The role of elastic deformation in the adhesion of solids

1978 ◽  
Vol 64 (3) ◽  
pp. 577-579 ◽  
Author(s):  
A.E Lee
Keyword(s):  
1951 ◽  
Vol 24 (2) ◽  
pp. 336-343
Author(s):  
B. A. Dogadkin ◽  
G. M. Bartenev ◽  
M. M. Reznikovskii˘

Abstract 1. The molecular mechanism of the relaxation of deformation of high-elastic polymers has been studied. 2. It is shown that the slow relaxation, which is typical of high-elastic polymers, may be best explained as a restoration process, which either partial or complete (depending on the degree of development of side chains in the molecular structure formed by the main valence chains) of the balanced configurations of the molecular chains. 3. It is shown that the rate of the relaxation process in this case is determined by the molecular activity of the particular polymer. 4. An approximate equation for the kinetics of high-elastic deformation which expresses qualitatively the mechanical properties of high-elastic polymers is proposed. 5. Hypotheses concerning the relation between the time of relaxation and the unbalanced stress are advanced. Equation (2) is derived as characteristic of this relation. 6. It is shown that the joint application of Equations (1) and (2) makes it possible to describe qualitatively the relaxation of stress at constant deformation.


1983 ◽  
Vol 105 (4) ◽  
pp. 509-511 ◽  
Author(s):  
M. M. Carroll ◽  
N. Katsube

It has been shown that the overall strain of a fluid-filled porous elastic solid is not governed by the Terzaghi effective stress law. We show, in the context of anisotropic linear elasticity, that the overall strain may be resolved into a component which is the average strain of the solid matrix and a component due to change in relative pore geometry, and that the latter is determined by the Terzaghi effective stress. This leads to a simple form of the response laws and, in particular, to effective stress laws for overall strain (obtained previously) and for strain of the pore space.


2021 ◽  
Vol 2 (1) ◽  
Author(s):  
Julia Christmann ◽  
Veit Helm ◽  
Shfaqat Abbas Khan ◽  
Thomas Kleiner ◽  
Ralf Müller ◽  
...  

AbstractFuture projections of global mean sea level change are uncertain, partly because of our limited understanding of the dynamics of Greenland’s outlet glaciers. Here we study Nioghalvfjerdsbræ, an outlet glacier of the Northeast Greenland Ice Stream that holds 1.1 m sea-level equivalent of ice. We use GPS observations and numerical modelling to investigate the role of tides as well as the elastic contribution to glacier flow. We find that ocean tides alter the basal lubrication of the glacier up to 10 km inland of the grounding line, and that their influence is best described by a viscoelastic rather than a viscous model. Further inland, sliding is the dominant mechanism of fast glacier motion, and the ice flow induces persistent elastic strain. We conclude that elastic deformation plays a role in glacier flow, particularly in areas of steep topographic changes and fast ice velocities.


2017 ◽  
Vol 120 (3) ◽  
pp. 36002 ◽  
Author(s):  
A.G. Akulichev ◽  
A. Tiwari ◽  
L. Dorogin ◽  
A. T. Echtermeyer ◽  
B. N. J. Persson

1978 ◽  
Vol 44 (518) ◽  
pp. 155-160
Author(s):  
Seiki MATSUI ◽  
Katsuo SYOJI ◽  
Masafumi MORIMURA ◽  
Kenji TANAKA
Keyword(s):  

2013 ◽  
Vol 577 ◽  
pp. S404-S407 ◽  
Author(s):  
Masaki Tahara ◽  
Hee Young Kim ◽  
Tomonari Inamura ◽  
Hideki Hosoda ◽  
Shuichi Miyazaki

2019 ◽  
Vol 126 ◽  
pp. 245-255 ◽  
Author(s):  
Wenbin Liu ◽  
Lirong Chen ◽  
Yangyang Cheng ◽  
Long Yu ◽  
Xin Yi ◽  
...  

1951 ◽  
Vol 24 (2) ◽  
pp. 344-353
Author(s):  
B. A. Dogadkin ◽  
V. Gul

Abstract 1. The construction of an apparatus (elastometer) for the mechanical investigation of high elastic substances is described. This apparatus makes it possible to draw deformation curves and curves of the relaxation of stress atconstant temperature and in different gaseous media, and also to investigate the life at multiple deformations. The sensitivity of the apparatus is: ΔP=0.01 g., Δl=0.01 cm. 2. The molecular weight of the segments of the chains between the bonds of the spatial network of the vulcanizate, calculated by means of Flory's equation, increases with swelling, and approaches a certain maximum value. This is evidence of the rupture of the local intermolecular bonds on swelling. 3. The maximum time of relaxation, calculated according to the equation of Dogadkin, Bartenev, and Reznikovskil, as a consequence of swelling, generally does not change uniformly; it decreases with swelling of natural rubbers in benzene and chloroform in the initial stages, then increases, and finally decreases again in the last stages of swelling. 4. An increase of temperature displaces the minimum times of relaxation to lower degrees of swelling. 5. The increase of the maximum time of relaxation as a result of swelling causes a decrease of the life of the vulcanizate; a decrease of this factor is accompanied, at least within certain limits, by an increase of life. 6. Swelling causes a decrease of tensile strength and of the relative elongation of vulcanizates. 7. The changes recorded above in the equilibrium and kinetic characteristics of high elastic deformation are explained by the presence in the vulcanizate of different intermolecular bonds.


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