Fabrication and Testing of 2-Dimensional Z-Expandable Auxetic Textile. Structures for Impact Protective Clothing Applications

Size: px
Start display at page:

Download "Fabrication and Testing of 2-Dimensional Z-Expandable Auxetic Textile. Structures for Impact Protective Clothing Applications"

Transcription

1 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 1 Fabrication and Testing of 2-Dimensional Z-Expandable Auxetic Textile Structures for Impact Protective Clothing Applications ASTM Student Project Grant Harini Ramaswamy University of Minnesota-Twin Cities Advisor: Lucy Dunne 12/31/2014

2 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 2 ABSTRACT Auxetic textiles become thicker when subjected to a stretch and are incorporated in functional clothing design (Alderson, 2005). These counter-intuitive smart materials grow in dimensions, in a direction that is perpendicular to the applied force. Among several applications in technical textiles, auxetic materials are incorporated in elbow pads, knee pads and body armor for impact protection and shock absorption. Unlike conventional substances that compress at the point of impact and become vulnerable to breakage when subjected to a tensile stress, auxetic planar materials push towards the point of impact, thereby making the material more resistant to breakage. Since the ratio of the transverse to longitudinal strains (Poisson s ratio) for these materials are negative, these are also referred to as Negative Poisson s Ratio (NPR) materials. Most existing auxetic structures are two-dimensional and grow in the Y axis when stretched along the X axis or vice-versa. Limited research has been directed towards the creation and testing of three-dimensional auxetics that grow in the Z-direction, when subjected to stresses along the X or Y axis. Further, the manufacture of 2D and 3D auxetics is generally complex (Mslija, A., &. Lantada, D. A.). The purpose of this study was to engineer Z-expandable auxetic structures that can be manufactured easily from a sheet-like textile material, for incorporation in an application such as a kneepad. An adaptation of the ASTM D Standard Test Method for Breaking Strength and Elongation of Textile Fabrics and ASTM D Standard Test Method for Thickness of Textile Material was used to determine the engineering Poisson s ratio-- a negative value of which confirms auxeticity. The stresses that come into play during growth and recovery were identified.

3 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 3 INTRODUCTION Classification The word Auxetics has been derived from the Greek word Auxetikos meaning that which tends to increase. These materials exist in various forms ranging from the microscopic to macroscopic as shown in Figure 1. Figure 1: Classification of Auxetics (Scott et al, 2000) Poisson s Ratio The Poisson s ratio is defined as the negative ratio of the transverse strain to the axial strain in the direction of loading (Wan et al. 2004). Conventional materials have positive Poisson s ratio, whereas auxetic materials have negative Poisson s ratio (Goud, 2010). Production of Auxetics Auxetic textiles may be produced in several ways. Inherently auxetic textile fibers could be used to make a fabric that exhibits auxetic behavior. Alternatively, conventional fibers could be made into an auxetic structure as well (Alderson et. al., 2012). A recent study employed various warp knitted 3D spacer auxetic fabrics, which were constructed using a novel geometrical structure with parallelograms. The highest auxetic behavior was examined when stretched in the weft direction and the lowest was observed in warp direction.

4 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 4 The auxetic behavior also reduced with increase in tensile strain. It was also revealed that the auxetic fabric will retain 65% of its effect after 10 cycles of extension. These novel auxetic geometric configurations make it attractive for potential applications like sports and protection (Wang et al., 2013). In another recent research study, rotating square auxetic structures (Figure 2) with enhanced mechanical properties were designed and manufactured for the application of stents for palliative treatment of esophageal cancer. Polyurethane foam sheets were laser cut to the desired structures using the CNC guided laser cutter and the compressive stress-strain behavior was tested on the Instron. Employing the auxetic cell geometry improved the stenting outcomes. The material could get wider when stretched, offer stiffness without being brittle and minimize stresses (Bhullar S.K., et al., 2013). Figure 2: Rotating Square Auxetics with holes (left) and without holes (right) (Bhullar S.K., et al., 2013, p 44) Properties Auxetic materials are suitable for fitting the human body. The ability of the structure to open out when stretched leads to enhanced air permeability under tension. (Wang, et. al., 2013). Auxetic materials exhibit synclastic behavior in that they curve in the same direction of the bending force (Lakes, 1987; Evans, 1990; Cherfas, 1990). In the case of wearable auxetics, this means that the structure would offer more conformability while offering impact protection.

5 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 5 Applications Auxetic polymeric materials are often used in combination with other materials for personal protective sportswear such as crash helmets, knee pads, shin pads, ballistic protection and gloves due to their ability to absorb energy (Liu, et al, 2010). The Defence Clothing and Textile Agency (DCTA) in Colchester has been looking at applications of auxetic textiles for military purposes as shown in Figure 4 (Liu, 2006). Figure 4: Auxetic Materials for Ballistic Protection (Alderson, 1999) It is significant to note that compared to auxetic fibers and auxetic yarns, studies of auxetic fabrics and sheet structures are limited (Wang et.al, 2013). Existing 2D auxetics are generally X-Y expandable (i.e., when stretched along the X-axis, these structures grow in dimensions along the Y axis and vice-versa). There is limited research directed towards developing auxetics that transform from 2D planar structures to 3D, and the growth of auxetics in the Z-direction, when stretched along the X or Y axis that can be incorporated in impact protective clothing. Figure 5: x, y and z axes

6 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 6 METHODOLOGY Figure 6 highlights the scope for innovation in auxetics related to this project. Figure 6: Mind map showing scope for innovation in Auxetics The objectives of this project were to create auxetic textile structures that: (i) Demonstrate growth in the Z direction (normal to the plane), when stretched along the X or Y axis, thereby transforming from 2D to 3D in the process. (ii) Are elastic in nature (i.e., auxetics return to their original configuration once the stresses that they are subjected to are removed). In other words, the deformation that these structures undergo would not be permanent and the growth along Z- direction is retained only as long as the structure is subjected to a stress along the X or Y direction. (iii) Can be easily fabricated from a sheet-type textile material such foam and (or) fabric.

7 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 7 Ideation Various material and design directions were explored as part of open and structured ideation. Explanation for the creation of these structures is beyond the scope of this report. Herringbone Structures Wave and Arc Structures Swastika ( 卐 ) inspired structures (i)paper prototypes with slits (ii)open-celled foam prototypes (iii)closed-celled foam prototypes (iv) Origami prototypes (iv)fabric and industrial felt/foam integrated prototypes Figure 7: Thumbnails of some materials and methods used

8 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 8 Manufacturing Rotating Triangles The following schematic diagrams shows the simplest repeating unit of the rotating triangles structure, which combines four triangular sub-units of polyurethane foam that were sewn together in areas indicated by the red dots. Following this, holes were punched in these triangles and an embroidery floss was threaded through for tensioning purposes, as indicated by the yellow arrows. In order to prevent the floss from cutting into the polyurethane foam, the punched holes were secured with metallic eyelets. Figure 8: Simplest Unit of Rotating Triangles Slot Pop-up The slot pop-up structure was made from two sheets of foam with slots cut out as shown in the diagram. Corresponding flaps from the two structures were spot welded with glue or sewn together with a single stitch. Figure 9: Slot pop-up

9 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 9 Testing Rotating triangles and slot pop-up that were refined and considered for final testing are presented in this study. Images and videos were captured. The images below show front and side views of the prototypes, when subjected to a stretch test on the Instron. Figures 8 (i)-(vi)rotating Triangles (labelled from left to right) (i)(ii)relaxed Views (iii)(iv)intermediate Stretch Positions (v)(vi)completely stretched Figures 9 (i)-(iv) Slot Pop-up (labelled from left to right) (i)(ii) Relaxed View (iii)(iv) Completely stretched The ASTM D Standard Test Method for Breaking Strength and Elongation of Textile Fabrics and ASTM D Standard Test Method for Thickness of Textile Material were adapted for the purpose of this study. The structures considered were made to 9.25 inches (length) x 5 inches (width) and inches (thickness), from closed-cell polyurethane sheets.

10 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 10 Tensile Testing Machine The testing was performed on the Instron 5544 Constant Rate of Elongation (CRE) type machine in which the specimen is subjected to elongation of 0.50 inches at a uniform rate. Measurement The amount of stretch or elongation that the specimen undergoes during tensile testing is expressed in the form of strain. For the purposes of this study, engineering strain (the ratio of the change in length to the original length) of the specimen was determined for the Y and Z axes. Using these values, the engineering Poisson s ratio (ratio of the transverse strain to the longitudinal strain) was determined. Clamping or Holding Devices Specimens were mounted on the clamps manually. Clamp liners were used in order to preclude slippage and minimize specimen failure in the clamped areas. Calibrating Devices The machine had a steel rule running along the longitudinal direction to measure length. A ruler was also attached along the transverse direction in order to measure the change in thickness. In the case of the rotating triangles structure, thickness was determined by measuring the distance between a pair of cardboard sheets without parallax error. Length and thickness measurements were recorded. Images and videos of the mounted structures in various positions were also captured. Figure 10: Measuring Thickness of Samples

11 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 11 Mechanics during Growth and Recovery The stresses that come into play along the longitudinal and transverse directions were identified as shown in Table 1. Type of stress during growth and recovery along longitudinal direction (Y-Axis) Type of stress during growth along transverse direction (Z-Axis) Type of stress during recovery along transverse direction (Z-Axis) Rotating Triangles Tension Buckling/bending (combination of tension and compression) Buckling/bending (combination of tension and compression) Slot Pop-up Shear Radial Radial Table 1: Mechanics of Structures during Growth and Recovery

12 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 12 RESULTS AND DISCUSSION For various lengths of stretch, corresponding thicknesses were recorded, until two consecutive thickness values were obtained, as shown in Table 2 indicating saturation. At 12.5 inches, in the case of the rotating triangles structure, the structure did not expand beyond 2 inches and in the case of the slot pop-up, the slots started reversing beyond an extension of 10.5 inches and reached 0.25 inches. No. Length (Inches) Thickness (Inches) Rotating Triangles Slot Pop-up (when mounted in relaxed position) and (actual) 0.25 (when mounted in relaxed position) and (actual) Table 2: Thickness obtained for Various Lengths Rotating Triangles: Length vs. Thickness Slot Pop-up: Length vs. Thickness Graphs for Rotating Triangles and Slot Pop-up

13 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 13 Auxeticity of both the structures were determined from the Engineering Poisson s ratio values, based on the formula provided below. Strain Transverse T2-T1 Engineering Poisson s Ratio = - = - T1 Strain Longitudinal L2-L1 L1 It is to be noted that in the case of a conventional non-auxetic material, when the value of Strain Longitudinal is positive, Strain Transverse is negative because a stretch along the longitudinal direction will result in a compression along the transverse direction. The formula is usually assigned a negative sign, so that the resultant Poisson s ratio is positive. However, in the case of auxetic materials, since a stretch along the longitudinal direction would result in expansion along the transverse direction, the Strain Longitudinal and Strain Transverse will carry positive signs, and therefore, the resultant Poisson s ratio will be negative. The samples were subjected to ten cycles of minimum and maximum (Table 3) stretch and the average values of these were used to calculate the Poisson s ratio. Rotating Triangles Slot Pop-up Length Thickness Length Thickness Average Minimum Stretch(inches) 9.25 (L1) (T1) 9.25 (L1) (T1) Average Maximum Stretch (inches) 11 (L2) 2 (T2) 10.5 (L2) 1.25 (T2) Engineering Poisson s Ratio Table 3: Minimum and Maximum Stretch Values The structures considered for this study are anisotropic because they do not have identical properties along every direction. Poisson s ratio for isotropic materials that stretch uniformly in all directions ranges between -1 to 0.5. Anisotropic materials can an arbitrary value of any magnitude, as is the case for these two structures (Ting, T. C. T., & Chen, T., 2005).

14 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 14 CONCLUSIONS Conventional auxetics grow along the Y axis when stretched along X axis and vice-versa. The manufacture of auxetics is generally complex. This endeavor demonstrates successful creation of easily manufacturable 2D Z-expandable auxetic structures that can be incorporated in an impact protective application such as kneepad. These materials would grow thicker and retain their expanded configuration along the Z axis (transverse direction) for as long as there is a stretch along the Y axis (longitudinal direction). Various material and design directions were explored during the course of open and structured idea generation phases. Rotating Triangles and Slot Pop-up structures were fabricated from Polyurethane foam. The ASTM D for elongation and ASTM D method for thickness were adapted and applied. The mechanics during growth and recovery were also identified. The results reveal that the structures are anisotropic (do not have identical properties along every direction) and are therefore characterized by unusual Engineering Poisson s ratio values.

15 2D Z-EXPANDABLE AUXETIC TEXTILES FOR IMPACT PROTECTION 15 REFERENCES Alderson, A., A triumph of lateral thought, Chemistry & Industry, pp , 17 May Alderson K, Alderson A,. (2005) Expanding materials and applications: exploiting auxetic textiles, Tech Textiles Int. 777, pp Alderson, K., Alderson, A., Anand, S., Simkins, V., Nazare, S., & Ravirala, N. (2012). Auxetic warp knit textile structures. physica status solidi (b), 249(7), pp Askew, G. N., Formenti, F., & Minetti, A. E. (2012). Limitations imposed by wearing armour on Medieval soldiers' locomotor performance. Proceedings of the Royal Society B: Biological Sciences, 279(1729), Bhullar S.K., A. MawananeHewage T, Alderson A, Alderson K, Martin B. G. Jun. Influence of Negative Poisson's Ratio on Stent Applications. Advances in Materials.Vol. 2, No. 3, 2013, pp doi: /j.am Cherfas, J., Stretching the point, Science, p.247 & 630, Evans, K.E., Tailoring the negative Poisson s ratio, Chem. Ind., Vol.20, pp , Goud, V. S. (2010). Auxetic textiles. Colourage, 57(6), pp Lakes, R.S. (1987a), Foam structures with a negative Poisson's ratio, Science, Vol. 235, pp Lim, T. C., Alderson, A., & Alderson, K. L. (2013). Experimental studies on the impact properties of auxetic materials. physica status solidi (b). Liu, Y., & Hu, H. (2010). A review on auxetic structures and polymeric materials. Scientific Research and Essays, 5(10), Liu, Y., Hu, H., Long, H., & Zhao, L. (2012). Impact compressive behavior of warp-knitted spacer fabrics for protective applications. Textile Research Journal,82(8), Liu, Q. (2006). Literature Review: Materials with Negative Poisson's Ratios and Potential Applications to Aerospace and Defence (No. DSTO-GD-0472). Defence Science and Technology Organization Victoria (Australia) Air Vehicles Division. Maldovan, M., & Thomas, E. L. (2009). Periodic Materials and Interference Lithography: For Photonics, Phononics and Mechanics. John Wiley & Sons, p 234. Muslija, A., & Lantada, A. D. (2014). Deep reactive ion etching of auxetic structures: present capabilities and challenges. Smart Materials and Structures, 23(8), Stott, P.J., R. Mitchell, K. Alderson and A. Alderson, A growing industry, Materials World, vol. 8, pp.12-14, Smith, C.W., Evans, K.E. and Lehaman, F., Strain densification during indentation in auxetic foams, Cell. Poly., Vol.18, pp , Ting, T. C. T., & Chen, T. (2005). Poisson's ratio for anisotropic elastic materials can have no bounds. The quarterly journal of mechanics and applied mathematics, 58(1), Wang, Z., & Hu, H. (2013). 3D auxetic warp knitted spacer fabrics. physica status solidi (b).

International Journal of Scientific & Engineering Research Volume 8, Issue 12, December-2017 ISSN

International Journal of Scientific & Engineering Research Volume 8, Issue 12, December-2017 ISSN 362 Study of the Effects of Random Inclusions in Composite Construction with Isotropic Negative Poisson s Ratio [Kundan Singh Deshwal1, a and Dr. Satyendra Singh2, b] 1 Assistant Professor, Department

More information

Lab Exercise #5: Tension and Bending with Strain Gages

Lab Exercise #5: Tension and Bending with Strain Gages Lab Exercise #5: Tension and Bending with Strain Gages Pre-lab assignment: Yes No Goals: 1. To evaluate tension and bending stress models and Hooke s Law. a. σ = Mc/I and σ = P/A 2. To determine material

More information

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

INFLUENCE KINDS OF MATERIALS ON THE POISSON S RATIO OF WOVEN FABRICS ISSN 1846-6168 (Print), ISSN 1848-5588 (Online) ID: TG-217816142553 Original scientific paper INFLUENCE KINDS OF MATERIALS ON THE POISSON S RATIO OF WOVEN FABRICS Željko PENAVA, Diana ŠIMIĆ PENAVA, Željko

More information

Analysis of the geometrical dependence of auxetic behavior in reentrant structures by finite elements

Analysis of the geometrical dependence of auxetic behavior in reentrant structures by finite elements Acta Mech. Sin. (2016) 32(2):295 300 DOI 10.1007/s10409-015-0534-2 RESEARCH PAPER Analysis of the geometrical dependence of auxetic behavior in reentrant structures by finite elements V. H. Carneiro 1

More information

ORE Open Research Exeter

ORE Open Research Exeter ORE Open Research Exeter TITLE Manufacture and Characterisation of a Novel, Low Modulus, Negative Poisson s Ratio Composite AUTHORS Miller, W.; Hook, P.B.; Smith, Christopher W.; et al. JOURNAL Composites

More information

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

3-dimensional joint torque calculation of compression sportswear using 3D-CG human model 3-dimensional joint torque calculation of compression sportswear using 3D-CG human model Akihiro Matsuda, University of Tsukuba Hirokazu Tanaka, University of Tsukuba Hitoshi Aoki, University of Tsukuba

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

548 Advances of Computational Mechanics in Australia

548 Advances of Computational Mechanics in Australia Applied Mechanics and Materials Online: 2016-07-25 ISSN: 1662-7482, Vol. 846, pp 547-552 doi:10.4028/www.scientific.net/amm.846.547 2016 Trans Tech Publications, Switzerland Geometric bounds for buckling-induced

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

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

Statics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia):

Statics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia): Unit 2 Review Statics Statics Principles The laws of motion describe the interaction of forces acting on a body Newton s First Law of Motion (law of inertia): An object in a state of rest or uniform motion

More information

THE MANUFACTURE AND MECHANICAL PROPERTIES OF A NOVEL NEGATIVE POISSON S RATIO 3-COMPONENT COMPOSITE

THE MANUFACTURE AND MECHANICAL PROPERTIES OF A NOVEL NEGATIVE POISSON S RATIO 3-COMPONENT COMPOSITE 20 th International Conference on Composite Materials THE MANUFACTURE AND MECHANICAL PROPERTIES OF A NOVEL NEGATIVE POISSON S RATIO 3-COMPONENT COMPOSITE G.H. Zhang 1, O. Ghita 2, K.E. Evans 3 1 College

More information

An Analytical Model for Long Tube Hydroforming in a Square Cross-Section Die Considering Anisotropic Effects of the Material

An Analytical Model for Long Tube Hydroforming in a Square Cross-Section Die Considering Anisotropic Effects of the Material Journal of Stress Analysis Vol. 1, No. 2, Autumn Winter 2016-17 An Analytical Model for Long Tube Hydroforming in a Square Cross-Section Die Considering Anisotropic Effects of the Material H. Haghighat,

More information

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

Chapter 6: Mechanical Properties of Metals. Dr. Feras Fraige Chapter 6: Mechanical Properties of Metals Dr. Feras Fraige Stress and Strain Tension Compression Shear Torsion Elastic deformation Plastic Deformation Yield Strength Tensile Strength Ductility Toughness

More information

Module III - Macro-mechanics of Lamina. Lecture 23. Macro-Mechanics of Lamina

Module III - Macro-mechanics of Lamina. Lecture 23. Macro-Mechanics of Lamina Module III - Macro-mechanics of Lamina Lecture 23 Macro-Mechanics of Lamina For better understanding of the macromechanics of lamina, the knowledge of the material properties in essential. Therefore, the

More information

Three-dimensional stiff cellular structures with negative Poisson's ratio

Three-dimensional stiff cellular structures with negative Poisson's ratio ! Three-dimensional stiff cellular structures with negative Poisson's ratio Dong Li a, Jie Ma a, Liang Dong b and Roderic S. Lakes c a College of Sciences, Northeastern University, Shenyang 110819, PR

More information

EXPERIMENTAL EVALUATION OF SHEAR STRENGTH OF WOVEN WEBBINGS

EXPERIMENTAL EVALUATION OF SHEAR STRENGTH OF WOVEN WEBBINGS EXPERIMENTAL EVALUATION OF SHEAR STRENGTH OF WOVEN WEBBINGS Kevin L. Peil +, Ever J. Barbero +, Eduardo M. Sosa* + Department of Mechanical and Aerospace Engineering, West Virginia University (WVU), Morgantown,

More information

Physical Properties Testing Technical Bulletin

Physical Properties Testing Technical Bulletin Technical Bulletin MANUFACTURER Raven Lining Systems 13105 E. 61 st Street, Suite A Broken Arrow, OK 74012 (918) 615-0020 TENSILE TESTING OF PLASTICS ASTM D638, ISO 527 Tensile tests measure the force

More information

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

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture five mechanics www.carttalk.com of materials Mechanics of Materials 1 Mechanics of Materials MECHANICS MATERIALS

More information

Choi, J. B. and Lakes, R. S., "Nonlinear properties of polymer cellular materials with a negative Poisson's. ratio",

Choi, J. B. and Lakes, R. S., Nonlinear properties of polymer cellular materials with a negative Poisson's. ratio, 1 Choi, J. B. and Lakes, R. S., "Nonlinear properties of polymer cellular materials with a negative Poisson's ratio", J. Materials Science, 27, 4678-4684 (1992). Cover issue. ABSTRACT Negative Poisson's

More information

INDUSTRIAL FORMING SIMULATION OF MULTI-LAYERED UD NON-CRIMP-FABRICS. 13. LS-DYNA FORUM, , BAMBERG.

INDUSTRIAL FORMING SIMULATION OF MULTI-LAYERED UD NON-CRIMP-FABRICS. 13. LS-DYNA FORUM, , BAMBERG. Sebastian Kreissl, Thomas Senner, Arnulf Lipp, Josef Meinhardt. INDUSTRIAL FORMING SIMULATION OF MULTI-LAYERED UD NON-CRIMP-FABRICS. 13. LS-DYNA FORUM, 07.10.2014, BAMBERG. OUTLINE. BMW i. Production Process

More information

DEFORMATION PATTERN AND FAILURE CRITERIA OF WOVEN COMPOSITE PREFORM IN GENERAL BIAS EXTENSION

DEFORMATION PATTERN AND FAILURE CRITERIA OF WOVEN COMPOSITE PREFORM IN GENERAL BIAS EXTENSION DEFORMATION PATTERN AND FAILURE CRITERIA OF WOVEN COMPOSITE PREFORM IN GENERAL BIAS EXTENSION B. Zhu 1,2*, T.X. Yu 1, X.M. Tao 2 1 Department of Mechanical Engineering, Hong Kong University of Science

More information

Chapter 7. Highlights:

Chapter 7. Highlights: Chapter 7 Highlights: 1. Understand the basic concepts of engineering stress and strain, yield strength, tensile strength, Young's(elastic) modulus, ductility, toughness, resilience, true stress and true

More information

Planar auxeticity from various inclusions

Planar auxeticity from various inclusions Planar auxeticity from various inclusions Artur A. Poźniak 1 Krzysztof W. Wojciechowski 2 Joseph N. Grima 3 Luke Mizzi 4 1 Institute of Physics, Poznań Universty of Technology, Piotrowo 3, 6-695 Poznań

More information

TENSILE TESTS (ASTM D 638, ISO

TENSILE TESTS (ASTM D 638, ISO MODULE 4 The mechanical properties, among all the properties of plastic materials, are often the most important properties because virtually all service conditions and the majority of end-use applications

More information

MAE 322 Machine Design. Dr. Hodge Jenkins Mercer University

MAE 322 Machine Design. Dr. Hodge Jenkins Mercer University MAE 322 Machine Design Dr. Hodge Jenkins Mercer University What is this Machine Design course really about? What you will learn: How to design machine elements 1) Design so they won t break under varying

More information

INTRODUCTION TO STRAIN

INTRODUCTION TO STRAIN SIMPLE STRAIN INTRODUCTION TO STRAIN In general terms, Strain is a geometric quantity that measures the deformation of a body. There are two types of strain: normal strain: characterizes dimensional changes,

More information

EFFECT OF TEXTILE ARCHITECTURE ON ENERGY ABSORPTION OF WOVEN FABRICS SUBJECT TO BALLISTIC IMPACT

EFFECT OF TEXTILE ARCHITECTURE ON ENERGY ABSORPTION OF WOVEN FABRICS SUBJECT TO BALLISTIC IMPACT THE 9 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS EFFECT OF TEXTILE ARCHITECTURE ON ENERGY ABSORPTION OF WOVEN FABRICS SUBJECT TO BALLISTIC IMPACT C. Yang,*, P. Tran, T. Ngo, P. Mendis, B. Humphries

More information

GG303 Lab 12 11/7/18 1

GG303 Lab 12 11/7/18 1 GG303 Lab 12 11/7/18 1 DEFORMATION AROUND A HOLE This lab has two main objectives. The first is to develop insight into the displacement, stress, and strain fields around a hole in a sheet under an approximately

More information

Module-4. Mechanical Properties of Metals

Module-4. Mechanical Properties of Metals Module-4 Mechanical Properties of Metals Contents ) Elastic deformation and Plastic deformation ) Interpretation of tensile stress-strain curves 3) Yielding under multi-axial stress, Yield criteria, Macroscopic

More information

Plane Strain Test for Metal Sheet Characterization

Plane Strain Test for Metal Sheet Characterization Plane Strain Test for Metal Sheet Characterization Paulo Flores 1, Felix Bonnet 2 and Anne-Marie Habraken 3 1 DIM, University of Concepción, Edmundo Larenas 270, Concepción, Chile 2 ENS - Cachan, Avenue

More information

Tensile stress strain curves for different materials. Shows in figure below

Tensile stress strain curves for different materials. Shows in figure below Tensile stress strain curves for different materials. Shows in figure below Furthermore, the modulus of elasticity of several materials effected by increasing temperature, as is shown in Figure Asst. Lecturer

More information

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

An integrated approach to the design of high performance carbon fibre reinforced risers - from micro to macro - scale An integrated approach to the design of high performance carbon fibre reinforced risers - from micro to macro - scale Angelos Mintzas 1, Steve Hatton 1, Sarinova Simandjuntak 2, Andrew Little 2, Zhongyi

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

2 Experiment of GFRP bolt

2 Experiment of GFRP bolt 16 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS FATIGUE LIFE EVALUATION OF BOLT MADE OF WOVEN FABRIC FRP Takeshi INOUE*, Hiroaki NAKAI**, Tetsusei KURASHIKI**, Masaru ZAKO**, Yuji KOMETANI*** *Graduate

More information

Geology 229 Engineering Geology. Lecture 5. Engineering Properties of Rocks (West, Ch. 6)

Geology 229 Engineering Geology. Lecture 5. Engineering Properties of Rocks (West, Ch. 6) Geology 229 Engineering Geology Lecture 5 Engineering Properties of Rocks (West, Ch. 6) Common mechanic properties: Density; Elastic properties: - elastic modulii Outline of this Lecture 1. Uniaxial rock

More information

STRAIN ANALYSIS OF HDPE BUTT FUSION JOINT IN SIDE BEND TEST

STRAIN ANALYSIS OF HDPE BUTT FUSION JOINT IN SIDE BEND TEST STRAIN ANALYSIS OF HDPE BUTT FUSION JOINT IN SIDE BEND TEST Meng Xiangli (Shawn), McElroy Manufacturing, Inc., Tulsa, OK Abstract The standard practice ASTM F3183-16 (F3183) has been developed for conducting

More information

Chapter 2 Complex Modulus Variation by Manipulation of Mechanical Test Method and Print Direction

Chapter 2 Complex Modulus Variation by Manipulation of Mechanical Test Method and Print Direction Chapter 2 Complex Modulus Variation by Manipulation of Mechanical Test Method and Print Direction Megan L. Liu, Katherine K. Reichl, and Daniel J. Inman Abstract 3D printing technologies have made creating

More information

MECHANICS OF MATERIALS. Analysis of Beams for Bending

MECHANICS OF MATERIALS. Analysis of Beams for Bending MECHANICS OF MATERIALS Analysis of Beams for Bending By NUR FARHAYU ARIFFIN Faculty of Civil Engineering & Earth Resources Chapter Description Expected Outcomes Define the elastic deformation of an axially

More information

DRAPING SIMULATION. Recent achievements and future trends. Dr. Sylvain Bel LGCIE University Lyon 1

DRAPING SIMULATION. Recent achievements and future trends. Dr. Sylvain Bel LGCIE University Lyon 1 DRAPING SIMULATION Recent achievements and future trends 1 Dr. Sylvain Bel LGCIE University Lyon 1 2 DRAPING SIMULATION Why? How? What? DRAPING SIMULATION WHY? Clamps Punch Fabric Die 1 2 Resin 3 4 Fig.

More information

The strain response of silicone dielectric elastomer actuators

The strain response of silicone dielectric elastomer actuators The strain response of silicone dielectric elastomer actuators G. Yang a, G. Yao b, W. Ren a, G. Akhras b, J.P. Szabo c and B.K. Mukherjee a* a Department of Physics, Royal Military College of Canada,

More information

POE Practice Test - Materials

POE Practice Test - Materials Class: Date: POE Practice Test - Materials Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A student weighs 150 lbs and is standing on a beam which spans

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

Advanced Structural Analysis EGF Section Properties and Bending

Advanced Structural Analysis EGF Section Properties and Bending Advanced Structural Analysis EGF316 3. Section Properties and Bending 3.1 Loads in beams When we analyse beams, we need to consider various types of loads acting on them, for example, axial forces, shear

More information

ME 582 Advanced Materials Science. Chapter 2 Macromechanical Analysis of a Lamina (Part 2)

ME 582 Advanced Materials Science. Chapter 2 Macromechanical Analysis of a Lamina (Part 2) ME 582 Advanced Materials Science Chapter 2 Macromechanical Analysis of a Lamina (Part 2) Laboratory for Composite Materials Research Department of Mechanical Engineering University of South Alabama, Mobile,

More information

Theory at a Glance (for IES, GATE, PSU)

Theory at a Glance (for IES, GATE, PSU) 1. Stress and Strain Theory at a Glance (for IES, GATE, PSU) 1.1 Stress () When a material is subjected to an external force, a resisting force is set up within the component. The internal resistance force

More information

EXPERIMENTAL AND FINITE ELEMENT ANALYSIS OF MULTILAYERED HONEYCOMB COMPOSITE MATERIAL SUBJECT TO STATIC LOADING

EXPERIMENTAL AND FINITE ELEMENT ANALYSIS OF MULTILAYERED HONEYCOMB COMPOSITE MATERIAL SUBJECT TO STATIC LOADING U.P.B. Sci. Bull., Series B, Vol. 79, Iss. 3, 2017 ISSN 1454-2331 EXPERIMENTAL AND FINITE ELEMENT ANALYSIS OF MULTILAYERED HONEYCOMB COMPOSITE MATERIAL SUBJECT TO STATIC LOADING Cormos RAUL 1, Horia-Alexandru

More information

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

12/8/2009. Prof. A.K.M.B. Rashid Department of MME BUET, Dhaka Prof. A.K.M.B. Rashid Department of MME BUET, Dhaka Introduction and classes of properties Case studies showing selection of the right material for the job Deformation of material under the action of a

More information

Elasticity: Term Paper. Danielle Harper. University of Central Florida

Elasticity: Term Paper. Danielle Harper. University of Central Florida Elasticity: Term Paper Danielle Harper University of Central Florida I. Abstract This research was conducted in order to experimentally test certain components of the theory of elasticity. The theory was

More information

Chapter 2: Elasticity

Chapter 2: Elasticity OHP 1 Mechanical Properties of Materials Chapter 2: lasticity Prof. Wenjea J. Tseng ( 曾文甲 ) Department of Materials ngineering National Chung Hsing University wenjea@dragon.nchu.edu.tw Reference: W.F.

More information

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

Outline. Tensile-Test Specimen and Machine. Stress-Strain Curve. Review of Mechanical Properties. Mechanical Behaviour Tensile-Test Specimen and Machine Review of Mechanical Properties Outline Tensile test True stress - true strain (flow curve) mechanical properties: - Resilience - Ductility - Toughness - Hardness A standard

More information

Design of Structural Composite with Auxetic Behavior

Design of Structural Composite with Auxetic Behavior Design of Structural Composite with Auxetic Behavior A Major Qualifying Project Submitted to the faculty of Worcester Polytechnic Institute In partial fulfillment of the requirements for the Degree of

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

Calibration and Experimental Validation of LS-DYNA Composite Material Models by Multi Objective Optimization Techniques

Calibration and Experimental Validation of LS-DYNA Composite Material Models by Multi Objective Optimization Techniques 9 th International LS-DYNA Users Conference Optimization Calibration and Experimental Validation of LS-DYNA Composite Material Models by Multi Objective Optimization Techniques Stefano Magistrali*, Marco

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

[5] Stress and Strain

[5] Stress and Strain [5] Stress and Strain Page 1 of 34 [5] Stress and Strain [5.1] Internal Stress of Solids [5.2] Design of Simple Connections (will not be covered in class) [5.3] Deformation and Strain [5.4] Hooke s Law

More information

The in-plane linear elastic constants and out-ofplane bending of 3-coordinated ligament and cylinder-ligament honeycombs.

The in-plane linear elastic constants and out-ofplane bending of 3-coordinated ligament and cylinder-ligament honeycombs. University of Bolton UBIR: University of Bolton Institutional Repository IMRI: Journal Articles (Peer-Reviewed) Institute for Materials Research and Innovation 200 The in-plane linear elastic constants

More information

INVESTIGATION OF THE PROCESSING PARAMETERS OF A 3D WOVEN REINFORCEMENT

INVESTIGATION OF THE PROCESSING PARAMETERS OF A 3D WOVEN REINFORCEMENT INVESTIGATION OF THE PROCESSING PARAMETERS OF A 3D WOVEN REINFORCEMENT Andreas Endruweit, Dhiren K. Modi and Andrew C. Long School of Mechanical, Materials and Manufacturing Engineering, University of

More information

Elastic Properties of Solids (One or two weights)

Elastic Properties of Solids (One or two weights) Elastic properties of solids Page 1 of 8 Elastic Properties of Solids (One or two weights) This is a rare experiment where you will get points for breaking a sample! The recommended textbooks and other

More information

Comparative Study of Hyper Elastic Material Models

Comparative Study of Hyper Elastic Material Models International Journal of Engineering and Manufacturing Science. ISSN 2249-3115 Volume 7, Number 2 (2017), pp. 149-170 Research India Publications http://www.ripublication.com Comparative Study of Hyper

More information

Exercise 2: Bending Beam Load Cell

Exercise 2: Bending Beam Load Cell Transducer Fundamentals The Strain Gauge Exercise 2: Bending Beam Load Cell EXERCISE OBJECTIVE When you have completed this exercise, you will be able to explain and demonstrate the operation of a board,

More information

Members Subjected to Torsional Loads

Members Subjected to Torsional Loads Members Subjected to Torsional Loads Torsion of circular shafts Definition of Torsion: Consider a shaft rigidly clamped at one end and twisted at the other end by a torque T = F.d applied in a plane perpendicular

More information

Bending Load & Calibration Module

Bending Load & Calibration Module Bending Load & Calibration Module Objectives After completing this module, students shall be able to: 1) Conduct laboratory work to validate beam bending stress equations. 2) Develop an understanding of

More information

Materials and Structures. Indian Institute of Technology Kanpur

Materials and Structures. Indian Institute of Technology Kanpur Introduction to Composite Materials and Structures Nachiketa Tiwari Indian Institute of Technology Kanpur Lecture 16 Behavior of Unidirectional Composites Lecture Overview Mt Material ilaxes in unidirectional

More information

COURSE TITLE : THEORY OF STRUCTURES -I COURSE CODE : 3013 COURSE CATEGORY : B PERIODS/WEEK : 6 PERIODS/SEMESTER: 90 CREDITS : 6

COURSE TITLE : THEORY OF STRUCTURES -I COURSE CODE : 3013 COURSE CATEGORY : B PERIODS/WEEK : 6 PERIODS/SEMESTER: 90 CREDITS : 6 COURSE TITLE : THEORY OF STRUCTURES -I COURSE CODE : 0 COURSE CATEGORY : B PERIODS/WEEK : 6 PERIODS/SEMESTER: 90 CREDITS : 6 TIME SCHEDULE Module Topics Period Moment of forces Support reactions Centre

More information

Strain Measurement Techniques for Composite Coupon Testing

Strain Measurement Techniques for Composite Coupon Testing Strain Measurement Techniques for Composite Coupon Testing Introduction Characterization of the properties of anisotropic and inhomogeneous composite materials for use in demanding structural applications

More information

Dynamic Tests for Energy Absorption by Selected Auxetic Fabrics

Dynamic Tests for Energy Absorption by Selected Auxetic Fabrics Dynamic Tests for Energy Absorption by Selected Auxetic Fabrics Piotr Szurgott, PhD, Marian Klasztorny, PhD, Tadeusz Niezgoda, PhD Danuta Miedzinska, PhD, Roman Gieleta, PhD Military University of Technology,

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

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

4.MECHANICAL PROPERTIES OF MATERIALS

4.MECHANICAL PROPERTIES OF MATERIALS 4.MECHANICAL PROPERTIES OF MATERIALS The diagram representing the relation between stress and strain in a given material is an important characteristic of the material. To obtain the stress-strain diagram

More information

Evaluation of in-plane orthotropic elastic constants of paper and paperboard

Evaluation of in-plane orthotropic elastic constants of paper and paperboard Evaluation of in-plane orthotropic elastic constants of paper and paperboard T. Yokoyama and K. Nakai Department of Mechanical Engineering, Okayama University of Science - Ridai-cho, Okayama 7-5, Japan

More information

Determination of Poisson s Ratio of Rock Material by Changing Axial Stress and Unloading Lateral Stress Test

Determination of Poisson s Ratio of Rock Material by Changing Axial Stress and Unloading Lateral Stress Test Rock Mech Rock Eng DOI 10.1007/s00603-014-0586-9 TECHNICAL NOTE Determination of Poisson s Ratio of Rock Material by Changing Axial Stress and Unloading Lateral Stress Test Xiangtao Xu Runqiu Huang Hua

More information

FIBRE WAVINESS INDUCED BENDING IN COMPRESSION TESTS OF UNIDERECTIONAL NCF COMPOSITES

FIBRE WAVINESS INDUCED BENDING IN COMPRESSION TESTS OF UNIDERECTIONAL NCF COMPOSITES FIBRE WAVINESS INDUCED BENDING IN COMPRESSION TESTS OF UNIDERECTIONAL NCF COMPOSITES Dennis Wilhelmsson 1, Leif E. Asp 1, Renaud Gutkin 2, Fredrik Edgren 3 1 Chalmers University of Technology, Dept. Industrial

More information

Mechanical properties 1 Elastic behaviour of materials

Mechanical properties 1 Elastic behaviour of materials MME131: Lecture 13 Mechanical properties 1 Elastic behaviour of materials A. K. M. B. Rashid Professor, Department of MME BUET, Dhaka Today s Topics Deformation of material under the action of a mechanical

More information

Stress-strain response and fracture behaviour of plain weave ceramic matrix composites under uni-axial tension, compression or shear

Stress-strain response and fracture behaviour of plain weave ceramic matrix composites under uni-axial tension, compression or shear Xi an 2-25 th August 217 Stress-strain response and fracture behaviour of plain weave ceramic matrix composites under uni-axial tension compression or shear Heyin Qi 1 Mingming Chen 2 Yonghong Duan 3 Daxu

More information

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

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

More information

Computational Modelling of Vibrations Transmission Loss of Auxetic Lattice Structure

Computational Modelling of Vibrations Transmission Loss of Auxetic Lattice Structure Vibrations in Physical Systems Vol. 27 (2016) Abstract Computational Modelling of Vibrations Transmission Loss of Auxetic Lattice Structure Eligiusz IDCZAK Institute of Applied Mechanics, Poznan University

More information

9 MECHANICAL PROPERTIES OF SOLIDS

9 MECHANICAL PROPERTIES OF SOLIDS 9 MECHANICAL PROPERTIES OF SOLIDS Deforming force Deforming force is the force which changes the shape or size of a body. Restoring force Restoring force is the internal force developed inside the body

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

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

Qualitative analysis of aramide polymers by FT-IR spectroscopy

Qualitative analysis of aramide polymers by FT-IR spectroscopy International Journal of Engineering Science Invention ISSN (Online): 2319 6734, ISSN (Print): 2319 6726 Volume 3 Issue 2 ǁ February 2014 ǁ PP.01-07 Qualitative analysis of aramide polymers by FT-IR spectroscopy

More information

Testing and Analysis

Testing and Analysis Testing and Analysis Testing Elastomers for Hyperelastic Material Models in Finite Element Analysis 2.6 2.4 2.2 2.0 1.8 1.6 1.4 Biaxial Extension Simple Tension Figure 1, A Typical Final Data Set for Input

More information

NUMERICAL AND EXPERIMENTAL STUDY OF FAILURE IN STEEL BEAMS UNDER IMPACT CONDITIONS

NUMERICAL AND EXPERIMENTAL STUDY OF FAILURE IN STEEL BEAMS UNDER IMPACT CONDITIONS Blucher Mechanical Engineering Proceedings May 2014, vol. 1, num. 1 www.proceedings.blucher.com.br/evento/10wccm NUMERICAL AND EXPERIMENTAL STUDY OF FAILURE IN STEEL BEAMS UNDER IMPACT CONDITIONS E. D.

More information

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

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS EDEXCEL NATIONAL CERTIICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQ LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS 1. Be able to determine the effects of loading in static engineering

More information

ME 207 Material Science I

ME 207 Material Science I ME 207 Material Science I Chapter 3 Properties in Tension and Compression Dr. İbrahim H. Yılmaz http://web.adanabtu.edu.tr/iyilmaz Automotive Engineering Adana Science and Technology University Introduction

More information

International Journal of Scientific & Engineering Research, Volume 5, Issue 1, January ISSN

International Journal of Scientific & Engineering Research, Volume 5, Issue 1, January ISSN International Journal of Scientific & Engineering Research, Volume 5, Issue 1, January-214 29 An Experimental Analysis of Stress Relaxation in Nonwoven Fabrics Sajid Ahmed Qureshi ABSTRACT - The current

More information

Stress-Strain Behavior

Stress-Strain Behavior Stress-Strain Behavior 6.3 A specimen of aluminum having a rectangular cross section 10 mm 1.7 mm (0.4 in. 0.5 in.) is pulled in tension with 35,500 N (8000 lb f ) force, producing only elastic deformation.

More information

Simulation of Geometrical Cross-Section for Practical Purposes

Simulation of Geometrical Cross-Section for Practical Purposes Simulation of Geometrical Cross-Section for Practical Purposes Bhasker R.S. 1, Prasad R. K. 2, Kumar V. 3, Prasad P. 4 123 Department of Mechanical Engineering, R.D. Engineering College, Ghaziabad, UP,

More information

Analysis Of Naca 2412 For Automobile Rear Spoiler Using Composite Material *

Analysis Of Naca 2412 For Automobile Rear Spoiler Using Composite Material * Analysis Of Naca 2412 For Automobile Rear Spoiler Using Composite Material * Kamprasad Chodagudi 1, T.b.s Rao 2 -----------------------------------------------------------------------------------------------------------------------------

More information

The Relationship between the Applied Torque and Stresses in Post-Tension Structures

The Relationship between the Applied Torque and Stresses in Post-Tension Structures ECNDT 6 - Poster 218 The Relationship between the Applied Torque and Stresses in Post-Tension Structures Fui Kiew LIEW, Sinin HAMDAN * and Mohd. Shahril OSMAN, Faculty of Engineering, Universiti Malaysia

More information

Modeling the application of fluid filled foam in motorcycle helmets

Modeling the application of fluid filled foam in motorcycle helmets Modeling the application of fluid filled foam in motorcycle helmets B.G. Vossen MT 10.10 Eindhoven University of Technology Department of Mechanical Engineering Mechanics of Materials Massachusetts Institute

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

MECHANICAL PROPERTIES OF SOLIDS

MECHANICAL PROPERTIES OF SOLIDS Chapter Nine MECHANICAL PROPERTIES OF SOLIDS MCQ I 9.1 Modulus of rigidity of ideal liquids is (a) infinity. (b) zero. (c) unity. (d) some finite small non-zero constant value. 9. The maximum load a wire

More information

Optimum Height of Plate Stiffener under Pressure Effect

Optimum Height of Plate Stiffener under Pressure Effect The st Regional Conference of Eng. Sci. NUCEJ Spatial ISSUE vol., No.3, 8 pp 459-468 Optimum Height of Plate Stiffener under Pressure Effect Mazin Victor Yousif M.Sc Production Engineering University of

More information

MECHANICAL FAILURE OF A COMPOSITE HELICOPTER STRUCTURE UNDER STATIC LOADING

MECHANICAL FAILURE OF A COMPOSITE HELICOPTER STRUCTURE UNDER STATIC LOADING MECHANICAL FAILURE OF A COMPOSITE HELICOPTER STRUCTURE UNDER STATIC LOADING Steven Roy, Larry Lessard Dept. of Mechanical Engineering, McGill University, Montreal, Québec, Canada ABSTRACT The design and

More information

An overview of Carbon Fiber modeling in LS-DYNA. John Zhao October 23 th 2017

An overview of Carbon Fiber modeling in LS-DYNA. John Zhao October 23 th 2017 An overview of Carbon Fiber modeling in LS-DYNA John Zhao zhao@lstc.com October 23 th 2017 Outline Manufacturing of Carbon Fiber Compression molding *MAT_277 & 278 *MAT_293 *MAT_249 Resin transform molding

More information

3.22 Mechanical Properties of Materials Spring 2008

3.22 Mechanical Properties of Materials Spring 2008 MIT OpenCourseWare http://ocw.mit.edu 3.22 Mechanical Properties of Materials Spring 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. Quiz #1 Example

More information

Lecture 8 Viscoelasticity and Deformation

Lecture 8 Viscoelasticity and Deformation Read: pg 130 168 (rest of Chpt. 4) 1 Poisson s Ratio, µ (pg. 115) Ratio of the strain in the direction perpendicular to the applied force to the strain in the direction of the applied force. For uniaxial

More information

NUMERICAL SIMULATION OF DAMAGE IN THERMOPLASTIC COMPOSITE MATERIALS

NUMERICAL SIMULATION OF DAMAGE IN THERMOPLASTIC COMPOSITE MATERIALS 5 th European LS-DYNA Users Conference Composites NUMERICAL SIMULATION OF DAMAGE IN THERMOPLASTIC COMPOSITE MATERIALS Kevin Brown 1, Richard Brooks, Nicholas Warrior School of Mechanical, Materials and

More information

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

High Tech High Top Hat Technicians. An Introduction to Solid Mechanics. Is that supposed to bend there? High Tech High Top Hat Technicians An Introduction to Solid Mechanics Or Is that supposed to bend there? Why don't we fall through the floor? The power of any Spring is in the same proportion with the

More information