Features and design of elastomer / textile engineered structures. D Boast, C Eng. F Mech E.

Similar documents
Static and Time Dependent Failure of Fibre Reinforced Elastomeric Components. Salim Mirza Element Materials Technology Hitchin, UK

An integrated approach to the design of high performance carbon fibre reinforced risers - from micro to macro - scale

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture

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.

CHEM-C2410: Materials Science from Microstructures to Properties Composites: basic principles

STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS

[5] Stress and Strain

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

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS

INVESTIGATION OF THE PROCESSING PARAMETERS OF A 3D WOVEN REINFORCEMENT

1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor.

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

Chapter 6: Mechanical Properties of Metals. Dr. Feras Fraige

Advanced Structural Analysis EGF Cylinders Under Pressure

Local Stresses in Belt Turnovers in Conveyor Belt

Outline. Tensile-Test Specimen and Machine. Stress-Strain Curve. Review of Mechanical Properties. Mechanical Behaviour

Fibre Friction WHAT IS FIBRE

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

PERIYAR CENTENARY POLYTECHNIC COLLEGE PERIYAR NAGAR - VALLAM THANJAVUR. DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK

QUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A

Geometric and Material Property Effects on the Strength of Rubber-Toughened Adhesive Joints

A Study on the Tube of Integral Propeller Shaft for the Rear-wheel Drive Automobile Using Carbon Composite Fiber

Science 7 Unit B: Structures and Forces. Topic 4. Forces, Loads, & Stresses. pp WORKBOOK. Name:

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE

MATERIALS SCIENCE POLYMERS

ROTATING RING. Volume of small element = Rdθbt if weight density of ring = ρ weight of small element = ρrbtdθ. Figure 1 Rotating ring

Mechanical Properties of Materials

DEPARTMENT OF MECHANICAL ENIGINEERING, UNIVERSITY OF ENGINEERING & TECHNOLOGY LAHORE (KSK CAMPUS).

MECHANICS OF MATERIALS

Materials and Shape. Part 1: Materials for efficient structure. A. K. M. B. Rashid Professor, Department of MME BUET, Dhaka. Learning Objectives

UNIT 1 STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS 1. Define stress. When an external force acts on a body, it undergoes deformation.

The University of Melbourne Engineering Mechanics

DETERMINING THE STRESS PATTERN IN THE HH RAILROAD TIES DUE TO DYNAMIC LOADS 1

ME 243. Mechanics of Solids

Chapter 7. Highlights:

SHEAR STRENGTH OF SOIL UNCONFINED COMPRESSION TEST

12/8/2009. Prof. A.K.M.B. Rashid Department of MME BUET, Dhaka

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

Optimization of blank dimensions to reduce springback in the flexforming process

STRENGTH OF MATERIALS-I. Unit-1. Simple stresses and strains

CHAPTER 4: BENDING OF BEAMS

Pressure Vessels Stresses Under Combined Loads Yield Criteria for Ductile Materials and Fracture Criteria for Brittle Materials


High Tech High Top Hat Technicians. An Introduction to Solid Mechanics. Is that supposed to bend there?

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola

3-dimensional joint torque calculation of compression sportswear using 3D-CG human model

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, Shear Modulus, (S) N/m 2

two structural analysis (statics & mechanics) APPLIED ACHITECTURAL STRUCTURES: DR. ANNE NICHOLS SPRING 2017 lecture STRUCTURAL ANALYSIS AND SYSTEMS

3.032 Problem Set 2 Solutions Fall 2007 Due: Start of Lecture,

Failure analysis of serial pinned joints in composite materials

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

BIAXIAL STRENGTH INVESTIGATION OF CFRP COMPOSITE LAMINATES BY USING CRUCIFORM SPECIMENS

Analysis of Composite Pressure Vessels

Advanced Structural Analysis EGF Section Properties and Bending

Module 5: Theories of Failure

Mechanical Behavior of Circular Composite Springs with Extended Flat Contact Surfaces

INFLUENCE KINDS OF MATERIALS ON THE POISSON S RATIO OF WOVEN FABRICS

Strain Measurement Techniques for Composite Coupon Testing

A Novel Approach for Measurement of Fiber-on-fiber Friction

2 Experiment of GFRP bolt

Sean Carey Tafe No Lab Report: Hounsfield Tension Test

Torsion of Shafts Learning objectives

Influence of the filament winding process variables on the mechanical behavior of a composite pressure vessel

Micro-meso draping modelling of non-crimp fabrics

Earthquakes. Forces Within Eartth. Faults form when the forces acting on rock exceed the rock s strength.

ASPECTS CONCERNING TO THE MECHANICAL PROPERTIES OF THE GLASS / FLAX / EPOXY COMPOSITE MATERIAL

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.

18.Define the term modulus of resilience. May/June Define Principal Stress. 20. Define Hydrostatic Pressure.

Modelling Tension and Torque Properties of Fibre Ropes and splices

INTRODUCTION TO STRAIN

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

Mechanical properties 1 Elastic behaviour of materials

3.22 Mechanical Properties of Materials Spring 2008

Introduction to Engineering Materials ENGR2000. Dr. Coates

SAULTCOLLEGE of AppliedArtsand Technology SaultSte. Marie COURSEOUTLINE

ENG1001 Engineering Design 1

CO~RSEOUTL..INE. revisedjune 1981 by G. Frech. of..a.pqij~t(..~ttsa.fidteconol.q.gy. Sault ",Ste'...:M~ri,e.: SAUl. ir.ft\,nl~t';~l' G ". E b:.

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

Non-conventional Glass fiber NCF composites with thermoset and thermoplastic matrices. F Talence, France Le Cheylard, France

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA SCIENCE FOR TECHNICIANS OUTCOME 1 - STATIC AND DYNAMIC FORCES TUTORIAL 3 STRESS AND STRAIN

Springs Lecture 3. Extension Springs

Mechanics of Materials Primer

R13. II B. Tech I Semester Regular Examinations, Jan MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) PART-A

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

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

DEPARTMENT OF CIVIL ENGINEERING

Downloaded from Downloaded from / 1

Unit Workbook 1 Level 4 ENG U8 Mechanical Principles 2018 UniCourse Ltd. All Rights Reserved. Sample

Lecture 15 Strain and stress in beams

Design and Analysis of a Formula Student Carbon Fibre Rim

Q. 1 Q. 5 carry one mark each.

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV

Module-4. Mechanical Properties of Metals

PES Institute of Technology

FME461 Engineering Design II

Table of Contents. Preface...xvii. Part 1. Level

International Journal of Advance Engineering and Research Development

Module 7: Micromechanics Lecture 29: Background of Concentric Cylinder Assemblage Model. Introduction. The Lecture Contains

Experimental Stress Analysis of Curved Beams Using Strain Gauges

N = Shear stress / Shear strain

Transcription:

Features and design of elastomer / textile engineered structures D Boast, C Eng. F Mech E.

Title of meeting IOM Bla blah

Topics Materials: Environmental acids, water, oil, radiation etc. Bonding. Cost. Processing Methods. Design issues resulting from processing. Where features needed to perform function favour particular processes. Methods for effective design of important details and design criteria. Failure and selection of failure examples for discussion. Videos showing tyre manufacture and filament winding methods of manufacture.

Ways to combine fabrics and elastomers Elastomer is applied to the fabric by spreading an elastomer solution co extruding onto the fibre or textile calendering compression moulding. Products are made and cured or made and shaped and cured. Products are made from joined cured sheets by bonding or welded in the case of thermoplastic elastomers.

Textiles used in rubber composites Commonly used fabric materials, Polyamide, Aramid, Polyester, Rayon, Steel Speciality fabrics, Glass, Carbon, PEEK. Fabric constructions: Woven (square woven cords), also highly anisotropic cords as in tyre manufacture where the weft is very small compared with the warp. Knitted Braided Short fibres (tyre sidewall, conveyor belting) Oriented (by process) felted (random and overlapping) Filament winding methods (Taniq BV)) Tapes

Fabric parameters that define the mechanical performance Cord material, manmade polymer, wool, silk, glass, mineral, carbon, etc. Cord diameter. Cord strength, stiffness and stress strain curve. Cord density, Ends per m (warp), Picks per m (weft). Tex is a unit of measure for the linear mass density of fibres and is defined as the mass in grams per 1000 meters. (Dtex is 1/10 tex). Twist turns per m. Construction: S or Z denotes either left hand or right hand and of the twist, different layers can be built up.

Methods of stress analysis Often rubber / fabric structures see large strains. Rubber can undergo large strains fabrics change shape by the a change in the geometry of the cords. There often is strain concentration around the fabric / rubber interface. Finite element analysis is used by many people but is difficult to do correctly with rubbers and fabrics. Classical theory develops from the geometry of the textile fibres. It gives good results and also a visual appreciation of the construction and stress / strain issues issues involved.

Membrane theory Tension = Pressure * radius (for one radius of curvature). Pressure = Tension / Radius For 2 radii of curvature P = T 1 /R 1 +T 2 /R 2 For the case of the inside bends of hoses then r2 is ive and T1 (hoop stress) is larger.

Relationship between cord angles and deformation Cords crossing at A, X, B and Y assumed to be pin jointed Poisson's ratio is not a singular constant

Cord stress resolved in non isotropic materials

Neutral angle in hose Hoop tension = P * hose rad = Tc*n*sin 2 θ (N/m) Where Tc is cord tension and θ the angle to the axis, n is number f cords per m Axial tension = (½)* pressure * radius = Tc*n*cos 2 θ Hoop stress = 2* axial stress tan 2 θ = 2, θ = 54.7 or neutral angle. The relationship between the forces in the circumferential and meridional directions in a tyre is also is related to tan 2 α, where α is the cord angle to the circumference.

Typical shaped component (airspring)

Cord Terminations bead type Combined friction and e μγ T 1 /T 2 =e μα Friction (and bonded). Clips, jubilee and other types, swaged rings

Shear strain due to unequal strain in top and bottom cords Bead termination design

Tension link details: 6 tonne break load, 2E5 fatigue cycles at 0-4 tonnes cyclic load 15 articulation and able to alter axial length when supplied with internal pressure cm

Crawler track, product example Individual cord break load 1 tonne, fabric strength 250 tonne / m. Cord diameter 3 mm Total strength in 300 mm wide track = 50 tonnes.

Crawler track, product example

Hovercraft skirt Skirt pressure 0.1 MPa, skirt tension (static) 200 kn / m Cured fabric /.

Failure Fibres Tension fatigue Mechanical fatigue Abrasion / fretting Chemical changes Fibres should not be used in compression Elastomer, especially at the fabric / elastomer interface. But this also is a complex stress / strain field. Part failed products are important to look at to find the initiation.

General failure criteria for fibre stress in rubber composites Most commonly used is the ratio of burst to working stress so: Burst pressure / working pressure > 4. Tyres use 9 or 10. note that working stress is often difficult to get and mostly involves an unknown spectrum of loads. Even when the spectrum is known then it is not easy to combine high numbers of cycles at low loads with low numbers of cycles at higher loads. Can be built up from various factors such as: Load sharing between cords (0.5 to 0.7). Cord and rubber fatigue factors. Design factors, stress concentrations etc. Safety factors. Note that we are often working with engineers used to calculating the stress based on well known and understood fatigue levels for steals. With some well established safety factor (i.e.. Norske VERITAS factor for pipelines is 1.4). Comprehensive fatigue testing is desirable but not always possible.

Rubber technology issues Can good consolidation pressure be applied? What is the method of heat application and can the correct temperatures be applied thorough the component to get uniform heat history? Do the materials in the composite have the appropriate cure rates so that everything cures together? Bonding between layers

Strain measurement, (0 to 20%, or 50% maximum) Strain gauges (<15% static). Other resistivity or electrical property methods (Peratech). Visual methods Grids and photo s (for instance the photographic measurement of strain in the fabric of supersonic parachutes, G. Brown and J. E. Ferrier ). Also pixel analysis. Photo elastic. Video strain analysis (i.e. La Vision). Laser Stain Master. Acceleration and double integrate (but big drift). Getting the signal (wires) out (?).

End Thanks to: Cooper / Avon tyres Yokohama fenders as used by Fendercare Marine Taniq La Vision Strain Master