Approximation of the plastic zone by circular arcs during the sliding of a cylinder on the rigid-plastic half-space

Author(s):  
Anastasia A. Bukhanko ◽  
Svetlana A. Ovchinnikova
2017 ◽  
Vol 09 (03) ◽  
pp. 1750036 ◽  
Author(s):  
Jing Yang ◽  
Kun Zhou

The plastic zones at crack tips play a significant role in fracture behaviors of materials. In this paper, a semi-analytic solution is proposed for the plastic zone size of cracks in an elastic-perfectly plastic half-space under prescribed loading. This solution also considers the subsurface stress distribution influenced by the plastic zones at crack tips. The cracks can be treated as a distribution of edge dislocations with unknown densities by using the distributed dislocation technique. In order to calculate the plastic zone sizes of crack tips, two stripes ahead of crack tips are introduced as plastic zones based on the Dugdale model of small scale yielding. The numerical values can be determined by canceling the stress intensity factor due to the closure stress and that due to the applied load. It is noted that the plastic zone sizes are affected by the crack length and depth, yield strength of substrates and loading conditions.


1992 ◽  
Vol 59 (4) ◽  
pp. 706-710 ◽  
Author(s):  
David Durban ◽  
Norman A. Fleck

The essential features of the active plastic zone at the tip of a penetrating rigid cone are investigated for a rigid/perfectly plastic solid. An exact solution is suggested for the plastic zone. A rigid zone exists ahead of the cone and is separated from the plastic zone by a conical surface of discontinuity. It is assumed that the material yields instantaneously by going through a “shear shock” across the rigid/plastic interface. The orientation of the interface is determined by an ad hoc requirement for minimum shear strain jump at the shear shock. Results are presented for different cone angles and friction factors. The stresses within the plastic zone admit a logarithmic singularity whose level increases with cone angle and wall friction.


2000 ◽  
Vol 627 ◽  
Author(s):  
Prabhu R. Nott ◽  
K. Kesava Rao ◽  
L. Srinivasa Mohan

ABSTRACTThe slow flow of granular materials is often marked by the existence of narrow shear layers, adjacent to large regions that suffer little or no deformation. This behaviour, in the regime where shear stress is generated primarily by the frictional interactions between grains, has so far eluded theoretical description. In this paper, we present a rigid-plastic frictional Cosserat model that captures thin shear layers by incorporating a microscopic length scale. We treat the granular medium as a Cosserat continuum, which allows the existence of localised couple stresses and, therefore, the possibility of an asymmetric stress tensor. In addition, the local rotation is an independent field variable and is not necessarily equal to the vorticity. The angular momentum balance, which is implicitly satisfied for a classical continuum, must now be solved in conjunction with the linear momentum balances. We extend the critical state model, used in soil plasticity, for a Cosserat continuum and obtain predictions for flow in plane and cylindrical Couette devices. The velocity profile predicted by our model is in qualitative agreement with available experimental data. In addition, our model can predict scaling laws for the shear layer thickness as a function of the Couette gap, which must be verified in future experiments. Most significantly, our model can determine the velocity field in viscometric flows, which classical plasticity-based model cannot.


2015 ◽  
Vol 37 (4) ◽  
pp. 303-315 ◽  
Author(s):  
Pham Chi Vinh ◽  
Nguyen Thi Khanh Linh ◽  
Vu Thi Ngoc Anh

This paper presents  a technique by which the transfer matrix in explicit form of an orthotropic layer can be easily obtained. This transfer matrix is applicable for both the wave propagation problem and the reflection/transmission problem. The obtained transfer matrix is then employed to derive the explicit secular equation of Rayleigh waves propagating in an orthotropic half-space coated by an orthotropic layer of arbitrary thickness.


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