THE MODELING OF THE LIMIT STATE OF DUCTILE THICK-WALLED PIPES WITH AXIAL SURFACE DEFECTS Orynyak I.V., Ageyev S.M. G.S. Pisarenko Institute for Problems.

Slides:



Advertisements
Similar presentations
Codes and Standards Future Work
Advertisements

Mechanics of Materials II
Theoretical solutions for NATM excavation in soft rock with non-hydrostatic in-situ stresses Nagasaki University Z. Guan Y. Jiang Y.Tanabasi 1. Philosophy.
STATICALLY DETERMINATE STRESS SYSTEMS
CTC / MTC 222 Strength of Materials Chapter 12 Pressure Vessels.
1 By Terence James Haydock Pressure Vessel A simulated response in ANSYS.
Batura A.S., Orynyak I.V. IPS NASU Pisarenko’ Institute for Problems of Strength, Kyiv, Ukraine National Academy of Sciences of Ukraine Pisarenko’ Institute.
MODELLING OF DEFORMATION AND DAMAGE OF SPECIMENS UNDER STATIC AND DYNAMIC LOADING Kondryakov E.A., Lenzion S.V., and Kharchenko V.V.
Second Hungarian-Ukrainian Joint Conference on Safety, Reliability and Risk of Engineering Plants and Components, Kiev, September 2007 Second Hungarian-Ukrainian.
3 Torsion.
ITER VV supports Cadarache 6 September 2007 A. Capriccioli.
Analysis of Simple Cases in Heat Transfer P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Gaining Experience !!!
1 TRC 2008 The Effect of (Nonlinear) Pivot Stiffness on Tilting Pad Bearing Dynamic Force Coefficients – Analysis Jared Goldsmith Research Assistant Dr.
Lecture #19 Failure & Fracture
Application Solutions of Plane Elasticity
Tests of Hardened Concrete. Stress Balance for equilibrium  loads = external forces  internal forces = stress Axial tension.
Copyright © 2011 Pearson Education South Asia Pte Ltd
University of Stuttgart Institute of Construction Materials (IWB) 1/34 Discrete Bond Element for 3D Finite Element Analysis of RC Structures Steffen Lettow.
MECHANICS OF MATERIALS 7th Edition
13.4. GENERAL DESIGN CONSIDERATIONS: PRESSURE VESSELS
Orynyak I.V., Radchenko S.A. IPS NASU Pisarenko’ Institute for Problems of Strength, Kyiv, Ukraine National Academy of Sciences of Ukraine Pisarenko’ Institute.
CHAPTER OBJECTIVES Analyze the stress developed in thin-walled pressure vessels Review the stress analysis developed in previous chapters regarding axial.
FAILURE INVESTIGATION OF UNDERGROUND DISTANT HEATING PIPELINE
CTC / MTC 222 Strength of Materials Final Review.
Orynyak I.V., Borodii M.V., Batura A.S. IPS NASU Pisarenko’ Institute for Problems of Strength, Kyiv, Ukraine National Academy of Sciences of Ukraine Pisarenko’
G.S.Pisarenko Institute for Problems of strength National Academy of Sciences, Ukraine G. V. Stepanov Decrease of residual stresses in structure elements.
High strength materials are being increasingly used in designing critical components to save weight or meet difficult service conditions. Unfortunately.
FE Exam Preparation Design
9 Torsion.
IPS NASU DYNAMICAL ANALYSIS AND ALLOWABLE VIBRATION DETERMINATION FOR THE PIPING SYSTEMS. G.S. Pisarenko Institute for Problems of Strength of National.
©Teaching Resource in Design of Steel Structures IIT Madras, SERC Madras, Anna Univ., INSDAG 1 COMPOSITE FLOORS - II.
Example: Radially Polarized Tube. Introduction This is a 2D static axisymmetric piezoelectric benchmark problem A radially polarized piezoelectric tube.
CHAPTER OBJECTIVES Analyze the stress developed in thin-walled pressure vessels Review the stress analysis developed in previous chapters regarding axial.
Optimization Of a Viscous Flow Between Parallel Plates Based On The Minimization Of Entropy Generation Presentation By Saeed Ghasemi.
Order of Magnitude Scaling of Complex Engineering Problems Patricio F. Mendez Thomas W. Eagar May 14 th, 1999.
Mechanical Design of Process Equipment FUNDAMENTAL PRINCIPLES AND EQUATIONS Principal stresses Theories of failure
3 Torsion.
LIMIT LOAD CALCULATION MODEL OF DUCTILE FAILURE OF DEFECTIVE PIPE AND PRESSURE VESSEL Orynyak I.V. G.S. Pisarenko Institute for Problems of Strength, National.
Task 2.2 – Identification of most suitable face-sheets and optimization of panel properties Duration: month 1 to month 12 Partners involved: MOTULAB (WP.
I. M. DMYTRAKH and V. V. PANASYUK Karpenko Physico-Mechanical Institute, National Academy of Sciences of Ukraine 5 Naukova Street, Lviv, 79601, UKRAINE.
1 Wardenier “Tubular Structures Course” Examples Hollow Section Trusses Design Procedure.
Lecture # 21 This chapter serves as a review of the stress analysis that has been developed in the previous chapters regarding axial load, torsion, bending.
COMBINED LOADING.  Analyze the stress developed in thin-walled pressure vessels  Review the stress analysis developed in previous chapters regarding.
Mechanics of Materials
LATHE VIBRATIONS ANALYSIS ON SURFACE ROUHHNESS OF MACHINED DETAILS LATHE VIBRATIONS ANALYSIS ON SURFACE ROUHHNESS OF MACHINED DETAILS * Gennady Aryassov,
Differential Equations Linear Equations with Variable Coefficients.
CAD and Finite Element Analysis Most ME CAD applications require a FEA in one or more areas: –Stress Analysis –Thermal Analysis –Structural Dynamics –Computational.
1 - An AISI 1020 cold- rolled steel tube has an OD of 3.0 inch. The internal pressure in the tube is 6,840 psi. Determine the thickness of the tube using.
EGM 5653 Advanced Mechanics of Materials
Bay Zoltán Foundation for Applied Reseach Institute for Logistics and Production Systems BAY-LOGI Assessment of crack like defect in dissimilar welded.
Combined Loadings Thin-Walled Pressure Vessels Stress caused by Combined Loadings.
Solid Mechanics Course No. ME213.
Design Factor Collapse
Design Factors The axial load on the casing can be either tensile or compressive, depending on the operating conditions.
DEPARTMENT OF MECHANICAL AND MANUFACTURING ENGINEERING
Seismic analysis of Bridges Part II
The Thick Walled Cylinder
Chapter 3: One-Dimensional Steady-State Conduction
G H Patel College of Engineering And Technology Design of Machine Elements cylindrical pressure vessel subjected to internal and external.
Orynyak I.V., Borodii M.V., Batura A.S.
The Thick Walled Cylinder
CAD and Finite Element Analysis
Christopher R. McGann, Ph.D. Student University of Washington
DEPARTMENT OF MECHANICAL AND MANUFACTURING ENGINEERING
3 Torsion.
Chapter 7 Transverse Shear.
CLAVARINO’S EQUATION MAXIMUM NORMAL STRAIN THEORY
DEPARTMENT OF MECHANICAL AND MANUFACTURING ENGINEERING
Copyright ©2014 Pearson Education, All Rights Reserved
Yielding And Fracture Under Combine Stresses
Presentation transcript:

THE MODELING OF THE LIMIT STATE OF DUCTILE THICK-WALLED PIPES WITH AXIAL SURFACE DEFECTS Orynyak I.V., Ageyev S.M. G.S. Pisarenko Institute for Problems of Strength, Kiev, Ukraine

Plan Existing models for pipes with defects. The problems of modeling of the thick-walled pipes. The proposed analytical model for thick-walled pipes. The theoretical analysis of the results. The comparison with experimental data. Discussion. Application to a repair technology.

Existing models for pipes with defects C – crack half-length ℓ – crack half-width a – crack depth - dimensionless ligament thickness - dimensionless crack length dimensionless limit pressure or strength reduction coefficient - «local» formula of the Battelle Memorial Institute - «global» formula of the Battelle Memorial Institute - «global» formula Staat - «local» formula Staat - formula DNV

The problems of modeling of the thick-walled pipes 1. The choice of limit characteristic. 2. The choice of criterion of ductile failure. 3. The irregularity of defect’s form. 4. Interaction of closely situated defects. 5. The taking into account the wall thickness. 6. External/internal defects.

The choice of limit characteristic

The choice of criterion of ductile failure (for unflawed thick-walled pipes). № mm Specimen orientation MPa 1 88,9 4,0 longitudinal 336 486 42,7-47,0 45,8 52,9 2 8,8 324 457 94,2-100,6 100,8 116,4 3 22,2 288 438 307,1 303,1 350,0 4 101,6 10,0 284 408 97,5 89,9 103,3 5 transverse 390 100,2 115,7 6 139,7 12,5 266 400 73,5-76,0 78,9 91,1 7 338 432 85,2 98,4 8 512 642 57,9-61,8 60,5 69,93 9 506 634 135,4-170,7 139,9 161,5 10 473 614 416,9-421,8 424,9 490,6 11 689 740 183-175 162,2 187,3 12 717 759 166,4 192,1 13 648 702 152,0 138,4 159,8 14 668 719 141,8 163,7

The proposed analytical model for thick-walled pipes The proposed analytical model for thick-walled pipes. Analytical model of the Institute for problems of strength (for thin-walled pipes) the equation of forces equilibrium in the radial direction - the circumferential force; х – axial coordinate; - transverse force - limit condition - external - internal dimensionless limit pressure for the thin-walled pipe with axial surface defect

External/internal defects the limit bending moment

The taking into account the wall thickness local equation of equilibrium for thin-walled pipe the solution of differential equation The pipe with external defect The pipe with internal defect

The theoretical analyze of the results The dimensionless limit pressure versus dimensionless crack length for the model of thick-walled pipes with external/internal defects. The comparison of analytical models for thin-walled pipe: and for the thick-walled pipe:

The comparison with experimental data (Staat’s data) № 1 3,105 0,8 0,865 0,85 0,851 0,014 -0,001 0,826 -0,025 2 1,769 0,5 0,681 0,639 0,744 -0,063 -0,105 0,704 0,598 -0,04 -0,146 3 3,656 0,566 0,549 0,583 -0,017 -0,034 0,605 0,533 0,022 -0,05 4 9,63 0,52 0,518 0,502 0,018 0,016 0,541 0,497 0,039 -0,005 5 4,009 0,35 0,408 0,393 0,417 -0,009 -0,024 0,473 0,377 0,096 internal № 1 3,642 0,48 0,564 0,546 0,633 -0,069 -0,087 0,585 0,476 -0,048 -0,157 2 6,549 0,525 0,518 0,506 0,019 0,012 0,551 0,451 0,045 -0,055 3 15,018 0,49 0,52 0,519 0,491 0,029 0,028 0,536 0,445 -0,046 4 1,044 0,284 0,693 0,622 0,705 -0,012 -0,083 0,689 0,424 -0,016 -0,281 5 2,456 0,433 0,396 0,477 -0,044 -0,081 0,495 0,309 0,018 -0,168 6 3,783 0,31 0,389 0,371 -0,035 -0,053 0,45 0,306 0,026 -0,118 7 6,69 0,327 0,321 0,35 -0,023 -0,029 0,378 0,263 8 6,775 0,3 0,338 0,332 0,311 0,027 0,021 0,387 0,274 0,076 -0,037 9 15,159 0,302 0,009 0,008 0,339 0,251 0,037 -0,051 10 15,244 0,24 0,262 0,281 -0,018 -0,019 0,294 0,209 0,013 -0,072 11 1,411 0,091 0,415 0,337 0,584 -0,169 -0,247 0,527 0,133 -0,057 -0,451 12 0,034 0,362 0,249 0,574 -0,212 -0,295 0,502 0,051 -0,523 external

1. The comparison our models with experimental data for the pipe with internal defect. - “external” formula - “internal” formula 2. The comparison our models with Staat’s “local” formula. internal external 3. The comparison our models with Staat’s “global” formula. internal external

Discussion external (Staat) Influence of the form of the defects № 11 1,186 0,091 0,492 (0,415) 0,404 (0,337) 0,584 12 1,172 0,034 0,448 (0,362) 0,355 (0,279) 0,574

Application - pipe’s geometry - defect’s geometry the pipe with sleeve the pipe with defect - pipe’s geometry - defect’s geometry 1. - the pipe without defect 2. - the pipe with defect 3. Numerical analyze and simplify analytical model - the added thick pipe’s wall as a result of used sleeve (equal 8 MPa) 4. - the pipe with sleeve 5. - experiment