Free volume and internal structural evolution during creep in model amorphous polyethylene by Molecular Dynamics simulations

被引:50
作者
Bowman, A. L. [1 ,6 ]
Mun, S. [1 ]
Nouranian, S. [2 ]
Huddleston, B. D. [1 ,6 ]
Gwaltney, S. R. [3 ]
Baskes, M., I [4 ,5 ]
Horstemeyer, M. F. [7 ]
机构
[1] Mississippi State Univ, CAVS, Mississippi State, MS 39762 USA
[2] Univ Mississippi, Dept Chem Engn, University, MS 38677 USA
[3] Mississippi State Univ, Dept Chem, Mississippi State, MS 39762 USA
[4] Mississippi State Univ, Off Res & Econ Dev, Mississippi State, MS 39762 USA
[5] Los Alamos Natl Lab, Los Alamos, NM 87545 USA
[6] Mississippi State Univ, Dept Mech Engn, Mississippi State, MS 39762 USA
[7] Liberty Univ, Sch Engn, Lynchburg, VA 24515 USA
关键词
Molecular dynamics; Voids; Creep; Damage; Chain dynamics; EMBEDDED-ATOM-METHOD; MECHANICAL-PROPERTIES; TEMPERATURE-DEPENDENCE; GLASS-TRANSITION; UNITED ATOM; TOPOLOGICAL ANALYSIS; PLASTIC-DEFORMATION; NONLINEAR CREEP; FORCE-FIELD; VOID GROWTH;
D O I
10.1016/j.polymer.2019.02.060
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
All-atom Molecular Dynamics (MD) simulations were employed to investigate the structural and free volume evolution (correlated with damage) during creep of model amorphous polyethylene (PE) at various applied stress states (tension, shear, compression), stress levels (10-200 MPa), and temperatures (175-325 K). The Modified Embedded-Atom Method for saturated hydrocarbons is applied to show that the phenomenological macroscale creep response of PE can be captured through MD simulations. The model adequately predicts the three classical stages of creep (primary, secondary, and tertiary) and provides detailed insight into the underlying molecular mechanisms. The calculated glass transition temperature (T-g) was found to be very close to the experimental T-g. Simulations were performed at temperatures below T-g (175 K) to above T-g (325 K) and demonstrate that the transition from glassy to rubbery state is reflected in the chain dynamics and damage evolution. Under all the stress states and temperatures simulated, the evolution of void volume, nucleation, growth, and coalescence are shown to directly correlate with specific stages of the creep response and the underlying chain dynamics within each stage. A correlation between the steady-state creep rate and steady-state void nucleation rate is found, suggesting that secondary creep is heavily driven by void nucleation, while tertiary creep is driven by void growth and coalescence.
引用
收藏
页码:85 / 100
页数:16
相关论文
共 98 条
[11]   Molecular response of a glassy polymer to active deformation [J].
Capaldi, FM ;
Boyce, MC ;
Rutledge, GC .
POLYMER, 2004, 45 (04) :1391-1399
[12]  
Chandler Mei Qiang, 2013, CONTINUUM MODEL HYDR, V21, P55028, DOI [10.1088/0965-0393/21/5/055028, DOI 10.1088/0965-0393/21/5/055028]
[13]  
Chehab A. G., 2006, PIPELINE DIV SPEC C, V1, P762, DOI [10.1061/40854(211)87, DOI 10.1061/40854(211)87]
[14]   MOLECULAR TRANSPORT IN LIQUIDS AND GLASSES [J].
COHEN, MH ;
TURNBULL, D .
JOURNAL OF CHEMICAL PHYSICS, 1959, 31 (05) :1164-1169
[15]   Internal state variable plasticity-damage modeling of the copper tee-shaped tube hydroforming process [J].
Crapps, J. ;
Marin, E. B. ;
Horstemeyer, M. F. ;
Yassar, R. ;
Wang, P. T. .
JOURNAL OF MATERIALS PROCESSING TECHNOLOGY, 2010, 210 (13) :1726-1737
[16]   GLASS TRANSITION OF POLYETHYLENE - VOLUME RELAXATION [J].
DAVIS, GT ;
EBY, RK .
JOURNAL OF APPLIED PHYSICS, 1973, 44 (10) :4274-4281
[17]   EMBEDDED-ATOM METHOD - DERIVATION AND APPLICATION TO IMPURITIES, SURFACES, AND OTHER DEFECTS IN METALS [J].
DAW, MS ;
BASKES, MI .
PHYSICAL REVIEW B, 1984, 29 (12) :6443-6453
[18]  
Deng M, 1998, J BIOMED MATER RES, V40, P214, DOI 10.1002/(SICI)1097-4636(199805)40:2<214::AID-JBM6>3.3.CO
[19]  
2-M
[20]   STUDIES IN NEWTONIAN FLOW .2. THE DEPENDENCE OF THE VISCOSITY OF LIQUIDS ON FREE-SPACE [J].
DOOLITTLE, AK .
JOURNAL OF APPLIED PHYSICS, 1951, 22 (12) :1471-1475