What is so exciting about non-linear viscous flow in glass, molecular dynamics simulations of brittle fracture and semiconductor–glass quantum composites

1998 ◽  
Vol 239 (1-3) ◽  
pp. 1-15 ◽  
Author(s):  
Joseph H. Simmons
2007 ◽  
Vol 42 (12) ◽  
pp. 4159-4169 ◽  
Author(s):  
Krishna Muralidharan ◽  
Ki-Dong Oh ◽  
P. A. Deymier ◽  
K. Runge ◽  
J. H. Simmons

2019 ◽  
Vol 21 (40) ◽  
pp. 22188-22202 ◽  
Author(s):  
Simone Pezzotti ◽  
Daria Ruth Galimberti ◽  
Marie-Pierre Gaigeot

Through the prism of the rather controversial and elusive silica/water interface, ab initio DFT-based molecular dynamics simulations of the structure and non-linear SFG spectroscopy of the interface are analysed.


2011 ◽  
Vol 1301 ◽  
Author(s):  
Abhishek Singh ◽  
Yaroslava G. Yingling

ABSTRACTMolecular dynamics simulations were performed to estimate sequence dependent force required to stretch single stranded DNA (ssDNA) homo oligonucleotides. Simulations suggest that polyA and polyC oligonucleotides exhibit similar force profiles and corresponding elongation. Among single stranded DNA strands polyT is the most flexible and needs the most force to unwind from an equilibrium folded structure. In contrast, polyG had a very small recoverable deformation prior to a non-linear stretching. Our results indicate that mechanical properties of ssDNA chains are directly related to their sequence.


Soft Matter ◽  
2021 ◽  
Author(s):  
Gaurav Prakash Shrivastav ◽  
Gerhard Kahl

In real crystals and at finite temperatures point defects are inevitable. Under shear their dynamics severely influence the mechanical properties of these crystals, giving rise to non-linear effects, such as...


1995 ◽  
Vol 409 ◽  
Author(s):  
Pep Español ◽  
Miguel A. Rubio ◽  
Ignacio Zúñiga

AbstractWe present results obtained by molecular dynamics simulations on the propagation of fast cracks in triangular 2D lattices. Our aim is to simulate Mode I fracture of brittle isotropic materials. We propose a force law that respects the isotropy of the material. The code yields the correct imposed sound c║, shear c┴ and surface VR wave speeds. Different notch lengths are systematically studied. We observe that initially the cracks are linear and always branch at a particular critical velocity c* ≈0.8VR and that this occurs when the crack tip reaches the position of a front emitted from the initial crack tip and propagating at a speed c = 0.6 8VR.


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