Study on the Energy Absorption and the Local Buckling of the Expansion Tubes

Size: px
Start display at page:

Download "Study on the Energy Absorption and the Local Buckling of the Expansion Tubes"

Transcription

1 * Study on the Energy Absorption and the Local Buckling of the Expansion Tubes Kwanghyun Ahn * Jinsung Kim Hoon Huh School of Mechanical, Aerospace & System Engineering, Korea Advanced Institute of Science and Technology, Science town, Daejeon 3-71, Korea (Received / Accepted) Abstract : This paper deals with the local buckling characteristics and the energy absorption of the expansion tubes with the various dimensions of tubes and punch shapes The local buckling load and absorbed energy during the tube flaring process were discussed for each cases of tube and punch shapes by finite element analysis Absorbed energy of expansion tube is affected by the diameter and the wall thickness of tubes Punch angle and expansion ratio also affect to the energy absorption According to the buckling analysis, local buckling can occurs in some cases The absorbed energy of expansion tube significantly decreases when local buckling occurs For enhancement of energy absorption, it is important to predict local buckling load accurately In this study local buckling load is predicted by modification of equation Key words : Expansion tube( ), Energy absorption( ), Local buckling( ) 1 1) Device) (Light Collision Safety (Expansion Tube), 4 MJ 1,2) * ankh-1128@kaistackr

2 Table 1 Dimension of tube Parameter Range Thickness, t (mm) 1 t 3 Inner radius, r i (mm) 3 r i 46 Length, L (mm) 1 L 2 Friction coefficient, f 1 f FEM(Finete Element Method), FEM 3),,,, Fig 1 2 mm, 39 mm, 1 mm, 3 Table 1 Table 2 Table 2 Dimension of punch Parameter Range Punch angle, α 1 α 4 Expansion ratio, e(r p/r i) 12 e 1 Engineering stress (MPa) UTS = 9 MPa Yield = 43 MPa Engineering strain Fig 2 Engineering stress-strain curve of TWIP TWIP Fig 2 TWIP Fig 3 α=3, e=13, L=1 mm, r=39 mm 1 mm Fig 3 1, 1 mm 1 mm Fig 4 α=3, e=13, L=1 mm, t=2 mm Fig 1 Finite element model of tube and punch

3 t=3 mm t=2 mm t=2 mm t=1 mm t=1 mm L=1 L=12 L=1 L=17 L= Tube wall thickness (mm) Fig 3 Effect of tube wall thickness: Absorbed energy; Absorbed energy at punch stroke of 1 mm r=47 mm r=43 mm r=39 mm r=3 mm r=31 mm Tube length (mm) Fig Effect of tube length: Absorbed energy; Absorbed energy at punch stroke of 1 mm Fig α=3, e=13, r=39 mm, t=2 mm 222 Fig 6 Fig 7 t=2 mm, r=39 mm, L=1 mm Tube radius (mm) Fig 4 Effect of tube radius: Absorbed energy; Absorbed energy at punch stroke of 1 mm 23

4 1 1 α=6 o α=4 o α=3 o α=1 o e=1 e=14 e=13 e= Punch angle (degree) Fig 6 Effect of punch angle: Absorbed energy; Absorbed energy at punch stroke of 1 mm Expansion ratio Fig 7 Effect of expansion ratio: Absorbed energy; Absorbed energy at punch stroke of 1 mm Table 3 4 4) t=2 mm, r=39 mm, L=1 mm 1 Table σ σ α σ σ α α (1) σ σ α α Table 3 Four types of buckling behavior 4) Buckling Buckling Theory behavior load (kn) Elastic column buckling Euler formula Inelastic Tangent modulus column buckling formula Elastic local buckling Batdorf Inelastic local buckling equation 217 FEM result () 226 where α σ σ cr : buckling stress σ y : yield stress E : Young's modulus D : tube diameter (1) Table 4

5 Table 4 Dimension of tube Parameter Range Thickness, t (mm) 1 t 3 Radius, r (mm) 3 r Length, L (mm) 1 Friction coefficient, f (perfectly plastic) equation Stress (MPa) Stress strain curve of TWIP Average of stress distribution through thickness direction Strain Fig 9 Averaged stress distribution through thickness direction at the point that buckling occur Fig Tube wall thickness (mm) (perfectly plastic) equation Tube radius (mm) Fig 8 Local buckling load of expansion tubes using equation: buckling load wrt the tube wall thickness; buckling load wrt the tube radius Fig 8 Fig 1 (2) π ε (2) where σ ε (Ludwik model) ε : buckling strain Fig 11 Fig 11 2

6 (using averaged stress) equation Tube wall thickness (mm) (using averaged stress) equation Tube radius (mm) Fig 1 Local buckling load of expansion tubes using equation (2): buckling load wrt the tube wall thickness; bucklin load wrt the tube radius 32 Fig 11 Buckling strain wrt the tube wall thickness and tube radius Buckling load by equation (2) Bucklin load Punch angle (degree) Fig 12 Buckling load wrt the punch angle Fig 12 1 % 4 References 1) W M Choi, H S Jung, W H Yu, J S Ku and T S Kwon, "The basic study on the design of the light collision safety device", Proc KSR fall conference, pp26~31, 26 2) J S Kim, H Huh, J W Lee, T S Kwon, "Dynamic tensile characteristics of the steel sheets for a train", Proc KSAE spring conference, pp231~236, 27 3) Hibbit, Karlsson and Sorensen, User's Manual, John wiley & Sons, England, ) Bruce G Johnston, Guide to Stability Design Criteria for Metal Structures, Wiley-Interscience, pp261~329, 1976

THE EFFECTS OF LOCAL BUCKLING ON THE CRASH ENERGY ABSORPTION OF THIN-WALLED EXPANSION TUBES

THE EFFECTS OF LOCAL BUCKLING ON THE CRASH ENERGY ABSORPTION OF THIN-WALLED EXPANSION TUBES THE EFFECTS OF LOCAL BUCKLING ON THE CRASH ENERGY ABSORPTION OF THIN-WALLED EXPANSION TUBES Kwanghyun Ahn, Jin Sung Kim, Hoon Huh * School of Mechanical, Aerospace and System Engineering, KAIST, 335 Gwahangno,

More information

N = Shear stress / Shear strain

N = Shear stress / Shear strain UNIT - I 1. What is meant by factor of safety? [A/M-15] It is the ratio between ultimate stress to the working stress. Factor of safety = Ultimate stress Permissible stress 2. Define Resilience. [A/M-15]

More information

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS CHAPTER THE EFFECTS OF FORCES ON MATERIALS EXERCISE 1, Page 50 1. A rectangular bar having a cross-sectional area of 80 mm has a tensile force of 0 kn applied to it. Determine the stress in the bar. Stress

More information

A Repeated Dynamic Impact Analysis for 7x7 Spacer Grids by using ABAQUS/ Standard and Explicit

A Repeated Dynamic Impact Analysis for 7x7 Spacer Grids by using ABAQUS/ Standard and Explicit A Repeated Dynamic Impact Analysis for 7x7 Spacer Grids by using ABAQUS/ Standard and Explicit Kim, Jae-Yong, and Yoon, Kyung-Ho* * Korea Atomic Energy Research Institute ABSTRACT Spacer grids(sg) are

More information

Mechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002

Mechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002 student personal identification (ID) number on each sheet. Do not write your name on any sheet. #1. A homogeneous, isotropic, linear elastic bar has rectangular cross sectional area A, modulus of elasticity

More information

Critical Load columns buckling critical load

Critical Load columns buckling critical load Buckling of Columns Buckling of Columns Critical Load Some member may be subjected to compressive loadings, and if these members are long enough to cause the member to deflect laterally or sideway. To

More information

A novel technique of friction and material property measurement by tip test in cold forging

A novel technique of friction and material property measurement by tip test in cold forging A novel technique of friction and material property measurement by tip test in cold forging Y T Im*, S H Kang, and J S Cheon Department of Mechanical Engineering, Korea Advanced Institute of Science and

More information

Chapter 5 Torsion STRUCTURAL MECHANICS: CE203. Notes are based on Mechanics of Materials: by R. C. Hibbeler, 7th Edition, Pearson

Chapter 5 Torsion STRUCTURAL MECHANICS: CE203. Notes are based on Mechanics of Materials: by R. C. Hibbeler, 7th Edition, Pearson STRUCTURAL MECHANICS: CE203 Chapter 5 Torsion Notes are based on Mechanics of Materials: by R. C. Hibbeler, 7th Edition, Pearson Dr B. Achour & Dr Eng. K. El-kashif Civil Engineering Department, University

More information

VORONOI APPLIED ELEMENT METHOD FOR STRUCTURAL ANALYSIS: THEORY AND APPLICATION FOR LINEAR AND NON-LINEAR MATERIALS

VORONOI APPLIED ELEMENT METHOD FOR STRUCTURAL ANALYSIS: THEORY AND APPLICATION FOR LINEAR AND NON-LINEAR MATERIALS The 4 th World Conference on Earthquake Engineering October -7, 008, Beijing, China VORONOI APPLIED ELEMENT METHOD FOR STRUCTURAL ANALYSIS: THEORY AND APPLICATION FOR LINEAR AND NON-LINEAR MATERIALS K.

More information

Sean Carey Tafe No Lab Report: Hounsfield Tension Test

Sean Carey Tafe No Lab Report: Hounsfield Tension Test Sean Carey Tafe No. 366851615 Lab Report: Hounsfield Tension Test August 2012 The Hounsfield Tester The Hounsfield Tester can do a variety of tests on a small test-piece. It is mostly used for tensile

More information

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy Stress Analysis Lecture 3 ME 276 Spring 2017-2018 Dr./ Ahmed Mohamed Nagib Elmekawy Axial Stress 2 Beam under the action of two tensile forces 3 Beam under the action of two tensile forces 4 Shear Stress

More information

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS Name :. Roll No. :..... Invigilator s Signature :.. 2011 SOLID MECHANICS Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are required to give their answers

More information

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. D : SOLID MECHANICS Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. Q.2 Consider the forces of magnitude F acting on the sides of the regular hexagon having

More information

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering Mechanics Of Solids Suraj kr. Ray (surajjj2445@gmail.com) Department of Civil Engineering 1 Mechanics of Solids is a branch of applied mechanics that deals with the behaviour of solid bodies subjected

More information

Numerical simulation of sheet metal forming processes using a new yield criterion

Numerical simulation of sheet metal forming processes using a new yield criterion Key Engineering Materials Vol. 344 (007) pp. 833-840 online at http://www.scientific.net (007) Trans Tech Publications, Switzerland Numerical simulation of sheet metal forming processes using a new yield

More information

Compact energy absorbing cellular structure

Compact energy absorbing cellular structure Structures Under Shock and Impact IX 413 Compact energy absorbing cellular structure M. Ali 1, A. Qamhiyah 2, D. Flugrad 1 & M. Shakoor 1 1 Department of Mechanical Engineering, Iowa State University,

More information

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

6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and 6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa (15.5 10 6 psi) and an original diameter of 3.8 mm (0.15 in.) will experience only elastic deformation when a tensile

More information

SELECTED PROBLEMS OF SHORT CIRCUIT WITHSTANDABILITY Section II - POWER TRANSFORMER October 2004, Vigo - Spain

SELECTED PROBLEMS OF SHORT CIRCUIT WITHSTANDABILITY Section II - POWER TRANSFORMER October 2004, Vigo - Spain Dr. Władysław Pewca Institute of Power Engineering, Transformer Division (IenOT( IenOT), Poland SELECTED PROBLEMS OF SHORT CIRCUIT WITHSTANDABILITY Section II - POWER TRANSFORMER 28-30 October 2004, Vigo

More information

External Pressure... Thermal Expansion in un-restrained pipeline... The critical (buckling) pressure is calculated as follows:

External Pressure... Thermal Expansion in un-restrained pipeline... The critical (buckling) pressure is calculated as follows: External Pressure... The critical (buckling) pressure is calculated as follows: P C = E. t s ³ / 4 (1 - ν ha.ν ah ) R E ³ P C = Critical buckling pressure, kn/m² E = Hoop modulus in flexure, kn/m² t s

More information

STANDARD SAMPLE. Reduced section " Diameter. Diameter. 2" Gauge length. Radius

STANDARD SAMPLE. Reduced section  Diameter. Diameter. 2 Gauge length. Radius MATERIAL PROPERTIES TENSILE MEASUREMENT F l l 0 A 0 F STANDARD SAMPLE Reduced section 2 " 1 4 0.505" Diameter 3 4 " Diameter 2" Gauge length 3 8 " Radius TYPICAL APPARATUS Load cell Extensometer Specimen

More information

Introduction to Engineering Materials ENGR2000. Dr. Coates

Introduction to Engineering Materials ENGR2000. Dr. Coates Introduction to Engineering Materials ENGR2 Chapter 6: Mechanical Properties of Metals Dr. Coates 6.2 Concepts of Stress and Strain tension compression shear torsion Tension Tests The specimen is deformed

More information

ENG1001 Engineering Design 1

ENG1001 Engineering Design 1 ENG1001 Engineering Design 1 Structure & Loads Determine forces that act on structures causing it to deform, bend, and stretch Forces push/pull on objects Structures are loaded by: > Dead loads permanent

More information

ScienceDirect. Bauschinger effect during unloading of cold-rolled copper alloy sheet and its influence on springback deformation after U-bending

ScienceDirect. Bauschinger effect during unloading of cold-rolled copper alloy sheet and its influence on springback deformation after U-bending Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 81 (2014 ) 969 974 11th International Conference on Technology of Plasticity, ICTP 2014, 19-24 October 2014, Nagoya Congress

More information

Module 5: Theories of Failure

Module 5: Theories of Failure Module 5: Theories of Failure Objectives: The objectives/outcomes of this lecture on Theories of Failure is to enable students for 1. Recognize loading on Structural Members/Machine elements and allowable

More information

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts. NORMAL STRESS The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts. σ = force/area = P/A where σ = the normal stress P = the centric

More information

SIMPLIFIED MODELING OF THIN-WALLED TUBES WITH OCTAGONAL CROSS SECTION AXIAL CRUSHING. Authors and Correspondance: Abstract:

SIMPLIFIED MODELING OF THIN-WALLED TUBES WITH OCTAGONAL CROSS SECTION AXIAL CRUSHING. Authors and Correspondance: Abstract: SIMPLIFIED MODELING OF THIN-WALLED TUBES WITH OCTAGONAL CROSS SECTION AXIAL CRUSHING Authors and Correspondance: Yucheng Liu, Michael L. Day Department of Mechanical Engineering University of Louisville

More information

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY Spring 2006 Final Examination STUDENT S NAME (please print) STUDENT S SIGNATURE STUDENT NUMBER IDE 110 CLASS SECTION INSTRUCTOR S NAME Do not turn this page until instructed to start. Write your name on

More information

Strength of Material. Shear Strain. Dr. Attaullah Shah

Strength of Material. Shear Strain. Dr. Attaullah Shah Strength of Material Shear Strain Dr. Attaullah Shah Shear Strain TRIAXIAL DEFORMATION Poisson's Ratio Relationship Between E, G, and ν BIAXIAL DEFORMATION Bulk Modulus of Elasticity or Modulus of Volume

More information

COLUMNS: BUCKLING (DIFFERENT ENDS)

COLUMNS: BUCKLING (DIFFERENT ENDS) COLUMNS: BUCKLING (DIFFERENT ENDS) Buckling of Long Straight Columns Example 4 Slide No. 1 A simple pin-connected truss is loaded and supported as shown in Fig. 1. All members of the truss are WT10 43

More information

IMPACT STRENGTH AND RESPONSE BEHAVIOR OF CFRP GUARDER BELT FOR SIDE COLLISION OF AUTOMOBILES

IMPACT STRENGTH AND RESPONSE BEHAVIOR OF CFRP GUARDER BELT FOR SIDE COLLISION OF AUTOMOBILES IMPACT STRENGTH AND RESPONSE BEHAVIOR OF CFRP GUARDER BELT FOR SIDE COLLISION OF AUTOMOBILES AOKI Y.*, BEN G.**, KIM H. S.* *College of Science & Technology, Nihon University **College of Industrial Technology,

More information

ME 243. Mechanics of Solids

ME 243. Mechanics of Solids ME 243 Mechanics of Solids Lecture 2: Stress and Strain Ahmad Shahedi Shakil Lecturer, Dept. of Mechanical Engg, BUET E-mail: sshakil@me.buet.ac.bd, shakil6791@gmail.com Website: teacher.buet.ac.bd/sshakil

More information

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection Mechanics of Materials II Chapter III A review of the fundamental formulation of stress, strain, and deflection Outline Introduction Assumtions and limitations Axial loading Torsion of circular shafts

More information

6.37 Determine the modulus of resilience for each of the following alloys:

6.37 Determine the modulus of resilience for each of the following alloys: 6.37 Determine the modulus of resilience for each of the following alloys: Yield Strength Material MPa psi Steel alloy 550 80,000 Brass alloy 350 50,750 Aluminum alloy 50 36,50 Titanium alloy 800 116,000

More information

Expansion of circular tubes by rigid tubes as impact energy absorbers: experimental and theoretical investigation

Expansion of circular tubes by rigid tubes as impact energy absorbers: experimental and theoretical investigation Expansion of circular tubes by rigid tubes as impact energy absorbers: experimental and theoretical investigation M Shakeri, S Salehghaffari and R. Mirzaeifar Department of Mechanical Engineering, Amirkabir

More information

CIVIL DEPARTMENT MECHANICS OF STRUCTURES- ASSIGNMENT NO 1. Brach: CE YEAR:

CIVIL DEPARTMENT MECHANICS OF STRUCTURES- ASSIGNMENT NO 1. Brach: CE YEAR: MECHANICS OF STRUCTURES- ASSIGNMENT NO 1 SEMESTER: V 1) Find the least moment of Inertia about the centroidal axes X-X and Y-Y of an unequal angle section 125 mm 75 mm 10 mm as shown in figure 2) Determine

More information

Lateral Crushing of Square and Rectangular Metallic Tubes under Different Quasi-Static Conditions

Lateral Crushing of Square and Rectangular Metallic Tubes under Different Quasi-Static Conditions Vol:, No:1, 2 Lateral Crushing of Square and Rectangular Metallic Tubes under Different Quasi-Static Conditions Sajjad Dehghanpour, Ali Yousefi International Science Index, Mechanical and Mechatronics

More information

Parameter Design of High Speed Coupling for 6 MW Wind Turbine Considering Torsional Vibration

Parameter Design of High Speed Coupling for 6 MW Wind Turbine Considering Torsional Vibration Parameter Design of High Speed Coupling for 6 MW Wind Turbine Considering Torsional Vibration JongHun Kang 1, Junwoo Bae 2, Seungkeun Jeong 3, SooKeun Park 4 and Hyoung Woo Lee 1 # 1 Department of Mechatronics

More information

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work.

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work. It is most beneficial to you to write this mock final exam UNDER EXAM CONDITIONS. This means: Complete the exam in 3 hours. Work on your own. Keep your textbook closed. Attempt every question. After the

More information

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich UNIVERSITY OF SASKATCHEWAN ME 313.3 MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich A CLOSED BOOK EXAMINATION TIME: 3 HOURS For Marker s Use Only LAST NAME (printed): FIRST

More information

Stresses Analysis of Petroleum Pipe Finite Element under Internal Pressure

Stresses Analysis of Petroleum Pipe Finite Element under Internal Pressure ISSN : 48-96, Vol. 6, Issue 8, ( Part -4 August 06, pp.3-38 RESEARCH ARTICLE Stresses Analysis of Petroleum Pipe Finite Element under Internal Pressure Dr.Ragbe.M.Abdusslam Eng. Khaled.S.Bagar ABSTRACT

More information

Analysis of asymmetric radial deformation in pipe with local wall thinning under internal pressure using strain energy method

Analysis of asymmetric radial deformation in pipe with local wall thinning under internal pressure using strain energy method Analysis of asymmetric radial deformation in pipe with local wall thinning under internal pressure using strain energy method V.M.F. Nascimento Departameto de ngenharia Mecânica TM, UFF, Rio de Janeiro

More information

The crash response of a train of masses connected by springs and of a single coach B.C. Webb & K. Kormi ± LCO CU// C/6 IT) III

The crash response of a train of masses connected by springs and of a single coach B.C. Webb & K. Kormi ± LCO CU// C/6 IT) III The crash response of a train of masses connected by springs and of a single coach B.C. Webb & K. Kormi /OT* *-r I S± r\ (l U/ U 1}fl U> I Tl (j f* L- Cl U/ i\pqpfl1tr) ± LCO CU// C/6 IT) III Abstract

More information

Chapter 4-b Axially Loaded Members

Chapter 4-b Axially Loaded Members CIVL 222 STRENGTH OF MATERIALS Chapter 4-b Axially Loaded Members AXIAL LOADED MEMBERS Today s Objectives: Students will be able to: a) Determine the elastic deformation of axially loaded member b) Apply

More information

Peak Strain and Displacement Sensors for Structural Health Monitoring

Peak Strain and Displacement Sensors for Structural Health Monitoring Peak Strain and Displacement Sensors for Structural Health Monitoring AKIRA MITA and SHINPEI TAKAHIRA ABSTRACT Simple and inexpensive passive sensors that can monitor the peak strain or displacement of

More information

THE COLLAPSE LOAD IN SUBMARINE PIPELINES UNDER COMPRESSIVE LOAD AND INTERNAL PRESSURE

THE COLLAPSE LOAD IN SUBMARINE PIPELINES UNDER COMPRESSIVE LOAD AND INTERNAL PRESSURE SDSS Rio 010 STABILITY AND DUCTILITY OF STEEL STRUCTURES E. Batista,. Vellasco, L. de Lima (Eds.) Rio de Janeiro, Brazil, September 8-10, 010 THE COLLASE LOAD IN SUBMARINE IELINES UNDER COMRESSIVE LOAD

More information

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING ME 354, MECHANICS OF MATERIALS LABATY COMPRESSION AND BUCKLING PURPOSE 01 January 2000 / mgj The purpose of this exercise is to study the effects of end conditions, column length, and material properties

More information

Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS

Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS Unit 2: Unit code: QCF Level: Credit value: 15 Engineering Science L/601/10 OUTCOME 1 - TUTORIAL COLUMNS 1. Be able to determine the behavioural characteristics of elements of static engineering systems

More information

MAHALAKSHMI ENGINEERING COLLEGE

MAHALAKSHMI ENGINEERING COLLEGE MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAALLI - 6113. QUESTION WITH ANSWERS DEARTMENT : CIVIL SEMESTER: V SUB.CODE/ NAME: CE 5 / Strength of Materials UNIT 3 COULMNS ART - A ( marks) 1. Define columns

More information

Local Buckling. Local Buckling in Columns. Buckling is not to be viewed only as failure of the entire member

Local Buckling. Local Buckling in Columns. Buckling is not to be viewed only as failure of the entire member Local Buckling MORGAN STATE UNIVERSITY SCHOOL OF ARCHITECTURE AND PLANNING LECTURE V Dr. Jason E. Charalamides Local Buckling in Columns Buckling is not to e viewed only as failure of the entire memer

More information

THE S-S CURVE APPROXIMATION FOR GFRP TENSILE SPECIMEN BY USING INVERSE METHOD AND OPTIMIZATION

THE S-S CURVE APPROXIMATION FOR GFRP TENSILE SPECIMEN BY USING INVERSE METHOD AND OPTIMIZATION THE S-S CURVE APPROXIMATION FOR GFRP TENSILE SPECIMEN BY USING INVERSE METHOD AND OPTIMIZATION D. S. Shin and E. S. Jeon Department of Mechanical Engineering, Kongju National University, Korea E-Mail:

More information

CPO Science Foundations of Physics. Unit 8, Chapter 27

CPO Science Foundations of Physics. Unit 8, Chapter 27 CPO Science Foundations of Physics Unit 8, Chapter 27 Unit 8: Matter and Energy Chapter 27 The Physical Properties of Matter 27.1 Properties of Solids 27.2 Properties of Liquids and Fluids 27.3 Properties

More information

ME 2570 MECHANICS OF MATERIALS

ME 2570 MECHANICS OF MATERIALS ME 2570 MECHANICS OF MATERIALS Chapter III. Mechanical Properties of Materials 1 Tension and Compression Test The strength of a material depends on its ability to sustain a load without undue deformation

More information

Towards The. Design of Super Columns. Prof. AbdulQader Najmi

Towards The. Design of Super Columns. Prof. AbdulQader Najmi Towards The Design of Super Columns Prof. AbdulQader Najmi Description: Tubular Column Square or Round Filled with Concrete Provided with U-Links welded to its Walls as shown in Figure 1 Compression Specimen

More information

needed to buckle an ideal column. Analyze the buckling with bending of a column. Discuss methods used to design concentric and eccentric columns.

needed to buckle an ideal column. Analyze the buckling with bending of a column. Discuss methods used to design concentric and eccentric columns. CHAPTER OBJECTIVES Discuss the behavior of columns. Discuss the buckling of columns. Determine the axial load needed to buckle an ideal column. Analyze the buckling with bending of a column. Discuss methods

More information

UNIT I SIMPLE STRESSES AND STRAINS

UNIT I SIMPLE STRESSES AND STRAINS Subject with Code : SM-1(15A01303) Year & Sem: II-B.Tech & I-Sem SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) UNIT I SIMPLE STRESSES

More information

Structural Metals Lab 1.2. Torsion Testing of Structural Metals. Standards ASTM E143: Shear Modulus at Room Temperature

Structural Metals Lab 1.2. Torsion Testing of Structural Metals. Standards ASTM E143: Shear Modulus at Room Temperature Torsion Testing of Structural Metals Standards ASTM E143: Shear Modulus at Room Temperature Purpose To determine the shear modulus of structural metals Equipment Tinius-Olsen Lo-Torq Torsion Machine (figure

More information

Analysis of Thermal Stress in Fatigue Fracture Specimen using Lock-in Thermography

Analysis of Thermal Stress in Fatigue Fracture Specimen using Lock-in Thermography Analysis of Thermal Stress in Fatigue Fracture Specimen using Lock-in Thermography Won-Tae Kim*, Man-Yong Choi**, Jung-Hak Park** * Major of Bio-mechanical Engineering, Kongju National University, Chungnam,

More information

Downloaded from Downloaded from / 1

Downloaded from   Downloaded from   / 1 PURWANCHAL UNIVERSITY III SEMESTER FINAL EXAMINATION-2002 LEVEL : B. E. (Civil) SUBJECT: BEG256CI, Strength of Material Full Marks: 80 TIME: 03:00 hrs Pass marks: 32 Candidates are required to give their

More information

The Effects of Convolution Geometry and Boundary Condition on the Failure of Bellows

The Effects of Convolution Geometry and Boundary Condition on the Failure of Bellows Indian Journal of Science and Technology, Vol 8(S1), 462 466, January 2015 ISSN (Online) : 0974-5645 ISSN (Print) : 0974-6846 DOI: 10.17485/ijst/2015/v8iS1/59417 The Effects of Convolution Geometry and

More information

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. GTE 2016 Q. 1 Q. 9 carry one mark each. D : SOLID MECHNICS Q.1 single degree of freedom vibrating system has mass of 5 kg, stiffness of 500 N/m and damping coefficient of 100 N-s/m. To make the system

More information

The Effect of Geometry on the Stress Behavior of Flexible Tube with the

The Effect of Geometry on the Stress Behavior of Flexible Tube with the The Effect of Geometry on the Stress Behavior of Flexible Tube with the Lateral Deflection Jinbong Kim The Effect of Geometry on the Stress Behavior of Flexible Tube with the Lateral Deflection 1 Jinbong

More information

Ultimate shear strength of FPSO stiffened panels after supply vessel collision

Ultimate shear strength of FPSO stiffened panels after supply vessel collision Ultimate shear strength of FPSO stiffened panels after supply vessel collision Nicolau Antonio dos Santos Rizzo PETROBRAS Rio de Janeiro Brazil Marcelo Caire SINTEF do Brasil Rio de Janeiro Brazil Carlos

More information

Spiral Cylindrical Torsion Spring Analysis

Spiral Cylindrical Torsion Spring Analysis Spiral Cylindrical Torsion Spring Analysis Theory & FEA JingheSu: alwjybai@gmail.com Introduction A torsion spring is a spring that works by torsion or twisting; that is, a fleible elastic object that

More information

MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS

MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS 3 rd Edition Michael S. Mamlouk Arizona State University John P. Zaniewski West Virginia University Solution Manual FOREWORD This solution manual includes

More information

End forming of thin-walled tubes

End forming of thin-walled tubes Journal of Materials Processing Technology 177 (2006) 183 187 End forming of thin-walled tubes M.L. Alves a, B.P.P. Almeida b, P.A.R. Rosa b, P.A.F. Martins b, a Escola Superior de Tecnologia e Gestão

More information

Elasticity. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University Modified by M.

Elasticity. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University Modified by M. Elasticity A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University Modified by M. Lepore Elasticity Photo Vol. 10 PhotoDisk/Getty BUNGEE jumping utilizes

More information

CALCULATION OF A SHEET PILE WALL RELIABILITY INDEX IN ULTIMATE AND SERVICEABILITY LIMIT STATES

CALCULATION OF A SHEET PILE WALL RELIABILITY INDEX IN ULTIMATE AND SERVICEABILITY LIMIT STATES Studia Geotechnica et Mechanica, Vol. XXXII, No. 2, 2010 CALCULATION OF A SHEET PILE WALL RELIABILITY INDEX IN ULTIMATE AND SERVICEABILITY LIMIT STATES JERZY BAUER Institute of Mining, Wrocław University

More information

OPTIMAL DESIGN OF CLUTCH PLATE BASED ON HEAT AND STRUCTURAL PARAMETERS USING CFD AND FEA

OPTIMAL DESIGN OF CLUTCH PLATE BASED ON HEAT AND STRUCTURAL PARAMETERS USING CFD AND FEA International Journal of Mechanical Engineering and Technology (IJMET) Volume 9, Issue 5, May 2018, pp. 717 724, Article ID: IJMET_09_05_079 Available online at http://www.iaeme.com/ijmet/issues.asp?jtype=ijmet&vtype=9&itype=5

More information

Course in. Geometric nonlinearity. Nonlinear FEM. Computational Mechanics, AAU, Esbjerg

Course in. Geometric nonlinearity. Nonlinear FEM. Computational Mechanics, AAU, Esbjerg Course in Nonlinear FEM Geometric nonlinearity Nonlinear FEM Outline Lecture 1 Introduction Lecture 2 Geometric nonlinearity Lecture 3 Material nonlinearity Lecture 4 Material nonlinearity it continued

More information

Solid Mechanics Homework Answers

Solid Mechanics Homework Answers Name: Date: Solid Mechanics Homework nswers Please show all of your work, including which equations you are using, and circle your final answer. Be sure to include the units in your answers. 1. The yield

More information

3 Hours/100 Marks Seat No.

3 Hours/100 Marks Seat No. *17304* 17304 14115 3 Hours/100 Marks Seat No. Instructions : (1) All questions are compulsory. (2) Illustrate your answers with neat sketches wherever necessary. (3) Figures to the right indicate full

More information

FEM Analysis of Punching-Process in Consideration of Micro Die Wear

FEM Analysis of Punching-Process in Consideration of Micro Die Wear FEM Analysis of Punching-Process in Consideration of Micro Die Wear Takashi Ueda 1,a, Takashi Iizuka 1 and Shinichi Enoki 2 1 Department of Mechanical and System Engineering, Kyoto Institute of Technology,

More information

Impact Simulation of Extreme Wind Generated Missiles on Radioactive Waste Storage Facilities

Impact Simulation of Extreme Wind Generated Missiles on Radioactive Waste Storage Facilities Impact Simulation of Extreme Wind Generated Missiles on Radioactive Waste Storage Facilities Gianluca Barbella Sogin S.p.A. Structural Design Department barbella@sogin.it Rotterdam - october 24, 2013 Outline

More information

THE EFFECT OF GEOMETRY ON FATIGUE LIFE FOR BELLOWS

THE EFFECT OF GEOMETRY ON FATIGUE LIFE FOR BELLOWS Advanced Materials Development and Performance (AMDP2011) International Journal of Modern Physics: Conference Series Vol. 6 (2012) 343-348 World Scientific Publishing Company DOI: 10.1142/S2010194512003418

More information

ABSTRACT INTRODUCTION

ABSTRACT INTRODUCTION Optimization of soil anchorages M. Teschner, C. Mattheck Kernforschungszentrum Karlsruhe GmbH, Institut fur Materialforschung II, W-7500 Karlsruhe 1, Postfach 3640, Germany ABSTRACT A new optimization

More information

: APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4021 COURSE CATEGORY : A PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 75 CREDIT : 5 TIME SCHEDULE

: APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4021 COURSE CATEGORY : A PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 75 CREDIT : 5 TIME SCHEDULE COURSE TITLE : APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4021 COURSE CATEGORY : A PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 75 CREDIT : 5 TIME SCHEDULE MODULE TOPIC PERIODS 1 Simple stresses

More information

Design of Steel Structures Prof. S.R.Satish Kumar and Prof. A.R.Santha Kumar

Design of Steel Structures Prof. S.R.Satish Kumar and Prof. A.R.Santha Kumar 5.4 Beams As stated previousl, the effect of local buckling should invariabl be taken into account in thin walled members, using methods described alread. Laterall stable beams are beams, which do not

More information

Conceptual question Conceptual question 12.2

Conceptual question Conceptual question 12.2 Conceptual question 12.1 rigid cap of weight W t g r A thin-walled tank (having an inner radius of r and wall thickness t) constructed of a ductile material contains a gas with a pressure of p. A rigid

More information

The University of Melbourne Engineering Mechanics

The University of Melbourne Engineering Mechanics The University of Melbourne 436-291 Engineering Mechanics Tutorial Four Poisson s Ratio and Axial Loading Part A (Introductory) 1. (Problem 9-22 from Hibbeler - Statics and Mechanics of Materials) A short

More information

Question 1. Ignore bottom surface. Solution: Design variables: X = (R, H) Objective function: maximize volume, πr 2 H OR Minimize, f(x) = πr 2 H

Question 1. Ignore bottom surface. Solution: Design variables: X = (R, H) Objective function: maximize volume, πr 2 H OR Minimize, f(x) = πr 2 H Question 1 (Problem 2.3 of rora s Introduction to Optimum Design): Design a beer mug, shown in fig, to hold as much beer as possible. The height and radius of the mug should be not more than 20 cm. The

More information

MEASUREMENT OF THERMAL STRESS AND PREDICTION OF FATIGUE FOR STS USING LOCK-IN THERMOGRAPHY

MEASUREMENT OF THERMAL STRESS AND PREDICTION OF FATIGUE FOR STS USING LOCK-IN THERMOGRAPHY 12 th A-PCNDT 2006 Asia-Pacific Conference on NDT, 5 th 10 th Nov 2006, Auckland, New Zealand MEASUREMENT OF THERMAL STRESS AND PREDICTION OF FATIGUE FOR STS USING LOCK-IN THERMOGRAPHY Won-Tae Kim 1+,

More information

Modelling and numerical simulation of the wrinkling evolution for thermo-mechanical loading cases

Modelling and numerical simulation of the wrinkling evolution for thermo-mechanical loading cases Modelling and numerical simulation of the wrinkling evolution for thermo-mechanical loading cases Georg Haasemann Conrad Kloß 1 AIMCAL Conference 2016 MOTIVATION Wrinkles in web handling system Loss of

More information

ANALYSIS OF GATE 2018*(Memory Based) Mechanical Engineering

ANALYSIS OF GATE 2018*(Memory Based) Mechanical Engineering ANALYSIS OF GATE 2018*(Memory Based) Mechanical ME Industrial 4% General Aptitude 15% Mathematics 14% Mechanics 4% Manufacturing 14% Mechanics of Materials 14% Thermodynamics 10% Heat Transfer 2% Fluid

More information

EE C247B / ME C218 INTRODUCTION TO MEMS DESIGN SPRING 2016 C. NGUYEN PROBLEM SET #4

EE C247B / ME C218 INTRODUCTION TO MEMS DESIGN SPRING 2016 C. NGUYEN PROBLEM SET #4 Issued: Wednesday, March 4, 2016 PROBLEM SET #4 Due: Monday, March 14, 2016, 8:00 a.m. in the EE C247B homework box near 125 Cory. 1. This problem considers bending of a simple cantilever and several methods

More information

Chapter Two: Mechanical Properties of materials

Chapter Two: Mechanical Properties of materials Chapter Two: Mechanical Properties of materials Time : 16 Hours An important consideration in the choice of a material is the way it behave when subjected to force. The mechanical properties of a material

More information

Failure in Flexure. Introduction to Steel Design, Tensile Steel Members Modes of Failure & Effective Areas

Failure in Flexure. Introduction to Steel Design, Tensile Steel Members Modes of Failure & Effective Areas Introduction to Steel Design, Tensile Steel Members Modes of Failure & Effective Areas MORGAN STATE UNIVERSITY SCHOOL OF ARCHITECTURE AND PLANNING LECTURE VIII Dr. Jason E. Charalambides Failure in Flexure!

More information

Lecture 8. Stress Strain in Multi-dimension

Lecture 8. Stress Strain in Multi-dimension Lecture 8. Stress Strain in Multi-dimension Module. General Field Equations General Field Equations [] Equilibrium Equations in Elastic bodies xx x y z yx zx f x 0, etc [2] Kinematics xx u x x,etc. [3]

More information

Application of Thermal Stress Device for Measuring Thermal Stresses

Application of Thermal Stress Device for Measuring Thermal Stresses Application of Thermal Stress Device for Measuring Thermal Stresses *Sang-Lyul Cha 1) and Jin-Keun Kim 2) 1), 2) Department of Civil Engineering, KAIST, Daejeon 305-600, Korea 1) maikuraki@kaist.ac.kr

More information

Problem d d d B C E D. 0.8d. Additional lecturebook examples 29 ME 323

Problem d d d B C E D. 0.8d. Additional lecturebook examples 29 ME 323 Problem 9.1 Two beam segments, AC and CD, are connected together at C by a frictionless pin. Segment CD is cantilevered from a rigid support at D, and segment AC has a roller support at A. a) Determine

More information

Accordingly, the nominal section strength [resistance] for initiation of yielding is calculated by using Equation C-C3.1.

Accordingly, the nominal section strength [resistance] for initiation of yielding is calculated by using Equation C-C3.1. C3 Flexural Members C3.1 Bending The nominal flexural strength [moment resistance], Mn, shall be the smallest of the values calculated for the limit states of yielding, lateral-torsional buckling and distortional

More information

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2 Samantha Ramirez, MSE Stress The intensity of the internal force acting on a specific plane (area) passing through a point. Δ ΔA Δ z Δ 1 2 ΔA Δ x Δ y ΔA is an infinitesimal size area with a uniform force

More information

Analysis of Tube End Formability of AA 2024 Tubes Using FEM

Analysis of Tube End Formability of AA 2024 Tubes Using FEM International Journal of Current Engineering and Technology, Vol.2, No.1 (March 2012) ISSN 2277-4106 Research Article Analysis of Tube End Formability of AA 2024 Tubes Using FEM Bharathi. P a*, Venkateswarlu.

More information

Numerical simulation the bottom structures. grounding test by LS-DYNA

Numerical simulation the bottom structures. grounding test by LS-DYNA 5 th European LS-DYNA Users Conference Methods and Techniques (3) Numerical simulation the bottom structures grounding test by LS-DYNA Ainian Zhang Graduate School of Frontier Sciences, The University

More information

Agricultural Science 1B Principles & Processes in Agriculture. Mike Wheatland

Agricultural Science 1B Principles & Processes in Agriculture. Mike Wheatland Agricultural Science 1B Principles & Processes in Agriculture Mike Wheatland (m.wheatland@physics.usyd.edu.au) Outline - Lectures weeks 9-12 Chapter 6: Balance in nature - description of energy balance

More information

The Dynamical Loading of the WWER440/V213 Reactor Pressure Vessel Internals during LOCA Accident in Hot and Cold Leg of the Primary Circuit

The Dynamical Loading of the WWER440/V213 Reactor Pressure Vessel Internals during LOCA Accident in Hot and Cold Leg of the Primary Circuit The Dynamical Loading of the WWER440/V213 Reactor Pressure Vessel Internals during LOCA Accident in Hot and Cold Leg of the Primary Circuit ABSTRACT Peter Hermansky, Marian Krajčovič VUJE, Inc. Okružná

More information

OPTIMAL DESIGN OF COMPOSITE INSERTS FOR A HYBRID ULTRACENTRIFUGE ROTOR

OPTIMAL DESIGN OF COMPOSITE INSERTS FOR A HYBRID ULTRACENTRIFUGE ROTOR 18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS OPTIMAL DESIGN OF COMPOSITE INSERTS Hak Gu Lee 1*, Jisang Park 1, Ji Hoon Kim 1 1 Composite Materials Group, KIMS, Changwon, Korea * Corresponding

More information

Maan Jawad Global Engineering & Technology Camas, Washington, U.S.A.

Maan Jawad Global Engineering & Technology Camas, Washington, U.S.A. Proceedings of the ASME 018 Symposium on Elevated Temperature Application of Materials for Fossil, Nuclear, and Petrochemical Industries ETAM018 April 3-5, 018, Seattle, WA, USA ETAM018-6737 ALLOWABLE

More information

COURSE TITLE : APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4017 COURSE CATEGORY : A PERIODS/WEEK : 6 PERIODS/ SEMESTER : 108 CREDITS : 5

COURSE TITLE : APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4017 COURSE CATEGORY : A PERIODS/WEEK : 6 PERIODS/ SEMESTER : 108 CREDITS : 5 COURSE TITLE : APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4017 COURSE CATEGORY : A PERIODS/WEEK : 6 PERIODS/ SEMESTER : 108 CREDITS : 5 TIME SCHEDULE MODULE TOPICS PERIODS 1 Simple stresses

More information

Mechanics of Materials Primer

Mechanics of Materials Primer Mechanics of Materials rimer Notation: A = area (net = with holes, bearing = in contact, etc...) b = total width of material at a horizontal section d = diameter of a hole D = symbol for diameter E = modulus

More information

Design Project 1 Design of a Cheap Thermal Switch ENGR 0135 October 13, 2016 Sangyeop Lee Jordan Gittleman Noah Sargent Seth Strayer Desmond Zheng

Design Project 1 Design of a Cheap Thermal Switch ENGR 0135 October 13, 2016 Sangyeop Lee Jordan Gittleman Noah Sargent Seth Strayer Desmond Zheng 1 Design Project 1 Design of a Cheap Thermal Switch ENGR 0135 October 13, 2016 Sangyeop Lee Jordan Gittleman Noah Sargent Seth Strayer Desmond Zheng 2 Abstract This report will analyze our calculations,

More information