Dynamic viscoelastic properties of polyvinyl chloride with physical aging
|
|
- Dominic Ferguson
- 5 years ago
- Views:
Transcription
1 Korea-Australia Rheology Journal, 27(4), (November 2015) DOI: /s Dynamic viscoelastic properties of polyvinyl chloride with physical aging Fang Tian 1, Yingshe Luo 1, *, Shuiping Yin 1, Hong Wang 2 and Chun Cao 3 1 College of Civil Engineering and Mechanics, Central South University of Forestry and Technology, Changsha , P.R. China 2 College of Science, Central South University of Forestry and Technology, Changsha , P.R. China 3 China North Vehicle Research Institute, Beijing , P.R. China (Received December 15, 2014; final revision received October 8, 2015; accepted October 17, 2015) The experimental research of dynamic viscoelastic properties of polyvinyl chloride was conducted by the dynamic mechanical analysis method in this paper. And the fitting equation of dynamic modulus of polymers has been presented. Based on the time-aging time equivalent principle, horizontal shift factor and vertical shift factor of aging time are carried out, which proposes a novel method for the research on time-aging time equivalent analysis of dynamic mechanical properties of polymers during physical aging. Keywords: aging, polyvinyl chloride, dynamical viscoelasticity 1. Introduction # This paper is based on work presented at the 6th Pacific Rim Conference on Rheology, held in the University of Melbourne, Australia from 20 th to 25 th July *Corresponding author; lys0258@sina.com Polymers have been widely applied in many fields such as aerospace, machinery manufacturing, building energy and biological engineering due to their high strength, light weight, corrosion resistance and good glass-forming ability (Ma, 2012; Tian et al., 2013). Compared with metals and ceramics, one of the most important mechanical properties of polymers is their viscoelastic properties, which means that the stress response of polymers depends not only on the strain but also the changing rate of strain, that is, the mechanical properties of polymers are time-dependent. There is a characteristic time scalar exiting in polymers, which is different to natural time scalar and sensitive to environmental factors, such as temperature, aging, stress, strain and so on (Zhao et al., 2008). So, viscoelastic solids usually exhibit complicate mechanical behaviors. Previous researchers have made lots effort to establish relationships between the characteristic time scalar of polymers and various influence factors. Based on the free volume theory, first proposed by Flory et al. (Knauss and Emri, 1987), Williams et al. (Williams et al., 1955) introduced the temperature shift factor and established the time-temperature equivalent function (WLF function) by supposing that the effect of temperature on viscoelastic properties of polymers is equivalent to the horizontal shift of time axis and all the viscoelastic curves with different temperatures keep in the same shape. Based on WLF function, Luo et al. (2001) further considered the effect of stress and established the time-temperature-stress equivalent function, which makes it possible to predict the viscoelastic behavior polymers with low-stress level and long-time load by shift-factor introduced superposition method. Based on experimental research, Plazek (Plazek et al., 1995) pointed out that the mechanical behaviors of many polymers are not consistent with the WLF function for viscoelastic modulus curves with temperature change not only their position but also their shape, which is known as the complexity of thermal rheology. Thus, in this paper, considering the change of position and shape of modulus curves, the horizontal shift factor and the vertical shift factor are introduced at the same time. With the passage of time, reversible physical changes and irreversible chemical changes occur continuously in the interior of polymers, which affects many mechanical properties of polymers, performances of polymer-based composites and so on. The occurrence of aging causes deterioration of mechanical properties of polymers, leading to its premature failure that not only makes the economy suffered huge losses, leading to a waste of resources, but also causes serious environmental pollutions due to the decomposition of materials (Liu et al., 2012). Struik made lots of experimental researches on 40 different kinds of polymers and pointed out that viscoelastic mechanical behaviors of polymers are affected by physical aging and then established the time-aging time superposition principle based on his experiments (Struik, 1987a; 1987b; 1989a; 1989b). Based on Struik s research, Shaukat discussed the practical application of the time-aging time superposition principle (Montes et al., 2006). Joshi (Awasthi and Joshi, 2009; Joshi, 2014) analyzed the relationship between real time and aging time by the effective time approach and further predicted the long-term creep behavior of polymers. However, previous researches on the time-aging time equivalent principle mainly focused on conditions of static load, which failed to take dynamic loads and multi-temperature tests into consideration (Bandyopadhyay et al., 2015 The Korean Society of Rheology and Springer pissn X eissn
2 Fang Tian, Yingshe Luo, Shuiping Yin, Hong Wang and Chun Cao 2010; Chen et al., 2010). Yet, in fact, structures made by polymers and polymer-based composites are usually subject to linear and nonlinear dynamic loads in their working environments accompanied by physical aging (He et al., 2007; Zhang et al., 2007) such as rotating tires, transferring gears and damping rubbers and so on (Guo, 2002). So, the importance of research on dynamic viscoelasticity of polymers during physical aging can never be exaggerated. This paper makes an experimental research on effects of physical aging on linear dynamic viscoelastic mechanical behaviors of polymers with different testing temperatures by dynamic mechanical thermal instrument. Furthermore, the application of time-aging time superposition on dynamic conditions is discussed in this paper. 2. Presentation of Models A proper function to describe relationships between dynamic modulus and load frequency is the foundation of research on dynamic viscoelastic properties of polymers with different aging time. Presently, study about relationships between dynamic viscoelastic properties and load frequencies is still not enough, while research methods for static viscoelastic properties are relatively mature. Struik used the three-parameter Kohlrausch model to describe short-term creep curves of polymers accompanied by physical aging and made a comparison of fitting curves and relevant experimental data, which proved that the three-parameter Kohlrausch model is suitable to describe short-term creep curves of polymers. The fitting function of creep compliance is as follows: S( logt; S 0, γ, β; t e ) = S 0 exp logt (1) γ where S is the compliance; t is the test time; S 0, γ, β are fitting parameters, t e is the aging time. For creep compliance of polymers is a function of the aging time, fitting parameters S 0, γ, β are related to the aging time t e. Based on the fitting function of creep compliance, Eq. (1), supposing β = 1 for simplicity and replacing the test time t with the test frequency f, the fitting function of dynamic modulus can be written as follows: E( log f; S 0, γ ; t e ) = S 0 exp log f (2) γ where E is the dynamic modulus, f is the test frequency. For further discussion, a reference aging time should be chosen out based on experiments. The dynamic modulus curve of polymer sample undergoing the reference aging time is called the reference modulus curve, which is given by: R( log f ) = E( log f ; S R, γ R ; t eref ) β (3) where t eref is the reference aging time; S R, γ R are fitting parameters of reference modulus curve. Shift factors can be obtained by analyzing relationships between the reference modulus curve R (log f ) and dynamic modulus curves S with different aging time, which makes it possible to predict dynamic modulus of polymers with an arbitrary aging time t e based on the reference modulus curve R. Taking horizontal shift into consideration, the function is given by: E( log f ; S 0, γ ; t e ) = R( a t log f ) (4) where a t is the aging-time horizontal shift factor. When considering horizontal shift and vertical shift of modulus curves at the same time, the function is given by: E( log f ; S 0, γ ; t e ) = b t Ra ( t log f ) (5) where b t is the aging-time vertical shift factor. Putting Eqs. (2) and (3) into Eq. (5), the dynamic modulus function considering the aging-time horizontal shift factor and the aging-time vertical shift factor is given by: E( logf; S 0, γ; t e ) = S 0 exp logt = b. (6) γ t S R exp a t log f γ R Then the aging-time horizontal shift factor and the agingtime vertical shift factor are separately given by: a t = γ R ----, (7) γ b t = S (8) S R 3. Application of Models in Physical Aging Analysis of Polyvinyl Chloride 3.1. Experiments Experimental samples of polyvinyl chloride (PVC) were cut into strips with dimension of 50 mm 5 mm 1 mm. In order to eliminate the effects of thermal history, test samples were put into an air convection oven at 90 o C for 30 minutes before suffered by thermal physical aging at 55 o C for various periods. Frequency sweep tests were conducted by dynamic mechanical analyzer, GABO EPLEXOR 500N. Strain controlling method was adopted in all tests of this paper. The maximum static strain is 1% and the maximum dynamic strain is 0.05%. In frequency sweep tests, the frequency scan range was from 0.01 Hz to 100 Hz, and nine constant temperature levels (15 o C, 35 o C, 45 o C, 55 o C, 65 o C, 70 o C, 75 o C, 80 o C, 85 o C) were considered. Values of storage modulus and loss modulus with different test temperatures and load frequencies were recorded by frequency sweep tests. 260 Korea-Australia Rheology J., 27(4), 2015
3 Dynamic viscoelastic properties of polyvinyl chloride with physical aging Fig. 1. (Color online) Test data and fit curves of storage modulus E' of PVC with different aging time Application of models in the analysis of dynamic modulus of polyvinyl chloride Experimental data of storage modulus and loss modulus of PVC samples with different temperature levels (15 o C, 35 o C, 45 o C, 55 o C, 65 o C, 70 o C, 75 o C, 80 o C, 85 o C) and different aging time (20 d, 40 d, 60 d) were separately shown in Figs. 1 and 2 and fitted by dynamic modulus function, Eq. (2). The experimental data of storage modulus are shown in Fig. 1 as hollow points, and solid lines are corresponding fitting curves of the dynamic modulus function, Eq. (2), wherein parameters of this fitting function are shown in Figs. 2 and 3. As shown in Fig. 1a-c, the modulus change with aging time depends on the test temperature rather than the test frequency, that is, the modulus changing with aging time keep the same variation tendency at different test frequency but different variation tendency for different test temperature. For that, taking the fixed frequency f = 10 Hz as an example, the modulus changes with aging time at different test temperature are shown in Fig. 1d-f. It Korea-Australia Rheology J., 27(4),
4 Fang Tian, Yingshe Luo, Shuiping Yin, Hong Wang and Chun Cao Fig. 2. (Color online) Fit parameter S 0 of storage modulus E'. Fig. 3. (Color online) Fit parameter γ of storage modulus E'. can be seen that with increasing aging time periods when the test temperature is lower than the aging temperature 55 o C, values of storage modulus decrease, and fitting parameters S 0 ' and γ ' present the same tendency; when the test temperature is equal to the aging temperature 55 o C, values of the storage modulus do not change much; when the temperature is higher than the aging temperature 55 o C, values of storage modulus and values of fitting parameters S 0 ' and γ ' show increasing trends as a whole. Experimental data of loss modulus of PVC samples are shown in Fig. 4 as hollow points, and solid lines are corresponding fitting curves of the dynamic modulus function, Eq. (2), wherein parameters of this fitting function are shown in Figs. 5 and 6. It can be seen that when the test temperature is lower than or equal to the aging temperature 55 o C, fitting parameters S 0 '' and γ '' increase with increasing test temperature; when the test temperature is between 65 and 70 o C, there is a peak value of the fitting parameter S 0 ', and values of fitting parameters γ ' change discontinuously around temperature 65 o C. In addition, the minimum value of parameter γ '' appears at 65 o C, while Fig. 4. (Color online) Test data and fit curves of loss modulus E'' of PVC with different aging time. the maximum value is at 70 o C during the test temperature range; When the test temperature is higher than or equal to 75 o C, fitting parameters S 0 '' and γ '' are decreased with increasing test temperature. Figs. 1 and 4 show that the dynamic modulus fitting function, Eq. (2) presented in this paper is a proper mechanical model to simulate storage modulus curves and loss modulus curves of PVC samples. In addition, experimental results show that fitting parameters of the function, Eq. (2) are closely related to test temperatures. 262 Korea-Australia Rheology J., 27(4), 2015
5 Dynamic viscoelastic properties of polyvinyl chloride with physical aging Fig. 5. (Color online) Fit parameter S 0 of loss modulus E''. Fig. 6. (Color online) Fit parameter γ 0 of loss modulus E'' Application of models in analysis of time-aging time equivalent principle of polyvinyl chloride Taking 20 days as the reference aging time and putting fitting parameters S 0 ' and γ ' of storage modulus (shown in Figs. 2 and 3) into the aging-time horizontal shift factor function, Eq. (7) and the aging-time vertical shift factor function, Eq. (8), values of the aging-time horizontal shift factor a t ' (shown in Table 1) and the aging-time vertical shift factor b t ' (shown in Table 2) of storage modulus curves of samples with different test temperatures and aging time periods can be carried out. According to Table 1 and Table 2, values of the horizontal shift factor a t ' and the vertical shift factor b t ' of storage modulus of samples with the reference aging time are equal to 1. When the test temperature is lower than the aging temperature 55 o C, the aging-time horizontal shift factor a t ' would be greater than or equal to 1 (only when t e = t eref = 20 d), and the agingtime vertical shift factor b t ' would be less than or equal to 1 (only when t e = t eref = 20 d), which indicates that with increasing aging time periods storage modulus curves of PVC samples would generate a shift horizontally to right and vertically to downwards relative to reference storage modulus curves, which means that effects of aging on storage modulus equal to increasing frequency and temperature; when the test temperature is above the aging temperature 55 o C, the aging-time horizontal shift factor a t ' would be less than or equal to 1 (only when t e = t eref =20 d), and the aging-time vertical shift factor b t ' would be greater than or equal to 1(only when t e = t eref = 20 d), which suggests that with increasing aging time periods storage modulus curves of PVC samples would make a shift horizontally to left and vertically to upwards relative to their corresponding reference storage modulus curves, which implies that effects of aging equal to decreasing frequency and temperature. Therefore, values of the agingtime horizontal shift factor a t ' and the aging-time vertical shift factor b t ' of PVC samples are closely related to test temperatures that greatly affect the movement of molecular chains. Based on the aging-time shift factor (shown in Tables 1 and 2), experimental data of storage modulus (shown in Fig. 3) are shifted horizontally and vertically (shown as hollow dots in Fig. 7). Taking fitting parameters S 0 ' and γ ' of samples with the reference aging time into the dynamic Table 1. Aging-time horizontal shifting factors a t of storage modulus E'. a t 15 o C 35 o C 45 o C 55 o C 65 o C 70 o C 75 o C 80 o C 85 o C 20 d d d Table 2. Aging-time vertical shifting factors b t of storage modulus E'. b t 15 o C 35 o C 45 o C 55 o C 65 o C 70 o C 75 o C 80 o C 85 o C 20 d d d Korea-Australia Rheology J., 27(4),
6 Fang Tian, Yingshe Luo, Shuiping Yin, Hong Wang and Chun Cao Fig. 7. (Color online) Aging-time shifting curves of storage modulus E' of PVC ( t eref = 20 d ). modulus function, Eq. (2), the reference storage modulus curves is derived (shown as solid lines in Fig. 7). Fig. 7 shows that reference fitting curves of storage modulus can be used to describe the variation of storage modulus of PVC samples along with the load frequency by using the aging-time horizontal shift factor a t ' and the aging-time vertical shift factor b t '. Taking fitting parameters S 0 '' and γ '' of loss modulus (shown in Figs. 5 and 6) into the aging-time horizontal shift factor function, Eq. (7) and the aging-time vertical shift factor function, Eq. (8), values of the aging-time horizontal shift factor a t '' (shown in Table 3) and the agingtime vertical shift factor b t '' (shown in Table 4) of loss modulus curves of samples with different test temperatures and aging time periods can be carried out. Values of the horizontal shift factor a t '' and the vertical shift factor b t '' of loss modulus of samples with the reference aging time are equal to 1. When the value of the aging-time horizontal shift factor a t '' is greater than 1, it s suggested that loss modulus curve generate a shift to right related to their corresponding reference loss modulus curves; when the value is less than 1, there would be a shift to left. When the value of the vertical shift factor b t '' is greater than 1, it s indicated that loss modulus curves generate a shift to upward related to their corresponding reference loss modulus, and when the value is less than 1, there would be a shift to downward. Thus, when the test temperature is above on or equals to 70 o C, values of the horizontal shift factor a t '' are less than (except for t e =60 d, T =65 o C) or equal to (only when t e = t eref = 20 d) 1, and values of the vertical shift factor b t '' are greater than or equals to (only when t e = t eref = 20 d) 1, which proves that with increasing aging-time periods the loss modulus of PVC samples would shift horizontally to left and vertically to upward, indicating that effects of aging on loss modulus equal to decreasing frequency and temperature; when the test temperature is lower than 70 o C, the aging-time shift factors of loss modulus are greatly affected by temperatures. Based on the aging-time shift factor (shown in Tables 3 and 4), experimental data of loss modulus (shown in Fig. Table 3. Aging-time horizontal shifting factors a t of loss modulus E''. a t 15 o C 35 o C 45 o C 55 o C 65 o C 70 o C 75 o C 80 o C 85 o C 20 d d d Table 4. Aging-time vertical shifting factors b t of loss modulus E''. b t 15 o C 35 o C 45 o C 55 o C 65 o C 70 o C 75 o C 80 o C 85 o C 20 d d d Korea-Australia Rheology J., 27(4), 2015
7 Dynamic viscoelastic properties of polyvinyl chloride with physical aging 4. Conclusions This paper presents a dynamic modulus fitting function of polymers, which is in good agreement with the experimental data. It can be used for both storage modulus and loss modulus calculations of PVC. Based on the dynamic modulus fitting function, this paper introduces the aging time horizontal shift factor and vertical shift factor and establish the equivalent relationship of dynamic modulus of PVC with different aging time. And the effects of test temperatures on shift factors are also discussed in this paper. A new method for research on time-aging time equivalent principle of dynamic mechanic behaviors of polymers is presented. Acknowledgements This work was supported by the National Natural Science Foundation (No ), the Education Department of Hunan Province (No.12C0464) and the Postgraduate Innovation Funding of Central South University of Forestry and Technology (No. CX2013B33). References Fig. 8. (Color online) Aging-time shifting curves of loss modulus E'' of PVC ( t eref = 20 d ). 8) are shifted horizontally and vertically (shown as hollow dots in Fig. 8). Taking fitting parameters S 0 '' and γ '' of samples with the reference aging time into the dynamic modulus function, Eq. (2), reference curves off loss modulus are derived (shown as solid line in Fig. 8). From this figure, it can be seen that reference curves of loss modulus can describe the variation of loss modulus of PVC samples along with the load frequency by using the aging-time horizontal shift factor a t '' and the aging-time vertical shift factor b t ''. Awasthi, V. and Y. Joshi, 2009, Effect of temperature on aging and time-temperature superposition in nonergodic laponite suspensions, Soft Matter 5, Bandyopadhyay R., P.H. Mohan, and Y.M. Joshi, 2010, Stress relaxation in aging soft colloidal glasses, Soft Matter 6, Chen, H., T. Hou, and Y. Feng, 2010, Fractional model for the physical aging, Sci. Sinica Phys. Mech. Astron. 40, Guo, M., 2002, Polymer Composites with Dynamic Mechanical Thermal Analysis of Polymers and Composites, Chemical Industry Press, Beijing. He, C., Z. Zhang, Y. Li, and Z. Sun, 2007, Dynamic viscoelasticities of CF/ GF hybrid reinforced epoxy composites under high load, Acta Mat. Compos. Sinica 24, Joshi, Y.M., 2014, Long time response of aging glassy polymers, Rheol. Acta 53, Knauss, W.G. and I. Emri, 1987, Volume change and the nonlinearly thermo-viscoelastic constitution of polymers, Polym. Eng. Sci. 27, Luo, W., T. Yang, and Q. An, 2001, Time-temperature-stress equivalence and its application to nonlinear viscoelastic materials, Acta Mech. Solida Sin. 14, Liu, Y., C. Qiao, and J. Yao, 2012, Progress of physical aging of polymers, Polym. Bull. 3, Ma, D., 2012, Structure and Properties of Polymers, Science Press, Beijing. Montes, H., V. Viasnoff, S. Jurine, and F. Lequeux, 2006 Aging in glassy polymers under various thermal histories, J. Stat. Mech. Theory Exp. 3, P Plazek, D.J., I.C. Chay, K.L. Ngai, and C.M. Roland, 1995, Vis- Korea-Australia Rheology J., 27(4),
8 Fang Tian, Yingshe Luo, Shuiping Yin, Hong Wang and Chun Cao coelastic properties of polymers. 4. Thermorheological complexity of the softening dispersion in polyisobutylene, Macromolecules 28, Struik, L.C.E., 1987a, The mechanical behavior and physical aging of semicrystalline polymers: 1, Polymer 28, Struik, L.C.E., 1987b, The mechanical behavior and physical aging of semicrystalline polymers: 2, Polymer 28, Struik, L.C.E., 1989a, The mechanical behavior and physical aging of semicrystalline polymers: 3, Polymer 30, Struik, L.C.E., 1989b, The mechanical behavior and physical aging of semicrystalline polymers: 4, Polymer 30, Tian, F., S. Xing, and Y. Luo, 2013, Research on the influence of the tension on dielectric strength of the unique direction glass fiber reinforced composites, Adv. Mat. Res , Williams, M.L., R.F. Landel, and J.D. Ferry, 1955, The temperature dependence of relaxation mechanisms in amorphous polymers and other glass-forming liquids, J. Am. Chem. Soc. 77, Zhang, Z., C. He, Y. Li, and Z. Sun, 2007, Dynamic viscoelasticity of carbon fiber reinforced polymers under high load: Effects of static and dynamic loads, Polym. Polym. Compos. 15, Zhao, R., C. Chen, Q. Li, and W. Luo, 2008, Effect of stress and physical aging on nonlinear creep behavior of poly(methy methacrylate), J Cent. South Univ. T. 15, Korea-Australia Rheology J., 27(4), 2015
Application of Time-Temperature-Stress Superposition Principle to Nonlinear Creep of Poly(methyl methacrylate)
Key Engineering Materials Vols. 34-341 (27) pp. 191-196 online at http://www.scientific.net (27) rans ech Publications, Switzerland Application of ime-emperature-stress Superposition Principle to Nonlinear
More informationModeling of Nonlinear Viscoelastic Creep of Polycarbonate
e-polymers 7, no. 7 http://www.e-polymers.org ISSN 68-79 Modeling of Nonlinear Viscoelastic Creep of Polycarbonate Wenbo Luo, * Said Jazouli, Toan Vu-Khanh College of Civil Engineering and Mechanics, Xiangtan
More informationMSE 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 informationEffect of temperature on aging and time temperature superposition in nonergodic laponite suspensions
PAPER www.rsc.org/softmatter Soft Matter Effect of temperature on aging and time temperature superposition in nonergodic laponite suspensions Varun Awasthi and Yogesh M. Joshi* Received 27th July 2009,
More information548 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 informationExperiment Study on Rheological Model of Soft Clay
Send Orders for Reprints to reprints@benthamscience.ae 344 The Open Civil Engineering Journal, 2014, 8, 344-350 Experiment Study on Rheological Model of Soft Clay Open Access Donglin Wang*, Qiuling Lv
More informationVISCOELASTIC PROPERTIES OF POLYMERS
VISCOELASTIC PROPERTIES OF POLYMERS John D. Ferry Professor of Chemistry University of Wisconsin THIRD EDITION JOHN WILEY & SONS New York Chichester Brisbane Toronto Singapore Contents 1. The Nature of
More informationA Hydrophilic/Hydrophobic Janus Inverse-Opal
Supporting information A Hydrophilic/Hydrophobic Janus Inverse-Opal Actuator via Gradient Infiltration Dajie Zhang #, Jie Liu //#, Bo Chen *, Yong Zhao, Jingxia Wang * //, Tomiki Ikeda, Lei Jiang //. CAS
More informationAbvanced Lab Course. Dynamical-Mechanical Analysis (DMA) of Polymers
Abvanced Lab Course Dynamical-Mechanical Analysis (DMA) of Polymers M211 As od: 9.4.213 Aim: Determination of the mechanical properties of a typical polymer under alternating load in the elastic range
More informationMechanical Properties of Polymer Rubber Materials Based on a New Constitutive Model
Mechanical Properties of Polymer Rubber Materials Based on a New Constitutive Model Mechanical Properties of Polymer Rubber Materials Based on a New Constitutive Model J.B. Sang*, L.F. Sun, S.F. Xing,
More informationExperimental Study on Electromechanical Performances of Two Kinds of the Integral Arrayed Cymbal Harvesters
Journal of Applied Science and Engineering, Vol. 18, No. 4, pp. 339 344 (2015) DOI: 10.6180/jase.2015.18.4.04 Experimental Study on Electromechanical Performances of Two Kinds of the Integral Arrayed Cymbal
More informationDynamic mechanical properties of ZN-35 silicone rubber materials based on H-N model Tieneng Guo1,a Yunchao Gu2,b Shiming Ma3,c Li Wang4,d
4th International Conference on Machinery, Materials and Computing Technology (ICMMCT 2016) Dynamic mechanical properties of ZN-35 silicone rubber materials based on H-N model Tieneng Guo1,a Yunchao Gu2,b
More informationMeasurement Engineering Group, Paderborn University, Warburger Straße 100, Paderborn, Germany
Nadine Feldmann 1, Fabian Bause 1, Bernd Henning 1 1 Measurement Engineering Group, Paderborn University, Warburger Straße 100, 33098 Paderborn, Germany feldmann@emt.uni-paderborn.de Abstract The present
More informationActa Materiae Compositae Sinica Vol123 No11 February 2006
Acta Materiae Compositae Sinica Vol123 No11 February 2006 : 100023851 (2006) 0120026205 23 1 2 2006 /, 3,, (, 100083) : GABO EPL EXOR 500 N 648 DMA, 500 N, ;, : ; ; ; : TB332 : A Dynamic viscoelasticity
More informationA Piezoelectric Screw Dislocation Interacting with an Elliptical Piezoelectric Inhomogeneity Containing a Confocal Elliptical Rigid Core
Commun. Theor. Phys. 56 774 778 Vol. 56, No. 4, October 5, A Piezoelectric Screw Dislocation Interacting with an Elliptical Piezoelectric Inhomogeneity Containing a Confocal Elliptical Rigid Core JIANG
More informationPrediction of Elastic Constants on 3D Four-directional Braided
Prediction of Elastic Constants on 3D Four-directional Braided Composites Prediction of Elastic Constants on 3D Four-directional Braided Composites Liang Dao Zhou 1,2,* and Zhuo Zhuang 1 1 School of Aerospace,
More informationFUNDAMENTAL CONSTITUTIVE MODEL FOR GLASSY POLYMERS
Nonlinear Viscoelastic Behavior of Glassy Polymers and Its Effect on the Onset of Irreversible Deformation of the Matrix Resin in Continuous Fiber Composites J. M. Caruthers and G. A. Medvedev School of
More informationGlass Transition as the Rheological Inverse of Gelation
NNF Summer reading group, July 18 th 2017 Glass Transition as the Rheological Inverse of Gelation ACS Macromolecules 46, 2425-2432 (2013) H Henning Winter Department of Chemical Engineering and Department
More informationPSD Analysis and Optimization of 2500hp Shale Gas Fracturing Truck Chassis Frame
Send Orders for Reprints to reprints@benthamscience.ae The Open Mechanical Engineering Journal, 2014, 8, 533-538 533 Open Access PSD Analysis and Optimization of 2500hp Shale Gas Fracturing Truck Chassis
More informationDYNAMIC AND TRANSIENT TESTING OF ASPHALT BINDER AND PAVING MIX
66 6th RILEM Symposium PTEBM'03, Zurich, 2003 DYNAMIC AND TRANSIENT TESTING OF ASPHALT BINDER AND PAVING MIX L. Zanzotto, O.J. Vacin and J. Stastna University of Calgary, Canada Abstract: A commercially
More informationElement size effect on the analysis of heavy-duty machine cross-rail Jianhua Wang1,Jianke Chen1,a,Tieneng Guo1 Bin Song 2, Dongliang Guo3
4th International Conference on Machinery, Materials and Computing Technology (ICMMCT 2016) Element size effect on the analysis of heavy-duty machine cross-rail Jianhua Wang1,Jianke Chen1,a,Tieneng Guo1
More informationLecture 7 Constitutive Behavior of Asphalt Concrete
Lecture 7 Constitutive Behavior of Asphalt Concrete What is a Constitutive Model? A constitutive model or constitutive equation is a relation between two physical quantities that is specific to a material
More informationEffect of temperature on the terminal relaxation of branched polydimethysiloxane
Downloaded from http://polymerphysics.net Journal of Non-Crystalline Solids 307 310 (2002) 835 841 www.elsevier.com/locate/jnoncrysol Effect of temperature on the terminal relaxation of branched polydimethysiloxane
More informationSimulation Analysis of Microchannel Deformation during LTCC Warm Water Isostatic Pressing Process Lang Ping, Zhaohua Wu*
International Conference on Information Sciences, Machinery, Materials and Energy (ICISMME 2015) Simulation Analysis of Microchannel Deformation during LTCC Warm Water Isostatic Pressing Process Lang Ping,
More informationThe Effect of Well Patterns on Surfactant/Polymer Flooding
International Journal of Energy and Power Engineering 2016; 5(6): 189-195 http://www.sciencepublishinggroup.com/j/ijepe doi: 10.11648/j.ijepe.20160506.13 ISSN: 2326-957X (Print); ISSN: 2326-960X (Online)
More informationThe Large Amplitude Oscillatory Strain Response of Aqueous Foam: Strain Localization and Full Stress Fourier Spectrum
The Large Amplitude Oscillatory Strain Response of Aqueous Foam: Strain Localization and Full Stress Fourier Spectrum By F. Rouyer, S. Cohen-Addad, R. Höhler, P. Sollich, and S.M. Fielding The European
More informationAnalysis of Cantilever-Beam Bending Stress Relaxation Properties of Thin Wood Composites
Analysis of Cantilever-Beam Bending Stress Relaxation Properties of Thin Wood Composites John F. Hunt, a, * Houjiang Zhang, b and Yan Huang b An equivalent strain method was used to analyze and determine
More informationConstitutive equation and damping function for entangled polymers
Korea-Australia Rheology Journal Vol. 11, No. 4, December 1999 pp.287-291 Constitutive equation and damping function for entangled polymers Kunihiro Osaki Institute for Chemical Research, Kyoto University
More informationMulti-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 informationNon-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 informationControlling the Period-Doubling Bifurcation of Logistic Model
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.20(2015) No.3,pp.174-178 Controlling the Period-Doubling Bifurcation of Logistic Model Zhiqian Wang 1, Jiashi Tang
More informationChemical Engineering 160/260 Polymer Science and Engineering. Lecture 14: Amorphous State February 14, 2001
Chemical Engineering 160/260 Polymer Science and Engineering Lecture 14: Amorphous State February 14, 2001 Objectives! To provide guidance toward understanding why an amorphous polymer glass may be considered
More informationElastic parameters prediction under dynamic loading based on the. unit cell of composites considering end constraint effect
Elastic parameters prediction under dynamic loading based on the unit cell of composites considering end constraint effect Wang Meng 1,, Fei Qingguo 1,, Zhang Peiwei 1, (1. Institute of Aerospace Machinery
More informationResearch of concrete cracking propagation based on information entropy evolution
Research of concrete cracking propagation based on information entropy evolution Changsheng Xiang 1, Yu Zhou 2, Bin Zhao 3, Liang Zhang 4, Fuchao Mao 5 1, 2, 5 Key Laboratory of Disaster Prevention and
More informationQuiz 1 Introduction to Polymers (Please answer each question even if you guess)
080407 Quiz 1 Introduction to Polymers (Please answer each question even if you guess) This week we explored the definition of a polymer in terms of properties. 1) The flow of polymer melts and concentrated
More informationInfluence of steady shear flow on dynamic viscoelastic properties of un-reinforced and Kevlar, glass fibre reinforced LLDPE
Bull. Mater. Sci., Vol. 27, No. 5, October 2004, pp. 409 415. Indian Academy of Sciences. Influence of steady shear flow on dynamic viscoelastic properties of un-reinforced and Kevlar, glass fibre reinforced
More informationMeasurement and Prediction of Fluid Viscosities at High Shear Rates
Chapter 5 Measurement and Prediction of Fluid Viscosities at High Shear Rates Jeshwanth K. Rameshwaram and Tien T. Dao Additional information is available at the end of the chapter http://dx.doi.org/10.5772/54282
More informationNondestructive Testing and Performance Prediction of Soybean Stalk Board
Nondestructive Testing and Performance Prediction of Soybean Stalk Board Wei Lu, a Jia Yao, a, * Xiangdong Liu, a Lili Ma, a and Yuhua Wang b Crop straw-reinforced industrial materials can be effectively
More informationNonlinear Controller Design of the Inverted Pendulum System based on Extended State Observer Limin Du, Fucheng Cao
International Conference on Automation, Mechanical Control and Computational Engineering (AMCCE 015) Nonlinear Controller Design of the Inverted Pendulum System based on Extended State Observer Limin Du,
More informationG. R. Strobl, Chapter 5 "The Physics of Polymers, 2'nd Ed." Springer, NY, (1997). J. Ferry, "Viscoelastic Behavior of Polymers"
G. R. Strobl, Chapter 5 "The Physics of Polymers, 2'nd Ed." Springer, NY, (1997). J. Ferry, "Viscoelastic Behavior of Polymers" Chapter 3: Specific Relaxations There are many types of relaxation processes
More informationADVANCED DYNAMIC MECHANICAL ANALYSIS OF A TIRE SAMPLE BY NANOINDENTATION
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
More informationTemperature Dependence of Mechanical and Dielectric Relaxation in cis-1,4-polyisoprene
Downloaded from http://polymerphysics.net Macromolecules 1998, 31, 3715-3719 3715 Temperature Dependence of Mechanical and Dielectric Relaxation in cis-1,4-polyisoprene P. G. Santangelo and C. M. Roland*
More informationElements of Polymer Structure and Viscoelasticity. David M. Parks Mechanics and Materials II February 18, 2004
Elements of Polymer Structure and Viscoelasticity David M. Parks Mechanics and Materials II 2.002 February 18, 2004 Outline Elements of polymer structure Linear vs. branched; Vinyl polymers and substitutions
More informationOn the Universality of Chain Dynamics
wnloaded from http://polymerphysics.net Macromolecules 2008, 41, 3925-3929 3925 On the Universality of Chain Dynamics K. L. Ngai,*, D. J. Plazek, and C. M. Roland*, NaVal Research Laboratory, Washington,
More informationarxiv: v1 [astro-ph.im] 25 Apr 2014
CPC(HEP & NP), 9, 33(X): 5 Chinese Physics C Vol. 33, No. X, Xxx, 9 A linear calibration method on DNL error for energy spectrum * arxiv:44.633v [astro-ph.im] 5 Apr 4 LU Bo() ;) FU Yan-Hong(), CHEN Yong()
More informationSupporting Information. Controlled Structure Evolution of Graphene Networks in Polymer Composites
Supporting Information Controlled Structure Evolution of Graphene Networks in Polymer Composites Stephen C. Boothroyd,,# David W. Johnson,,# Michael P. Weir, Carl D. Reynolds, James M. Hart, Andrew J.
More informationSupporting Information
Supporting Information Oscillatory normal forces of magnetorheological fluids Xinglong Gong *, Chaoyang Guo, Shouhu Xuan, Taixiang Liu, Luhang Zong, Chao Peng Department of Modern Mechanics, CAS Key Laboratory
More informationGeneralized projective synchronization between two chaotic gyros with nonlinear damping
Generalized projective synchronization between two chaotic gyros with nonlinear damping Min Fu-Hong( ) Department of Electrical and Automation Engineering, Nanjing Normal University, Nanjing 210042, China
More informationModelling the Rheology of Semi-Concentrated Polymeric Composites
THALES Project No 1188 Modelling the Rheology of Semi-Concentrated Polymeric Composites Research Team Evan Mitsoulis (PI), Professor, NTUA, Greece Costas Papoulias (Research Student), NTUA, Greece Souzanna
More informationEXPERIMENTALLY 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 informationDetermination 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 informationLaser on-line Thickness Measurement Technology Based on Judgment and Wavelet De-noising
Sensors & Transducers, Vol. 168, Issue 4, April 214, pp. 137-141 Sensors & Transducers 214 by IFSA Publishing, S. L. http://www.sensorsportal.com Laser on-line Thickness Measurement Technology Based on
More informationConstitutive Model for High Density Polyethylene to Capture Strain Reversal
Constitutive Model for High Density Polyethylene to Capture Strain Reversal Abdul Ghafar Chehab 1 and Ian D. Moore 2 1 Research Assistant, GeoEngineering Centre at Queen s RMC, Queen s University, Kingston,
More informationViscoelastic Mechanical Analysis for High Temperature Process of a Soda-Lime Glass Using COMSOL Multiphysics
Viscoelastic Mechanical Analysis for High Temperature Process of a Soda-Lime Glass Using COMSOL Multiphysics R. Carbone 1* 1 Dipartimento di Ingegneria dei Materiali e della Produzione sez. Tecnologie
More informationDynamic Mechanical Analysis of Solid Polymers and Polymer Melts
Polymer Physics 2015 Matilda Larsson Dynamic Mechanical Analysis of Solid Polymers and Polymer Melts Polymer & Materials Chemistry Introduction Two common instruments for dynamic mechanical thermal analysis
More informationLinear Elastic Fracture Mechanics
Measure what is measurable, and make measurable what is not so. - Galileo GALILEI Linear Elastic Fracture Mechanics Krishnaswamy Ravi-Chandar Lecture presented at the University of Pierre and Marie Curie
More information:,,, T, Yamamoto PACC: 9260X, China Academic Journal Electronic Publishing House. All rights reserved.
55 6 2006 6 100023290Π2006Π55 (06) Π3180208 ACTA PHYSICA SINICA Vol. 55,No. 6,June,2006 ν 2006 Chin. Phys. Soc. 3 1) 2) 2) 3) g 3) 4) 1) (, 225009) 2) ( 2, 100029) 3) (,, 100081) 4) (, 100029) (2005 7
More informationOverhead catenary system-pantograph coupled system dynamics modelling and analysis
Acta Technica 62 (2017), No. 6A, 109 118 c 2017 Institute of Thermomechanics CAS, v.v.i. Overhead catenary system-pantograph coupled system dynamics modelling and analysis Luo Jianguo 2, Liu Hang 2, 4,
More informationCharacteristic Temperatures of Waxy Crude Oils
2007 Petroleum Science Vol.4 No.3 Characteristic Temperatures of Waxy Crude Oils Zhu Yingru, Zhang Jinjun, Li Hongying and Chen Jun (Beijing Key Laboratory of Urban Oil and Gas Distribution Technology,
More informationPHYSICAL AGING AND CREEP CHARACTERIZATION OF A CARBON/POLYIMIDE COMPOSITE
PHYSICAL AGING AND CREEP CHARACTERIZATION OF A CARBON/POLYIMIDE COMPOSITE I. M. Daniel 1, J. J. Luo 2, and Z. Sun 3 1 Walter P. Murphy Professor, Departments of Civil and Mechanical Engineering, Robert
More informationStudy on High-Temperature Glass Lens Molding Process Using FEM Simulation
Send Orders for Reprints to reprints@benthamscience.ae 14 The Open Materials Science Journal, 2015, 9, 14-19 Open Access Study on High-Temperature Glass Lens Molding Process Using FEM Simulation Zhang
More informationDynamic 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 informationDynamic 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 informationNumerical-experimental method for elastic parameters identification of a composite panel
THEORETICAL & APPLIED MECHANICS LETTERS 4, 061001 (2014) Numerical-experimental method for elastic parameters identification of a composite panel Dong Jiang, 1, 2, a) Rui Ma, 1, 2 Shaoqing Wu, 1, 2 1,
More informationTuning the Shell Number of Multi-Shelled Metal Oxide. Hollow Fibers for Optimized Lithium Ion Storage
Supporting Information Tuning the Shell Number of Multi-Shelled Metal Oxide Hollow Fibers for Optimized Lithium Ion Storage Jin Sun, Chunxiao Lv, Fan Lv, ǁ Shuai Chen, Daohao Li, Ziqi Guo, Wei Han, Dongjiang
More informationMechanical Models for Asphalt Behavior and Performance
Mechanical Models for Asphalt Behavior and Performance All Attendees Are Muted Questions and Answers Please type your questions into your webinar control panel We will read your questions out loud, and
More informationDynamic stiffness of ageing rubber vibration isolators
Dynamic stiffness of ageing rubber vibration isolators Leif Kari Structure-borne sound Source Receiver Physical principle Hard Hard Soft F without F with Force transmissibility T F = F with F without F
More informationTHREE-DIMENSIONAL HAUSDORFF DERIVATIVE DIFFUSION MODEL FOR ISOTROPIC/ANISOTROPIC FRACTAL POROUS MEDIA
Cai, W., et al.: Three-Dimensional Hausdorff Derivative Diffusion Model... THERMAL SCIENCE: Year 08, Vol., Suppl., pp. S-S6 S THREE-DIMENSIONAL HAUSDORFF DERIVATIVE DIFFUSION MODEL FOR ISOTROPIC/ANISOTROPIC
More informationSmall-Scale Effect on the Static Deflection of a Clamped Graphene Sheet
Copyright 05 Tech Science Press CMC, vol.8, no., pp.03-7, 05 Small-Scale Effect on the Static Deflection of a Clamped Graphene Sheet G. Q. Xie, J. P. Wang, Q. L. Zhang Abstract: Small-scale effect on the
More informationStress-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 informationMechanical properties of polymers: an overview. Suryasarathi Bose Dept. of Materials Engineering, IISc, Bangalore
Mechanical properties of polymers: an overview Suryasarathi Bose Dept. of Materials Engineering, IISc, Bangalore UGC-NRCM Summer School on Mechanical Property Characterization- June 2012 Overview of polymer
More informationStress Overshoot of Polymer Solutions at High Rates of Shear
Stress Overshoot of Polymer Solutions at High Rates of Shear K. OSAKI, T. INOUE, T. ISOMURA Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan Received 3 April 2000; revised
More informationAnisotropic Damage Mechanics Modeling of Concrete under Biaxial Fatigue Loading
Open Journal of Civil Engineering, 2015, 5, 8-16 Published Online March 2015 in SciRes. http://www.scirp.org/journal/ojce http://dx.doi.org/10.4236/ojce.2015.51002 Anisotropic Damage Mechanics Modeling
More informationDielectric Properties and Lattice Distortion in Rhombohedral Phase Region and Phase Coexistence Region of PZT Ceramics
Commun. Theor. Phys. (Beijing, China) 43 (2005) pp. 855 860 c International Academic Publishers Vol. 43, No. 5, May 15, 2005 Dielectric Properties and Lattice Distortion in Rhombohedral Phase Region and
More informationbifunctional electrocatalyst for overall water splitting
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2017 Hierarchical Ni/NiTiO 3 derived from NiTi LDHs: a bifunctional electrocatalyst
More informationPolymer engineering syllabus (BSc)
Polymer engineering syllabus (BSc) First semester Math 1 Physics 1 Physics 1 lab General chemistry General chemistry lab workshop Second semester Math 2 Physics 2 Organic chemistry 1 Organic chemistry
More informationAging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology
Aging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology Outline Laponite Basic background. Laponite in suspension Bonn et al.,
More informationImproved stress prediction in adhesive bonded optical components
Improved stress prediction in adhesive bonded optical components J. de Vreugd 1a, M.J.A. te Voert a, J.R. Nijenhuis a, J.A.C.M. Pijnenburg a, E. Tabak a a TNO optomechatronics, Stieltjesweg 1, 2628 CK,
More informationNatural Boundary Element Method for Stress Field in Rock Surrounding a Roadway with Weak Local Support
Copyright 011 Tech Science Press CMES, vol.71, no., pp.93-109, 011 Natural Boundary Element Method for Stress Field in Rock Surrounding a Roadway with Weak Local Support Shuncai Li 1,,3, Zhengzhu Dong
More informationEIGEN THEORY OF VISCOELASTIC MECHANICS FOR ANISOTROPIC SOLIDS
ACTA MECHANICA SOLIDA SINICA, Vol. 14, No. 1, March 2001 Published by HUST, Wuhan, China ISSN0894-9166 EIGEN THEORY OF VISCOELASTIC MECHANICS FOR ANISOTROPIC SOLIDS Guo Shaohua ( College of Resources,
More informationInfluences of material dilatancy and pore water pressure on stability factor of shallow tunnels
Influences of material dilatancy and pore water pressure on stability factor of shallow tunnels YANG Xiao-li( ), HUANG Fu( ) School of Civil and Architectural Engineering, Central South University, Changsha
More informationExperimental Study on Durability and Mechanical Properties of Basalt Fiber Reinforced Concrete under Sodium Sulfate Erosion
961 A publication of CHEMICAL ENGINEERING TRANSACTIONS VOL. 62, 2017 Guest Editors: Fei Song, Haibo Wang, Fang He Copyright 2017, AIDIC Servizi S.r.l. ISBN 978-88-95608-60-0; ISSN 2283-9216 The Italian
More informationThe Simulation of Dropped Objects on the Offshore Structure Liping SUN 1,a, Gang MA 1,b, Chunyong NIE 2,c, Zihan WANG 1,d
Advanced Materials Research Online: 2011-09-02 ISSN: 1662-8985, Vol. 339, pp 553-556 doi:10.4028/www.scientific.net/amr.339.553 2011 Trans Tech Publications, Switzerland The Simulation of Dropped Objects
More informationGeneral Synthesis of Graphene-Supported. Bicomponent Metal Monoxides as Alternative High- Performance Li-Ion Anodes to Binary Spinel Oxides
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2016 Electronic Supplementary Information (ESI) General Synthesis of Graphene-Supported
More informationSupporting Information
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2018 Supporting Information Si/SiO x Hollow Nanospheres/Nitrogen-Doped Carbon
More informationAnisotropic modeling of short fibers reinforced thermoplastics materials with LS-DYNA
Anisotropic modeling of short fibers reinforced thermoplastics materials with LS-DYNA Alexandre Hatt 1 1 Faurecia Automotive Seating, Simplified Limited Liability Company 1 Abstract / Summary Polymer thermoplastics
More informationAnalysis of high loss viscoelastic composites
Analysis of high loss viscoelastic composites by C. P. Chen, Ph.D. and R. S. Lakes, Ph.D. Department of Engineering Physics Engineering Mechanics Program; Biomedical Engineering Department Materials Science
More informationCreep Compliance Analysis Technique for the Flattened Indirect Tension Test of Asphalt Concrete
Creep Compliance Analysis Technique for the Flattened Indirect Tension Test of Asphalt Concrete Eshan V. Dave Andrew F. Braham Prof. William G. Buttlar Prof. Glaucio H. Paulino CONCREEP8, Ise-Shima, Japan
More informationSTRUCTURAL DYNAMICS AND INTERFACIAL PROPERTIES OF ELASTOMER NANO-COMPOSITES
STRUCTURAL DYNAMICS AND INTERFACIAL PROPERTIES OF ELASTOMER NANO-COMPOSITES M. Klüppel, J. Fritzsche Deutsches Institut für Kautschuktechnologie e.v. Eupener Straße 33, D-30519 Hannover, Germany Manfred.Klueppel@DIKautschuk.de
More informationFinite element analysis of propellant of solid rocket motor during ship motion
Propulsion and Power Research 2013;2(1):50 55 http://ppr.buaa.edu.cn/ Propulsion and Power Research www.sciencedirect.com ORIGINAL ARTICLE Finite element analysis of propellant of solid rocket motor during
More informationEstimation of the Residual Stiffness of Fire-Damaged Concrete Members
Copyright 2011 Tech Science Press CMC, vol.22, no.3, pp.261-273, 2011 Estimation of the Residual Stiffness of Fire-Damaged Concrete Members J.M. Zhu 1, X.C. Wang 1, D. Wei 2, Y.H. Liu 2 and B.Y. Xu 2 Abstract:
More informationThe Experimental Research of the Effect of Heating Temperature and Heating Time for Oil Shale Crack
Yi Pan GENERAL et al., AND PHYSICAL J.Chem.Soc.Pak., Vol. 39, No. 02, 2017 177 The Experimental Research of the Effect of Heating Temperature and Heating Time for Oil Shale Crack Yi Pan*, Shidong Wang,
More informationPREDICTION OF OPEN HOLE COMPRESSIVE FAILURE FOR QUASI-ISOTROPIC CFRP LAMINATES BY MMF/ATM METHOD
HE 19 H INERNAIONAL CONFERENCE ON COMPOSIE MAERIALS PREDICION OF OPEN HOLE COMPRESSIVE FAILURE FOR QUASI-ISOROPIC CFRP LAMINAES BY MMF/AM MEHOD. Hioki 1*, M. Nakada 2, Y. Miyano 2, H. Katoh 3 1 Graduate
More informationA Phenomenological Model for Linear Viscoelasticity of Monodisperse Linear Polymers
Macromolecular Research, Vol. 10, No. 5, pp 266-272 (2002) A Phenomenological Model for Linear Viscoelasticity of Monodisperse Linear Polymers Kwang Soo Cho*, Woo Sik Kim, Dong-ho Lee, Lee Soon Park, Kyung
More informationThermal Analysis of Polysaccharides Mechanical Methods
Biopolymer Solutions Thermal Analysis of Polysaccharides Mechanical Methods John Mitchell John.Mitchell@biopolymersolutions.co.uk 1 Topics Covered Introduction to polymer viscoelasticity Examples Thermal
More informationDynamic Mechanical Analysis of Thermosetting Materials
Dynamic Mechanical Analysis of Thermosetting Materials R. Bruce Prime IBM (Retired) / Consultant rbprime@attglobal.net As described in an earlier paper Thermal Analysis in Thermoset Characterization, thermosetting
More informationDYNAMIC STABILITY OF NON-DILUTE FIBER SHEAR SUSPENSIONS
THERMAL SCIENCE, Year 2012, Vol. 16, No. 5, pp. 1551-1555 1551 DYNAMIC STABILITY OF NON-DILUTE FIBER SHEAR SUSPENSIONS by Zhan-Hong WAN a*, Zhen-Jiang YOU b, and Chang-Bin WANG c a Department of Ocean
More informationThe Mathematical Analysis of Temperature-Pressure-Adsorption Data of Deep Shale Gas
International Journal of Oil, Gas and Coal Engineering 2018; 6(6): 177-182 http://www.sciencepublishinggroup.com/j/ogce doi: 10.11648/j.ogce.20180606.18 ISSN: 2376-7669 (Print); ISSN: 2376-7677(Online)
More informationTwo-step multiscale homogenization of polymer nanocomposites for large size RVEs embodying many nanoparticles
Two-step multiscale homogenization of polymer nanocomposites for large size RVEs embodying many nanoparticles *Kyungmin Baek 1), Hyunseong Shin 2), Jin-Gyu Han 3) and Maenghyo Cho 4) 1), 2), 3), 4) Department
More informationViscoelasticity, Creep and Oscillation Experiment. Basic Seminar Applied Rheology
Viscoelasticity, Creep and Oscillation Experiment Basic Seminar Applied Rheology Overview Repetition of some basic terms Viscoelastic behavior Experimental approach to viscoelasticity Creep- and recovery
More information