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For each stage of normal stress the shearing displacement was 2 mm.
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For materials with a crystalline structure, these shearing displacements are usually associated with defects within the crystal lattice.
Under greater deformation, such elastic solids exhibit either brittleness (in which the internal elastic forces are broken down) or ductility (in which certain internal mechanisms permit shearing displacements to occur within the atomic structure).
Roosta et al. (2006) developed a visco-plastic multilaminate model to model the shear stress-shear displacement and normal displacement shear displace of artificial joint specimen at constant normal load conditions.
Fig. 4 Shear displacement under the track.
(a) normal stress, shear resistance and shear displacement (b) pore-water pressure, shear resistance and shear displacement.
For an applied normal stress, shear displacement increases until the maximum shear stress is reached.
Figure 1 Typical evolution of the coefficient of friction with shear displacement.
Figure 17 Analytical results of flow through the fracture and shear displacement.
The shear displacement was corrected with machine stiffness (4.4 × 108 N/m).
The mobilized friction as a function of shear displacement was also calculated and plotted.
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