2-a: Grid of the fissured rectangular plate

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 5/14 3.3 Sizes tested and results The values of the rate of refund are tested for five values of imposed horizontal displacement. One compares the results got for three different crowns of integration: crown 1: R inf =0,15 mm ; R sup =0,6mm crown 2: R inf =0,3 mm ; R sup =0,9mm crown 3: R inf =0,9 mm ; R sup =1,5 mm Imposed displacement ( mm ) G N /mm crown 1 G N /mm crown 2 G N /mm crown 3 0.02 3.29 3.20 3.20 0.04 13.60 13.24 13.24 0.06 31.97 31.22 31.24 0.08 58.99 57.74 57.76 0.1 91.42 89.64 89.71 The results are satisfactory: the maximum variation enters the values of G obtained on the three crowns of integration is lower than 2 %.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 6/14 4 Modeling B 4.1 Characteristics of modeling It is about a calculation in elastoplasticity under the assumption of great displacements, in plane constraints. 4.2 Characteristics of the grid The grid is identical to that of modeling A. 4.3 Sizes tested and results The values of the rate of refund are tested for the same crowns of integration as in modeling A. Imposed displacement ( mm ) G N /mm crown 1 G N /mm crown 2 G N /mm crown 3 0.02 3.26 3.17 3.18 0.04 13.36 13.03 13.07 0.06 31.02 30.50 30.67 0.08 56.33 55.90 56.51 0.1 85.84 85.91 87.47 The results are satisfactory: the maximum variation enters the values of G obtained on the three crowns of integration is lower than 2 %. The effect of the terms of second order in the deformation is relatively weak: the difference between the results of two modelings is increasing with imposed displacement and is worth to the maximum 6%, cf [Figure 4.4-a].

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 7/14 G (N/mm) 100 90 80 70 60 50 40 30 20 10 0 MODELISATION A MODELISATION B 0 0,02 0,04 0,06 0,08 0,1 0,12 Deplacement imposé (mm) Figure 4.4-a: Comparison of the rates of refund of energy of two modelings

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 8/14 5 Modeling C 5.1 Characteristics of modeling It is about a calculation in nonlinear elasticity under the assumption of small displacements, with method X-FEM (crack nonwith a grid). Modeling is in plane constraints. 5.2 Characteristics of the grid The grid is composed of linear elements (560 meshs QUA4-600 nodes). The refinement of the grid is uniform (18 elements according to x and 31 elements according to y ). 5.3 Sizes tested and results The component is tested DY displacement at the two points where the crack emerges (points of each lip), at the last moment of calculation (imposed displacement 0,1mm ). This test is carried out on the field of displacement created by the operator POST_CHAM_XFEM. The value of reference is the solution obtained in modeling A. Lip considered Reference ( mm ) Code_Aster ( mm ) Difference ( % ) Lip y>0 9,876.10-2 9,516.10-2 -3,6% Lip y<0-9,876.10-2 -9,516.10-2 -3,6% This test validates calculation in nonlinear elasticity for models X-FEM.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 9/14 6 Modeling D 6.1 Characteristics of modeling It is about a calculation in elastoplasticity under the assumption of small displacements, with method X-FEM (crack nonwith a grid). One represents the opening of the crack and his closing by activating the contact on the lips. Compared to modeling C one replaces non-linear elasticity by elastoplasticity. Until moment 0.1 the loading is monotonous and the results are thus identical between modelings C and D. In modeling D, one carries out then a discharge and one applies an opposed loading, thus activating the contact to the lips of the crack. 6.2 Characteristics of the grid The grid is identical to that of modeling C. 6.3 Sizes tested and results Two sizes are tested: the component DY displacement at the two points where the crack emerges (points of each lip), at moment 0.1 of calculation (imposed displacement 0,1 mm ) and at last moment 0.3 (imposed displacement 0,1mm ); values of the effective plastic deformation ( V1 ) on the mesh M277, in item 10 and at moments 0,1,0,14 and 0.3. For moment 0.1, the value of reference of displacement is the solution obtained in modeling A. For the rest, the tests are of not-regression.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 10/14 Displacement Reference ( mm ) Code_Aster ( mm ) Difference ( % ) Lip y 0, t=0.1 9,876.10-2 9,532.10-2 -3,5% Lip y 0, t=0.1-9,876.10-2 -9,533.10-2 -3,5% Lip y 0, t=0.3 1,782.10-2 Not-regression Lip y 0, t=0.3-1,782.10-2 Not-regression Effective plastic deformation ( V1 on M277 ) t=0.1 1.270.10-2 Not-regression t=0.14 1.270.10-2 Not-regression t=0.3 2.451.10-2 Not-regression This test validates calculation in elastoplasticity for models X-FEM.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 11/14 7 Modeling E 7.1 Characteristics of modeling It is about a calculation in nonlinear elasticity under the assumption of small displacements, in plane deformations. 7.2 Characteristics of the grid The grid is identical to that of modeling A. 7.3 Sizes tested and results The size tested is the rate of refund G, calculated for the first crown of integration defined in modeling A and for ten values of imposed horizontal displacement ( varying 0 with 0,2mm ). Two series distinct from calculations are carried out: initially, one takes a law of behaviour to linear work hardening. Three calculations are carried out with the various methods available to define the same curve of work hardening ( TRACTION, ECRO_LINE and ECRO_PUIS). One compares between them the solutions obtained by these three calculations; then one chooses a law of behaviour with work hardening in law power and one compares the got results enters ELAS_VMIS_TRAC and ELAS_VMIS_PUIS. The test is of standard not-regression. It is checked that: three various calculations in linear work hardening lead exactly to the same result on G ; two calculations in work hardening in law power lead to very close results (lower deviation than 0,3%). The variation decreases if the step of time of calculation is decreased.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 12/14 Imposed displacement ( mm ) G N /mm - linear work hardening: ELAS_VMIS_TRAC G N /mm - linear work hardening: ELAS_VMIS_LINE G N /mm - linear work hardening: ELAS_VMIS_PUIS 0.02 3.59 3.59 3.59 0.04 14.47 14.47 14.47 0.06 32.88 32.88 32.88 0.08 59.42 59.42 59.42 0.10 94.50 94.50 94.50 0.12 134.98 134.98 134.98 0.14 178.95 178.95 178.95 0.16 226.24 226.24 226.24 0.18 276.47 276.47 276.47 0.20 329.61 329.61 329.61 Imposed displacement ( mm ) G N /mm - work hardening power: ELAS_VMIS_TRAC G N /mm - work hardening power: ELAS_VMIS_PUIS 0.02 3.59 3.59 0.04 14.44 14.44 0.06 32.76 32.76 0.08 58.99 58.98 0.10 93.76 93.77 0.12 136.14 136.18 0.14 184.04 184.09 0.16 236.31 236.38 0.18 292.38 292.46 0.20 351.82 351.90 This test validates the calculation of G in linear elasticity for the various methods of definition of the curve of work hardening.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 13/14 8 Modeling F 8.1 Characteristics of modeling idem modeling C with quadratic elements. 8.2 Characteristics of the grid The grid is composed of linear elements (560 meshs QUA8-600 nodes). The refinement of the grid is uniform (18 elements according to x and 31 elements according to y ), identical to modeling C. 8.3 Sizes tested and results The component is tested DY displacement at the two points where the crack emerges (points of each lip), at the last moment of calculation (imposed displacement 0,1mm ). This test is carried out on the field of displacement created by the operator POST_CHAM_XFEM. The value of reference is the solution obtained in modeling A. Lip considered Reference ( mm ) Difference ( % ) Lip y 0 9,876.10-2 2 % Lip y 0-9,876.10-2 2 % This test validates calculation in nonlinear elasticity for models X-FEM and of the quadratic elements in plane constraints.

Titre : SSNP110 - Fissure de bord dans une plaque rectangu[...] Date : 21/07/2017 Page : 14/14 9 Summary of the results This case test aims at validating the calculation of the rate of refund of the constraints in elastoplasticity: modelings A and B make it possible to make sure of the invariance of the calculation of the rate of refund of energy by the method theta according to the crowns of integration for laws of perfectly plastic behavior of the elastic type -. One also notes the weak contribution of the terms of second order in the deformation; modeling E validates the various methods of definition of the curve of work hardening. Modelings C, D and F allow to validate the calculation of the field of displacement for models X-FEM.