Abstract
An accurate determination of Hoek–Brown constant mi is of great significance in the estimation of the failure criteria of brittle rock materials. So far, different approaches such as rigidity index method (R-index), uniaxial compressive strength-based method, and tensile strength-based method, and the combination of these two methods (combination based method) have been proposed to calculate the value of mi. This paper aims to thoroughly review the previously existing methods to calculate the value of mi and make comparison between the obtain results to propose the new material constants that provide the best fit with the experimental data. In order to fulfill this goal, a large number of data for different quasi-isotropic intact rock types from the literature were collected and statistically analyzed. Additionally, based on rock types, new material constants are introduced for igneous, sedimentary, and metamorphic rocks. The obtained results proves that for different rock groups (igneous, sedimentary, and metamorphic rocks), R-index method provides the best fit with the experimental data among the others, and it is also independent of rock type. Interestingly enough, there is significant differences in the predicted mi values using different methods, which is more probably due to the quantity and quality of data used in the statistical analysis.
Similar content being viewed by others
Avoid common mistakes on your manuscript.
1 Introduction
The Hoek–Brown failure criterion is widely used in rock mechanics and rock engineering practice for determining the strength of brittle intact rock and rock masses. This nonlinear semiempirical failure criterion was introduced by Hoek and Brown [33], and the following form was suggested for intact rock (see also [17]) (Eq. 1):
where \(\sigma_{1}\) and \(\sigma_{3}\) are major and minor principal stress at failure, respectively, mi is Hoek–Brown material constant, and \(\sigma_{c}\) is the uniaxial compressive strength of intact rock. According to Eq. (1), two independent parameters are necessary, namely the:
-
Uniaxial compressive strength (\(\sigma_{c}\))
-
Hoek–Brown material constant of the intact rock (mi)
Although several practical, empirical, and probabilistic approaches have been presented in the literature to address uniaxial compressive strength (UCS) [12, 34, 36, 73, 80], the accurate determination of mi is still challenging task and is influenced by many factors such as mineral composition, grain size, and cementation of rock. Generally, mi presents curve-fitting parameter for Hoek–Brown failure envelope [37]. However, researches by Zuo et al. [84] showed that mi is not a curve-fitting parameter but has physical meanings and can be derived from micro-mechanical principles (Hoek and Martin [38]).
Hoek and Brown [33,34,35] suggested that these values should be determined by numerous triaxial tests, applying different confining pressures (\({\sigma }_{3}\)) between zero and 0.5 \({\sigma }_{c}\). These laboratory tests are time-consuming, expensive, and in many cases, there are not enough (or suitable) samples. Singh et al. [70], Peng et al. [55], and Shen and Karakus [65] demonstrated that the reliability of mi values measured from triaxial test analysis depends on the quality and quantity of test data used in the analysis. They concluded that the range of \({\sigma }_{3}\) could have a significant influence on the calculation of mi. It is the reason why several methods were developed for determining the Hoek–Brown constant (mi) [72].
There are several techniques available to calculate mivalues in the absence of triaxial test. These approaches are entitled, Guidelines [32, 33], R-index [10, 33, 52, 59, 60, 62], UCS-based model [65, 74], tensile strength (TS)-based approach [77], and crack initiation stress-based model [10]. These methods are based on the rock lithological classifications and rock properties that can be easily obtained at an early stage of a project, which can be used in preliminary designs of engineering projects when triaxial test data are not available.
Aladejare and Wang [1] published a paper and introduced a new method for the determination of mi value. They developed a Bayesian approach for probabilistic characterization of Hoek–Brown constant mi through Bayesian integration of information from Hoek’s guideline chart, regression model, and site-specific UCS data. The UCS data used in this paper were obtained from testing granite samples collected from the Forsmark site, Sweden. In addition, several sets of simulated data are used to explore the evolution of mi as the number of site-specific data increases.
Wei et al. [78] experimentally investigated the effect of confining pressure \({\sigma }_{3}\) and critical crack parameter on determination of mi value. They applied ultrasonic test and load test results of limestone and verified the exponential impact of \({\sigma }_{3}\) on limestone, while the negative correlation was observed between critical crack parameter and mi.
Recently, Wen et al. [79] developed an empirical relation for estimation mi from \({\sigma }_{3}\) and \(\beta\), where \({\sigma }_{3}\) is minor principal stress and \(\beta\) is an angle between the major principal stress and weak plane based on substantial uniaxial and triaxial compression test data. They considered the effect of anisotropy on the value of Hoek constant (mi).
In the present study, however, we focused on the quasi-isotropic intact rocks and utilized the existing methods in the literature for predicting mi values. Furthermore, the detailed comparison is drawn between the obtained values of each approach to calculate which method provides the best estimation for the investigated rocks based on the calculated error function. Accordingly, new material constants are proposed for different igneous, sedimentary, and metamorphic rocks.
2 Determination of Hoek–Brown constant m i
In the absence of triaxial tests, there are several different methods available to estimate the Hoek–Brown constant mi, which are referred to as the R-index method [33], UCS-based model [65, 74], TS-based model [77], and combination method [3, 66] below. By using these methods, the H-B constant mi is obtained for the collected data, the achieved results are compared, and then, the error function was calculated and accordingly considering the lowest error value, the best data fit was presented and finally new material constants introduced.
2.1 Guideline method
Hoek and Brown [33] and Hoek [32] provided values of mi constants for different types of rocks. The values of mi are between 7 and 35; however, several factors that influence these values, such as mineral composition, foliation, grain size (texture), and cementation are among others [10].
The updated values of constant mi for intact rock were collected by [10], using the published values of Hoek [32] (Table 1). Possible data ranges are shown by a variation range value immediately following the suggested mi value. For example, for sandstones, the mi values can vary between 13 and 21, and for slates, between 3 and 11.
2.2 Calculation the rigidity of the rock (R-index)
This method was introduced by [33] and also developed by [48, 59,60,61]. Cai [10] published the paper and showed that Hoek–Brown’s strength parameter (mi) could be determined from the ratio of the uniaxial compressive strength (\(\sigma_{c}\)) and the tensile strength (\(\sigma_{t}\)), and the suggested relationship is:
As can be seen from Fig. 1, when R > 8, the error for approximating mi (Eq. 2) by R (Eq. 4) is less than 1.6%.
It has been observed that when the R is higher than 8, the value of R is nearly equal to Hoek–Brown material constant (mi). Note, that according to [38] mi is not a curve fitting parameter, but has a physical meaning and can be derived from micro-mechanics principles. The referred mi model is express in Eq. (3):
where \(\sigma_{c}\) and \(\sigma_{t}\) are the uniaxial compressive strength (UCS) and tensile strength (TS) of intact rock, respectively. While \(\mu\) is the coefficient of friction for pre-existing sliding crack surfaces, \(\beta\) is an intermediate fracture mechanics parameter that can be obtained from experimental data. It means when \(R > 8\):
In recent years, Hoek and Brown [34] analyzed several published data and proposed the following approximate relationship between the compressive to tensile strength ratio, \(\frac{{\sigma_{c} }}{{|\sigma_{t} |}}\), and the Hoek–Brown parameter mi (see Fig. 2):
It means that the Hoek–Brown constant (mi) can be calculated using the following relationship, using the uniaxial compressive strength (\(\sigma_{c}\)) and the tensile strength (\(\sigma_{t}\)) data of the intact rock.
2.3 UCS-based model
Firstly, Shen and Karakus [65] and later Vásárhelyi et al. [74] also emphasized the difficulties in determining the mi values of rocks. They suggested normalizing the Hoek–Brown constant \(\left( {m_{{{\text{in}}}} = \frac{{m_{i} }}{{\sigma_{c} }}} \right)\) by using the strength of the rock \(\left( {m_{{{\text{in}}}} = \frac{{m_{i} }}{{\sigma_{c} }}} \right)\), i.e.:
where \(a\) and \(b\) are constants that depend on rock types.
2.4 TS-based model
The tensile strength-based calculation method was suggested by Wang and Shen [77]. In this method, the mi value is determined from the tensile strength (\(\sigma_{t}\)) of the intact rock.
where \(A\) and \(B\) are material constants that depend on rock types. In general, the constants \(A\) and \(B\) are curve-fitting parameters.
However, according to the theory of Zuo et al. [84] the mi value can be estimated from the coefficient of friction for the pre-existing sliding crack surfaces, and fracture mechanics. From this point of view, the constants \(A\) and \(B\) for the TS-based model seem to have its physical meaning, which have possible relations with the micro-mechanics principles. However, investigating the potential relationships between these constants and other rock properties and explaining the possible physical meanings need to carry out further research to get appropriate amount of reliable data.
2.5 Combination method (UCS and TS)
Analyzing the published data of Sheorey [66], Arshadnejad and Nick [3] suggested a new equation to calculate the Hoek–Brown material constant (mi) based on uniaxial compressive strength (\(\sigma_{c}\)) and the tensile strength (\(\sigma_{t}\)) parameters of the intact rock:
where \(a\), \(b\), and \(c\) are material constants. The suggested constants are summarized in Table 2, according to Arshadnejad and Nick [3].
2.6 Crack initiation stress-based model
According to [10], the Hoek–Brown constant (mi) depends on the confining pressure. For practical estimate of mi, it was found that for strong, brittle rocks, applicable to high confining zone the following equation could be used:
For low confinement stress to tension zone, especially for the tension zone the suggested equation is:
In these equations, \({\sigma }_{c}\) and \({\sigma }_{ci}\) are the uniaxial compressive strength and the crack initiation stress, respectively.
2.7 Bayesian approach
The proposed approach [1] derives the probability density function (PDF) of mi based on the integration of Hoek’s guideline chart, regression model, and site-specific UCS data, under a Bayesian framework. A large number of equivalent samples of mi are generated from the PDF using Markov Chain Monte Carlo (MCMC) simulation.
3 Experimental data
A wide range of data from literature by [72] were selected and analyzed. The published data of the investigated rocks are illustrated in Appendices 1, 2, and 3 for igneous, sedimentary, and metamorphic rocks, respectively. In these tables, calculated data are also given. Statistical analyses of the measured mi values for different rock types are summarized in Table 3. In this table, parameters such as number of data sets, maximum (Max.), minimum (min.), average (Ave.), and standard deviation (std.) of measured mi for three different groups are presented (see the appendix for more details).
4 Analyzing the data
4.1 Comparing the published m i values with the guideline
Comparing the published values of mi by [72] with the guidelines [10, 32, 33] given for igneous rocks, the value of mi for basalt is between 20 and 30, whereas the minimum published value of mi for Basalt is 4.31 (see Appendix 1) which does not fall within the expected range. The minimum published value of mi for basalt is even less than mi value for volcanic tuffs. The latter one is between 8 and 13. The published values of mi for granite are between 11.68 and 34.03, but the expected range based on the guidelines is between 29 and 35. The same discrepancy was observed for gabbro. The expected range based on the guideline values is between 24 and 30, whereas the published results are in between 15.31 and 20.74.
For diorite, the value of mi based on the guidelines is between 20 and 30; however, according to published data, the value of mi is between 6.1 and 11. For granodiorite, based on the guideline, the value of mi changes between 26 and 32, while based on published results, it is between 11 and 18.15. For diabase, according to the guidelines, the value of mi is between 10 and 20; nevertheless, based on published data it is between 15.3 and 20.3. For andesite and rhyolite, the value of mi based on the guidelines is between 20 and 30; however, the published values are 6.22 and 5.43 for andesite and rhyolite, respectively. For agglomerate, the value of mi is between 16 and 22, but the published value is 7.92, which does not fit the guideline range.
For sedimentary rocks, the minimum value of mi for shale is 3.76 which is close to the estimated range of mi which is between 4 and 8 (see Appendix 2). Also, the maximum published value of mi for sandstone is 35.11 which is much higher than the estimated range of mi value and based on guideline which varies between 13 and 21. Moreover, for dolomite, the value of mi based on guidelines is between 6 and 12, whereas the value of mi based on published data is between 7.8 and 17.5. For limestone, the value of mi based on guideline is between 7 and 15; however, based on published data, the value of mi is between 5.3 and 14.6.
For metamorphic rocks, it is interesting to know that both maximum and minimum published values are for slate with the amounts of 1.42 and 29.54, respectively (see Appendix 3). However, based on guideline the values of mi for slate changes between 3 and 11. It means that the range of published value for slate does not fit the estimated range given by the guidelines. For gneiss, the value of mi based on guidelines is between 23 and 33; however, based on published data, the value ranges between 5.3 and 27. For schist, the published value of mi is 20.42, but the values based on guideline vary between 9 and 15. For quartzite, the published value of mi is between 7.36 and 22.7; however, based on guideline it is between 17 and 23. Also, the values of mi were calculated according to [10].
The differences between the published values of mi and the guideline values are displayed in Table 4 and Fig. 3. As shown, the published values of mi do not fit well with the guideline. As it is clear from the graph that there is a good consistency between published experimental data for mi and R-index method, whereas other methods have significant errors in estimation of mi for all studied rock samples. The obtained results based on different proposed calculation method are presented in Appendices 4, 5, and 6 for igneous, sedimentary, and metamorphic rocks, respectively. It should be noted that the constant parameters were derived from the existing Eqs. 2, 6, 7, 8, and 9, respectively.
4.2 Evaluation of R-index model
According to our analyses for determination of mi in respect to Eq. 2 (R-index method) and Eq. 5, it was observed that mi value is independent of rock type. The correlations between mi and the ratio between uniaxial compressive strength (UCS) and tensile strength (TS), which is called R-index method, for different rocks (sandstone, shale, slate, and gneiss) are presented in Fig. 4. As shown for different rock types, correlation value \(R^{2} = 1\) and it is not influenced by rock type.
4.3 Evaluation of UCS-based model
The relationship between mi and uniaxial compressive strength (UCS) for the investigated rock samples (UCS-based method) shows an opposite result, compared to R-index method. It is evident that based on this approach, no correlation was found for the studied rock samples (Fig. 5).
4.4 Evaluation of TS-based model
Based on our analyses for determination of mi value by applying TS-based method, the established correlations for the investigated rock types were weak except for slate where the value of \(R^{2} = 0.66\) (Fig. 6).
In order to examine the relationship between mi and rigidity of rock (R-index method) for different rock groups, analyses were also carried out based on three different rock types (igneous, sedimentary, and metamorphic) and the results are illustrated in Fig. 7. Additionally, the error function was calculated for each rock type. The calculated amount of error function represents the value of \(\left( {\frac{\mu }{\beta }} \right)\) as mentioned earlier in Eq. (3).
The obtained results of regression analyses based on proposed approaches for determination of mi are summarized in Table 5 (according to rock group) and Table 6 (according to different investigated rock samples), and the statistical results are illustrated in Table 7.
In the proposed method by Arshadnejad and Nick [3], (combination method), (i), (j), and (k) are presented as material constants. Specifically explaining, based on their analyses for different rock groups (igneous, sedimentary, and metamorphic), there are different material constants. See Table 2 for their obtained results.
4.5 Evaluation of combination method (UCS and TS methods)
We analyzed the data set based on Eq. 9 as proposed by [3]. The results are depicted in Fig. 8. The graphs clearly illustrate that the Hoek constant (mi) is independent of rock type. Accordingly, it is worth to mention the point that the intact rocks are known to contain a wide-ranging uncertainty owing to inherent heterogeneities. For rock mass classification in respect to uncertainties, GSI (Geological Strength Index) provides good classification of rock mass category as it relies on structure as well as surface conditions of existing discontinuities which are highly associated with high uncertainties in rock mass. Ván and Vásárhelyi [72] investigated the sensitivity of Hoek material constant for rock mass (mb) in relation to GSI. Based on their measurement, they calculated that 10% deviation in the GSI value; the relative sensitivity of mb is at least double the uncertainties of the GSI values and may be 7 times higher in case of large disturbance parameters and low and high GSI values.
5 Discussion
When triaxial test data are not available, mi values can be estimated by six existing methods entitled, guidelines [32, 33], R-index [10, 33, 52, 59, 60, 62], UCS-based model [65, 74], TS-based model [77], crack initiation stress-based model [10], combination based model [3, 66], and Bayesian approach [1] to evaluate the prediction performance of existing methods, large database of triaxial tests for eight common rock types (slate, shale, limestone, quartzdiorite, sandstone, quartzite, gneiss, and granite) from literature was selected and analyzed as indicated in Appendices 1, 2, and 3.
In the present research, to ensure the quantity and quality of data, the statistical analysis with the help of SPSS software was performed on quasi-isotropic rocks. The results are presented in Fig. 9. As shown, normal distribution function and standard deviation were calculated for each rock group. According to Fig. 9, for igneous rock, the calculated standard deviation is 7.21 with the mean value of 15.36, for sedimentary rock is 6.32 with the mean value of 12, and for metamorphic rocks is 10.07 with the mean value of 13.37. Interestingly enough, metamorphic rocks exhibit higher standard deviation, which can be can associated with the foliated texture of the investigated metamorphic rocks.
Similarly, Aladejare and Wang [1] investigated the values of mi for 30,000 equivalent granite samples based on Bayesian approach and realized that the histogram peaks at a mi value of around 30, and roughly about 27,479 out of the total 30,000 samples representing about 91.5% are within mi range of 18 and 48. Therefore, the 90% interperceptual range of mi is roughly between mi values of 18 and 48 (Fig. 9d). In comparison with our results, however, Wen et al. [79] published an interesting paper about anisotropic rocks, which has drawn our attention to their new empirical relation. The large number of the data set (738) of different rock types was analyzed. They observed that the more anisotropic the rock is, the more significant decrease in mi value is evident. Using this relation, the H–B strength criterion is modified, and its performance is evaluated in two examples. The results illustrate the improved ability of the modified criterion to determine the strength of metamorphic and sedimentary rocks.
Based on the empirical model by Wen et al. [79], most of the estimated values of mi are within the upper/lower limit of 90%, which accounts for 96.6% of all the data, and that all the estimated values are within the upper/lower limit of 80%. This result indicates that the developed relation estimates of mi agree well with the experimental observations, demonstrating that the developed relation has an excellent ability to estimate mi accurately. The comparison graph between our results and recently published paper by Wen et al. [79] is presented in Fig. 10.
Moreover, Wen et al. [80,81,82] thoroughly investigated the impact of minor principal stress (σ3) on rock ductile–brittle behavior. Based on their measurement, under a low minor principal stress, rocks experience dilatancy and brittleness that causes the exciting microcrack inside the rock to coalesce, which result in an increase in volume; In contrast, applying the high minor principal stress, the rock undergoes ductility which leads to microcrack opening.
In the recently published paper by He et al. [27], they suggested that the constant mi of the H–B criterion can be continuously estimated during drilling. Therefore, a method to estimate the constant mi from drilling data was proposed. Based on the proposed method for mi determination, for the granite, slate, the obtained values of mi in their work were lower than the suggested values for granite and sandstone from [33], and they were higher than the suggested value for slate and limestone.
To establish the correlations for specific rock types, Shen and Karakus [65], Wang and Shen [77] considered five of the most common rock types (coal, granite, limestone, marble, and sandstone) from the database in the Rocscience [61], in which there are at least 12 groups of data with 115 triaxial tests available. Results illustrate that four rock types have trends of decreasing mi with increasing \(\sigma_{ci}\); however, such a correlation for limestone was not observed. It is worth noting that this finding is also in agreement with our obtained results for limestone. This may be due to the fact that limestone has a wide array of test data with different compositions and cementations; for example, there are different guidelines-based mi values for three types of limestone, crystalline (mi = 12 ± 3), sparitic (mi = 10 ± 2), and micritic (mi = 9 ± 2), in the Hoek guidelines [32]. Therefore, the data sets for limestone are quite widely scattered compared with those for the other four rock types.
The observed value of mi for limestone is between 5.3 and 14.6; In contrast, according to guideline, the mi value of limestone is between 7 and 15, according to R-index method mi is between 5.32 and 14.67, according to UCS-based method mi is between 19.8 and 22.1, based on TS-based method mi is between 6.18 and 13.05, and based on combination method mi is between 4.9 and 13. Thus, R-index method gives the best estimate of mi value among the others. However, based on [65], UCS-based method provides a better prediction of mi value than the guidelines-based and R-index methods and according to [77], TS-based model exhibits the best performance for granites, limestone, and marble.
Additionally, the observed value of mi for slate is between 1.42 and 30.97; however, based on guideline, the mi value of slate is between 3 and 11, based on R-index method mi is between 1.59 and 31.23, based on UCS-based method mi is between 7.2 and 22.3, based on TS-based method mi is between 3.82 and 48.42, and based on combination method mi is between 1.98 and 32.44. So, R-index method gives the best estimate of mi value among the others. The achieved value of mi is inconsistent with the obtained value of mi by [16], which they used the internal friction angel method for estimating the value of mi for dolomite, slate, dike, and granodiorite. The obtained values of mi were 6.28, 5.1, 12.8, and 13.7, respectively.
Moreover, the observed value of mi for shale is between 3.76 and 25.31, but, according to guideline, the mi value of shale is between 4 and 8, according to R-index method mi is between 3.7 and 24.9, according to UCS-based method mi is between 17.82 and 22.1, based on TS-based method mi is between 6.52 and 29.87, and based on combination method mi is between 3.65 and 24.3. Therefore, R-index method gives the best estimate of mi value among the others.
Furthermore, the observed value of mi for sandstone is between 3.97 and 35.1; nevertheless, according to guideline, the mi value of sandstone is between 13 and 21, according to R-index method mi is between 3.9 and 35, according to UCS-based method mi is between 17.82 and 22.23, based on TS-based method mi is between 5.48 and 29.87, and based on combination method mi is between 3.83 and 38.5. As a result, R-index method gives the best estimate of mi value among the others. Nevertheless, based on [77], UCS-based model gives the best prediction for sandstone.
As well as that, the observed value of mi for quartzite is between 7.36 and 30.1, while, according to guideline, the mi value of quartzite is between 17 and 23, according to R-index method mi is between 7.36 and 30.14, according to UCS-based method mi is between 8.45 and 21.1, based on TS-based method mi is between 5.66 and 10.43, and based on combination method mi is between 6.55 and 31.10. Hence, R-index method gives the best estimate of mi value among the others.
In addition, the observed value of mi for gneiss is between 5.34 and 32.33, whereas, according to guideline, the mi value of gneiss is between 23 and 33, according to R-index method mi is between 5.3 and 32.3, according to UCS-based method mi is between 8.07 and 22.46, based on TS-based method mi is between 4.68 and 11.44, and based on combination method mi is between 4.92 and 34.28. Therefore, R-index method gives the best estimate of mi value among the others.
Finally, the observed value of mi for granite is between 11.68 and 34.03; on the other hand, according to guideline, the mi value of granite is between 29 and 35, according to R-index method mi is between 11.7 and 34.1, according to UCS-based method mi is between 8.92 and 22.8, based on TS-based method mi is between 7.42 and 15.42, and based on combination method mi is between 10.22 and 36.95. Thus, R-index method gives the best estimate of mi value among the others.
6 Conclusion
This paper comprehensively reviewed the proposed methods for determination of mi value using the triaxial data set published by [66]. New linear and nonlinear correlations were found. New material constants were suggested for igneous, sedimentary, and metamorphic rocks such as granite, quartzdiorite, sandstone, shale, limestone, gneiss, quartzite, and slate. Furthermore, the error function was calculated for each rock type. According to our analyses, R-index approach with new material constants provides the best fit for all the studied lithotypes including igneous, sedimentary, and metamorphic rocks. Moreover, it is worth mentioning that comparison graph between out achieved results for quasi-isotropic rocks and anisotropic rocks was developed. The data scattering of quasi-isotropic rocks differs from the anisotropic rocks in that quasi-isotropic rocks exhibit normal distribution in narrower range between 1.43 and 35.11, whereas anisotropic rocks display wider range of data distribution between 1 and 80.
The combination methods (UCS) and (TS) provide the best fit for investigated rock data, when the determination coefficient and error function are considered. For various rock types such as igneous, sedimentary, and metamorphic rocks, the different approaches resulted in non-uniform correlations. For instance, TS-based approach works well for the granite and gives estimation fit with \(R^{2} = 0.89\). For quartzites, UCS-based approach displays the best approximation with \(R^{2} = 0.91\), and for slate, TS-based model exhibits the best correlation with \(R^{2} = 0.67\).
R-index method, the value of mi is not influenced by rock type. In other words, this method gives the best estimation for all the investigated rock types and is independent of rock type. However, in all the other approaches, the rock type plays a significant role in correlation values and results.
Abbreviations
- m i :
-
Hoek–Brown material constant
- m b :
-
Hoek material constant for rock mass
- GSI:
-
Geological Strength Index
- TS:
-
Tensile strength
- UCS:
-
Uniaxial compressive strength
- R :
-
Rigidity index
- β :
-
Intermediate fracture mechanics parameter
- μ :
-
The coefficient of friction for pre-existing sliding crack surfaces
- \(\sigma_{1} ,\sigma_{3}\) :
-
Major and minor principal stress
- \(\sigma_{c}\) :
-
Uniaxial compressive strength (UCS)
- \(\sigma_{{{\text{ci}}}}\) :
-
Crack initiation stress
- \(\sigma_{t}\) :
-
Tensile strength (TS)
References
Aladejare A, Wang Y (2019) Probabilistic characterization of Hoek–Brown constant mi of rock using Hoek’s guideline chart, regression model and uniaxial compression test. Geotech Geol Eng 37:5045–5060. https://doi.org/10.1007/s10706-019-00961-7
Aldritch MJ (1969) Pore pressure effects on Berea sandstone subjected to experimental deformation. Geol Soc Am Bull 80:1577–1586. https://doi.org/10.1130/0016-7606(1969)80
Arshadnejad S, Nick N (2016) Empirical models to evaluate of “mi” as an intact rock constant in the Hoek–Brown rock failure criterion. 19th Southeast Asian Geotechnical Conference & 2nd AGSSEA Conference (19SEAGC & 2AGSSEA) Kuala Lumpur, June 2016.
Attewell PB, Sandford MR (1974) Intrinsic shear strength of a brittle anisotropic rock—I: experimental and mechanical interpretation. Int J Rock Mech Min Sci Geomech Abstr 11:423–430. https://doi.org/10.1016/0148-9062(74)90453-7
Barat D (1995) Personal communication from C.M.R.I., Dhanbad (from Sheorey, 1997)
Betourney MC, Gorski B, Labrie D, Jackson R, Gyenge M (1991) New considerations in the determination of Hoek and Brown material constants. In: Wittke W (ed) 7th Int. Cong. Rock Mech. (ISRM), Aachen, vol 1, pp 195–200
Borecki M, Kwasniewski M, Pacha J, Oleksy S, Berszakiewicz Z, Guzik (1982) Triaxial compressive strength of two mineralogic/diagenetic varieties of coal. measure, fine-medium grained Pniowek and Anna sandstones tested under confining pressure up to 60 MPa. Prace Instytutu PBKIOP Politechniki Slaskiej, 119/2, Gliwice
Brace WF (1964) Brittle fracture of rocks. In: Judd WR (ed) State of stress in the Earth's Crust. Elsevier, pp 111–174
Broch E (1974) The influence of water on some rock properties. In: Advances in rock mechanics. 3rd Int. Cong. Rock Mech., Denver, vol 2, pp 33–38
Cai M (2010) Practical estimates of tensile strength and Hoek–Brown strength parameter mi of brittle rocks. Rock Mech Rock Eng 43:167–184. https://doi.org/10.1007/s00603-009-0053-1
Chan SSM, Crocker TJ, Wardell GG (1972) Engineering properties of rocks and rock masses in the deep mines of the Coeur d’Alene Mining District, Idaho. Trans Soc Min Eng AIME 252:353–361
Davarpanah M, Somodi G, Kovács L, Vásárhelyi B (2020) Experimental determination of the mechanical properties and deformation constants of Mórágy Granitic Rock Formation (Hungary). Geotech Geol Eng 38:3215–3229. https://doi.org/10.1007/s10706-020-01218-4
Dayre M, Giraud A (1986) Mechanical properties of granodiorite from laboratory tests. Eng Geol 23:109–124. https://doi.org/10.1016/0013-7952(86)90033-5
Dlugosz M, Gustkiewicz J, Wysocki A (1981) Apparatus for investigation of rocks in a triaxial state of stress. Part II. Some investigation results concerning certain rocks. Archiwum Gornictwa 26:29–41
Donath FA (1964) Strength variations and deformational behaviour in anisotropic rock. In: Judd WR (ed) State of stress in the Earth's Crust. Elsevier, New York, pp 281–297
Dunikowski A, Korman S, Kohsling J (1969) Laboratory test indices of physico-mechanical properties of rocks in three-axial state of stress. Przeglad Gorniczy 25:523–528
Eberhardt E (2012) The Hoek–Brown failure criterion. Rock Mech Rock Eng 45:981–988. https://doi.org/10.1007/s00603-012-0276-4
Everling G (1960) Rock mechanical investigations and basis for determination of rock pressure according to deformation of drill holes. Gluckauf 96:390–409
Fayed LA (1968) Shear strength of some argillaceous rocks. Int J Rock Mech Min Sci 5(1):79–85. https://doi.org/10.1016/0148-9062(68)90024-7
Franklin JA, Hoek E (1970) Developments in triaxial testing technique. Rock Mech 2:223–228. https://doi.org/10.1007/BF01245576
Glushko VT, Kirnichanskiy GT (1974) Engineering—geological prognosticating of stability of the openings in deep coal mines. Nedra, Moscow
Gnirk PF, Cheatham JB (1965) An experimental study of single bit tooth penetration into dry rock at confining pressures of 0–5000 psi. J Soc Pet Eng 5:117–130
Gowd TN, Rummel F (1980) Effect of confining pressure on the fracture behavior of a porous rock. Int J Rock Mech Min Sci Geomech Abstr 17:225–229. https://doi.org/10.1016/0148-9062(80)91089-X
Gustkiewicz J (1984) Personal communication from M.A. Kwasniewski, Gliwice, 1995 (from Sheorey, 1997)
Hareland G, Polston CE, White WE (1993) Normalised rock failure envelope as a function of grain size. Int J Rock Mech Min Sci Geomech Abstr 30:715–717. https://doi.org/10.1016/0148-9062(93)90012-3
Harza Engineering Co. (1976) Comprehensive ground control study of a mechanized longwall operation, final report, 2. USBM OFR 5(2)-775(2)-77 (published as NTIS report)
He M, Zhang Z, Zheng J. et al. (2020) A new perspective on the constant mi of the Hoek–Brown failure criterion and a new model for determining the residual strength of rock. Rock Mech Rock Eng. 53:3953–3967. https://doi.org/10.1007/s00603-020-02164-6
Heard HC, Abey AE, Bonner BP, Schock RN (1974) Mechanical behaviour of dry Westerly granite at high confining pressure. Lawrence Livermore Laboratory Rept. No. UCRL 51642, 14 p
Hobbs DW (1964) The strength and the stress-strain characteristics of coal in triaxial compression. J Geol 72:214–231. https://doi.org/10.1086/626977
Hobbs DW (1970) Behaviour of broken rocks under triaxial compression. Int J Rock Mech Min Sci 7:125–148. https://doi.org/10.1016/0148-9062(70)90008-2
Hoek E (1983) Strength of jointed rock masses. Geotechnique 33:87–223. https://doi.org/10.1680/geot.1983.33.3.187
Hoek E (2007) Practical rock engineering—chapter 11: rock mass properties. https://www.rocscience.com/learning/hoeks-corner
Hoek E, Brown ET (1980) Underground excavation in rock. Institution of Mining and Metallurgy, London
Hoek E, Brown ET (1997) Practical estimates of rock mass strength. Int J Rock Mech Min Sci 34(8):1165–1186. https://doi.org/10.1016/S1365-1609(97)80069-X
Hoek E, Brown ET (2019) The Hoek–Brown Failure criterion and GSI—2018 edition. J Rock Mech Geotech Eng 11:445–463. https://doi.org/10.1016/j.jrmge.2018.08.001
Hoek E, Carter TG, Diederichs MS (2013) Quantification of the geological strength index chart. In: 47th US rock mechanics/geomechanics symposium, San Francisco, June 2013
Hoek E, Marinos P (2000) Predicting tunnel squeezing problems in weak heterogeneous rock masses. Tunnels Tunn Int 32(11):45–51
Hoek E, Martin CD (2014) Fracture initiation and propagation in intact rock—a review. J Rock Mech Geotech Eng 6(4):287–300. https://doi.org/10.1016/j.jrmge.2014.06.001
Horino FG, Ellickson ML (1970) A method for estimating strength of rock containing planes of weakness. USBM Rep Inv 7449, 26 p
Hoshino K, Koide H, Inami K, Iwamura S, Mitsui S (1972) Mechanical properties of Japanese tertiary sedimentary rocks under high confining pressures. Rept Geol Survey 244
Hossaini SME, Vutukuri VS (1993) On the accuracy of multifailure triaxial test for the determination of peak and residual strength of rocks. In: Szwedzicki (ed) Aust. Conf. Geotech. Instrumentation and Monitoring in Open Pit and underground Mining, Kalgoorlie, pp 223–228
Illnitskaya EI, Teder RI, Vatolin ES, Kuntysh MF (1969) Properties of rock and methods of their determination. Nedra, Moscow
Johnson B, Friedman M, Hopkins TN (1987) Strength and microfracturing of Westerly granite extended wet and dry at temperatures to 800 °C and pressures to 200 MPa. In: Farmer IW, Daeman JJK, Desai CS, Glass CE, Newman SP (eds) 28th US Symp. Rock Mech., Tucson, pp 399–412
Kovári K, Tisa A (1975) Multiple failure state and strain controlled triaxial tests. Rock Mech 7:17–33. https://doi.org/10.1007/BF01239232
Kuntysh MF (1964) Investigation of methods of determining the basic physico-mechanical characteristics of rocks, used while solving the problem of rock pressure. Cand. Techn. Sci. Thesis, Moscow
Kwasniewski MA (1983) Deformational and strength properties of the three structural varieties of carboniferous sandstones. In: 5th Int. Cong. Rock Mech. (ISRM), 1, Balkema, Rotterdam, pp A 105–A 115.
McLamore R, Gray KE (1967) The mechanical behaviour of anisotropic sedimentary rocks. Trans Am Soc Mech Eng Ser B 89:62–76
Mehrishal A, Sharifzadeh M, Shahryar K (2015) Estimating of Hoek–Brown mi using internal friction angle. In: Proceedings of the 24th International Mining Congress of Turkey, IMCET 2015, pp 488–493
Misra B (1972) Correlation of rock properties with machine performance. Ph.D. thesis, Leeds University
Mogi K (1965) Deformation and fracture of rocks under confining pressure, (2): Elasticity and plasticity of some rocks. Bull Earthquake Res Inst (Tokyo Univ) 42:349–379
Mogi K (1966) Some precise measurements of fracture strength of rocks under uniform compressive stress. Rock Mech Eng Geol IV:41–55
Mostyn G, Douglas K (2000) Strength of intact rock and rock masses. In: Proceedings of international conference on geotechnical and geological engineering, vol 1. Technomic Publishing, Lancaster, pp 1389–1421
Murrel SAF (1965) The effect of triaxial stress systems on the strength of rock at atmospheric temperature. Geophys J 10:231–281. https://doi.org/10.1111/j.1365-246X.1965.tb03155.x
Ouyang Z, Elsworth D (1991) A phenomenological failure criterion for brittle rock. Rock Mech Rock Eng 24:133–153. https://doi.org/10.1007/BF01042858
Peng J, Rong G, Cai M, Wang X, Zhou C (2013) An empirical failure criterion for intact rocks. Rock Mech Rock Eng 47(2):347–356. https://doi.org/10.1007/s00603-013-0514-4
Ramamurthy T (1989) Personal communication from I. I. T., Delhi (from Sheorey, 1997)
Ramez MRH (1967) Fractures and strength of a sandstone under triaxial compression. Int J Rock Mech Min Sci 4:257–268. https://doi.org/10.1016/0148-9062(67)90010-1
Rao KS, Rao GV, Ramamurthy T (1983) Strength anisotropy of a Vindhyan sandstone. In: Indian Geotech Conf, Madras, vol 1, pp 141–148
Read S, Richards L (2014) Correlation of direct and indirect tensile tests for use in the Hoek–Brown constant mi. In: Rock engineering and rock mechanics: structures in and on rock masses. Taylor and Francis, London
Richards L, Read S (2011) A comparative study of mi, the Hoek–Brown constant for intact rock material. In: Proceedings 45th US rock mechanics/geomechanics symposium. American Rock Mechanics Association, San Francisco
Rocscience (2012) RocData. http://www.rocscience.com/products/4/RocDataæ (March 7, 2014)
Sari M (2010) A simple approximation to estimate the Hoek–Brown parameter mi for intact rocks. In: Rock mechanics in civil and environmental engineering. Taylor and Francis, London
Schwartz AE (1964) Failure of rock in the triaxial shear test. In: Proceedings of the 6th rock mechanics symposium. University of Missouri, USA
Shea-Albin VR, Hansen DR, Gerlick RE (1991) Elastic wave velocity and attenuation as used to define phases of loading and failure in coal. USBM Rept Inv 9355, 43 p
Shen J, Karakus M (2014) Simplified method for estimating the Hoek–Brown constant for intact rocks. J Geotech Geoenviron Eng 140(1):0401–4025. https://doi.org/10.1061/(ASCE)GT.1943-5606.0001116
Sheorey PR (1997) Empirical rock failure criteria. Central Mining Research Institute, India
Sheorey PR, Biswas AK, Choubey VD (1989) An empirical failure criterion for rocks and jointed rock masses. Engg Geol 26:141–159. https://doi.org/10.1016/0013-7952(89)90003-3
Singh SK (1995) Personal communication from C.M.R.I., Dhanbad (from Sheorey, 1997)
Singh M, Sabu AK, Srivastava RK, Tiwari RP (1992) Evaluation and applicability of strength for rocks: sandstones and quartzites of Mirzapur region. In: Asian Regional Symp. Rock Slopes, Oxford and IBH, New Delhi, pp 117–124
Singh M, Raj A, Singh B (2011) Modified Mohr-Coulomb criterion for non-linear triaxial and polyaxial strength of intact rocks. Int J Rock Mech Min Sci 48(4):546–555. https://doi.org/10.1016/j.ijrmms.2011.02.004
Stowe RL (1969) Strength and deformation properties of granite, basalt, limestone and tuff at various loading rates. U.S Army Corps Eng., Waterways Exp. Stn., Vicksburg Miss., Misc. Paper C-69-1
Ván P, Vásárhelyi B (2014) Sensitivity analysis of GSI based mechanical parameters of the rock mass. Period Polytech Civil Eng 58(4):379–386. https://doi.org/10.3311/PPci.7507
Vásárhelyi B, Kovács D (2016) Empirical methods of calculating the mechanical parameters of the rock mass. Period Polytech Civ Eng 61(1):39–50. https://doi.org/10.3311/PPci.10095
Vásárhelyi B, Kovács L, Török A (2016) Analysing the modified Hoek–Brown failure criteria using Hungarian granitic rocks. Geomech Geophys Geo-energ Geo-resour 2:131–136. https://doi.org/10.1007/s40948-016-0021-7
Vutukuri VS , Farough Hossani SM (1993) Correlation between the effect of confining pressure on compressive strength in triaxial test and the effect of dia/height ratio on compressive strength in unconfined compression test. In: Peng SS (ed) 12th Conf. Ground Control in Mining, Morgantown, pp 316–321
Wang R, Kemeny JM (1995) A new empirical failure criterion for rock under polyaxial compressive stresses. In: Daemen JJK, Schultz RA (eds) 35th US Symp. Rock Mech., Balkema, Rotterdam, pp 453–458
Wang W, Shen J (2017) Comparison of existing methods and a new tensile strength based model in estimating the Hoek–Brown constant mi, for intact rocks. Eng Geol 224:87–96. https://doi.org/10.1016/j.enggeo.2017.05.008
Wei X, Zuo J, Shi Y, Liu H, Jiang Y, Liu C (2020) Experimental verification of parameter m in Hoek–Brown failure criterion considering the effects of natural fractures. J Rock Mech Geotech Eng 12(5):1036–1045. https://doi.org/10.1016/j.jrmge.2020.01.006
Wen T, Tang H, Huang L, Hamza A, Wang Y (2020) An empirical relation for parameter mi in the Hoek–Brown criterion of anisotropic intact rocks with consideration of the minor principal stress and stress-to-weak-plane angle. Acta Geotech. https://doi.org/10.1007/s11440-020-01039-y
Wen T, Tang HM, Wang YK, Ma JW (2020) Evaluation of methods for determining rock brittleness under compression. J Nat Gas Sci Eng. https://doi.org/10.1016/j.jngse.2020.103321
Wen T, Tang H, Huang L, Wang YK, Ma JW (2020) Energy evolution: a new perspective on the failure mechanism of purplish-red mudstones from the Three Gorges Reservoir area, China. Eng Geol. https://doi.org/10.1016/j.enggeo.2019.105350
Wen T, Tang HM, Wang YK (2020) Brittleness evaluation based on the energy evolution throughout the failure process of rocks. J Pet Sci Eng. https://doi.org/10.1016/j.petrol.2020.107361
Wilhelmi B, Somerton WH (1967) Simultaneous measurement of pore and elastic properties of rocks under triaxial stress conditions. J Soc Pet Engrs 7:283–294
Zuo J, Liu H, Li H (2015) A theoretical derivation of the Hoek–Brown failure criterion for rock materials. J Rock Mech Geotech Eng 7(4):361–366. https://doi.org/10.1016/S1365-1609(00)00049-6
Acknowledgements
The project presented in this article is supported by National Research, Development, Innovation Office (NKFIH 124508). The financial support of TKP2020 Institution Excellence Subprogram, Grant No. TKP2020 BME-IKA-VÍZ of the National Research Development and Innovation Office of Hungary is acknowledged.
Funding
Open access funding provided by Budapest University of Technology and Economics.
Author information
Authors and Affiliations
Corresponding author
Additional information
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Appendices
Appendix 1: Published values of triaxial parameters for Hoek–Brown criterion using data set for igneous rocks [66]
No | Rock name | \(\sigma_{c}\)(MPa) | \(\sigma_{t}\)(MPa) | m i | \(\frac{{\sigma_{c} }}{{\sigma_{t} }}\) | \(\frac{{m_{i} }}{{\sigma_{c} }}\) | Source |
---|---|---|---|---|---|---|---|
1 | Agglomerate tuff | 92 | 11.43 | 7.926 | 8.05 | 0.09 | Betourney et al. [6] |
2 | Tuff | 125.2 | 5.44 | 22.963 | 23.01 | 0.18 | Wang and Kemeny [76] |
3 | Andesite | 201.9 | 31.64 | 6.225 | 6.38 | 0.03 | Betourney et al. [6] |
4 | Basalt | 79.1 | 17.45 | 4.313 | 4.53 | 0.05 | Betourney et al. [6] |
5 | Diabase | 322.9 | 15.85 | 20.324 | 20.37 | 0.06 | Betourney et al. [6] |
6 | Diabase | 532 | 34.6 | 15.310 | 15.38 | 0.03 | Brace [8] |
7 | Diorite | 67.8 | 10.82 | 6.103 | 6.27 | 0.09 | Betourney et al. [6] |
8 | Diorite | 124.3 | 18.57 | 6.548 | 6.69 | 0.05 | |
9 | Diorite | 279.7 | 25.21 | 11.004 | 11.09 | 0.04 | Mogi [50] |
10 | Gabbro | 379.1 | 25.1 | 15.033 | 15.10 | 0.04 | Broch [9] |
11 | Gabbro | 226.9 | 10.92 | 20.738 | 20.78 | 0.09 | |
12 | Granite | 241.3 | 11.34 | 21.227 | 21.28 | 0.09 | Betourney et al. [6] |
13 | Granite | 318.2 | 10.31 | 30.816 | 30.86 | 0.10 | Brace [8] |
14 | Granite | 260 | 18.56 | 13.936 | 14.01 | 0.05 | Franklin and Hoek [20] |
15 | Granite | 220.6 | 8.28 | 26.589 | 26.64 | 0.12 | Heard et al. [28] |
16 | Granite | 193.1 | 13.83 | 13.884 | 13.96 | 0.07 | Johnson et al. [43] |
17 | Granite | 115.7 | 9.83 | 11.681 | 11.77 | 0.10 | |
18 | Granite | 163.5 | 10.92 | 14.900 | 14.97 | 0.09 | |
19 | Granite | 306.5 | 23.24 | 13.115 | 13.19 | 0.04 | Mogi [50] |
20 | Granite | 337.7 | 15.45 | 21.812 | 21.86 | 0.06 | Mogi [51] |
21 | Granite | 93.8 | 2.75 | 34.034 | 34.11 | 0.36 | Schwartz [63] |
22 | Granite breccia | 334.9 | 21.06 | 15.837 | 15.90 | 0.05 | Betourney et al. [6] |
23 | Granodiorite | 113.1 | 10.16 | 11.043 | 11.13 | 0.10 | Betourney et al. [6] |
24 | Granodiorite | 259.1 | 14.23 | 18.150 | 18.21 | 0.07 | Dayre and Giraud [13] |
25 | Lamprophyre | 116.3 | 14.02 | 8.174 | 8.30 | 0.07 | Betourney et al. [6] |
26 | Quartzdiorite | 174.7 | 9.53 | 18.274 | 18.33 | 0.10 | Betourney et al. [6] |
27 | Quartzdiorite | 173.4 | 14.47 | 11.903 | 11.98 | 0.07 | |
28 | Quartzdiorite | 98.6 | 7.35 | 13.343 | 13.41 | 0.14 | |
29 | Quartzdiorite | 273.8 | 15.71 | 17.371 | 17.43 | 0.06 | Broch [9] |
30 | Quartzdiorite | 209.7 | 9.98 | 20.965 | 21.01 | 0.10 | |
31 | Quartzdiorite | 300.2 | 23.57 | 12.658 | 12.74 | 0.04 | Franklin and Hoek [20] |
32 | Rhyolite | 106.4 | 18.96 | 5.430 | 5.61 | 0.05 | Betourney et al. [6] |
Appendix 2: Published values of triaxial parameters for Hoek–Brown criterion using data set for sedimentary rocks [66]
No | Rock name | \(\sigma_{c}\)(MPa) | \(\sigma_{t}\)(MPa) | m i | \(\frac{{\sigma_{c} }}{{\sigma_{t} }}\) | \(\frac{{m_{i} }}{{\sigma_{c} }}\) | Source |
---|---|---|---|---|---|---|---|
1 | Dolomite | 145.3 | 18.2 | 7.859 | 7.98 | 0.05 | Brace [8] |
2 | Dolomite | 524.5 | 64.22 | 8.044 | 8.17 | 0.02 | |
3 | Dolomite | 218.7 | 12.46 | 17.493 | 17.55 | 0.08 | Mogi [60] |
4 | Limestone | 65.9 | 4.47 | 14.663 | 14.74 | 0.22 | Betourney et al. [6] |
5 | Limestone | 128.8 | 9.85 | 12.992 | 13.08 | 0.10 | |
6 | Limestone | 94.9 | 13.15 | 7.076 | 7.22 | 0.07 | Franklin and Hoek [20] |
7 | Limestone | 53.6 | 7.84 | 6.686 | 6.84 | 0.12 | |
8 | Limestone | 217.9 | 39.62 | 5.319 | 5.50 | 0.02 | Gnirk and Cheathan [22] |
9 | Limestone | 45 | 6.26 | 7.038 | 7.19 | 0.16 | Horino and Ellickson [39] |
10 | Limestone | 54.7 | 9.3 | 5.714 | 5.88 | 0.10 | |
11 | Limestone | 58.7 | 10.63 | 5.345 | 5.52 | 0.09 | |
12 | Limestone | 58 | 9.56 | 5.905 | 6.07 | 0.10 | |
13 | Limestone | 63.4 | 8.65 | 7.197 | 7.33 | 0.11 | |
14 | Limestone | 49.2 | 6.09 | 7.957 | 8.08 | 0.16 | |
15 | Limestone | 100.3 | 9.45 | 10.517 | 10.61 | 0.10 | Stowe [71] |
16 | Sandstone | 85.2 | 9.87 | 8.520 | 8.63 | 0.10 | Aldritch [2] |
17 | Sandstone | 75.5 | 8.72 | 8.543 | 8.66 | 0.11 | |
18 | Sandstone | 149.9 | 6.51 | 22.996 | 23.03 | 0.15 | Betourney et al. [6] |
19 | Sandstone | 129.9 | 18.15 | 7.017 | 7.16 | 0.05 | Borecki et al. [7] |
20 | Sandstone | 112.9 | 14.68 | 7.561 | 7.69 | 0.07 | |
21 | Sandstone | 109 | 8.0 | 13.367 | 13.44 | 0.12 | Dlugosz et al. [14] |
22 | Sandstone | 21.7 | 0.88 | 24.537 | 24.66 | 1.13 | Dunikowski [16] |
23 | Sandstone | 152.4 | 16.54 | 9.110 | 9.21 | 0.06 | Everling [18] |
24 | Sandstone | 74.2 | 5.98 | 12.33 | 12.41 | 0.17 | Franklin and Hoek [20] |
25 | Sandstone | 74.6 | 4.28 | 17.378 | 17.43 | 0.23 | |
26 | Sandstone | 211.7 | 18.09 | 11.618 | 11.70 | 0.05 | |
27 | Sandstone | 41.5 | 2.92 | 14.123 | 14.21 | 0.34 | Glushko and Kirnichanskiy [21] |
28 | Sandstone | 65.4 | 5.79 | 11.206 | 11.30 | 0.17 | Gowd and Rummel [23] |
29 | Sandstone | 93.9 | 3.78 | 24.761 | 24.84 | 0.26 | Gustkewicz [24] |
30 | Sandstone | 42.6 | 1.22 | 35.014 | 34.92 | 0.82 | |
31 | Sandstone | 150.6 | 14.8 | 10.079 | 10.18 | 0.07 | Hareland et al. [25] |
32 | Sandstone | 75.4 | 5.25 | 14.288 | 14.36 | 0.19 | |
33 | Sandstone | 93.3 | 9.74 | 9.474 | 9.58 | 0.10 | |
34 | Sandstone | 10 | 0.4 | 25.314 | 25.00 | 2.53 | Harza Engg Co. [26] |
35 | Sandstone | 163 | 10.41 | 15.602 | 15.66 | 0.10 | Hoshino et al. [40] |
36 | Sandstone | 173.7 | 14.9 | 11.570 | 11.66 | 0.07 | Hossaini and Vutukuri [41] |
37 | Sandstone | 236.1 | 56.05 | 3.975 | 4.21 | 0.02 | Ilnitskaya et al. [42] |
38 | Sandstone | 76.9 | 6.26 | 12.191 | 12.28 | 0.16 | Kovári and Tisa [44] |
39 | Sandstone | 72.1 | 5.48 | 13.082 | 13.16 | 0.18 | |
40 | Sandstone | 110.7 | 7.26 | 15.174 | 15.25 | 0.14 | Kuntysh [45] |
41 | Sandstone | 98.8 | 8.09 | 12.125 | 12.21 | 0.12 | Kwasniewski [46] |
42 | Sandstone | 103.6 | 10.63 | 9.643 | 9.75 | 0.09 | |
43 | Sandstone | 104.2 | 13.39 | 7.652 | 7.78 | 0.07 | |
44 | Sandstone | 44.2 | 3.39 | 12.972 | 13.04 | 0.29 | Misra [49] |
45 | Sandstone | 61 | 5.75 | 10.510 | 10.61 | 0.17 | |
46 | Sandstone | 48.2 | 2.87 | 16.759 | 16.79 | 0.35 | |
47 | Sandstone | 99.5 | 7.39 | 13.379 | 13.46 | 0.13 | |
48 | Sandstone | 162.1 | 16.47 | 9.741 | 9.84 | 0.06 | |
49 | Sandstone | 102.1 | 5.82 | 17.498 | 17.54 | 0.17 | |
50 | Sandstone | 110.3 | 6.33 | 17.382 | 17.42 | 0.16 | |
51 | Sandstone | 86.7 | 4.38 | 19.734 | 19.79 | 0.23 | |
52 | Sandstone | 72.7 | 3.8 | 19.065 | 19.13 | 0.26 | Murrel [53] |
53 | Sandstone | 28.9 | 3.93 | 7.216 | 7.35 | 0.25 | Ramamurthy [56] |
54 | Sandstone | 111.9 | 14.21 | 7.748 | 7.87 | 0.07 | Ramez [57] |
55 | Sandstone | 116.4 | 5.86 | 19.813 | 19.86 | 0.17 | Rao et al. [58] |
56 | Sandstone | 104.9 | 5.88 | 17.793 | 17.84 | 0.17 | |
57 | Sandstone | 119.2 | 7.18 | 16.551 | 16.60 | 0.14 | |
58 | Sandstone | 54.8 | 1.56 | 35.107 | 35.13 | 0.64 | Schwartz [63] |
59 | Sandstone | 70.8 | 7.68 | 9.115 | 9.22 | 0.13 | Sheorey et al. [67] |
60 | Sandstone | 64.8 | 5.02 | 12.824 | 12.91 | 0.20 | Singh et al. [69] |
61 | Sandstone | 62.9 | 9.64 | 6.370 | 6.52 | 0.10 | Vutukuri and Farough Hossani [75] |
62 | Sandstone | 45 | 3.04 | 14.754 | 14.80 | 0.33 | Wilhelmi and Somerton [83] |
63 | Siltstone | 65.2 | 6.73 | 9.582 | 9.69 | 0.15 | Hobbs [30] |
64 | Shale | 220.6 | 33.85 | 6.364 | 6.52 | 0.03 | McLamore and Gray [47] |
65 | Shale | 184.7 | 25.29 | 7.164 | 7.30 | 0.04 | |
66 | Shale | 154 | 17.56 | 8.655 | 8.77 | 0.06 | |
67 | Shale | 84.5 | 5.35 | 15.737 | 15.79 | 0.19 | |
68 | Shale | 185 | 26.47 | 6.848 | 6.99 | 0.04 | |
69 | Shale | 190.2 | 27.28 | 6.830 | 6.97 | 0.04 | |
70 | Shale | 175 | 21.34 | 8.078 | 8.20 | 0.05 | |
71 | Shale | 193.9 | 26.86 | 7.082 | 7.22 | 0.04 | |
72 | Shale | 112 | 23.52 | 4.555 | 4.76 | 0.04 | |
73 | Shale | 107.9 | 26.9 | 3.762 | 4.01 | 0.03 | |
74 | Shale | 78.8 | 15.73 | 4.808 | 5.01 | 0.06 | |
75 | Shale | 57.4 | 11.15 | 4.959 | 5.15 | 0.09 | |
76 | Shale | 66.8 | 13.15 | 4.886 | 5.08 | 0.07 | |
77 | Shale | 93.2 | 22.07 | 3.986 | 4.22 | 0.04 | |
78 | Shale | 99.3 | 21.88 | 4.318 | 4.54 | 0.04 | |
79 | Shale | 58 | 8.08 | 7.043 | 7.18 | 0.12 | |
80 | Shale | 80.4 | 13.76 | 5.672 | 5.84 | 0.07 | Sheorey et al. [67] |
81 | Shale | 66.9 | 4.21 | 15.826 | 15.89 | 0.24 | Singh [68] |
82 | Shale | 25.9 | 2.23 | 11.509 | 11.61 | 0.44 | |
83 | Shale | 28.7 | 3.72 | 7.568 | 7.72 | 0.26 | |
84 | Shale | 10 | 0.4 | 25.314 | 25.00 | 2.53 | |
85 | Coal | 14.1 | 0.93 | 15.1232 | 15.16 | 1.07 | Hobbs [29] |
86 | Coal | 23.6 | 2.26 | 10.334 | 10.44 | 0.44 | |
87 | Coal | 58.9 | 13.27 | 4.213 | 4.44 | 0.07 | |
88 | Coal | 36.5 | 4.13 | 8.728 | 8.84 | 0.24 | |
89 | Coal | 30.3 | 3.45 | 8.673 | 8.78 | 0.29 | |
90 | Coal | 40.1 | 3.96 | 10.034 | 10.13 | 0.25 | |
91 | Coal | 28.2 | 1.63 | 17.300 | 17.30 | 0.61 | |
92 | Coal | 26.2 | 2.1 | 12.401 | 12.48 | 0.47 | |
93 | Coal | 10.8 | 0.59 | 18.403 | 18.31 | 1.70 | |
94 | Coal | 10.6 | 0.38 | 28.021 | 27.89 | 2.64 | |
95 | Coal | 32.3 | 3.17 | 10.101 | 10.19 | 0.31 | |
96 | Coal | 31.3 | 3.47 | 8.915 | 9.02 | 0.28 | |
97 | Coal | 18.7 | 1.46 | 12.763 | 12.81 | 0.68 | |
98 | Coal | 15.6 | 0.61 | 25.643 | 25.57 | 1.64 | |
99 | Coal | 35.6 | 3.97 | 8.871 | 8.97 | 0.25 | |
100 | Coal | 33 | 3.13 | 10.420 | 10.54 | 0.32 | |
101 | Coal | 38 | 4.13 | 9.090 | 9.20 | 0.24 | |
102 | Coal | 17.2 | 1.33 | 12.940 | 12.93 | 0.75 | |
103 | Coal | 19.6 | 1.35 | 14.483 | 14.52 | 0.74 | |
104 | Coal | 32.5 | 3.29 | 9.784 | 9.88 | 0.30 | |
105 | Coal | 25.1 | 2.12 | 11.792 | 11.84 | 0.47 | |
106 | Coal | 28.9 | 1.87 | 15.382 | 15.45 | 0.53 | |
107 | Coal | 17.1 | 0.97 | 17.579 | 17.63 | 1.03 | Shea-Albin et al. [64] |
Appendix 3: Published values of triaxial parameters for Hoek–Brown criterion using data set for metamorphic rocks [66]
No | Rock name | \(\sigma_{c}\)(MPa) | \(\sigma_{t}\)(MPa) | m i | \(\frac{{\sigma_{c} }}{{\sigma_{\tau } }}\) | \(\frac{{m_{i} }}{{\sigma_{c} }}\) | Source |
---|---|---|---|---|---|---|---|
1 | Schist | 133.6 | 6.59 | 20.246 | 20.27 | 0.15 | Barat [5] |
2 | Slate | 148.6 | 18.64 | 7.844 | 7.97 | 0.05 | Attewell and Sandford [4] |
3 | Slate | 108.7 | 28.66 | 3.528 | 3.79 | 0.03 | |
4 | Slate | 53.4 | 27.5 | 1.428 | 1.94 | 0.03 | |
5 | Slate | 62.3 | 21.7 | 1.980 | 2.87 | 0.03 | |
6 | Slate | 98 | 41.56 | 1.933 | 2.36 | 0.02 | |
7 | Slate | 129.4 | 39.96 | 2.930 | 3.24 | 0.02 | |
8 | Slate | 178.3 | 19.97 | 8.819 | 8.93 | 0.05 | |
9 | Slate | 57.8 | 1.86 | 30.965 | 31.08 | 0.54 | Donath [15] |
10 | Slate | 14.5 | 0.64 | 22.700 | 22.66 | 1.57 | |
11 | Slate | 44.2 | 4.6 | 9.504 | 9.61 | 0.22 | |
12 | Slate | 68.1 | 4.03 | 16.853 | 16.90 | 0.25 | |
13 | Slate | 155.1 | 10.85 | 14.217 | 14.29 | 0.09 | |
14 | Slate | 167.6 | 12.22 | 13.644 | 13.72 | 0.08 | Fayed [19] |
15 | Slate | 242 | 39.35 | 5.988 | 6.15 | 0.02 | McLamore and Gray [47] |
16 | Slate | 181.9 | 40.14 | 4.311 | 4.53 | 0.02 | |
17 | Slate | 99.2 | 30.5 | 2.945 | 3.25 | 0.03 | |
18 | Slate | 106.3 | 31.44 | 3.085 | 3.38 | 0.03 | |
19 | Slate | 124 | 27.16 | 4.345 | 4.57 | 0.04 | |
20 | Slate | 162.6 | 34.66 | 4.479 | 4.69 | 0.03 | |
21 | Slate | 220.3 | 44.09 | 4.797 | 5.00 | 0.02 | |
22 | Gneiss | 315.1 | 17.58 | 17.865 | 17.92 | 0.06 | |
23 | Gneiss | 75.3 | 13.63 | 5.343 | 5.52 | 0.07 | |
24 | Gneiss | 221.7 | 13.61 | 16.233 | 16.29 | 0.07 | Broch [9] |
25 | Gneiss | 195.4 | 29.86 | 6.389 | 6.54 | 0.03 | |
26 | Gneiss | 197.7 | 22.29 | 8.759 | 8.87 | 0.04 | |
27 | Gneiss | 106.4 | 11.17 | 9.423 | 9.53 | 0.09 | |
28 | Gniess | 272.8 | 11.32 | 24.061 | 24.10 | 0.09 | Horino and Ellickson [39] |
29 | Gniess | 234.8 | 7.8 | 30.063 | 30.10 | 0.13 | |
30 | Gniess | 222.2 | 7.54 | 29.438 | 29.47 | 0.13 | |
31 | Gniess | 224.8 | 7.66 | 29.301 | 29.35 | 0.13 | |
32 | Gniess | 212.5 | 6.57 | 32.329 | 32.34 | 0.15 | |
33 | Gniess | 252.8 | 9.7 | 26.014 | 26.06 | 0.10 | |
34 | Gniess | 254.2 | 10.93 | 23.229 | 23.26 | 0.09 | |
35 | Gniess | 226.4 | 7.21 | 31.387 | 31.40 | 0.14 | |
36 | Gniess | 267 | 8.98 | 29.700 | 29.73 | 0.11 | |
37 | Quartzite | 144.5 | 19.28 | 7.363 | 7.49 | 0.05 | Betourney et al. [6] |
38 | Quartzite | 657.6 | 21.82 | 30.102 | 30.14 | 0.05 | Brace [8] |
39 | Quartzite | 219 | 13.88 | 15.710 | 15.78 | 0.07 | Chan et al. [11] |
40 | Quartzite | 111.8 | 8.6 | 12.925 | 13.00 | 0.12 | Singh et al. [69] |
41 | Marble | 94.3 | 12.13 | 7.652 | 7.77 | 0.08 | Franklin and Hoek [20] |
42 | Marble | 91.2 | 10.56 | 8.525 | 8.64 | 0.09 | Gnirk and Cheatham [22] |
43 | Marble | 132 | 21.18 | 6.075 | 6.23 | 0.05 | Hoek [31] |
44 | Marble | 104.6 | 16.33 | 6.251 | 6.41 | 0.06 | Kovári and Tisa [44] |
45 | Marble | 109.2 | 15 | 7.145 | 7.28 | 0.07 | Ouyang and Elsworth [54] |
46 | Marble | 49.9 | 6.91 | 7.087 | 7.22 | 0.14 | Schwartz [63] |
Appendix 4: Measured and calculated values of m i based on different methods for igneous rocks
No | Rock name | \(m_{i}\)(measured) | \(\frac{{\sigma_{c} }}{{\sigma_{t} }}\) | \(m_{i}\)(R-index (Cai)) | \(m_{i}\)(UCS based) | \(m_{i}\)(TS based) | \(m_{i}\)(Hoek–Brown (2019)) | \(m_{i}\)(combination method) |
---|---|---|---|---|---|---|---|---|
1 | Agglomerate tuff | 7.93 | 8.05 | 7.92 | 7.69 | 14.03 | 1.26 | 7.00 |
2 | Tuff | 22.96 | 23.01 | 22.97 | 21.27 | 12.20 | 19.67 | 21.88 |
3 | Andesite | 6.23 | 6.38 | 6.22 | 13.54 | 10.34 | -0.79 | 5.63 |
4 | Basalt | 4.31 | 4.53 | 4.31 | 6.90 | 12.36 | -3.06 | 4.10 |
5 | Diabase | 20.32 | 20.37 | 20.32 | 18.99 | 12.72 | 16.42 | 18.84 |
6 | Diabase | 15.31 | 15.38 | 15.31 | 6.17 | 10.06 | 10.27 | 13.61 |
7 | Diorite | 6.10 | 6.27 | 6.11 | 9.55 | 14.26 | -0.93 | 5.53 |
8 | Diorite | 6.55 | 6.69 | 6.54 | 21.32 | 12.13 | -0.41 | 5.88 |
9 | Diorite | 11.00 | 11.09 | 11.00 | 22.50 | 7.21 | 5.01 | 9.62 |
10 | Gabbro | 15.03 | 15.10 | 15.04 | 14.73 | 11.08 | 9.94 | 13.34 |
11 | Gabbro | 20.74 | 20.78 | 20.73 | 15.40 | 14.22 | 16.92 | 19.29 |
12 | Granite | 21.23 | 21.28 | 21.23 | 16.25 | 14.06 | 17.53 | 19.86 |
13 | Granite | 30.82 | 30.86 | 30.83 | 19.50 | 12.13 | 29.32 | 32.14 |
14 | Granite | 13.94 | 14.01 | 13.94 | 8.92 | 11.68 | 8.59 | 12.29 |
15 | Granite | 26.59 | 26.64 | 26.60 | 22.13 | 10.57 | 24.13 | 26.39 |
16 | Granite | 13.88 | 13.96 | 13.89 | 21.92 | 8.86 | 8.53 | 12.24 |
17 | Granite | 11.68 | 11.77 | 11.69 | 21.15 | 9.96 | 5.84 | 10.22 |
18 | Granite | 14.90 | 14.97 | 14.91 | 21.67 | 9.61 | 9.78 | 13.21 |
19 | Granite | 13.12 | 13.19 | 13.11 | 22.64 | 7.42 | 7.58 | 11.52 |
20 | Granite | 21.81 | 21.86 | 21.81 | 22.80 | 8.53 | 18.24 | 20.52 |
21 | Granite | 34.03 | 34.11 | 34.08 | 20.84 | 15.42 | 33.31 | 36.95 |
22 | Granite breccia | 15.84 | 15.90 | 15.84 | 16.21 | 14.54 | 10.92 | 14.13 |
23 | Granodiorite | 11.04 | 11.13 | 11.04 | 9.10 | 13.14 | 5.05 | 9.65 |
24 | Granodiorite | 18.15 | 18.21 | 18.15 | 12.20 | 13.20 | 13.76 | 16.49 |
25 | Lamprophyre | 8.17 | 8.30 | 8.17 | 12.14 | 14.82 | 1.56 | 7.21 |
26 | Quartzdiorite | 18.27 | 18.33 | 18.28 | 8.08 | 13.07 | 13.91 | 16.62 |
27 | Quartzdiorite | 11.90 | 11.98 | 11.90 | 16.86 | 16.02 | 6.10 | 10.41 |
28 | Quartzdiorite | 13.34 | 13.41 | 13.34 | 13.92 | 12.75 | 7.86 | 11.73 |
29 | Quartzdiorite | 17.37 | 17.43 | 17.37 | 10.64 | 14.61 | 12.80 | 15.68 |
30 | Quartzdiorite | 20.97 | 21.01 | 20.96 | 31.69 | 11.99 | 17.20 | 19.56 |
31 | Quartzdiorite | 12.66 | 12.74 | 12.66 | 22.61 | 7.38 | 7.03 | 11.10 |
32 | Rhyolite | 7.36 | 7.49 | 5.43 | 14.36 | 13.24 | 0.58 | 4.99 |
Appendix 5: Measured and calculated values of m i based on different methods for sedimentary rocks
No | Rock name | \(m_{i}\)(measured) | \(\frac{{\sigma_{c} }}{{\sigma_{t} }}\) | \(m_{i}\)(R-index (Cai)) | \(m_{i}\)(UCS based) | \(m_{i}\)(TS based) | \(m_{i}\)(Hoek–Brown (2019)) | \(m_{i}\)(combination method) |
---|---|---|---|---|---|---|---|---|
1 | Dolomite | 7.86 | 7.98 | 7.86 | 21.49 | 8.06 | 1.18 | 6.95 |
2 | Dolomite | 8.04 | 8.17 | 8.04 | 23.51 | 5.23 | 1.41 | 7.10 |
3 | Dolomite | 17.49 | 17.55 | 17.50 | 22.12 | 9.18 | 12.95 | 15.81 |
4 | Limestone | 14.66 | 14.74 | 14.67 | 20.33 | 13.05 | 9.49 | 12.99 |
5 | Limestone | 12.99 | 13.08 | 13.00 | 21.31 | 9.95 | 7.44 | 11.41 |
6 | Limestone | 7.08 | 7.22 | 7.08 | 20.86 | 9.02 | 0.24 | 6.31 |
7 | Limestone | 6.69 | 6.84 | 6.69 | 20.04 | 10.77 | -0.23 | 6.00 |
8 | Limestone | 5.32 | 5.50 | 5.32 | 22.11 | 6.18 | -1.88 | 4.90 |
9 | Limestone | 7.04 | 7.19 | 7.05 | 19.80 | 11.63 | 0.20 | 6.29 |
10 | Limestone | 5.71 | 5.88 | 5.71 | 20.07 | 10.15 | -1.41 | 5.22 |
11 | Limestone | 5.35 | 5.52 | 5.34 | 20.17 | 9.70 | -1.85 | 4.92 |
12 | Limestone | 5.91 | 6.07 | 5.90 | 20.15 | 10.06 | -1.18 | 5.37 |
13 | Limestone | 7.20 | 7.33 | 7.19 | 20.28 | 10.41 | 0.38 | 6.41 |
14 | Limestone | 7.96 | 8.08 | 7.96 | 19.92 | 11.74 | 1.30 | 7.03 |
15 | Limestone | 10.52 | 10.61 | 10.52 | 20.94 | 10.10 | 4.41 | 9.19 |
16 | Sandstone | 8.52 | 8.63 | 8.52 | 20.70 | 9.95 | 1.98 | 7.49 |
17 | Sandstone | 8.54 | 8.66 | 8.54 | 20.53 | 10.38 | 2.01 | 7.51 |
18 | Sandstone | 23.00 | 23.03 | 22.98 | 21.54 | 11.47 | 19.68 | 21.89 |
19 | Sandstone | 7.02 | 7.16 | 7.02 | 21.32 | 8.07 | 0.16 | 6.26 |
20 | Sandstone | 7.56 | 7.69 | 7.56 | 21.11 | 8.68 | 0.82 | 6.71 |
21 | Sandstone | 13.37 | 13.44 | 13.37 | 21.06 | 10.64 | 7.89 | 11.75 |
22 | Sandstone | 24.54 | 24.66 | 24.62 | 18.81 | 22.79 | 21.69 | 23.87 |
23 | Sandstone | 9.11 | 9.21 | 9.11 | 21.56 | 8.33 | 2.69 | 7.98 |
24 | Sandstone | 12.33 | 12.41 | 12.33 | 20.50 | 11.81 | 6.62 | 10.80 |
25 | Sandstone | 17.38 | 17.43 | 17.37 | 20.51 | 13.25 | 12.80 | 15.68 |
26 | Sandstone | 11.62 | 11.70 | 11.62 | 22.06 | 8.08 | 5.75 | 10.16 |
27 | Sandstone | 14.12 | 14.21 | 14.14 | 19.69 | 15.11 | 8.84 | 12.48 |
28 | Sandstone | 11.21 | 11.30 | 11.21 | 20.32 | 11.94 | 5.25 | 9.79 |
29 | Sandstone | 24.76 | 24.84 | 24.80 | 20.84 | 13.83 | 21.91 | 24.10 |
30 | Sandstone | 35.01 | 34.92 | 34.89 | 19.72 | 20.38 | 34.31 | 38.20 |
31 | Sandstone | 10.08 | 10.18 | 10.08 | 21.55 | 8.66 | 3.88 | 8.81 |
32 | Sandstone | 14.29 | 14.36 | 14.29 | 20.53 | 12.35 | 9.03 | 12.62 |
33 | Sandstone | 9.47 | 9.58 | 9.47 | 20.83 | 9.99 | 3.14 | 8.30 |
34 | Sandstone | 25.31 | 25.00 | 24.96 | 17.82 | 29.87 | 22.11 | 24.30 |
35 | Sandstone | 15.60 | 15.66 | 15.59 | 21.66 | 9.77 | 10.62 | 13.89 |
36 | Sandstone | 11.57 | 11.66 | 11.57 | 21.76 | 8.64 | 5.70 | 10.12 |
37 | Sandstone | 3.98 | 4.21 | 3.97 | 22.23 | 5.48 | -3.46 | 3.82 |
38 | Sandstone | 12.19 | 12.28 | 12.20 | 20.55 | 11.63 | 6.47 | 10.68 |
39 | Sandstone | 13.08 | 13.16 | 13.08 | 20.46 | 12.17 | 7.54 | 11.49 |
40 | Sandstone | 15.17 | 15.25 | 15.18 | 21.09 | 11.05 | 10.11 | 13.48 |
41 | Sandstone | 12.13 | 12.21 | 12.13 | 20.92 | 10.65 | 6.38 | 10.62 |
42 | Sandstone | 9.64 | 9.75 | 9.64 | 20.99 | 9.70 | 3.35 | 8.44 |
43 | Sandstone | 7.65 | 7.78 | 7.65 | 21.00 | 8.96 | 0.93 | 6.78 |
44 | Sandstone | 12.97 | 13.04 | 12.96 | 19.77 | 14.35 | 7.40 | 11.38 |
45 | Sandstone | 10.51 | 10.61 | 10.51 | 20.22 | 11.97 | 4.41 | 9.19 |
46 | Sandstone | 16.76 | 16.79 | 16.73 | 19.89 | 15.20 | 12.02 | 15.03 |
47 | Sandstone | 13.38 | 13.46 | 13.39 | 20.93 | 10.99 | 7.92 | 11.77 |
48 | Sandstone | 9.74 | 9.84 | 9.74 | 21.66 | 8.35 | 3.47 | 8.52 |
49 | Sandstone | 17.50 | 17.54 | 17.49 | 20.97 | 11.92 | 12.94 | 15.80 |
50 | Sandstone | 17.38 | 17.42 | 17.37 | 21.08 | 11.58 | 12.79 | 15.67 |
51 | Sandstone | 19.73 | 19.79 | 19.74 | 20.73 | 13.14 | 15.71 | 18.20 |
52 | Sandstone | 19.07 | 19.13 | 19.08 | 20.47 | 13.80 | 14.89 | 17.48 |
53 | Sandstone | 7.22 | 7.35 | 7.22 | 19.19 | 13.64 | 0.41 | 6.43 |
54 | Sandstone | 7.75 | 7.87 | 7.75 | 21.10 | 8.78 | 1.05 | 6.86 |
55 | Sandstone | 19.81 | 19.86 | 19.81 | 21.16 | 11.90 | 15.79 | 18.28 |
56 | Sandstone | 17.79 | 17.84 | 17.78 | 21.01 | 11.88 | 13.30 | 16.11 |
57 | Sandstone | 16.55 | 16.60 | 16.54 | 21.20 | 11.09 | 11.78 | 14.83 |
58 | Sandstone | 35.11 | 35.13 | 35.10 | 20.07 | 18.73 | 34.57 | 38.53 |
59 | Sandstone | 9.12 | 9.22 | 9.11 | 20.44 | 10.84 | 2.70 | 7.99 |
60 | Sandstone | 12.82 | 12.91 | 12.83 | 20.31 | 12.54 | 7.24 | 11.26 |
61 | Sandstone | 6.37 | 6.52 | 6.37 | 20.27 | 10.03 | -0.61 | 5.74 |
62 | Sandstone | 14.75 | 14.80 | 14.74 | 19.80 | 14.90 | 9.57 | 13.05 |
63 | Siltstone | 9.58 | 9.69 | 9.58 | 20.32 | 11.34 | 3.28 | 8.39 |
64 | Shale | 6.35 | 6.52 | 6.36 | 22.13 | 6.52 | -0.62 | 5.74 |
65 | Shale | 7.16 | 7.30 | 7.17 | 21.86 | 7.20 | 0.34 | 6.38 |
66 | Shale | 8.66 | 8.77 | 8.66 | 21.58 | 8.16 | 2.15 | 7.61 |
67 | Shale | 15.74 | 15.79 | 15.73 | 20.69 | 12.27 | 10.79 | 14.02 |
68 | Shale | 6.85 | 6.99 | 6.85 | 21.86 | 7.09 | -0.04 | 6.13 |
69 | Shale | 6.83 | 6.97 | 6.83 | 21.90 | 7.02 | -0.06 | 6.11 |
70 | Shale | 8.08 | 8.20 | 8.08 | 21.77 | 7.64 | 1.45 | 7.13 |
71 | Shale | 7.08 | 7.22 | 7.08 | 21.93 | 7.06 | 0.24 | 6.31 |
72 | Shale | 4.56 | 4.76 | 4.55 | 21.10 | 7.39 | -2.78 | 4.29 |
73 | Shale | 3.76 | 4.01 | 3.76 | 21.05 | 7.05 | -3.71 | 3.65 |
74 | Shale | 4.81 | 5.01 | 4.81 | 20.59 | 8.48 | -2.48 | 4.50 |
75 | Shale | 4.96 | 5.15 | 4.95 | 20.14 | 9.54 | -2.31 | 4.61 |
76 | Shale | 4.89 | 5.08 | 4.88 | 20.35 | 9.02 | -2.39 | 4.55 |
77 | Shale | 3.99 | 4.22 | 3.99 | 20.83 | 7.55 | -3.45 | 3.83 |
78 | Shale | 4.32 | 4.54 | 4.32 | 20.93 | 7.57 | -3.06 | 4.10 |
79 | Shale | 7.04 | 7.18 | 7.04 | 20.15 | 10.65 | 0.19 | 6.28 |
80 | Shale | 5.67 | 5.84 | 5.67 | 20.62 | 8.88 | -1.45 | 5.18 |
81 | Shale | 15.83 | 15.89 | 15.83 | 20.36 | 13.32 | 10.91 | 14.12 |
82 | Shale | 11.51 | 11.61 | 11.53 | 19.05 | 16.57 | 5.65 | 10.08 |
83 | Shale | 7.57 | 7.72 | 7.59 | 19.18 | 13.90 | 0.85 | 6.73 |
84 | Shale | 25.31 | 25.00 | 24.96 | 17.82 | 29.87 | 22.11 | 24.30 |
85 | Coal | 15.12 | 15.16 | 15.10 | 18.25 | 22.37 | 10.01 | 13.40 |
86 | Coal | 10.33 | 10.44 | 10.35 | 18.92 | 16.49 | 4.20 | 9.04 |
87 | Coal | 4.21 | 4.44 | 4.21 | 20.17 | 8.99 | -3.18 | 4.02 |
88 | Coal | 8.73 | 8.84 | 8.72 | 19.51 | 13.41 | 2.23 | 7.66 |
89 | Coal | 8.67 | 8.78 | 8.67 | 19.26 | 14.27 | 2.16 | 7.62 |
90 | Coal | 10.03 | 10.13 | 10.03 | 19.64 | 13.61 | 3.82 | 8.77 |
91 | Coal | 17.30 | 17.30 | 17.24 | 19.16 | 18.45 | 12.64 | 15.54 |
92 | Coal | 12.40 | 12.48 | 12.40 | 19.06 | 16.91 | 6.71 | 10.86 |
93 | Coal | 18.40 | 18.31 | 18.25 | 17.92 | 26.14 | 13.88 | 16.59 |
94 | Coal | 28.02 | 27.89 | 27.86 | 17.89 | 30.40 | 25.67 | 28.03 |
95 | Coal | 10.10 | 10.19 | 10.09 | 19.34 | 14.69 | 3.89 | 8.82 |
96 | Coal | 8.92 | 9.02 | 8.91 | 19.30 | 14.24 | 2.45 | 7.82 |
97 | Coal | 12.76 | 12.81 | 12.73 | 18.62 | 19.16 | 7.11 | 11.16 |
98 | Coal | 25.64 | 25.57 | 25.53 | 18.38 | 25.85 | 22.82 | 25.02 |
99 | Coal | 8.87 | 8.97 | 8.86 | 19.48 | 13.60 | 2.39 | 7.77 |
100 | Coal | 10.42 | 10.54 | 10.45 | 19.37 | 14.75 | 4.33 | 9.13 |
101 | Coal | 9.09 | 9.20 | 9.09 | 19.57 | 13.41 | 2.68 | 7.97 |
102 | Coal | 12.94 | 12.93 | 12.86 | 18.51 | 19.78 | 7.27 | 11.28 |
103 | Coal | 14.48 | 14.52 | 14.45 | 18.68 | 19.68 | 9.22 | 12.77 |
104 | Coal | 9.78 | 9.88 | 9.78 | 19.35 | 14.50 | 3.51 | 8.55 |
105 | Coal | 11.79 | 11.84 | 11.76 | 19.01 | 16.86 | 5.92 | 10.28 |
106 | Coal | 15.38 | 15.45 | 15.39 | 19.19 | 17.60 | 10.37 | 13.68 |
107 | Coal | 17.58 | 17.63 | 17.57 | 18.50 | 22.05 | 13.04 | 15.88 |
Appendix 6: Measured and calculated values of m i based on different methods for metamorphic rocks
No | Rock name | \(m_{i}\)(measured) | \(\frac{{\sigma_{c} }}{{\sigma_{t} }}\) | \(m_{i}\)(R-index (Cai)) | \(m_{i}\)(UCS based) | \(m_{i}\)(TS based) | \(m_{i}\)(Hoek–Brown (2019)) | \(m_{i}\)(combination method) |
---|---|---|---|---|---|---|---|---|
1 | Schist | 20.25 | 20.27 | 20.22 | 8.41 | 11.73 | 16.30 | 18.73 |
2 | Slate | 7.84 | 7.97 | 7.85 | 8.47 | 6.23 | 1.17 | 6.94 |
3 | Slate | 3.53 | 3.79 | 3.53 | 8.29 | 4.80 | -3.97 | 3.46 |
4 | Slate | 1.43 | 1.94 | 1.43 | 7.88 | 4.92 | -6.25 | - |
5 | Slate | 1.98 | 2.87 | 2.52 | 7.97 | 5.68 | -5.11 | 2.59 |
6 | Slate | 1.93 | 2.36 | 1.93 | 8.23 | 3.83 | -5.74 | 1.98 |
7 | Slate | 2.93 | 3.24 | 2.93 | 8.39 | 3.92 | -4.66 | 2.95 |
8 | Slate | 8.82 | 8.93 | 8.82 | 8.58 | 5.98 | 2.34 | 7.74 |
9 | Slate | 30.97 | 31.08 | 31.04 | 7.93 | 25.31 | 29.58 | 32.44 |
10 | Slate | 22.70 | 22.66 | 22.61 | 7.20 | 48.42 | 19.23 | 21.46 |
11 | Slate | 9.50 | 9.61 | 9.50 | 7.78 | 14.60 | 3.18 | 8.32 |
12 | Slate | 16.85 | 16.90 | 16.84 | 8.02 | 15.82 | 12.14 | 15.13 |
13 | Slate | 14.22 | 14.29 | 14.22 | 8.49 | 8.66 | 8.94 | 12.56 |
14 | Slate | 13.64 | 13.72 | 13.64 | 8.54 | 8.06 | 8.23 | 12.01 |
15 | Slate | 5.99 | 6.15 | 5.99 | 22.27 | 6.19 | -1.08 | 5.44 |
16 | Slate | 4.31 | 4.53 | 4.31 | 21.83 | 6.15 | -3.07 | 4.10 |
17 | Slate | 2.95 | 3.25 | 2.94 | 20.92 | 6.76 | -4.64 | 2.96 |
18 | Slate | 3.09 | 3.38 | 3.09 | 21.03 | 6.69 | -4.48 | 3.09 |
19 | Slate | 4.35 | 4.57 | 4.35 | 21.25 | 7.03 | -3.02 | 4.13 |
20 | Slate | 4.48 | 4.69 | 4.48 | 21.66 | 6.47 | -2.87 | 4.23 |
21 | Slate | 4.80 | 5.00 | 4.80 | 22.13 | 5.95 | -2.49 | 4.49 |
22 | Gneiss | 17.87 | 17.92 | 17.87 | 8.93 | 6.46 | 13.41 | 16.19 |
23 | Gneiss | 5.34 | 5.52 | 5.34 | 8.07 | 7.54 | -1.84 | 4.92 |
24 | Gneiss | 16.23 | 16.29 | 16.23 | 8.71 | 7.55 | 11.40 | 14.52 |
25 | Gneiss | 6.39 | 6.54 | 6.39 | 8.63 | 4.68 | -0.59 | 5.76 |
26 | Gneiss | 8.76 | 8.87 | 8.76 | 8.64 | 5.59 | 2.27 | 7.69 |
27 | Gneiss | 9.42 | 9.53 | 9.42 | 8.27 | 8.51 | 3.08 | 8.25 |
28 | Gneiss | 24.06 | 24.10 | 24.06 | 22.46 | 9.49 | 21.00 | 23.19 |
29 | Gneiss | 30.06 | 30.10 | 30.07 | 22.23 | 10.78 | 28.39 | 31.06 |
30 | Gneiss | 29.44 | 29.47 | 29.44 | 22.14 | 10.91 | 27.61 | 30.18 |
31 | Gneiss | 29.30 | 29.35 | 29.31 | 22.16 | 10.85 | 27.46 | 30.01 |
32 | Gneiss | 32.33 | 32.34 | 32.31 | 22.07 | 11.44 | 31.14 | 34.29 |
33 | Gneiss | 26.01 | 26.06 | 26.02 | 22.34 | 10.01 | 23.42 | 25.64 |
34 | Gneiss | 23.23 | 23.26 | 23.21 | 22.35 | 9.61 | 19.97 | 22.17 |
35 | Gneiss | 31.39 | 31.40 | 31.37 | 22.17 | 11.08 | 29.98 | 32.91 |
36 | Gneiss | 29.70 | 29.73 | 29.70 | 22.43 | 10.28 | 27.93 | 30.54 |
37 | Quartzite | 7.36 | 7.49 | 7.36 | 8.45 | 6.11 | 5.8 | 6.54 |
38 | Quartzite | 30.10 | 30.14 | 30.10 | 9.40 | 5.66 | 28.43 | 31.11 |
39 | Quartzite | 15.72 | 15.78 | 15.71 | 8.70 | 7.46 | 10.77 | 14.00 |
40 | Quartzite | 12.93 | 13.00 | 12.92 | 21.10 | 10.43 | 7.35 | 11.34 |
41 | Marble | 7.65 | 7.77 | 7.65 | 20.85 | 9.27 | 0.92 | 6.77 |
42 | Marble | 8.53 | 8.64 | 8.52 | 20.80 | 9.72 | 1.98 | 7.50 |
43 | Marble | 6.08 | 6.23 | 6.07 | 21.35 | 7.66 | -0.97 | 5.50 |
44 | Marble | 6.25 | 6.41 | 6.25 | 21.00 | 8.37 | -0.76 | 5.65 |
45 | Marble | 7.15 | 7.28 | 7.14 | 21.07 | 8.62 | 0.31 | 6.37 |
46 | Marble | 7.09 | 7.22 | 7.08 | 19.94 | 11.24 | 0.24 | 6.32 |
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
Davarpanah, S.M., Sharghi, M., Vásárhelyi, B. et al. Characterization of Hoek–Brown constant mi of quasi-isotropic intact rock using rigidity index approach. Acta Geotech. 17, 877–902 (2022). https://doi.org/10.1007/s11440-021-01229-2
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s11440-021-01229-2