Virtual Medical Device Optimization using ABAQUS

Size: px
Start display at page:

Download "Virtual Medical Device Optimization using ABAQUS"

Transcription

1 Virtual Medical Device Optimization using ABAQUS Torben Strøm Hansen Novo Nordisk A/S Protein Delivery Systems Device Research & Technology, Brennum Park DK-3400 Hilleroed, Denmark In the development of medical devices, safety, robustness and reliability are crucial and have major priority. It is essential to be able to predict these device characteristics at the early development stages. Prediction and verification of the device functionality relied on iterative manufacturing and testing of hardware prototypes through many years. It still remains a challenge to provide prototypes with similar mechanical properties as those of the final components. Constitutive material behavior and frictional properties of the produced parts are usually different from those of the prototypes due to the nature of the manufacturing processes: Injection molding in running production versus the machining processes and simplified molding of the prototypes. This paper exemplifies how a virtual ABAQUS prototype including both non-linear instantaneous and viscoelastic polymer material response provides data that saved numerous prototype testing iterations. It will be shown how this model has been used in the process of mechanism optimization. Keywords: Design Optimization, Optimization, Viscoelasticity, Polymer, Hyperelasticity, Dynamics, Creep 1. Introduction 1.1 Subject of the analyses The FlexPen is a multiple use pre-filled dial-a-dose insulin pen device. The pen is purely mechanically operated and designed for primarily domestic use by diabetics worldwide. The user interface aims at simplicity and ease of use. The user simply attaches a sterile needle to the device, sets the desired insulin dose followed by injection typically in the abdomen. During the injection, the user depresses the push button as shown in Figure 1. It is of the outmost importance that the force required for this operation is limited as much as possible. Thus all mechanical subsystems interacting during the injection are optimized one by one. This paper deals with the Ratchet Nut subsystem which by rotation of the Ratchet in the fixed Nut provides indexing of the dose and secures that no reverse flow through the needle occur ABAQUS Users Conference 1

2 1.2 The analysis objective During the medication injection, the Ratchet rotates in the Nut forcing oscillation of the Ratchet arms in the teethed Nut and thus bend like a tip loaded cantilever beam. This sequence creates audible clicks, enabling the user to hear the number of unit doses injected. To secure correct operation of the Ratchet, both arms are slightly pre-stressed in the teethed Nut so the tip of the arms will engage with the bottom of the tooth for each operation cycle. The cyclic forced deformation of the Ratchet arms (10 40 Hz) causes a time dependent stress response and a rippling reaction moment. Since this interaction is one of the major contributors to the overall dosing force of the FlexPen, it should be as limited and as predictable as possible. The existing design already has an optimized reaction moment at a given rotational velocity. The objective is to optimize this Ratchet design further to make its mechanical operation less influenced by pen-injection velocity and storage time by limiting the viscous part of the stress response which will narrow the damping and stress relaxation. 2. Material characterization 2.1 Test approach The Ratchet is manufactured by polymer injection molding in multi-cavity molds for high volume production. The selected material is an acetal copolymer grade (POM). As for many other technical polymers, the selected POM resin has both a non-linear steady state and a strain rate dependent stress response at large strains and cyclic loading. The inevitable hysteretic energy dissipation is most unwanted in the Ratchet design, since it has a damping effect on the action of the Ratchet arms in the Nut causing rotational velocity dependence. Figure 2 shows the hysteretic stress response of the POM grade when subjected to different triangular loading unloading schemes. The hysteresis is caused by viscous dissipation which also occurs in the Ratchet arms during the cyclic displacement. Extensive material testing was consequently required to characterize the steady state and time dependent response. The course of the data generation and implementation was: Selection of applicable constitutive models for numerical implementation Define material test type, setup and test series Numerical implementation 1-element and multi element model vs. test data verification A test setup using ISO 527 tensile bars mounted in a high speed Instron elastomer tensile test bench (Figure 3) was used. The bench was equipped with proper load cells, extensometers and a climatic chamber. The uni-axial approach is only valid if the Poisson s ratio remains constant throughout the strain range specified in both compression and tension, which required a number of runs using dual extensometers for the sampling of the longitudinal and transversal straining. After verification of a constant Poisson s ratio within the specified temperature, humidity and strain ABAQUS Users Conference

3 range, the test series were defined. All the test series were performed at both room temperature and at elevated environmental conditions at each extreme of the product specification. For the non-linear steady state response in Figure 4, a low strain rate of 0.5 %/s was selected. For the relaxation measurement a strain rate of 150 %/s was used to quickly ramp the strain to a given level for the monitoring of the time dependent response of Figure Numerical implementation For the steady state response a hyperelastic constitutive model was used. The uni-axial test data of Figure 4 were implemented by using *Uniaxial Test Data. By pre-processing the input file, those test data could be compared with data from several of the material models available in ABAQUS. Data from two optional models are plotted together with the test data in Figure 4. Best fit was obtained using a second order polynomial formulation with a predefined Poisson s ratio: *Hyperelastic, n=2, test data input, poisson=0.4. The time dependent stress response was characterized by implementing the viscoelastic material model: *Viscoelastic, time=prony In ABAQUS, the Prony series represents the relaxation behavior of the bulk modulus and the shear modulus. Assuming similar relaxation of the two deformation modes, the terms of the Prony series were given by the values found from the uni-axial tensile test data by curve fitting. The Prony series representation can thus be written in terms of the time dependent modulus E(t) as: N E( t) = E(0) 1 e n= 1 P n (1 e t / τ n ) The test sample is subjected to a step strain similar to the peak strain of the Ratchet. The relative modulus e = E(t)/E(0) is plotted for the sampled relaxation data, and compared to the 1-term and the favoured 2-terms Prony parameters found from curve fitting in Figure 5. The 2-term series had a satisfactory fit. These parameters can also be provided by pre-processing test data in ABAQUS. Repeating the relaxation test for a number of strain levels, showed that the relaxation for this polymer is much strain level dependent: For high strain levels the relaxation became more dominant. Thus the Prony parameters had to be chosen from a given strain level relaxation test since the ABAQUS model is linear Viscoelastic. The peak strain relaxation results chosen for this analysis will cause overestimation of the mean stress relaxation of the time span of the analysis. Component reference testing has shown that the selected approach is applicable for relative comparison of different part versions. 3. Geometry optimization It is now obvious that by reducing the peak strain level, both the unwanted viscous dissipation (damping of the Ratchet arms) and the stress relaxation (pen storage influence to the overall behavior of the Ratchet) can be reduced. The peak strain level of the flex arms of the Ratchet can be reduced by changing the geometry towards a prolonged shape without disturbing the reaction force vs. displacement characteristic of the Ratchet arms ABAQUS Users Conference 3

4 3.1 Room of improvement demarcation by problem simplification The Ratchet arm was initially approximated by a simple cantilever beam as shown in Figure 6. The intention was to keep the compliance of the arm constant while reducing the peak strain causing the viscous dissipation. The relation between the beam compliance and the length and height of the beam can be derived from the Bernoulli equation for the vertical tip displacement u y and the resulting reaction R f : From u y 3 R f l = the compliance proportionality can be derived as: 3EI u R y f l h 3 3 The relation between the peak strain ε p of the beam and the length l, width w and height h of the beam can also be derived from the cantilever equation: From 6R l ε f p = the peak strain proportionality is: l 2 ε 2 wh E p h Consequently strain reduction can be gained by increasing the length and height of the Ratchet arms by the same rate for fixed compliance values. A simple parametric optimization model was defined in the CAD integrated FE-code. A preliminary analysis indicated a significant peak strain reduction of 40 % by extending the length and width as shown in figure 7. The resulting geometry was transferred to ABAQUS for virtual validation of the stress relaxation and dynamic behaviour of the optimized design. 4. ABAQUS models 4.1 Quasi-static model for Ratchet arm relaxation analysis The objective of this analysis was to evaluate the stress relaxation influence to the reaction force of the Ratchet arms when subjected to the assembly pre-stressing. A quasi-static model using the ABAQUS/Standard *Visco procedure allows time-dependent material response by implementation of explicit time integration. Both the *Viscoelastic and *Hyperelastic material models were implemented for this analysis. By applying a forced displacement similar to the assembly pre-stress to a rigid surface contacting the tip of one arm, the dissipated energy and reaction force can be monitored as a function of storage time and compared to the original design. Figure 7 shows the model and that the major part of the energy dissipation takes place in the early stage of the quasi instantaneous displacement. The reduction of the peak strain level has caused a reduction of 32% of the energy dissipation of Figure 8. The experimental verification setup is shown in Figure 9, where the forced displacement is applied by a probe attached to a tensile test bench. The effect of the relaxation to the pre-stress force can be monitored by sampling the load cell output. 4.2 Dynamic model for reaction moment of the improved design The purpose of this analysis was to analyze the dynamic behavior improvement of the optimized Ratchet. When the Ratchet rotates in the Nut and the arms are displaced in a cyclic manner ABAQUS Users Conference

5 causing interaction between inertia and elastic forces. Even though the strain energy share of the total energy is dominant at all times during the cycle, the kinetic energy can not be disregarded. ABAQUS/Explicit was chosen for the dynamic model depicted in Figure 10. The Ratchet was modeled as 3D solid and C3D10M tet meshed. The teethed Nut was modeled as analytical rigid. The discretization was refined until a strain gradient comparable with that of the quasi-static analysis was obtained. To impose the assembly pre-stress, artificial forces were imposed on each of the Ratchet arms in the first step and then released in the second step after turning the Ratchet- Nut contact surfaces on. The resulting impact would usually create substantial noise, but the viscoelasticity imposed an excellent damping which also helped to keep the reaction moment output signal stable at all times. From a prescribed rotational velocity, the resulting reaction moment was plotted (Figure 10). The reaction moment for both designs was almost identical, but the viscous dissipation plotted in Figure 11 differed between the two designs. The optimized design dissipated less energy than the original causing a reduced level of damping. The experimental test setup for the dynamic response for data verification is shown in Figure Implementation in the complete device model After assessing the optimization impact to the rotational reaction moment of the Ratchet-Nut subsystem on component level, the Ratchet was implemented in an ABAQUS/Explicit full system model of the FlexPen. This model contains all interacting mechanical parts from the dosing button to the Ratchet and is used to quantify the contribution of each mechanical sub system to the overall dosing force applied by the user. By prescribing a forced displacement to the dosing button, the resulting translatory movement is transferred to a rotational movement of the Ratchet through a thread on a scale drum as shown in Figure 13. One second of the dosing operation was analyzed using limited mass scaling which only influences elements of stagnant parts. A mixture of analytical and discrete rigids together with elastic solids is used to save computational time. The reaction force caused by the forced displacement was chosen as the guiding qualification parameter of the system. Implementing the optimized Ratchet in this model verified that the dosing force plotted in Figure 14 had become less velocity dependent than with the original design. 5. Future model improvements and next step Injection molded polymers are much influenced by the process parameters (injection pressure, packing pressure and thermal effects). As a consequence residual stresses and orthotropic material properties are inevitable in an injection molding process. Injection molding process analysis data transferal to ABAQUS would thus be an obvious next step. Pilot analyses have been defined for integration of Moldflow data in ABAQUS. Many polymers such as the POM grade used for the Ratchet exhibit non-linear strain dependent viscoelasticity. Implementation of non-linear viscoelasticity in ABAQUS will significantly improve the relaxation prediction of large strain analyses such as this. Machining and testing of the existing Ratchet has initially verified the impact of the design change. New injection molds based on the ABAQUS optimization analyses results are now being manufactured for production of samples for final validation ABAQUS Users Conference 5

6 6. Conclusion Limiting the peak strain successfully decreased both the stress relaxation and viscous damping. Accordingly the pre-stress stability has been improved and the device injection velocity dependence substantially reduced. Both the quasi-static and dynamic analyses have provided core data for assessing the optimization impact. The hyperelastic and viscoelastic material models have been viable for characterizing the polymer material response in the relative assessment of dynamic Ratchet response and stress relaxation improvement from original to enhanced design. Using ABAQUS in the optimization procedure has directly led to a much improved design which could not have been achieved from traditional trial and error methods and has also saved numerous prototype manufacturing and test cycles. Using the knowledge gained in this study will enable Novo Nordisk to simulate large strain dynamic polymer component behavior much more accurately. 7. References Brüeller, O.S. and Schmidt, H.H., On the Linear Viscoelastic Limit of Polymers Exemplified on PMMA Polymer Engineering and Science, September 1979 vol. 19. Kolberg, Raymond, Mechanical Response of Beams of a Nonlinear Viscoelastic Material, Polymer Engineering and Science, January ABAQUS 6 Version 6.4 documentation ABAQUS Users Conference

7 8. Acknowledgements I would like to thank Lars P. Mikkelsen of Risø National Laboratory, Materials Research dept. for his contribution in both the test planning phase and on the test execution. The FlexPen team of Novo Nordisk has provided excellent reference test data on the different sub-systems of the pen. Furthermore Jan Granlund of ABAQUS Scandinavia has advised on model refinement and material model selections which is most appreciated ABAQUS Users Conference 7

8 9. Figures Push Button operated by the user FlexPen The Nut The Ratchet Figure 1 The FlexPen and the selected sub system: The Ratchet Nut ABAQUS Users Conference

9 Ramp loaded samples At 0.5 kn/s Figure 2 The hysteresis of ramp loaded and unloaded polymer samples (POM) at different strain levels T-extensometer ISO 527 tensile bar Figure 3 Tensile testing using a high speed elastomer tensile test bench 2005 ABAQUS Users Conference 9

10 Figure 4 ABAQUS evaluation of steady state tensile test data (Polynomial and Ogden models) for the Hyperelastic model Figure 5 Fitting of Prony series parameters of the Viscoelastic model to relaxation test data where the modulus e = E(t)/E(0) is plotted vs. time for ABAQUS Users Conference

11 y x l u y Figure 6 Equivalent Cantilever Beam approach Figure 7 The static peak strain level of the original and optimized design 2005 ABAQUS Users Conference 11

12 Original design Optimized design Figure 8 ABAQUS Model for stress relaxation analysis Probe attached to a tensile test bench Figure 9 Experimental verification of the relaxation effect to the pre-stress force of the Ratchet arm ABAQUS Users Conference

13 Figure 10 The Ratchet subjected to a prescribed rotation velocity of 8 radians per second and the resulting reaction moment Figure 11 Viscous dissipation of the Ratchet during rotation of the original X and the optimized O design at 8 radians per second 2005 ABAQUS Users Conference 13

14 Figure 12 Experimental verification of the dynamic response of the Ratchet. Forced rotation is applied by the bench and the reaction moment is sampled from a load cell Forced displacement imposed on an analytical rigid top surface Small diameter parts modeled as discrete rigid Housing modeled as elastic solid Figure 13 Full system model of the FlexPen for the analysis of the required dosing force ABAQUS Users Conference

15 Figure 14 Full system reaction force response 2005 ABAQUS Users Conference 15

Modelling Rubber Bushings Using the Parallel Rheological Framework

Modelling Rubber Bushings Using the Parallel Rheological Framework Modelling Rubber Bushings Using the Parallel Rheological Framework Javier Rodríguez 1, Francisco Riera 1, and Jon Plaza 2 1 Principia, Spain; 2 Cikatek, Spain Abstract: Bushings are anti vibration components

More information

A Review On Methodology Of Material Characterization And Finite Element Modelling Of Rubber-Like Materials

A Review On Methodology Of Material Characterization And Finite Element Modelling Of Rubber-Like Materials IOSR Journal of Engineering (IOSRJEN) ISSN (e): 50-301, ISSN (p): 78-8719 PP 06-10 www.iosrjen.org A Review On Methodology Of Material Characterization And Finite Element Modelling Of Rubber-Like Materials

More information

Dynamic Finite Element Modeling of Elastomers

Dynamic Finite Element Modeling of Elastomers Dynamic Finite Element Modeling of Elastomers Jörgen S. Bergström, Ph.D. Veryst Engineering, LLC, 47A Kearney Rd, Needham, MA 02494 Abstract: In many applications, elastomers are used as a load-carrying

More information

Predeformation and frequency-dependence : Experiment and FE analysis

Predeformation and frequency-dependence : Experiment and FE analysis Predeformation and frequency-dependence : Experiment and FE analysis Nidhal Jridi 1,2,*, Michelle Salvia 2, Adel Hamdi 1, Olivier Bareille 2, Makrem Arfaoui 1, Mohammed Ichchou 2, Jalel Ben Abdallah 1

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

Non-Linear Viscoelastic Modeling of Epoxy Based Molding Compound for Large Deformations Encountered in Power Modules

Non-Linear Viscoelastic Modeling of Epoxy Based Molding Compound for Large Deformations Encountered in Power Modules 2017 IEEE 67th Electronic Components and Technology Conference Non-Linear Viscoelastic Modeling of Epoxy Based Molding Compound for Large Deformations Encountered in Power Modules Przemyslaw Gromala, Alexandru

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

MSC Elastomers Seminar Some Things About Elastomers

MSC Elastomers Seminar Some Things About Elastomers MSC Elastomers Seminar Some Things About Elastomers Kurt Miller, Axel Products, Inc. www.axelproducts.com Visit us at: axelproducts.com 2 Your Presenter Kurt Miller Founded Axel Products 1994 Instron Corporation,

More information

EXPERIMENTAL IDENTIFICATION OF HYPERELASTIC MATERIAL PARAMETERS FOR CALCULATIONS BY THE FINITE ELEMENT METHOD

EXPERIMENTAL IDENTIFICATION OF HYPERELASTIC MATERIAL PARAMETERS FOR CALCULATIONS BY THE FINITE ELEMENT METHOD Journal of KONES Powertrain and Transport, Vol. 7, No. EXPERIMENTAL IDENTIFICATION OF HYPERELASTIC MATERIAL PARAMETERS FOR CALCULATIONS BY THE FINITE ELEMENT METHOD Robert Czabanowski Wroclaw University

More information

2012 MECHANICS OF SOLIDS

2012 MECHANICS OF SOLIDS R10 SET - 1 II B.Tech II Semester, Regular Examinations, April 2012 MECHANICS OF SOLIDS (Com. to ME, AME, MM) Time: 3 hours Max. Marks: 75 Answer any FIVE Questions All Questions carry Equal Marks ~~~~~~~~~~~~~~~~~~~~~~

More information

Nonlinear Analysis Of An EPDM Hydraulic Accumulator Bladder. Richard Kennison, Race-Tec

Nonlinear Analysis Of An EPDM Hydraulic Accumulator Bladder. Richard Kennison, Race-Tec Nonlinear Analysis Of An EPDM Hydraulic Accumulator Bladder Richard Kennison, Race-Tec Agenda Race-Tec Overview Accumulator Experimental Testing Material Testing Numerical Analysis: 1. Linear Buckling

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

1 Static Plastic Behaviour of Beams

1 Static Plastic Behaviour of Beams 1 Static Plastic Behaviour of Beams 1.1 Introduction Many ductile materials which are used in engineering practice have a considerable reserve capacity beyond the initial yield condition. The uniaxial

More information

Testing Elastomers and Plastics for Marc Material Models

Testing Elastomers and Plastics for Marc Material Models Testing Elastomers and Plastics for Marc Material Models Presented by: Kurt Miller Axel Products, Inc. axelproducts.com We Measure Structural Properties Stress Strain Time-Temperature Test Combinations

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

Initial Stress Calculations

Initial Stress Calculations Initial Stress Calculations The following are the initial hand stress calculations conducted during the early stages of the design process. Therefore, some of the material properties as well as dimensions

More information

Finite Element Modelling with Plastic Hinges

Finite Element Modelling with Plastic Hinges 01/02/2016 Marco Donà Finite Element Modelling with Plastic Hinges 1 Plastic hinge approach A plastic hinge represents a concentrated post-yield behaviour in one or more degrees of freedom. Hinges only

More information

Predicting Fatigue Life with ANSYS Workbench

Predicting Fatigue Life with ANSYS Workbench Predicting Fatigue Life with ANSYS Workbench How To Design Products That Meet Their Intended Design Life Requirements Raymond L. Browell, P. E. Product Manager New Technologies ANSYS, Inc. Al Hancq Development

More information

BioMechanics and BioMaterials Lab (BME 541) Experiment #5 Mechanical Prosperities of Biomaterials Tensile Test

BioMechanics and BioMaterials Lab (BME 541) Experiment #5 Mechanical Prosperities of Biomaterials Tensile Test BioMechanics and BioMaterials Lab (BME 541) Experiment #5 Mechanical Prosperities of Biomaterials Tensile Test Objectives 1. To be familiar with the material testing machine(810le4) and provide a practical

More information

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

Non-linear and time-dependent material models in Mentat & MARC. Tutorial with Background and Exercises Non-linear and time-dependent material models in Mentat & MARC Tutorial with Background and Exercises Eindhoven University of Technology Department of Mechanical Engineering Piet Schreurs July 7, 2009

More information

Why Dynamic Analysis Is Needed?

Why Dynamic Analysis Is Needed? Impact of Wide-Base Tires on Pavement and Trucking Operation: Advanced Analysis Imad L. Al-Qadi Founder Professor of Engineering Illinois Center for Transportation Why Dynamic Analysis Is Needed? Quasi-static

More information

Modelling the nonlinear shear stress-strain response of glass fibrereinforced composites. Part II: Model development and finite element simulations

Modelling the nonlinear shear stress-strain response of glass fibrereinforced composites. Part II: Model development and finite element simulations Modelling the nonlinear shear stress-strain response of glass fibrereinforced composites. Part II: Model development and finite element simulations W. Van Paepegem *, I. De Baere and J. Degrieck Ghent

More information

Design issues of thermal induced effects and temperature dependent material properties in Abaqus

Design issues of thermal induced effects and temperature dependent material properties in Abaqus Materials Characterisation VII 343 Design issues of thermal induced effects and temperature dependent material properties in Abaqus I. Both 1, F. Wald 1 & R. Zaharia 2 1 Department of Steel and Timber

More information

EE C245 ME C218 Introduction to MEMS Design

EE C245 ME C218 Introduction to MEMS Design EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 16: Energy

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

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

Nonlinear Finite Element Modeling of Nano- Indentation Group Members: Shuaifang Zhang, Kangning Su. ME 563: Nonlinear Finite Element Analysis. ME 563: Nonlinear Finite Element Analysis Spring 2016 Nonlinear Finite Element Modeling of Nano- Indentation Group Members: Shuaifang Zhang, Kangning Su Department of Mechanical and Nuclear Engineering,

More information

EXPERIMENTALLY DETERMINING THE VISCOELASTIC BEHAVIOR OF A CURING THERMOSET EPOXY R. Thorpe 1, A. Poursartip 1*

EXPERIMENTALLY DETERMINING THE VISCOELASTIC BEHAVIOR OF A CURING THERMOSET EPOXY R. Thorpe 1, A. Poursartip 1* 19 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS EXPERIMENTALLY DETERMINING THE VISCOELASTIC BEHAVIOR OF A CURING THERMOSET EPOXY R. Thorpe 1, A. Poursartip 1* 1 Composites Group, Dept. of Materials

More information

REPORT TO D-FLEX LTD APRIL 2009 REPORT. (to D-Flex Ltd, NWDA Innovation Vouchers Award, 28 April 2009)

REPORT TO D-FLEX LTD APRIL 2009 REPORT. (to D-Flex Ltd, NWDA Innovation Vouchers Award, 28 April 2009) REPORT (to D-Flex Ltd, NWDA Innovation Vouchers Award, 28 April 2009) Finite Element Modelling of Rigidity of Fishing Rods with Various Cross-sections Report to D-Flex Ltd by Z Guan Department of Engineering,

More information

An orthotropic damage model for crash simulation of composites

An orthotropic damage model for crash simulation of composites High Performance Structures and Materials III 511 An orthotropic damage model for crash simulation of composites W. Wang 1, F. H. M. Swartjes 1 & M. D. Gan 1 BU Automotive Centre of Lightweight Structures

More information

Determination of Mechanical Properties of Elastomers Using Instrumented Indentation

Determination of Mechanical Properties of Elastomers Using Instrumented Indentation Determination of Mechanical Properties of Elastomers Using Instrumented Indentation, Antonios E. Giannakopoulos and Dimitrios Bourntenas University of Thessaly, Department of Civil Engineering, Volos 38334,

More information

Discrete Element Modelling of a Reinforced Concrete Structure

Discrete Element Modelling of a Reinforced Concrete Structure Discrete Element Modelling of a Reinforced Concrete Structure S. Hentz, L. Daudeville, F.-V. Donzé Laboratoire Sols, Solides, Structures, Domaine Universitaire, BP 38041 Grenoble Cedex 9 France sebastian.hentz@inpg.fr

More information

3. Overview of MSC/NASTRAN

3. Overview of MSC/NASTRAN 3. Overview of MSC/NASTRAN MSC/NASTRAN is a general purpose finite element analysis program used in the field of static, dynamic, nonlinear, thermal, and optimization and is a FORTRAN program containing

More information

MULTI-SCALE MODELLING OF FIBRE BUNDLES

MULTI-SCALE MODELLING OF FIBRE BUNDLES THE 19 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS MULTI-SCALE MODELLING OF FIBRE BUNDLES N. D. Chakladar 1, P. Mandal 1 *, P. Potluri 2 1 School of Mechanical, Aerospace and Civil Engineering,

More information

Final Project: Indentation Simulation Mohak Patel ENGN-2340 Fall 13

Final Project: Indentation Simulation Mohak Patel ENGN-2340 Fall 13 Final Project: Indentation Simulation Mohak Patel ENGN-2340 Fall 13 Aim The project requires a simulation of rigid spherical indenter indenting into a flat block of viscoelastic material. The results from

More information

VMS-GeoMil. Background

VMS-GeoMil. Background Background When using a drilling rig for cone penetration testing, a mechanical clamp can be mounted to the drilling head (by means of a special transition piece). The depth than can be achieved depends

More information

IMPROVING LATERAL STIFFNESS ESTIMATION IN THE DIAGONAL STRUT MODEL OF INFILLED FRAMES

IMPROVING LATERAL STIFFNESS ESTIMATION IN THE DIAGONAL STRUT MODEL OF INFILLED FRAMES IMPROVING LATERAL STIFFNESS ESTIMATION IN THE DIAGONAL STRUT MODEL OF INFILLED FRAMES I.N. Doudoumis 1 1 Professor, Dept. of Civil Engineering, Aristotle University of Thessaloniki, Thessaloniki, Greece

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

STRAIN ASSESSMENT USFOS

STRAIN ASSESSMENT USFOS 1 STRAIN ASSESSMENT IN USFOS 2 CONTENTS: 1 Introduction...3 2 Revised strain calculation model...3 3 Strain predictions for various characteristic cases...4 3.1 Beam with concentrated load at mid span...

More information

Mechanics PhD Preliminary Spring 2017

Mechanics PhD Preliminary Spring 2017 Mechanics PhD Preliminary Spring 2017 1. (10 points) Consider a body Ω that is assembled by gluing together two separate bodies along a flat interface. The normal vector to the interface is given by n

More information

L13 Structural Engineering Laboratory

L13 Structural Engineering Laboratory LABORATORY PLANNING GUIDE L13 Structural Engineering Laboratory Content Covered subjects according to the curriculum of Structural Engineering... 2 Main concept... 4 Initial training provided for laboratory

More information

Chapter 2: Deflections of Structures

Chapter 2: Deflections of Structures Chapter 2: Deflections of Structures Fig. 4.1. (Fig. 2.1.) ASTU, Dept. of C Eng., Prepared by: Melkamu E. Page 1 (2.1) (4.1) (2.2) Fig.4.2 Fig.2.2 ASTU, Dept. of C Eng., Prepared by: Melkamu E. Page 2

More information

Lecture 19. Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity

Lecture 19. Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity MECH 373 Instrumentation and Measurements Lecture 19 Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity Measuring Accepleration and

More information

Supplementary Figures

Supplementary Figures Fracture Strength (GPa) Supplementary Figures a b 10 R=0.88 mm 1 0.1 Gordon et al Zhu et al Tang et al im et al 5 7 6 4 This work 5 50 500 Si Nanowire Diameter (nm) Supplementary Figure 1: (a) TEM image

More information

Benchmarkingfiniteelement simulation of rigid indenters in elastomers S.J. Jerrams, N. Reece-Pinchin

Benchmarkingfiniteelement simulation of rigid indenters in elastomers S.J. Jerrams, N. Reece-Pinchin Benchmarkingfiniteelement simulation of rigid indenters in elastomers S.J. Jerrams, N. Reece-Pinchin Abstract Verifications of finite element techniques applied to elastomers are difficult to achieve since

More information

Virtual distortions applied to structural modelling and sensitivity analysis. Damage identification testing example

Virtual distortions applied to structural modelling and sensitivity analysis. Damage identification testing example AMAS Workshop on Smart Materials and Structures SMART 03 (pp.313 324) Jadwisin, September 2-5, 2003 Virtual distortions applied to structural modelling and sensitivity analysis. Damage identification testing

More information

HIGHLY ADAPTABLE RUBBER ISOLATION SYSTEMS

HIGHLY ADAPTABLE RUBBER ISOLATION SYSTEMS th World Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 24 Paper No. 746 HIGHLY ADAPTABLE RUBBER ISOLATION SYSTEMS Luis DORFMANN, Maria Gabriella CASTELLANO 2, Stefan L. BURTSCHER,

More information

SEMM Mechanics PhD Preliminary Exam Spring Consider a two-dimensional rigid motion, whose displacement field is given by

SEMM Mechanics PhD Preliminary Exam Spring Consider a two-dimensional rigid motion, whose displacement field is given by SEMM Mechanics PhD Preliminary Exam Spring 2014 1. Consider a two-dimensional rigid motion, whose displacement field is given by u(x) = [cos(β)x 1 + sin(β)x 2 X 1 ]e 1 + [ sin(β)x 1 + cos(β)x 2 X 2 ]e

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

Lecture 15 Strain and stress in beams

Lecture 15 Strain and stress in beams Spring, 2019 ME 323 Mechanics of Materials Lecture 15 Strain and stress in beams Reading assignment: 6.1 6.2 News: Instructor: Prof. Marcial Gonzalez Last modified: 1/6/19 9:42:38 PM Beam theory (@ ME

More information

Estimation of damping capacity of rubber vibration isolators under harmonic excitation

Estimation of damping capacity of rubber vibration isolators under harmonic excitation Estimation of damping capacity of rubber vibration isolators under harmonic excitation Svetlana Polukoshko Ventspils University College, Engineering Research Institute VSRC, Ventspils, Latvia E-mail: pol.svet@inbox.lv

More information

Examination of finite element analysis and experimental results of quasi-statically loaded acetal copolymer gears

Examination of finite element analysis and experimental results of quasi-statically loaded acetal copolymer gears Examination of finite element analysis and experimental results of quasi-statically loaded acetal copolymer gears Paul Wyluda Ticona Summit, NJ 07901 Dan Wolf MSC Palo Alto, CA 94306 Abstract An elastic-plastic

More information

8/1/2009. CAE 7962 Presentation

8/1/2009. CAE 7962 Presentation CAE 7962 Presentation Gavin Patey Dameion Moores Aaron Henstridge Ashley Burke Brendan Harvey Fabio Faragalli Introduction Choosing mesh properties Explanation of the types of studies available and the

More information

Hardened Concrete. Lecture No. 16

Hardened Concrete. Lecture No. 16 Hardened Concrete Lecture No. 16 Fatigue strength of concrete Modulus of elasticity, Creep Shrinkage of concrete Stress-Strain Plot of Concrete At stress below 30% of ultimate strength, the transition

More information

Fig. 1. Circular fiber and interphase between the fiber and the matrix.

Fig. 1. Circular fiber and interphase between the fiber and the matrix. Finite element unit cell model based on ABAQUS for fiber reinforced composites Tian Tang Composites Manufacturing & Simulation Center, Purdue University West Lafayette, IN 47906 1. Problem Statement In

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

MEASUREMENT METHODS FOR OBTAINING VOLUMETRIC COEFFICIENTS FOR HYPERELASTIC MODELLING OF FLEXIBLE ADHESIVES

MEASUREMENT METHODS FOR OBTAINING VOLUMETRIC COEFFICIENTS FOR HYPERELASTIC MODELLING OF FLEXIBLE ADHESIVES MEASUREMENT METHODS FOR OBTAINING VOLUMETRIC COEFFICIENTS FOR HYPERELASTIC MODELLING OF FLEXIBLE ADHESIVES by Louise Crocker and Bruce Duncan Project PAJex2 - Flexible Adhesives PAJex2 Report No 3 January

More information

Eshan V. Dave, Secretary of M&FGM2006 (Hawaii) Research Assistant and Ph.D. Candidate. Glaucio H. Paulino, Chairman of M&FGM2006 (Hawaii)

Eshan V. Dave, Secretary of M&FGM2006 (Hawaii) Research Assistant and Ph.D. Candidate. Glaucio H. Paulino, Chairman of M&FGM2006 (Hawaii) Asphalt Pavement Aging and Temperature Dependent Properties through a Functionally Graded Viscoelastic Model I: Development, Implementation and Verification Eshan V. Dave, Secretary of M&FGM2006 (Hawaii)

More information

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

DEPARTMENT OF MECHANICAL ENIGINEERING, UNIVERSITY OF ENGINEERING & TECHNOLOGY LAHORE (KSK CAMPUS). DEPARTMENT OF MECHANICAL ENIGINEERING, UNIVERSITY OF ENGINEERING & TECHNOLOGY LAHORE (KSK CAMPUS). Lab Director: Coordinating Staff: Mr. Muhammad Farooq (Lecturer) Mr. Liaquat Qureshi (Lab Supervisor)

More information

Experiment Two (2) Torsional testing of Circular Shafts

Experiment Two (2) Torsional testing of Circular Shafts Experiment Two (2) Torsional testing of Circular Shafts Introduction: Torsion occurs when any shaft is subjected to a torque. This is true whether the shaft is rotating (such as drive shafts on engines,

More information

Advanced Simulation of Sealings CADFEM GmbH Rainer Rauch

Advanced Simulation of Sealings CADFEM GmbH Rainer Rauch Advanced Simulation of Sealings CADFEM GmbH Rainer Rauch Recent developments in ANSYS V12 for the simulation of sealings Element technology Material models Contact Robust design and optimization -1- New

More information

THE MATRIX: EVOLUTIONS II

THE MATRIX: EVOLUTIONS II THE MATRIX: EVOLUTIONS II Pearl Sullivan Composites and Adhesives Group Department of Mechanical Engineering University of Waterloo IPR 28 th Annual Symposium, 16 May 2006 Scope: Multi-scale Analyses Atomic/Nanoscale

More information

Key words: Polymeric Composite Bearing, Clearance, FEM

Key words: Polymeric Composite Bearing, Clearance, FEM A study on the effect of the clearance on the contact stresses and kinematics of polymeric composite journal bearings under reciprocating sliding conditions Abstract The effect of the clearance on the

More information

Mechanical Principles

Mechanical Principles Unit 4: Mechanical Principles Unit code: F/601/1450 QCF level: 5 Credit value: 15 Aim This unit aims to develop learners understanding of an extended range of mechanical principles that underpin the design

More information

Lecture 8 Viscoelasticity and Deformation

Lecture 8 Viscoelasticity and Deformation HW#5 Due 2/13 (Friday) Lab #1 Due 2/18 (Next Wednesday) For Friday 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

More information

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

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC. BENDING STRESS The effect of a bending moment applied to a cross-section of a beam is to induce a state of stress across that section. These stresses are known as bending stresses and they act normally

More information

Example 37 - Analytical Beam

Example 37 - Analytical Beam Example 37 - Analytical Beam Summary This example deals with the use of RADIOSS linear and nonlinear solvers. A beam submitted to a concentrated load on one extremity and fixed on the other hand is studied.

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

ELASTOMER RATE-DEPENDENCE: A TESTING AND MATERIAL MODELING METHODOLOGY

ELASTOMER RATE-DEPENDENCE: A TESTING AND MATERIAL MODELING METHODOLOGY ELASTOMER RATE-DEPENDENCE: A TESTING AND MATERIAL MODELING METHODOLOGY Tod Dalrymple and Jaehwan Choi DASSAULT SYSTÈMES SIMULIA CORP. Great Lakes Region Northville, Michigan and Kurt Miller Axel Products

More information

Finite Element Modeling of an Aluminum Tricycle Frame

Finite Element Modeling of an Aluminum Tricycle Frame Finite Element Modeling of an Aluminum Tricycle Frame A. Rodríguez, B. Chiné*, and J. A. Ramírez Costa Rica Institute of Technology, School of Materials Science and Engineering, Cartago, Costa Rica *Corresponding

More information

PREDICTION OF OUT-OF-PLANE FAILURE MODES IN CFRP

PREDICTION OF OUT-OF-PLANE FAILURE MODES IN CFRP PREDICTION OF OUT-OF-PLANE FAILURE MODES IN CFRP R. R. Pinto 1, P. P. Camanho 2 1 INEGI - Instituto de Engenharia Mecanica e Gestao Industrial, Rua Dr. Roberto Frias, 4200-465, Porto, Portugal 2 DEMec,

More information

Software Verification

Software Verification PROGRAM NAME: SAFE 014 EXAMPLE 16 racked Slab Analysis RAKED ANALYSIS METHOD The moment curvature diagram shown in Figure 16-1 depicts a plot of the uncracked and cracked conditions, 1 State 1, and, State,

More information

The Finite Element Method for Mechonics of Solids with ANSYS Applicotions

The Finite Element Method for Mechonics of Solids with ANSYS Applicotions The Finite Element Method for Mechonics of Solids with ANSYS Applicotions ELLIS H. DILL 0~~F~~~~"P Boca Raton London New Vork CRC Press is an imprint 01 the Taylor & Francis Group, an Informa business

More information

OPTIMISING THE MECHANICAL CHARACTERISATION OF A RESILIENT INTERLAYER FOR THE USE IN TIMBER CON- STRUCTION

OPTIMISING THE MECHANICAL CHARACTERISATION OF A RESILIENT INTERLAYER FOR THE USE IN TIMBER CON- STRUCTION OPTIMISING THE MECHANICAL CHARACTERISATION OF A RESILIENT INTERLAYER FOR THE USE IN TIMBER CON- STRUCTION Luca Barbaresi, Federica Morandi, Juri Belcari, Andrea Zucchelli and Alice Speranza University

More information

Chapter 5 Structural Elements: The truss & beam elements

Chapter 5 Structural Elements: The truss & beam elements Institute of Structural Engineering Page 1 Chapter 5 Structural Elements: The truss & beam elements Institute of Structural Engineering Page 2 Chapter Goals Learn how to formulate the Finite Element Equations

More information

SERVICEABILITY LIMIT STATE DESIGN

SERVICEABILITY LIMIT STATE DESIGN CHAPTER 11 SERVICEABILITY LIMIT STATE DESIGN Article 49. Cracking Limit State 49.1 General considerations In the case of verifications relating to Cracking Limit State, the effects of actions comprise

More information

ROBUST DESIGN OF A MECHANICAL LATCH

ROBUST DESIGN OF A MECHANICAL LATCH LA-UR-15-21296 Page 1 of 20 ROBUST DESIGN OF A MECHANICAL LATCH François Hemez Technical Staff Member, XTD-Division, Los Alamos National Laboratory Adjunct Professor, University of California San Diego

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

Software Verification

Software Verification EXAMPLE 16 racked Slab Analysis RAKED ANALYSIS METHOD The moment curvature diagram shown in Figure 16-1 depicts a plot of the uncracked and cracked conditions, Ψ 1 State 1, and, Ψ State, for a reinforced

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

Analysis of parameters influencing the jamming effect in circular braids

Analysis of parameters influencing the jamming effect in circular braids This paper is part of the Proceedings of the 2 International Conference on nd High Performance and Optimum Design of Structures and Materials (HPSM 2016) www.witconferences.com Analysis of parameters influencing

More information

Proceedings of the 28th Risø international symposium on materials science, 3-6 Sept 2007.

Proceedings of the 28th Risø international symposium on materials science, 3-6 Sept 2007. Proceedings of the 28th Risø international symposium on materials science, 3-6 Sept 27. INFLUENCE OF TEMPERATURE ON COHESIVE PARAMETERS FOR ADHESIVES Anders Biel 1 and Thomas Carlberger 2 1 University

More information

MSE 383, Unit 3-3. Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept.

MSE 383, Unit 3-3. Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept. Dynamic Mechanical Behavior MSE 383, Unit 3-3 Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept. Scope Why DMA & TTS? DMA Dynamic Mechanical Behavior (DMA) Superposition Principles

More information

Deflection Analysis of Spur Polymer Gear Teeth

Deflection Analysis of Spur Polymer Gear Teeth Deflection Analysis of Spur Polymer Gear Teeth Boštjan Trobentar, Srečko Glodež Faculty of mechanical engineering University of Maribor Maribor, Slovenia bostjan.trobentar@student.um.si Boštjan Zafošnik

More information

MHA042 - Material mechanics: Duggafrågor

MHA042 - Material mechanics: Duggafrågor MHA042 - Material mechanics: Duggafrågor 1) For a static uniaxial bar problem at isothermal (Θ const.) conditions, state principle of energy conservation (first law of thermodynamics). On the basis of

More information

Introduction, Basic Mechanics 2

Introduction, Basic Mechanics 2 Computational Biomechanics 18 Lecture : Introduction, Basic Mechanics Ulli Simon, Lucas Engelhardt, Martin Pietsch Scientific Computing Centre Ulm, UZWR Ulm University Contents Mechanical Basics Moment

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

T1 T e c h n i c a l S e c t i o n

T1 T e c h n i c a l S e c t i o n 1.5 Principles of Noise Reduction A good vibration isolation system is reducing vibration transmission through structures and thus, radiation of these vibration into air, thereby reducing noise. There

More information

Finite Element Analysis of Silicone Rubber Spacers Used in Automotive Engine Control Modules

Finite Element Analysis of Silicone Rubber Spacers Used in Automotive Engine Control Modules Finite Element Analysis of Silicone Rubber Spacers Used in Automotive Engine Control Modules Fereydoon Dadkhah Arlene Zahiri Delphi Electronics and Safety Kokomo, IN Abstract Silicone Rubber Spacers in

More information

Mechanical Shock Testing for LIGA Materials Characterization

Mechanical Shock Testing for LIGA Materials Characterization Mechanical Shock Testing for LIGA Materials Characterization Vesta I. Bateman Alfredo M. Morales Principal Member of Technical Staff Sandia National Laboratories* P.O. Box 58, MS553 Albuquerque, NM 87185-553

More information

Dynamic Response of EPS Blocks /soil Sandwiched Wall/embankment

Dynamic Response of EPS Blocks /soil Sandwiched Wall/embankment Proc. of Second China-Japan Joint Symposium on Recent Development of Theory and Practice in Geotechnology, Hong Kong, China Dynamic Response of EPS Blocks /soil Sandwiched Wall/embankment J. C. Chai 1

More information

Modelling the behaviour of plastics for design under impact

Modelling the behaviour of plastics for design under impact Modelling the behaviour of plastics for design under impact G. Dean and L. Crocker MPP IAG Meeting 6 October 24 Land Rover door trim Loading stages and selected regions Project MPP7.9 Main tasks Tests

More information

THE NEW 1.1 MN m TORQUE STANDARD MACHINE OF THE PTB BRAUNSCHWEIG/GERMANY

THE NEW 1.1 MN m TORQUE STANDARD MACHINE OF THE PTB BRAUNSCHWEIG/GERMANY THE NEW 1.1 MN m TORQUE STANDARD MACHINE OF THE PTB BRAUNSCHWEIG/GERMANY D. Peschel 1, D. Mauersberger 1, D. Schwind 2, U. Kolwinski 2 1 Solid mechanics department, PTB, Germany 2 Gassmann Theiss Messtechnik

More information

Dynamic Mechanical Analysis (DMA) of Polymers by Oscillatory Indentation

Dynamic Mechanical Analysis (DMA) of Polymers by Oscillatory Indentation Dynamic Mechanical Analysis (DMA) of Polymers by Oscillatory Indentation By Jennifer Hay, Nanomechanics, Inc. Abstract This application note teaches the theory and practice of measuring the complex modulus

More information

Finite Element Analysis of Piezoelectric Cantilever

Finite Element Analysis of Piezoelectric Cantilever Finite Element Analysis of Piezoelectric Cantilever Nitin N More Department of Mechanical Engineering K.L.E S College of Engineering and Technology, Belgaum, Karnataka, India. Abstract- Energy (or power)

More information

Multi-mode revisited

Multi-mode revisited Multi-mode revisited Testing the application of shift factors S.J.M Hellenbrand 515217 MT 7.29 Coaches: Ir. L.C.A. van Breemen Dr. Ir. L.E. Govaert 2-7- 7 Contents Contents 1 Introduction 2 I Polymers

More information

ENGN 2290: Plasticity Computational plasticity in Abaqus

ENGN 2290: Plasticity Computational plasticity in Abaqus ENGN 229: Plasticity Computational plasticity in Abaqus The purpose of these exercises is to build a familiarity with using user-material subroutines (UMATs) in Abaqus/Standard. Abaqus/Standard is a finite-element

More information

Material Testing Overview (THERMOPLASTICS)

Material Testing Overview (THERMOPLASTICS) Material Testing Overview (THERMOPLASTICS) Table of Contents Thermal Conductivity... 3 Specific Heat... 4 Transition Temperature and Ejection Temperature... 5 Shear Viscosity... 7 Pressure-Volume-Temperature

More information

Multi Linear Elastic and Plastic Link in SAP2000

Multi Linear Elastic and Plastic Link in SAP2000 26/01/2016 Marco Donà Multi Linear Elastic and Plastic Link in SAP2000 1 General principles Link object connects two joints, i and j, separated by length L, such that specialized structural behaviour may

More information

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

Procedure for Performing Stress Analysis by Means of Finite Element Method (FEM) Procedure for Performing Stress Analysis by Means of Finite Element Method (FEM) Colaboração dos engºs Patrício e Ediberto da Petrobras 1. Objective This Technical Specification sets forth the minimum

More information

9.5 Compression Members

9.5 Compression Members 9.5 Compression Members This section covers the following topics. Introduction Analysis Development of Interaction Diagram Effect of Prestressing Force 9.5.1 Introduction Prestressing is meaningful when

More information