Abstract
True persistence of rock discontinuities (areas with insignificant tensile strength) is an important factor controlling the engineering behaviour of fractured rock masses, but is extremely difficult to quantify using current geological survey methodologies, even where there is good rock exposure. Trace length as measured in the field or using remote measurement devices is actually only broadly indicative of persistence for rock engineering practice and numerical modelling. Visible traces of discontinuities are treated as if they were open fractures within rock mass classifications, despite many such traces being non-persistent and actually retaining considerable strength. The common assumption of 100% persistence, based on trace length, is generally extremely conservative in terms of strength and stiffness, but not always so and may lead to a wrong prediction of failure mechanism or of excavatability. Assuming full persistence would give hopelessly incorrect predictions of hydraulic conductivity. A new technique termed forensic excavation of rock masses is introduced, as a procedure for directly investigating discontinuity persistence. This technique involves non-explosive excavation of rock masses by injecting an expansive chemical splitter along incipient discontinuities. On expansion, the splitter causes the incipient traces to open as true joints. Experiments are described in which near-planar rock discontinuities, through siltstone and sandstone, were opened up by injecting the splitter into holes drilled along the lines of visible traces of the discontinuities in the laboratory and in the field. Once exposed the surfaces were examined to investigate the pre-existing persistence characteristics of the incipient discontinuities. One conclusion from this study is that visible trace length of a discontinuity can be a poor indicator of true persistence (defined for a fracture area with negligible tensile strength). An observation from this series of experiments was that freshly failed surfaces through pre-existing rock bridges were relatively rough compared to sections of pre-existing weaker areas of geologically developed (though still incipient) discontinuities. Fractographic features such as hackle and rib marks were typical of the freshly broken rock bridges, whereas opened-up areas of incipient discontinuity were smoother. Schmidt hammer rebound values were generally higher for the rock bridge areas, probably reflecting their lower degree of chemical and physical weathering.
Highlights
Persistence is defined as the areal extent of a rock discontinuity (ISRM 1978)
Often only a small area of discontinuity is fully open and lacks significant tensile strength; much of the area represented by a visible discontinuity in exposures is incipient and maintains considerable shear and tensile strength; the third section, that maintains the geometry of the discontinuity, but without visible trace, comprises true ‘rock bridges’ in the sense of intact rock with no incipient geological weakness (Hencher 2014, 2015)
Laboratory- and field-based FERM experiments on two lithologies were performed as application examples
Summary
Persistence is defined as the areal extent of a rock discontinuity (ISRM 1978). Its implications for the strength of rock masses and their stability in rock engineering are obvious (e.g. Kemeny 2005), but this property is extremely difficult to determine in practice (e.g. O’Reilly 1980; Einstein and Baecher 1983; Park 2005; Kim et al 2007; Wasantha et al 2011; Bonilla-Sierra et al 2015; Tucky andStead 2016). The true cohesion measured from shearing the rock bridge was about 0.75 MPa (pro rata for the rock bridge area) which, significant, is small compared to what one might expect for intact slightly decomposed crystal tuff (in excess of 10 MPa). This indicates that the ‘bridge’ itself had some pre-existing (micro-fracturing) damage associated with original geological discontinuity propagation; it is evident that the ‘proto-joint’ has been gradually weathered and weakened (Hencher 2006), towards the condition where it would eventually become a true, through-going ‘joint’, lacking significant tensile strength as defined by ISRM (1978)
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