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International Journal of Rock Mechanics and Mining SciencesAnalysis of geo-structural defects in flexural toppling failure Abbas Majdi and Mehdi AminiAbstractThe in-situ rock structural weaknesses, referred to herein as geo-structural defects, such as naturally induced micro-cracks, are extremely responsive to tensile stresses. Flexural toppling failure occurs by tensile stress caused by the moment due to the weight of the inclined superimposed cantilever-like rock columns. Hence, geo-structural defects that may naturally exist in rock columns are modeled by a series of cracks in maximum tensile stress plane. The magnitude and location of the maximum tensile stress in rock columns with potential flexural toppling failure are determined. Then, the minimum factor of safety for rock columns are computed by means of principles of solid and fracture mechanics, independently. Next, a new equation is proposed to determine the length of critical crack in such rock columns. It has been shown that if the length of natural crack is smaller than the length of critical crack, then the result based on solid mechanics approach is more appropriate; otherwise, the result obtained based on the principles of fracture mechanics is more acceptable. Subsequently, for stabilization of the prescribed rock slopes, some new analytical relationships are suggested for determination the length and diameter of the required fully grouted rock bolts. Finally, for quick design of rock slopes against flexural toppling failure, a graphical approach along with some design curves are presented by which an admissible inclination of such rock slopes and or length of all required fully grouted rock bolts are determined. In addition, a case study has been used for practical verification of the proposed approaches.Keywords Geo-structural defects, In-situ rock structural weaknesses, Critical crack length1. IntroductionRock masses are natural materials formed in the course of millions of years. Since during their formation and afterwards, they have been subjected to high variable pressures both vertically and horizontally, usually, they are not continuous, and contain numerous cracks and fractures. The exerted pressures, sometimes, produce joint sets. Since these pressures sometimes may not be sufficiently high to create separate joint sets in rock masses, they can produce micro joints and micro-cracks. However, the results cannot be considered as independent joint sets. Although the effects of these micro-cracks are not that pronounced compared with large size joint sets, yet they may cause a drastic change of in-situ geomechanical properties of rock masses. Also, in many instances, due to dissolution of in-situ rock masses, minute bubble-like cavities, etc., are produced, which cause a severe reduction of in-situ tensile strength. Therefore, one should not replace this in-situ strength by that obtained in the laboratory. On the other hand, measuring the in-situ rock tensile strength due to the interaction of complex parameters is impractical. Hence, an appropriate approach for estimation of the tensile strength should be sought. In this paper, by means of principles of solid and fracture mechanics, a new approach for determination of the effect of geo-structural defects on flexural toppling failure is proposed. 2. A brief review of previous workConsiderable research has been performed in the field of flexural toppling failure 1, 2, 3, 4, 5, 6, 7, 8, 9 and 10. The first applied research was due to Goodman and Bray 2. These researchers proposed the indispensable condition for flexural toppling failure. In 1987, Aydan and Kawamoto, by employing the equations of limit equilibrium and the boundary conditions, proposed an equation for determination of inter-column forces of rock masses in open excavations and underground openings environment 5. They verified the method by carrying out laboratory base friction modeling. On the basis of these experiments, the total failure plane of flexural toppling is normal to the discontinuities. Hence, the angle between the total failure plane and the normal to the discontinuities is zero. It is also seen that they assumed that if the rock layers are stable under a given load condition in the upper part, the inter-column forces will be zero. Based on the aforementioned assumptions the factor of safety of all rock columns should be computed and consequently the extension of total failure plane can be determined. Adhikary et al., by carrying centrifuge modeling, made some changes to Aydan and Kawamotos equation for flexural toppling failure in open excavations 7, 8 and 9. On the basis of these experiments, the total failure plane of flexural toppling failure is around 10 above normal to the discontinuities. In 2008, Majdi and Amini 10 and Amini et al. 11, using the principles of compatibility and the equations of equilibrium along with the governing equations to elastic deformation for the beams, derived equations for determination inter-column forces in rock masses with potential of flexural toppling failure. The aforementioned researchers proved that the minimum factor of safety against toppling failure is equal to the factor of safety of a cantile： = (1) (2)where is the calculated lengths of rock columns used for computation of inter columns resultant force, C is a dimensionless geometrical parameter, H is the height of the slope, is the dip angle of the rock mass governing discontinuities, is the angle between total failure plane and the line normal to governing discontinuities, is the slope angle from slope face clockwise to horizontal, is the unit weight of intact rock, and is the slope angle from slope face counterclockwise to horizon and equal to 180.Hence, the factor of safety of rock columns against flexural toppling failure is computed by means of the following equation 10 and 11: （3）where t is the thickness of rock columns,t is the uniaxial tensile strength of rock columns, and FS is the factor of safety. To verify the method, they used the existing modeling results (base friction experiments of 6 and centrifuge modeling of 7).It is important to bear in mind that in all the above mentioned equations it was presumed that the rock columns are homogenous, isotropic, and continuous; hence the effect of in-situ rock structural weaknesses on the computed factor of safety was ignored. Therefore, the calculated factor of safety based on the aforementioned method is overestimated. Jennings 12 defined a parameter as “joint persistence” for investigation of the influence of geo-structural weaknesses in plane failure of rock slopes which is defined as follows: （4）where k is the joint persistence, an is the half-length of the nth joint, bn is the half-length of the nth rock bridge, N is the number of cracks, a is half of the average length of a presumed crack, and b is half of the average length of a presumed rock bridge.Determination of the exact value of the joint persistence (or “a” and “b” parameters), like many other in-situ geological factors such as dip and dip direction of discontinuities, spacing, etc., may not be possible. Therefore, these parameters must be determined with statistical approach. Therefore, the parameters a and b can be measured on the site by joint mapping of the rock masses (Fig. 1). The mean values of the statistical results can be used to compute the joint persistence. Fig. 1. Crack and rock bridge in a rock column with potential of flexural toppling failure.View Within ArticleIn this paper, the parameters a, b, and k are used for further analyses of geo-structural defects in flexural toppling failure.3. Effect of geo-structural defects on flexural toppling failure3.1. Critical section of the flexural toppling failureAs mentioned earlier, Majdi and Amini 10 and Amini et al. 11 have proved that the accurate factor of safety is equal to that calculated for a series of inclined rock columns, which, by analogy, is equivalent to the superimposed inclined cantilever beams as shown in Fig. 3. According to the equations of limit equilibrium, the moment M and the shearing force V existing in various cross-sectional areas in the beams can be calculated as follows: (5) ( 6)Since the superimposed inclined rock columns are subjected to uniformly distributed loads caused by their own weight, hence, the maximum shearing force and moment exist at the very fixed end, that is, at x=: (7) (8)If the magnitude of from Eq. (1) is substituted into Eqs. (7) and (8), then the magnitudes of shearing force and the maximum moment of equivalent beam for rock slopes are computed as follows: (9) (10)where C is a dimensionless geometrical parameter that is related to the inclinations of the rock slope, the total failure plane and the dip of the rock discontinuities that exist in rock masses, and can be determined by means of curves shown in Fig. Mmax and Vmax will produce the normal (tensile and compressive) and the shear stresses in critical cross-sectional area, respectively. However, the combined effect of them will cause rock columns to fail. It is well understood that the rocks are very susceptible to tensile stresses, and the effect of maximum shearing force is also negligible compared with the effect of tensile stress. Thus, for the purpose of the ultimate stability, structural defects reduce the cross-sectional area of load bearing capacity of the rock columns and, consequently, increase the stress concentration in neighboring solid areas. Thus, the in-situ tensile strength of the rock columns, the shearing effect might be neglected and only the tensile stress caused due to maximum bending stress could be used.3.2. Analysis of geo-structural defectsDetermination of the quantitative effect of geo-structural defects in rock masses can be investigated on the basis of the following two approaches.3.2.1. Solid mechanics approachIn this method, which is, indeed, an old approach, the loads from the weak areas are removed and likewise will be transferred to the neighboring solid areas. Therefore, the solid areas of the rock columns, due to overloading and high stress concentration, will eventually encounter with the premature failure. In this paper, for analysis of the geo-structural defects in flexural toppling failure, a set of cracks in critical cross-sectional area has been modeled as shown in Fig. 5. By employing Eq. (9) and assuming that the loads from weak areas are transferred to the solid areas with higher load bearing capacity (Fig. 6), the maximum stresses could be computed by the following equation (see Appendix A for more details): （11）Hence, with regard to Eq. (11), for determination of the factor of safety against flexural toppling failure in open excavations and underground openings including geo-structural defects the following equation is suggested: （12）From Eq. (12) it can be inferred that the factor of safety against flexural toppling failure obtained on the basis of principles of solid mechanics is irrelevant to the length of geo-structural defects or the crack length, directly. However, it is related to the dimensionless parameter “joint persistence”, k, as it was defined earlier in this paper. Fig. 2 represents the effect of parameter k on the critical height of the rock slope. This figure also shows the limiting equilibrium of the rock mass (Fs=1) with a potential of flexural toppling failureFig. 2. Determination of the critical height of rock slopes with a potential of flexural toppling failure on the basis of principles of solid mechanics.View Within Article3.2.2. Fracture mechanics approachGriffith in 1924 13, by performing comprehensive laboratory tests on the glasses, concluded that fracture of brittle materials is due to high stress concentrations produced on the crack tips which causes the cracks to extend (Fig. 3). Williams in 1952 and 1957 and Irwin in 1957 had proposed some relations by which the stress around the single ended crack tips subjected to tensile loading at infinite is determined 14, 15 and 16. They introduced a new factor in their equations called the “stress intensity factor” which indicates the stress condition at the crack tips. Therefore if this factor could be determined quantitatively in laboratorial, then, the factor of safety corresponding to the failure criterion based on principles of fracture mechanics might be computed.Fig. 3. Stress concentration at the tip of a single ended crack under tensile loadingView Within ArticleSimilarly, the geo-structural defects exist in rock columns with a potential of flexural toppling failure could be modeled. As it was mentioned earlier in this paper, cracks could be modeled in a conservative approach such that the location of maximum tensile stress at presumed failure plane to be considered as the cracks locations (Fig. 3). If the existing geo-structural defects in a rock mass, are modeled with a series cracks in the total failure plane, then by means of principles of fracture mechanics, an equation for determination of the factor of safety against flexural toppling failure could be proposed as follows: （13）where KIC is the critical stress intensity factor. Eq. (13) clarifies that the factor of safety against flexural toppling failure derived based on the method of fracture mechanics is directly related to both the “joint persistence” and the “length of cracks”. As such the length of cracks existing in the rock columns plays important roles in stress analysis. Fig. 10 shows the influence of the crack length on the critical height of rock slopes. This figure represents the limiting equilibrium of the rock mass with the potential of flexural toppling failure. As it can be seen, an increase of the crack length causes a decrease in the critical height of the rock slopes. In contrast to the principles of solid mechanics, Eq. (13) or Fig. 4 indicates either the onset of failure of the rock columns or the inception of fracture development.Fig. 4. Determination of the critical height of rock slopes with a potential of flexural toppling failure on the basis of principle of fracture mechanics.View Within Article4. Comparison of the results of the two approachesThe curves shown in Fig. represent Eqs. (12) and (13), respectively. The figures reflect the quantitative effect of the geo-structural defects on flexural toppling failure on the basis of principles of solid mechanics and fra