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Rock Mechanics.pdf - Mining and Blasting

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BEHAVIOUR OF ISOTROPIC ROCK MATERIAL IN UNIAXIAL COMPRESSION<br />

Yield occurs when there is a departure from elastic behaviour, i.e. when some of<br />

the deformation becomes irrecoverable as at A in Figure 4.2a. The yield stress (y in<br />

Figure 4.2) is the stress at which permanent deformation first appears.<br />

Failure is often said to occur at the peak strength or be initiated at the peak strength<br />

(Jaeger <strong>and</strong> Cook, 1979). An alternative engineering approach is to say that the rock<br />

has failed when it can no longer adequately support the forces applied to it or otherwise<br />

fulfil its engineering function. This may involve considerations of factors other than<br />

peak strength. In some cases, excessive deformation may be a more appropriate<br />

criterion of ‘failure’ in this sense.<br />

Effective stress is defined, in general terms, as the stress which governs the gross<br />

mechanical response of a porous material. The effective stress is a function of the<br />

total or applied stress <strong>and</strong> the pressure of the fluid in the pores of the material,<br />

known as the pore pressure or pore-water pressure. The concept of effective stress<br />

was first developed by Karl Terzaghi who used it to provide a rational basis for the<br />

underst<strong>and</strong>ing of the engineering behaviour of soils. Terzaghi’s formulation of the<br />

law of effective stress, an account of which is given by Skempton (1960), is probably<br />

the single most important contribution ever made to the development of geotechnical<br />

engineering. For soils <strong>and</strong> some rocks loaded under particular conditions, the effective<br />

stresses, ′<br />

ij , are given by<br />

′<br />

ij = ij − uij<br />

(4.1)<br />

where ij are the total stresses, u is the pore pressure, <strong>and</strong> ij is the Kronecker delta.<br />

This result is so well established for soils that it is often taken to be the definition of<br />

effective stress. Experimental evidence <strong>and</strong> theoretical argument suggest that, over a<br />

wide range of material properties <strong>and</strong> test conditions, the response of rock depends<br />

on<br />

′<br />

ij = ij − uij<br />

where 1, <strong>and</strong> is a constant for a given case (Paterson, 1978).<br />

4.3 Behaviour of isotropic rock material in uniaxial compression<br />

(4.2)<br />

4.3.1 Influence of rock type <strong>and</strong> condition<br />

Uniaxial compression of cylindrical specimens prepared from drill core, is probably<br />

the most widely performed test on rock. It is used to determine the uniaxial or<br />

unconfined compressive strength, c, <strong>and</strong> the elastic constants, Young’s modulus,<br />

E, <strong>and</strong> Poisson’s ratio, , of the rock material. The uniaxial compressive strength<br />

of the intact rock is used in rock mass classification schemes (section 3.7), <strong>and</strong> as<br />

a basic parameter in the rock mass strength criterion to be introduced later in this<br />

chapter.<br />

Despite its apparent simplicity, great care must be exercised in interpreting results<br />

obtained in the test. Obviously, the observed response will depend on the nature <strong>and</strong><br />

composition of the rock <strong>and</strong> on the condition of the test specimens. For similar mineralogy,<br />

c will decrease with increasing porosity, increasing degree of weathering <strong>and</strong><br />

increasing degree of microfissuring. As noted in section 1.2.4, c may also decrease<br />

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