Effect of sample dimensions, lubrication and deformation rate on uniaxial compression of gelatin gels

1985 ◽  
Vol 24 (3) ◽  
pp. 265-271 ◽  
Author(s):  
E. B. Bagley ◽  
W. J. Wolf ◽  
D. D. Christianson
Keyword(s):  
Uniaxial Compression ◽  
Deformation Rate ◽  
Gelatin Gels

Effect of deformation rate on the stress-strain curves of gelatin gels

1996 ◽  
Vol 93 ◽  
pp. 837-849 ◽  
Author(s):  
A Bot ◽  
IA van Amerongen ◽  
RD Groot ◽  
NL Hoekstra ◽  
WGM Agterof
Keyword(s):  
Deformation Rate ◽  
Stress Strain ◽  
Gelatin Gels

scholarly journals Deformation Behavior of Human Dentin under Uniaxial Compression

2012 ◽  
Vol 2012 ◽  
pp. 1-8 ◽  
Author(s):  
Dmitry Zaytsev ◽  
Sergey Grigoriev ◽  
Peter Panfilov
Keyword(s):  
Mechanical Properties ◽  
Crack Growth ◽  
Uniaxial Compression ◽  
Deformation Behavior ◽  
Deformation Rate ◽  
Hard Tissue ◽  
Rate Effects ◽  
Human Dentin ◽  
Root Dentin

Deformation behavior of a human dentin under compression including size and rate effects is studied. No difference between mechanical properties of crown and root dentin is found. It is mechanically isotropic high elastic and strong hard tissue, which demonstrates considerable plasticity and ability to suppress a crack growth. Mechanical properties of dentin depend on a shape of samples and a deformation rate.

Atomistic simulation of the uniaxial compression of black phosphorene nanotubes

2018 ◽  
Author(s):  
Van-Trang Nguyen ◽  
Minh-Quy Le
Keyword(s):  
Finite Element Method ◽  
Molecular Dynamics ◽  
Finite Element ◽  
Uniaxial Compression ◽  
Critical Stress ◽  
Atomistic Simulation ◽  
Critical Strain ◽  
Bond Breaking ◽  
Black Phosphorene ◽  
Weber Potential

We study through molecular dynamics finite element method with Stillinger-Weber potential the uniaxial compression of (0, 24) armchair and (31, 0) zigzag black phosphorene nanotubes with approximately equal diameters. Young's modulus, critical stress and critical strain are estimated with various tube lengths. It is found that under uniaxial compression the (0, 24) armchair black phosphorene nanotube buckles, whereas the failure of the (31, 0) zigzag one is caused by local bond breaking near the boundary.

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