2019
DOI: 10.1016/j.polymer.2019.03.006
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Molecular mechanism of material deformation and failure in butadiene rubber: Insight from all-atom molecular dynamics simulation using a bond breaking potential model

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Cited by 33 publications
(10 citation statements)
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“…comparable with that described above to account for the longer relaxation time of the crosslinked PB compared with the non-crosslinked PB. Moreover, in Area II, it was assumed that hi decreases due to the partial release of constraint in the polymer chain motion, which in turn is caused by unraveling of the polymer chain entanglement (Yashiro et al, 2003;Mahajan et al, 2010) or the occurrence of nano-voids (Payal et al, 2019), as predicted by molecular dynamics simulations. Another interpretation is that the degree of polymer fracture occurring under elongation conditions accelerates the molecular dynamics.…”
Section: Resultsmentioning
confidence: 99%
“…comparable with that described above to account for the longer relaxation time of the crosslinked PB compared with the non-crosslinked PB. Moreover, in Area II, it was assumed that hi decreases due to the partial release of constraint in the polymer chain motion, which in turn is caused by unraveling of the polymer chain entanglement (Yashiro et al, 2003;Mahajan et al, 2010) or the occurrence of nano-voids (Payal et al, 2019), as predicted by molecular dynamics simulations. Another interpretation is that the degree of polymer fracture occurring under elongation conditions accelerates the molecular dynamics.…”
Section: Resultsmentioning
confidence: 99%
“…The growth of voids (or excess volume) is another useful indicator for the structural evolution of the polymer nanocomposites under deformation. , Here, we define the excess volume fraction of the system as the volume outside the vdW radius of all constituent atoms. Here, vdW radii of 1.7, 1.5, and 1.2 Å are adopted for the C-, O-, and H-atoms, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…After equilibration, uniaxial tensile deformation is performed to obtain the stress–strain (σ T –ε T ) curves in the CGMD simulations, which was also utilized in our previous studies. , The simulation box is stretched in the Z -direction at a constant engineering strain rate ε̇ T (eq ), while the lengths in the X -directions and Y -directions are decreased to keep the volume of the simulation box constant. where L Z ( t ) and L Z (0) are the box length in the Z -direction at time t and at the beginning, and ε T is the tensile strain. The strain rate is set to 10 –9 /s . The tensile stress is expressed through the bias tensor of the pressure as where represents the isostatic pressure of the system, and ν represents the Poisson ratio of the system.…”
Section: Models and Methodsmentioning
confidence: 99%
“…The strain rate is set to 10 −9 /s. 49 The tensile stress is expressed through the bias tensor of the pressure as 50…”
Section: Models and Methodsmentioning
confidence: 99%