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Rock Mechanics.pdf - Mining and Blasting

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Figure 6.5 Superposition scheme<br />

demonstrating that generation of an<br />

excavation is mechanically equivalent<br />

to introducing a set of tractions on a<br />

surface in a continuum.<br />

Figure 6.6 Surface, element <strong>and</strong><br />

load distribution description for development<br />

of a quadratic, indirect boundary<br />

element formulation.<br />

METHODS OF STRESS ANALYSIS<br />

induced traction distribution is shown in Figure 6.5c. Superposition of Figures 6.5a<br />

<strong>and</strong> c confirms that their resultant is a stressed medium with an internal traction-free<br />

surface S. It is concluded from this that if a procedure is established for solving the<br />

problem illustrated in Figure 6.5c, the solution to the real problem (Figure 6.5b) is<br />

immediately available. Thus the following discussion deals with excavation-induced<br />

tractions, displacements <strong>and</strong> stresses, <strong>and</strong> the method of achieving particular induced<br />

traction conditions on a surface in a continuum.<br />

For a medium subject to general biaxial stress, the problem posed involves distributions<br />

of induced tractions, tx(S), ty(S), at any point on the surface S, as illustrated in<br />

Figure 6.6a. In setting up the boundary element solution procedure, the requirements<br />

are to discretise <strong>and</strong> describe algebraically the surface S, <strong>and</strong> to find a method of<br />

satisfying the imposed induced traction conditions on S.<br />

The geometry of the problem surface S is described conveniently in terms of the<br />

position co-ordinates, relative to global x, y axes, of a set of nodes, or collocation<br />

points, disposed around S. Three adjacent nodes, forming a representative boundary<br />

element of the surface S, are shown in Figure 6.6b. The complete geometry of this<br />

element of the surface may be approximated by a suitable interpolation between the<br />

position co-ordinates of the nodes. In Figure 6.6b an element intrinsic co-ordinate is<br />

defined, with the property that −1 ≤ ≤ 1 over the range of the element. Considering<br />

180

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