ADVANCED DYNAMIC MECHANICAL ANALYSIS OF A TIRE SAMPLE BY NANOINDENTATION

Similar documents
MECHANICAL PROPERTIES OF HYDROGEL USING NANOINDENTATION

CHARACTERIZATION OF VISCOELASTIC PROPERTIES OF POLYMERIC MATERIALS THROUGH NANOINDENTATION

Dynamic Mechanical Analysis (DMA) of Polymers by Oscillatory Indentation

Dynamic Mechanical Analysis of Solid Polymers and Polymer Melts

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

Characterization of Viscoelastic Properties of Polymeric Materials Through Nanoindentation

Characterisation Programme Polymer Multi-scale Properties Industrial Advisory Group 22 nd April 2008

Characterization of Viscoelastic Properties of Polymeric Materials Through Nanoindentation

Characterisation of the mechanical behaviour of a polyurethane elastomer based on indentation and tensile creep experiments

Session 11: Complex Modulus of Viscoelastic Polymers

ROCK TRIBOLOGY USING TRIBOMETER

Determining thermal noise limiting properties of thin films

Keysight Technologies Instrumented Indentation Testing with the Keysight Nano Indenter G200. Application Note

Introduction to Engineering Materials ENGR2000. Dr. Coates

Comparison between the visco-elastic dampers And Magnetorheological dampers and study the Effect of temperature on the damping properties

Chapter 7. Highlights:

FIDUCIAL MARKS AS MEASURES OF THIN FILM CRACK ARREST TOUGHNESS

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

Performance and Control of the Agilent Nano Indenter DCM

D Y N A M I C M E C H A N I C A L A N A L Y S I S A N D I T S A D V A N T A G E S O V E R D E F L E C T I O N T E M P E R A T U R E U N D E R L O A D

MSC Elastomers Seminar Some Things About Elastomers

Structure property Relationships in Polymer Composites with Micrometer and Submicrometer Graphite Platelets

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

Mechanical Properties of Polymers. Scope. MSE 383, Unit 3-1. Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept.

Mechanical properties of polymers: an overview. Suryasarathi Bose Dept. of Materials Engineering, IISc, Bangalore

Adhesiveness of Tape via Nanoindentation

Rheology of cellulose solutions. Puu Cellulose Chemistry Michael Hummel

Application of nanoindentation technique to extract properties of thin films through experimental and numerical analysis

Determination of Glass Transition Temperature of Double-Base Rocket Propellants with the Use of Dynamic Mechanical Analysis

Rubber Friction and Tire Dynamics:

University Graz / Austria Institut für Chemie Volker Ribitsch

NUMERICAL MODELLING AND EXPERIMENTAL INFLATION VALIDATION OF A BIAS TWO-WHEEL TIRE

HIGH FREQUENCY VISCOELASTIC PROPERTIES OF NANO PARTICLES-FILLED RUBBER COMPOUNDS BY ULTARSONIC MEASUREMENT

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

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

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

Deformation of Polymers. Version 2.1. Boban Tanovic, MATTER David Dunning, University of North London

Thin Solid Films 517 (2009) Contents lists available at ScienceDirect. Thin Solid Films. journal homepage:

Presented by: Sergio G. Arias, Ph. D. Simulia Community Conference 2012, Providence, RI Date: May 16, 2012

Dynamic Finite Element Modeling of Elastomers

Fine adhesive particles A contact model including viscous damping

CIRCUIT RACING, TRACK TEXTURE, TEMPERATURE AND RUBBER FRICTION. Robin Sharp, Patrick Gruber and Ernesto Fina

Improved stress prediction in adhesive bonded optical components

Improving the accuracy of Atomic Force Microscope based nanomechanical measurements. Bede Pittenger Bruker Nano Surfaces, Santa Barbara, CA, USA

Module 7 Design of Springs. Version 2 ME, IIT Kharagpur

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

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

Fundamentals of Polymer Rheology. Sarah Cotts TA Instruments Rubber Testing Seminar CUICAR, Greenville SC

BIOEN LECTURE 18: VISCOELASTIC MODELS

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

Abvanced Lab Course. Dynamical-Mechanical Analysis (DMA) of Polymers

Composite Materials Research Laboratory, State University of New York at Buffalo, Buffalo, NY , USA

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

(Refer Slide Time: 00:58)

How materials work. Compression Tension Bending Torsion

Chapter 26 Elastic Properties of Materials

FEM model of pneumatic spring assembly

Accelerated Testing Methodology for Long Term Durability of CFRP

New Die Attach Adhesives Enable Low-Stress MEMS Packaging

TORQUE CAPACITY ENHANCEMENT OF A MAGNETORHEOLOGICAL FLUID CLUTCH USING THE SQUEEZE-STRENGTHEN EFFECT

Objectives: After completion of this module, you should be able to:

STUDIES ON NANO-INDENTATION OF POLYMERIC THIN FILMS USING FINITE ELEMENT METHODS

Mat. Res. Soc. Symp. Proc. Vol Materials Research Society

Quiz 1 Introduction to Polymers

MOOC QP Set 1 Principles of Vibration Control

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

Keysight Technologies Young s Modulus of Dielectric Low-k Materials. Application Note

Summary PHY101 ( 2 ) T / Hanadi Al Harbi

FRICTION SLIPPING BEHAVIOR BETWEEN CONCRETE AND STEEL -AIMING THE DEVELOPMENT OF BOLTED FRICTION- SLIPPING JOINT -

MOOC QP Set 2 Principles of Vibration Control

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

Using Rheological Properties to Evaluate Storage Stability and Setting Behaviors of Emulsified asphalts

ME 207 Material Science I

Pharmaceutical compounding I Colloidal and Surface-Chemical Aspects of Dosage Forms Dr. rer. nat. Rebaz H. Ali

Peak Strain and Displacement Sensors for Structural Health Monitoring

A MECHANICAL MODEL FOR THE DYNAMICAL CONTACT OF ELASTIC ROUGH BODIES WITH VISCOELASTIC PROPERTIES

THERMOMECHANICAL ANALYSIS

Outline. 4 Mechanical Sensors Introduction General Mechanical properties Piezoresistivity Piezoresistive Sensors Capacitive sensors Applications

Polymer Dynamics and Rheology

Strength Study of Spiral Flexure Spring of Stirling Cryocooler

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

Testing Elastomers and Plastics for Marc Material Models

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

3.091 Introduction to Solid State Chemistry. Lecture Notes No. 5a ELASTIC BEHAVIOR OF SOLIDS

13 Solid materials Exam practice questions

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 4, No 1, 2013

Numerical Modelling of Dynamic Earth Force Transmission to Underground Structures

Supplementary Figures

VISCOELASTIC PROPERTIES OF POLYMERS

Micro-rheology of cells and soft matter with the NanoTracker

EFFECT OF SOY PROTEIN AND CARBOHYDRATE RATIO ON THE VISCOELASTIC PROPERTIES OF STYRENE-BUTADIENE COMPOSITES

Analysis of contact deformation between a coated flat plate and a sphere and its practical application

FRANK OHENE Department of Chemistry Grambliig State University Grambling, LA 71245

Module-4. Mechanical Properties of Metals

Pre-stressed concrete = Pre-compression concrete Pre-compression stresses is applied at the place when tensile stress occur Concrete weak in tension

Lecture Note October 1, 2009 Nanostructure characterization techniques

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

Thermal physics revision questions

Solid Mechanics Homework Answers

Quiz 1. Introduction to Polymers

Transcription:

ADVANCED DYNAMIC MECHANICAL ANALYSIS OF A TIRE SAMPLE BY NANOINDENTATION Duanjie Li and Pierre Leroux, Nanovea, Irvine, CA Abstract The viscoelastic properties of a tire sample are comprehensively studied by dynamical mechanical analysis (DMA) using nanoindentation technique with the Nanovea Mechanical Tester. We found that the tire possesses different viscoelastic mechanical properties across the tire layers. Such strategical distribution of the hardness and complex modulus at different layers meets the functionality requirements of the tire. The tire shows increased storage and loss modulus as the loading frequency increases from 0.1 to 20 Hz. The DMA frequency sweep test provides useful information on the viscoelastic behaviors of the tire running at different speeds, which is essential in improving the performance of tires for smoother and safer rides. Introduction An elastic material strains immediately when stressed and it returns to its original shape once the stress is removed. In comparison, a viscous material under the influence of external forces strains linearly with time. Viscoelastic materials such as polymers exhibit both viscous and elastic characteristics as they undergo deformation, and they are therefore characterized by the complex modulus: E* = E'+ ie'', where the storage modulus E' characterizes the elastic behavior, and the loss modulus E'' characterizes the viscous behavior (loss of energy due to internal friction between molecules). Dynamical mechanical analysis (DMA) is developed to investigate this behavior by applying a sinusoidal oscillatory stress in tension, compression, torsion or bending to a sample of known geometry. From the response of the sample subjected to the controlled stress or strain the complex modulus can be calculated. Nanovea Mechanical Tester performs the DMA measurement using nanoindentation technique. Compared to conventional macroscale DMA testers, nanoindentation does not require fabricating test samples into stringent geometry, thus cutting significant cost and time on sample preparation. More importantly, the small indentation size makes it possible to perform multiple measurements on one single sample, allowing mapping the viscoelastic properties of the sample as a function of location. Many nanoindentation systems on the market use a coil/magnet assembly as the actuator to apply sinusoidal oscillation to the indenter without measuring the load with a separate sensor. Because of mechanical and electrical delay from the order to move to the actual position, complex algorithms are needed to account for the delays in the calculation of the phase shift between the load and displacement 1234. In comparison, the Nanovea Mechanical Tester generates the sinusoidal load by a high-precision piezo actuator and directly measures the evolution of force and displacement using ultra-sensitive load cell and capacitor. The feedback load sensing not only eliminates complex algorithms, but also significantly improves the precision and accuracy of the data. The combination of easy setup and high accuracy makes the Nanovea Mechanical Tester an ideal tool for DMA tests. Tires are subjected to cyclical high deformations when vehicles are running on the road. When exposed to harsh road conditions, the service lifetime of the tires is jeopardized by many factors, such as the wear of the tread, the heat generated by friction, rubber aging, and others. As a result, tires usually have composite layer structures made of carbon-filled rubber, nylon cords, and steel wires, etc. In particular, the composition of rubber at different layers of the tire architecture is optimized to provide different functional properties, including but not limited to wear resistant tread, cushion rubber layer and hard rubber base layer. A reliable and repeatable test of the viscoelastic behavior of rubber is critical in R&D and quality control of new tires, as well as evaluation of life span of old tires. In addition, frequencies of the tire rotation and deformation change as the car accelerates to higher speeds. Such a change in cyclic stress and strain can result in variation in the viscoelastic properties of the tire and in turn influence the car performance. In this study, we evaluate the viscoelastic properties of different layers of the tire by DMA tests using nanoindentation technique. The complex modulus and mechanical behavior of the tire are mapped across the cross section of the tire. The DMA frequency sweep test is performed on the tire sample to investigate the effect of the cyclic stress/strain frequency on the complex modulus of the tire, which represents the viscoelastic properties of the tire at different car speed. SPE ANTEC Anaheim 2017 / 2030

Test Conditions The Nanovea Mechanical Tester is used to measure the viscoelastic properties of the polished cross section of a Continental tire sample by means of DMA tests. The sinusoidal oscillation was applied to a 100-μm spherical diamond tip. The Nanovea Mechanical Tester has true close feedback control on the load applied. The load applied by the fast piezo is independent from the load measured by a separate high sensitivity strain gage. This gives a distinct advantage during DMA since the phase between depth and load is measured directly from the data collected from the sensors. The calculation of phase shift is direct and does not need complex mathematical modeling that adds inaccuracy to the resulting loss and storage modulus. A series (40 points) of nanoindentation DMA was performed along the thickness of the tire sample and the distribution of the indentations is illustrated in Fig. 1. The 40 indentations along the tire thickness were spaced 0.38 mm apart for a total distance of ~15.5 mm. The test conditions are summarized in Table 1. DMA frequency sweep test by nanoindentation was performed on the tire sample. The test conditions are summarized in Table 2. Table 2: Test conditions of the DMA frequency sweep by nanoindentation. Loading voltage (V) 1 Loading rate (V /min) 2 Unloading rate (V /min) 2 Oscillation amplitude voltage (V) 0.1 Creep time at each frequency (s) 50 Frequency (Hz) 0.1, 1, 5, 10, 20 Results and Discussion 1. DMA mapping across the tire sample The Tan(δ), storage modulus, loss modulus and hardness measured from the DMA mapping along the thickness of the tire sample are summarized in Fig. 2 to Fig. 5. The distribution of the hardness and complex modulus meets the functionality requirements of the rubber at different layers of the tire. The rubber at the positions from 0.38 to 2.66 mm and from 8.22 and 11.64 mm exhibits a relatively low hardness below 2 MPa and low complex modulus. Such a relative soft feature allows the rubber in these regions to serve as a cushion layer and absorb the shocks and vibrations. In comparison, the rubber at the positions from 3.04 to 7.84 mm shows higher hardness and complex modulus, due to the composite structure consisting of high tensile-strength reinforcing fabric encased in the rubber compound. The enhanced mechanical properties of this layer provide strength and toughness to the tire structure. The positions from 12.02 to 15.82 mm reside in the tire tread and exhibit higher hardness and complex modulus compared with the cushion layer. The high carbon black concentration in this layer provides reinforced abrasion resistance, cut resistance as well as better traction. Fig. 1: Distribution of the indentation on the cross section of the tire sample. Table 1: Test conditions of the nanoindentation DMA along the thickness of the tire sample. Maximum force (mn) 75 Loading rate (mn /min) 150 Unloading rate (mn /min) 150 Creep (s) 20 Amplitude (mn) 15 Frequency (Hz) 10 SPE ANTEC Anaheim 2017 / 2031

Loss Modulus (MPa) Storage Modulus (MPa) Tan(δ) Hardness (MPa) 0.3 0.25 0.2 0.15 0.1 0.05 0 Fig. 2: Distribution of Tan(δ) at different locations of the tire. 80.0 70.0 60.0 50.0 40.0 30.0 20.0 10.0 0.0 Fig. 3: Distribution of Storage Modulus at different locations of the tire. 16.00 14.00 12.00 10.00 8.00 6.00 4.00 2.00 0.00 Fig. 4: Distribution of Loss Modulus at different locations of the tire. 8.00 7.00 6.00 5.00 4.00 3.00 2.00 1.00 0.00 Fig. 5: Distribution of Hardness at different locations of the tire. The desired functionality of the different tire layers is achieved by the strategical design of specific viscoelastic properties in these layers. Zones of high loss modulus will absorb differently than zones of low loss modulus. The DMA mapping tests allow one to develop tires for smoother and safer rides in different weather conditions. The Nanovea Mechanical Tester can perform the DMA tests at various temperatures and even in liquids. It can also be conducted at various frequencies to mimic the behavior of tires as the car runs at different speeds. In the following section, we further investigate the influence of the oscillation frequency during the DMA tests on the viscoelastic properties of the tire rubber. 2. DMA frequency sweep Long molecular chains in polymer materials contribute to their unique viscoelastic properties. Such a combination of the characteristics of both elastic solids and Newtonian fluid can be influenced by the oscillation frequency. The DMA frequency sweep at the maximum load measures the viscoelastic characteristics of the sample at different loading frequencies in one test. The load & depth curve of the full frequency scan is plotted in Fig. 6 and the load and depth as a function of time at each frequency is shown in Fig. 7. The phase shift and the amplitudes of the load and displacement waves at different frequencies, i.e. 0.1, 1, 5, 10 and 20 Hz in this DMA sweep test can be used to calculate a variety of fundamental material viscoelastic properties, including storage modulus, loss modulus and Tan (δ) as summarized in Fig. 8 and Fig. 9. Frequencies of 0.1, 1, 5, 10 and 20 Hz in this study, correspond to speeds of about 0.7, 7, 33, 67 and 134 km per hour. As the test frequency increases from 0.1 to 20 Hz, it can be observed that both the Storage Modulus and the Loss Modulus progressively increase. Tan (δ) decreases from ~0.27 to 0.18 as the frequency increases SPE ANTEC Anaheim 2017 / 2032

from 0.1 to 1 Hz, and then it gradually increases to ~0.55 when the frequency of 20 Hz is reached. The variation of Storage Modulus, Loss Modulus and Tan (δ) at different frequencies provides information on the movement of the monomers and cross-linking in polymers. The DMA frequency sweep test can also be performed at various temperatures and in different media to mimic the realistic working environment of the tire under different weather, providing a more complete picture of the nature of the molecular motion under different service conditions. Modulus (MPa) 60 55 50 45 40 35 30 25 20 15 10 5 0.1 Hz 1 Hz 5 Hz 10 Hz 20 Hz Oscillation Frequency Storage Modulus Loss Modulus Fig. 8: Storage and Loss Modulus at different frequencies. Fig. 6: Evolution of load & depth of the full DMA frequency sweep. 0.5 (a) 0.1 Hz: 0.4 Tan ( ) 0.3 0.2 (b) 1 Hz: 0.1 (c) 5 Hz: 0.0 0.1 Hz 1 Hz 5 Hz 10 Hz 20 Hz Oscillation frequency Fig. 9: Tan (δ) at different frequencies. Conclusion (d) 10 Hz: (e) 20 Hz: Fig. 7: Load and depth as a function of time at different frequencies. In this study, we comprehensively evaluated the viscoelastic properties of a tire sample by the DMA mapping and frequency sweep tests using the Nanovea Mechanical Tester. Unlike the nanoindentation systems that use coil actuator to generate oscillation, the Nanovea Mechanical Tester performs the nanoindentation by applying the load with a fast piezo that is independent from the load measurement done by a separate high sensitivity strain gage. This gives a distinct advantage during DMA since the phase between depth and load is measured directly from the data collected from the sensor, which significantly improves the accuracy of the calculated loss and storage modulus. The DMA mapping across the depth of the tire shows the change of the complex modulus at different tire layers, SPE ANTEC Anaheim 2017 / 2033

which meets the functionality requirements of the tire design. In the DMA frequency sweep test, the tire shows increased storage and loss modulus as the loading frequency increases from 0.1 to 20 Hz. This test provides useful information on the viscoelastic behaviors of the tire running at different speeds, which is essential in improving the performance of tires for smoother and safer rides. duanjie@nanovea.com. He has a B.S. degree from Tsinghua University in China and a Ph.D. from McGill University in Montreal, Québec, Canada. He specializes in advanced mechanical, tribological, and surface profile characterization techniques. He develops novel functions and algorithms to improve accuracy and versatility of the precision materials characterization instruments. In conclusion, the DMA measures the loss and storage modulus, complex modulus and Tan (δ) as a function of contact depth, time and frequency. Optional heating stage allows determination of materials phase transition temperature during DMA. In addition, the Nanovea Mechanical Tester provides unmatched multi-functional Nano and Micro/Macro modules, including scratch tester, hardness tester and wear tester modes. Bio Duanjie Li is the lead materials scientist at Nanovea, 6 Morgan, Ste. 156, Irvine CA 92618, email: 1 B.N. Lucas, W.C. Oliver, and J.E. Swindeman, in Fundamentals of Nanoindentation and Nanotribology, edited by N.R. Moody, W.W. Gerberich, N. Burnham, and S.P. Baker (Mater. Res. Soc. Symp. Proc. 522, Warrendale, PA, 1998), pp. 3 2 C. C. White, M. R. Vanlandingham, P. L. Drzal, N.-K. Chang, S.-H. Chang, Journal of Polymer Science: Part B: Polymer Physics (2005), Vol. 43, pp. 1812 1824 3 W.C. Oliver and G.M. Pharr, J. Mater. Res., Vol. 19, No. 1, Jan 2004, pp. 3-20 4 C. Klapperich, K. Komvopoulos, and L. Pruitt, Journal of Tribology. Vol. 123, 2001, pp. 624-631 SPE ANTEC Anaheim 2017 / 2034