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1 -z- <br />' Slopes containing weak rock zones may be stabilized by <br />slope flattening or incorporating step-outs. The forces is used <br />when designing the slopes, and the latter when unexpec~ed weak <br />rock zones are encountered during mining. <br />' INTRODUCTION <br />The rock mass classification methods described in this <br />~. paper evolved on projects undertaken by the consulting fire <br />Steffen, Robertson and Kirsten (SRK). Back analysis of failed <br />slopes involving rock mass materials which have been described <br />' by the SRK classification has enabled rock mass strengths to be <br />~ assigned to the various class intervals. Much of the initial <br />work in the development oP this technique was done by personnel <br />' Prom the Island Copper Mine, BHP-Utah Mines, Port Hardy, British <br />Columbia, to whom much of the credit goes for turning it into an <br />effective technique. <br />' FACTORS CONTROLLING THE STRENGTH OF WEAR ROCF: MASSES <br />Weak rock masses may occur as a result of a number of <br />' independent factors. These are illustrated in Figure 1. <br />it Weak rock material ~Fiaure 1(i)1 <br />' ' Where the sole reason far a weak rock mass strength is the <br />low strength of the rock material it is more properly classified <br />as having a sail like strength. An anaronriate classification <br />~ ' for rock and soil, based on simple tests, from which an estimate <br />can be made of the uniaxial compressive strength is given in <br />Table 1 (Jennings and Robertson, 1969). Extremely weak "rocks", <br />or more properly materials with a soil strength but a rock <br />'. appearance, can be tested in the laboratory to deteraine the <br />shear strength. Such material may be referred to as either <br />~, soils or rocks but use of the strength qualifies S1 to S5, as <br />indicated on Table 1, serves to indicate that their strength <br />falls into the soil classification. <br />t iil Intense Jointing (Figure 1(ii)) <br />Where the jointing is sufficiently intense and has a <br />' sufficient range of orientations, a stenned failure surface can <br />develop througri the mass, at any orientation, with a resu:.taut <br />low shear strength. Thus while the jointing may be non- <br />isotropic, the shear strength may be considerably less so. The <br />' spacing between joints may be sufficiently large that it ~.s <br />impractical to select a laboratory scale specimen which is <br />representative. The difficulty of cutting and preparing a~ <br />specimen without disturbing the joints and effecting the shear <br />strength of the specimen is an additional impediment to such <br />testing. <br />1 <br />1 <br />1 <br />