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Ultimate bearing capacity of an anisotropic discontinuous rock mass. Part I: Basic modes of failure

✍ Scribed by Serrano, A. ;Olalla, C.


Publisher
Elsevier Science
Year
1998
Tongue
English
Weight
567 KB
Volume
35
Category
Article
ISSN
0148-9062

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✦ Synopsis


The existence of a transverse strength isotropy concerning the strength in rock media due to the presence of a family of planes of weakness superimposed within an isotropic rock mass is considered. Six dierent mechanisms of failure are possible under a foundation depending on the boundary conditions and the orientation of the transverse isotropy. The theoretical bases for the determination of the ultimate load of a strip foundation on a rock mass are obtained, respectively, for the six dierent mechanisms. The following assumptions are adopted: (a) a non-linear behaviour through the rock mass, de®ned by the Hoek and Brown model (parameters m, s and the uncon®ned compressive strength, respectively) and (b) a linear strength behaviour along the planes of weakness, de®ned by their cohesion and angle of internal friction.


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Ultimate bearing capacity of an anisotro
✍ Serrano, A. ;Olalla, C. 📂 Article 📅 1998 🏛 Elsevier Science 🌐 English ⚖ 523 KB

Based on the six possible and dierent failure mechanisms de®ned in part I, a criterion to identify which is the particular failure mechanism is developed. The rock mass is assumed to have transverse isotropic strength. The particular mechanism depends on the geometrical situation, the geomechanical