Introduction

Tunnelling through heterogeneous rock masses is a major challenge that can impact the tunnel advancement significantly especially in the case of mechanised tunnelling (TBM). TBMs are usually selected for specific ground conditions and unexpected variances within the ground model and its mechanical behaviour, for instance, reduction in rock mass quality through faulting and folding or through lithological variation can lead to increased downtime, delivery delays and overall progress rates. Accurately predicting rock behaviour is paramount to the success of tunnelling projects; mistakes adversely affect both time and costs (Paraskevopoulou and Benardos 2012, 2013; Benardos et al. 2013; Bilgin et al. 2014; Paraskevopoulou and Boutsis 2020). A broad range of empirical models have been introduced to predict TBM performance. These are typically based on specific sites, geology and/or limited data, often leading to inaccurate predictions; especially when used outside their original applications and without good judgement.

It should be stated that in this paper, the heterogeneity is considered to be from the natural lithological variations in stratigraphic sequences using as a case study the Blue Lias Formation (BLI) formation of the Bristol Channel Basin (BCB) (Fig. 1). The Blue Lias Formation (BLI), as a result of fluctuating shallow seas, is characterised by its layered rock mass, comprising very strong limestone, interbedded with weak mudstone and shale layers (Hobbs et al. 2012). BLI is a representative rock mass when considering heterogeneity and for this purpose, the BLI is investigated in this study. BLI’s layering of limestone and mudstone/shale results in heterogeneous tunnelling conditions whilst directly hindering sound ground behaviour predictions and thus TBM performance which few empirical models currently address.

Fig. 1
figure 1

Distribution of the Lias Group and position of field localities (modified Simms et al. 2004; BGS 2019)

It is evident that a new approach/methodology is required for estimating machine performance in heterogeneous materials based on the overall rock mass behaviour. It is also common that available borehole data is often sparse and inadequate. Hence, it is common, practicable and often necessary, to compile predictions using only desk study information and field reconnaissance at least at the preliminary design stages of a tunnelling project. The latter forms the basis of this research work in which the rock mass is characterised by evaluating geotechnical properties and mechanical behaviour based on fieldwork observations and laboratory testing results. This research also addresses critical controls on the TBM performance and provides a comprehensive review of relevant models; compared to produce accurate performance estimations within the BLI. It is shown in the following sections that the Hassanpour et al. 2009 model gives better results in such heterogeneous environments. The aim of this paper is to propose a modified approach for predicting TBM performance in heterogeneous environments based on existing empirical models using primary collection datasets from field observations, in situ and lab testing.

The site and geology

Although several sites show natural lithological variations in stratigraphic sequences, the BLI which is exposed on the north and south shore of the BCB is selected in this research work (Fig. 2a). A desk study of published data of the BCB is completed, including review of reports, memoirs, satellite and geological maps aiming at developing a conceptual geological model and evaluate the rock mass behaviour with regard to TBM performance. It should be noted that field work was intentionally conducted to create an original dataset that can be further analysed to determine the geotechnical model.

Fig. 2
figure 2

a. Lower Jurassic palaeogeography (modified after Simms et al. 2004); b. Stratigraphy of the Lias group in the BCB (modified after Cox et al. (1999) and Simms et al. (2004)); and, c. Main structure of the BCB (modified after Glen et al. 2005).

Geological setting

The BCB is an exhumed fault-bounded graben, which developed in the early Mesozoic due to gradual rift-related subsidence. The basement rock consists of Devonian Old Red Sandstone and Carboniferous Limestone. This is overlain by Triassic (Mercia Mudstone Group and Penarth Group) and Early Jurassic (Lias Group) basin-fill deposits, of up to 2.25 km in thickness. The Lias Group was deposited in warm, shallow seas, similar to the modern Mediterranean. The Jurassic, basin subsidence and marine deposition occurred at similar rates, maintaining shallow water depth and building up the thick succession of the Lias Group. Sea-level fluctuations resulted in limestone interbedded with calcareous shale and mudstones. Within the BCB, a major difference in geological history between S. Wales and Somerset is the weathering domains, controlled by the extent of glaciation and peri glaciation (Hobbs et al. 2012).

The stratigraphy of the BCB Lias Group, summarised in Fig. 2a, has been investigated by numerous authors. Cox et al. (1999) introduced a lithostratigraphic framework, advising formational nomenclature as opposed to division into Lower, Middle and Upper. The Blue Lias previously formed part of the ‘Lower Lias’ along with the overlying Charmouth Mudstone. Whittaker and Green (1983), amongst others, present a detailed lithostratigraphy of the Somerset Lias Group. BGS (2019) defines the top of the Blue Lias to be ‘Bed 238’ by Whittaker and Green and is associated with a notable decrease in limestone beds. The S. Wales coast is less well documented but works include Sheppard et al. (2006). The Lias Group is highly fossiliferous including abundant ammonites, allowing sub-division into biostratigraphic zones, the BLI consists of the Bucklandi Zone (Bz), Angulata Zone (Az), Liasicus Zone (Lz) and Planorbis Zone (Pz). For S. Wales, the BLI is best divided into three distinct members (Fig. 2b); whilst for Somerset, no such members exist (Hobbs et al. 2012). For reporting purposes, the Bz of Somerset observed during fieldwork is hereby named SS Member.

The deformation history of the BCB is complex, dominated by NW trending strike–slip faults and E to ENE trending faults and folds; including the regional Bristol Channel Syncline (Fig. 2c). Normal faults formed as a result of N–S extension during the Late Jurassic, later followed by basin inversion, including both N–S and E–W contraction, resulting in numerous overprinting relationships and reactivated faulting (Glen et al. 2005). Most faults are planar normal faults, with some bedding-parallel faults and extensional shear zones. Bedding is highly persistent and dips north by 10–12° in the southern BCB. Vertical to sub-vertical joints are common with high frequency, 3–4 joints per m, within the limestone bands, oriented E–W, N–S or S–W. At depth, joints are predominantly tight and frequently infilled with calcite or gypsum deposits (Royal Haskoning 2009). According to Glen et al. (2005), the nature of folding and fracturing is controlled by the dominance of limestone beds, demonstrating the importance of the limestone–mudstone ratio investigated in this research work.

Tunnelling through BLI, considerations and ground behaviour

In this project research, a hypothetical mechanised tunnel is assumed to be excavated in the afore-described geological setting and an Earth Pressure Balance Machine (EPBM) is selected as it is applicable for the following conditions: soft ground, or if high water pressures and/or variable ground conditions are expected. EPBMs incorporate scrapers and/or disc cutters and can operate in open/closed mode. Important factors such as ground behaviour characterisation, groundwater conditions and faulting must be considered, with reference to their effect on TBM performance.

Rock mass classification systems are important as the behaviour of a rock mass is considered to be governed considerably more by discontinuities than the strength of the intact rock (Palmström 2001). They are generally empirical correlations, relating quantifiable rock mass properties and observed mechanical behaviour during excavations. The most widely used systems are Rock Mass Rating or RMR (Bieniawski 1973); Rock Tunnelling Quality Index or Q-System (Barton et al. 1974); and Geological Strength Index or GSI (Hoek et al. 1992). RQD was developed to provide a quantitative estimate of rock mass quality from drill logs (Deere and Deere 1988). An advantage of the GSI system is that it provides a field method for characterising rock masses, by basic geological observations (Marinos et al. 2005). It should be highlighted outcrops, although an extremely valuable data source, are susceptible to surface relaxation, weathering and alteration, which needs consideration when assessing the likely GSI values at depth (Sattler and Paraskevopoulou 2019). Marinos and Hoek (2001) developed extensions for heterogeneous and lithologically varied sedimentary rock masses, similar to the BLI and later advanced by Marinos (2019).

The Advance Rate (AR) is a measure of excavation speed, or distance bored divided by the total time taken (distance/time) and is extremely important in terms of total project costs and time estimates. AR is fundamentally twofold and can be divided into mining/excavating and support as shown in the following equation by Barton (1999):

$$ Advance\ Rate(AR)= Penetration\ Rate(PR)\times Utilisation(U) $$
(1)

where PR is the instantaneous penetration rate or distance mined during continuous boring (m/h) and U is the percentage of shift time that excavation occurs (%).

AR varies significantly, with the world record performance for long-distance tunnel drives being 2 m/h (over a period of 1 year). Typical advance rates for 6–10 m diameter TBMs is around 1.1 m/h (Barton 2014). The Crossrail EPB TBM AR ranged between 0.5 and 1.1 m/h (Kenyon, 2015). In terms of PR, typically this does not exceed 5m/h in practice, meaning calculated values higher than this are largely theoretical (Barton 2000). The lack of sufficient face pressure may result in face instabilities, despite stabilising pressure provided by EPB machines. Stability is controlled by regulation of the screw rotation and AR to manage face pressures (Anagnostou and Kovári 1996).

The PR prediction models can be categorised as: (i) empirical, based on field studies and data from TBM tunnelling; and, (ii) theoretical, based on laboratory tests. Due to the lack of access to required rock cutting laboratory tests, the empirical models are considered herein. Early models, circa the 1970s, were simple incorporating only single parameters, commonly the Uniaxial Compressive Strength or the tensile strength which were related to the cutter force e.g. Farmer and Glossop (1980). Over time, models expanded to incorporate a wider variety of input parameters, RQD, abrasivity, joint spacing etc. (Farrokh et al. 2012) which implies the difficulty in estimating performance. In hard rock, PR is limited by cuttability i.e. force required to break the rock provided by the cutter load (Gong and Zhao 2009). It is widely accepted that the intact rock strength (UCS) has a critical role. PR is also governed by the interaction between the machine parameters (torque, thrust and machine power) and the rock mass parameters (rock strength, joints, fractures, brittleness). Generally, discontinuities reduce the rock mass strength to a fraction of the intact strength. Predictions of PR that rely solely on intact rock strength are not representative of the in situ conditions (Alber 2000). Table 1 summarises the different models used for estimating PR. It should be noted that the results from different models are based on different geological conditions and/or machine specifications, which makes it challenging for comparison and can lead to misleading conclusions when used beyond their original applications. Given the fractured nature of the BLI, methods that incorporate rock mass characteristics, GSI (Flysch), should be preferred. Only a few models have been developed for tunnels in mixed-face ground conditions e.g. Vergara and Saroglou (2017) which are mostly based on granites. Alber (1996) mentions that heterogeneous-layered conditions may cause differential penetration of the discs, vibrations and disc damage, but does not propose a solution for managing these conditions. Tarkoy (2009) suggests that the anticipated PR for the most resistant material in the face can be used, likely resulting in considerable underestimates. Diederichs (2020) highlights that sedimentary or volcaniclastic layering creates challenges for tunnelling if not considered during the design stage as the anisotropic response is not directly taken into account in the common analysis methods. It should be noted, in this presented work that the model developed by Hassanpour et al. (2009) is the most relevant as it was developed based on dark shales, limy shales and argillaceous limestones with jointing characteristics similar to the BLI and regional structures analogous to the BCB. The afore scribed implies that a methodology for predicting TBM performance when dealing with heterogeneous rock masses similar to Flysch and BLI whilst using these empirical models is required. Such methodology is presented in the following sections.

Table 1 Summary of penetration rate (PR) models

Utilisation (U) is affected by numerous factors e.g. rock mass characteristics, site conditions, TBM limitations and downtime (Alber 1996). Where poor-quality rock is encountered, high PR may be possible but AR will be low due to support requirements (and operator reduced PR). U-coefficients could be as low as 5–10% (Sapigni et al. 2002). Alber (2000) presents a model correlating Factor of Safety (FS) and U. Barton (2000) proposed that, for time (T),

$$ Utilisation={T}^m $$
(2)

where m is negative to account for decay in U over time, normally taken as −0.2, but varies according to conditions. The Rock Mass Excavability (RME) model can be used to determine TBM AR; however, Drilling Rate Index (DRI) is required.

Site investigation and fieldwork

Given the absence of borehole data, a detailed site investigation was carried out involving field testing and sampling in July 2019. This enabled primary data collection from field observation and testing that was used to create both the ground (geological) and the geotechnical models presented in this work. The derived parameters were also used as input data for the empirical models previously described. The three localities under investigation selected are shown in Fig. 1, covering representative sections, based on accessibility and apparent exposure assessed from literature and aerial maps. The main activities during the fieldwork are summarised in Table 10.

Rock descriptions

Table 2 summarises the rock descriptions derived from the site investigation. They mainly comprise interbedded argillaceous and Carboniferous mudstone/shales with different mechanical characteristics. The thickness and ratio of beds varies considerably between members. The SS Member (Somerset) comprises very prominent mudstone beds, the Porthkerry (PO) and St Mary’s Well Bay (STM) members (S. Wales) are broadly similar, containing an equal bed ratio. However, the Lavernock Shale (LVN) member is fissile weathering to low slope angles likely resulting from the low limestone content, although, at depth, it is expected that the unit will be more massive. From Locality 2, the three S. Wales members of the BLI are clearly observed Fig. 3.

Table 2 Rock engineering description
Fig. 3
figure 3

S. Wales members (Locality 2)

Discontinuities surveys, scanlines and structure

An example scanline set-up is shown in Fig. 4a. Table 11 and Fig. 4b summarise the scanline discontinuity data. Scanlines were recorded in three dimensions and greater than 3 m were completed in places, to incorporate discontinuities with larger spacings as at depth these large-scale discontinuities are likely to be present. For all localities, three discontinuity sets (plus random) were observed. The joint sets broadly correlate between localities and express similar jointing characteristics. Joint Set 1 (J1) discontinuities are E–W oriented, vertical and highly persistent. J2 discontinuities are also vertical striking approximately N–S so are orthogonal to and bounded by J1, resulting in low horizontal persistence. J3 discontinuities only occur in the mudstone, they are sub-horizontal, including highly persistent bedding fractures and shear zones, often stained orange (indicative of water flow). For example, the discontinuities were observed at Locality 1, shown in Fig. 4c where they are more systematic with greater spacing in the limestone layers, creating a blocky appearance. The sub-vertical joints are often ‘stepped’ in the mudstone. Foliation and bedding planes also act as discontinuities, in terms of controlling failure. Within the fault zones, joints are more random and with higher frequency, but affected zones are often small ~0.5m (up to 4m).

Fig. 4
figure 4

a. Set up for Scanlines, b. Discontinuity stereonets, c. Block diagram of discontinuities based on Locality 1

Joint sets broadly correlate across localities, with differences in orientations attributed to local folding and faulting. The shallow dip angle (70°) for J1 (Joint set 3b), results from rotation by an obvious N–S fold. Discontinuities appear accountable for failure mechanisms and cliff stability e.g. J1 always runs parallel to the cliff face inferring control of cliff orientation. It should be noted that orientations are affected by local folding and faulting and not necessarily representative of regional structure.

Faulting is characterised by field observations, desk study and geological mapping of aerial photographs from Bing Maps (2019), summarised in Fig. 5. Generally, faults are highly persistent, often >100m, with relatively narrow fault zones (<4m). Gentle folding exists though the rock mass tends to be less folded where there is a higher limestone proportion. Bedding is sub-horizontal across all localities e.g. at Locality 3, the beds are northerly dipping at around 10° varying locally subject folding and faulting.

Fig. 5
figure 5

Faulting (a) Locality 1; (b) Locality 2; and, (c) Locality 3

Rock mass classification and characterisation

A summary of the rock mass classification results is show in Table 3. For all the classification systems (GSI, RMR, Q) and RQD (%) system, the joint characteristics are based on the scanline surveys.

Table 3 Summary of rock mass classification investigations

It should be stated that GSI (Flysch) is the most applicable classification system for the BLI. Usually, the lowest rock RMR-value is considered for slope stability i.e. by applying the ‘weakest’ parameters. However, for TBM ‘worst-case’ PR is when RMR-values are high, accommodated for in this research work by providing a range of input parameters (and results). Q-system’s given ranges account for both rock mass variability and uncertainty in parameters. For example, Jw could range from 0.66 to 1. Discontinuities are mostly dry but with potential to flow. SRF could be 1–2.5 for medium and low stress, respectively. Typical RQD values are >90%, decreasing within the more mudstone/shale prevalent areas and in proximity to faults.

Lithological logs

Based on field work observations, Fig. 6 shows the anticipated limestone percentage to the face of 7.0 m diameter TBM, compared to literature values. Figure 6a shows that the PO member comprises approximately equal proportions of limestone to mudstone and the STM member is similar and a variation in percentage according to stratigraphic position (Fig. 6b). Peaks at the base of the Bucklandi Zone (33%) and within the Angulata zone (46%) are attributed to prominent limestone beds. Figure 6c exemplifies the influence TBM diameter, TBMs of smaller diameter are much more sensitive to changes. The thickness of beds between localities also varied. The PO and STM members have similar bed thicknesses whilst the SS member has much thicker beds (Fig. 6d and e).

Fig. 6
figure 6

(a) Percentage limestone (a) PO member (Locality 1); (b) Somerset coast, including SS Member (Locality 3); and, (c) Size effect on limestone percentage. PO member (for this study); Bed thickness (d) PO member (Locality 1); (c) Somerset, including SS Member (Locality 3)

This assessment is used as a tool for tunnelling through the BLI, depending on the expected relevant stratigraphy, which can be identified by the ammonite zonation. The percentage of limestone in the face can indicate the potential for reduced PR and/or AR, increased wear to cutting tools and the potential for blockages within the screw conveyor caused by blocks of limestone. In addition to governing the rock mass behaviour and deformability, as postulated by Glen et al. (2005), stated that for simplicity, the calculation was based upon a ‘square’ geometry.

Schmidt Hammer

The L-Type Schmidt Hammer (SH) was selected, following the ISRM guidelines (Aydin 2009). Readings were taken on both limestone and mudstone (the more massive units) on dry, natural exposures. The orientation of the SH axis varied. For the limestone lithologies were achieved 20 readings whereas fewer readings for the mudstone/shale as was too weak with undulating surfaces. According to Aydin (2009), no readings were discarded to ensure that the heterogeneity and range of mechanical properties were encapsulated. The Deere and Miller (1966) method was selected to convert R values to UCS:

$$ UCS=6.9\times {10}^{\left(0.0087\gamma R+0.16\right)} $$
(3)

where: R is the rebound number normalised to vertical and γ density (g/cm3).

It should be stated that the use Eq. 3 is considered essential given the high rebound values greater than 60 were often recorded for the limestone, particularly at Locality 1, exceeding the upper bound of Deere and Miller (1966). Equation 3 was selected given its high regression coefficient and wide applications. For limestone and mudstone, the following unit weights 23kN/m3 and 22kN/m3 were used respectively as determined by a simple submersion test. A summary of 117 measurements and conversion to UCS is given in Table 4.

Table 4 Schmidt Hammer field work measurements and strength results

It is critical to note that many of the limestone SH readings are relatively high. This can occur due to exposure to wetting and drying cycles, that causes solution and re-precipitation of calcium carbonate (Flint et al. 1953), which is plausible given the dynamic tidal regime within the BCB.

Laboratory testing

To determine the geotechnical properties, laboratory tests were performed on collected samples. Moisture Content (MC), Point Load (PL), Uniaxial Compressive Strength (UCS), Brazilian Tensile Strength (BTS) and CERCHAR-Abrasivity Tests were completed to provide the required parameters for the discussed performance models. Sample preparation was completed by Soils Engineering Geoservices Ltd. All laboratory testing was conducted at the University of Leeds RMEGG Laboratories, in accordance with the ISRM Suggested Methods (Ulusay and Hudson 2007) unless stated otherwise.

Moisture content

Eight Moisture Content (MC) tests were completed, using PL-tested specimens. Table summarises the MC test results (Table 12). These values are extremely low, attributed the fact that field samples were not sealed, from exposed outcrops. The mudstone samples have a slightly higher MC than limestone, possibly due to their permeability allowing better water retention. In situ MC-values may be closer to ~13.2% as stated by Hobbs et al. (2012), for the BLI.

Uniaxial compressive strength (UCS) test

UCS testing was performed primarily on eight limestone samples and a massive mudstone sample (Table 13). The loading rates applied were calculated based on strength estimates to achieve a failure time compliant with the standard: Limestone (S. Wales) 11–15 kN/min; Limestone (Somerset) 8 kN/min and Mudstone (S. Wales) 2.5 kN/min. It should be stated that samples were 37 mm in diameter, rather than preferable 54mm due to core drilling limitations.

The SS member limestone specimen was very argillaceous, which explains the low UCS. The PO and STM member results were similar. It must be also noted that for two PO member specimens, a strength of 88 MPa was recorded. However, for one specimen, the ends were not squared and loading occurred at a slight angle, likely resulting in lower maximum stress. For the second sample, a crystalline nodule (Fig. 7a) was present in the centre but was not apparent from the exterior of the core. The crack likely propagated from the centre attributing the lower strength to the weaker nature of this infilling, which was very crumbly upon failure. Discounting these two readings would give a much higher mean strength of the PO member of 139 MPa.

Fig. 7
figure 7

(a) UCS test; (b) Point Load test; (c) Brazilian test; and, (d) CERCHAR test configuration and post and pre-tested sample mudstone examples for each test

Point load test

The PL test is an index test which can be used to predict the UCS, by applying a conversion factor to the PL strength Index (Is(50)). Rock specimens, comprising of cores and saw cut blocks, were broken by applying a load through two conical platens. Specimens of both lithologies were tested, but this technique is particularly important for application to the mudstone/shale samples, given these are unsuitable for UCS testing and PL testing is recommended for shales (e.g. Vallejo et al. (1989)). The mudstone/shales are anisotropic; therefore, it was ensured that loading was applied both parallel (II) and perpendicular (--I) to the laminations. This was done so that the strength anisotropy index (IA(50)) could also be determined. Due to invalid failures, 8 of the mudstone tests were discarded; all attributed to lamination effects. It should be noted that due to the limited sample number, specimens from each locality were classed as one sample set, despite likely variations where block samples are taken from different beds. The Is(50) results were then converted to UCS (MPa) using:

$$ UCS=22{I}_{s(50)} $$
(4)

after Brook (1985), as this correlation is supported by the ISRM (2007) and applicable to a variety of rock types. Figure 7b shows an example of PL-tested mudstone from the STM member.

The results (Table 14) are also dependent on the choice of conversion correlation. Low water contents may have resulted in higher than in situ UCS values, a correlation found by numerous authors e.g. Romana and Vasarhelyi (2007); who also found this to be more significant for mudstone than limestones, with ratios of UCSsat/UCSdry of 0.3 and 0.8–9, respectively. ‘Stepped’ fractures were observed both in the laboratory and field; attributed to the rock preferentially splitting along laminations. As expected, the strength parallel to laminations was found to be weaker than perpendicular, with IA(50) values of 1.92 and 1.58. Regionally, the bedding is mostly sub-horizontal, so typically the force exerted by the cutters would be parallel to the laminations.

Brazilian tensile test

A total of 20 BTS tests were completed on both lithologies on 37 mm diameter samples (Table 15, Fig. 7c). The loading rates applied were 300 N/s and 200 N/s for limestone and mudstone, respectively. For the limestone, the results are consistent and show a similar strength trend of reducing strength from PO, STM to SS member to the UCS testing. Relevant to the mudstone specimens given that for PO member, the strength parallel to laminations was higher than perpendicular. The anisotropy index (AI) defined for the STM member was in line with what was expected (1.7).

CERCHAR Abrasivity Test

The CERCHAR Abrasivity Index (CAI) Test involves a stylus scratching a rock specimen for 10mm, to measure the tip wear (Fig. 7d). This test was selected to measure rock abrasivity, due to its worldwide usage and acceptance for estimation of cutter consumption (Rostami et al. 2014; Bilgin et al. 2014). CAI is an input parameter for some performance prediction models and provides an estimate of the rate of cutter replacement. The tests were completed in accordance with the ISRM (Alber et al. 2014) to 6 samples and reporting details applicable for all tests (Table 16). The test was conducted under the following conditions: air-dryed environment, rockwell hardness HRC of stylus: 58, measurement method: side view, type of apparatus: type 1. Tests were completed on the fresh surface of post-PL tested specimens. With the exception of one test specimen, where saw-cut surfaces were used, this was then corrected for according to give CAI’. The side view method was used since Rostami et al. (2014) found this reduces the operator effect on the test, compared with the top view method. Four measurements were taken of each pin and a mean taken (excluding erroneous results) following the example in Alber et al. (2014).

The abrasivity of all the specimens is ‘low’ to ‘extremely low’, comparable with typical values for limestone 1–3, mudstone 1–2 and shale 0.5–1.5 (Bilgin et al. 2014). Rostami et al. (2014) suggests the CAI test may not be suitable for very soft rock where there is little to no wear on the stylus; such as the mudstone/shales in this study. Additionally, during tests the tip penetrated the mudstone. The applied correction factor for sawn surfaces is considered to overestimate the CAI for the mudstone. The quartz content between the lithologies is expected to be broadly similar. The higher CAI for limestone is shown to correlate with rock strength (Fig. 8), (Rostami et al. 2014).

Fig. 8
figure 8

Relations CAI vs UCS

Test result discussion

Table 5 summarises the various test lab results performed in both lithologies. The UCS values in Fig. 9 show that the intact rock strength of the S. Wales samples (PO and STM member) is notably higher than observed in Somerset (SS member). BGS data for the BLI, from Hobbs et al. (2012), show much lower UCS values, particularly from direct tests. However, their data set is also limited and there is no indication of sampling locations, making comparisons problematic. In the field, mudstone/shale was observed to be very weak to weak, indicative of UCS-values of 1–25 MPa, compared with 4–83 MPa, from laboratory tests. The strength variation is likely related to the carbonate content, as inferred by Hobbs et al. (2012) who observed strengths of <5 MPa for samples without carbonate.

Table 5 Summary of laboratory test results
Fig. 9
figure 9

UCS comparison (a) limestone; (b) mudstone/shale

Geological and geotechnical model

Based on the field observations and testing (in situ and lab), first a geological model is developed through the desk study which is further developed to a geotechnical model in order to define rock mass behaviour types, partly following the method of Marinos et al. (2019), Skolidis et al. (2020) and Paraskevopoulou et al. (in press).

Geological model

The conceptual geological models for both S. Wales and the Somerset coast have been developed and are shown in Fig. 10. Although detailed hydrogeology is unknown, it is rational that a higher percentage of limestone beds, which permit groundwater flow, will correlate with a higher K-value (Royal Haskoning 2009). Weathering is expected to differ either side of the BCB, primarily due to different glaciation histories. Faulting is fairly common and persistent at all localities in particularly at Locality 3, supported by Glen et al. (2005), geological mapping and aerial photography show faulting becoming less common. This suggests a variation in occurrence can be expected, accounting for unforeseen tunnelling conditions.

Fig. 10
figure 10

Proposed geological model along (a) S. Wales Coast Structure inferred from Digimaps.; and (b) Somerset Coast

Geotechnical model

The geological units have been defined and categorised into ground types (GTs), shown in Table 6 which are expected to behave similarly when excavated.

Table 6 Ground type definition and descriptions

The Geotechnical Types (GT) units are defined based on GSI, given the importance of discontinuities. The limestone and mudstone are observed to behave in brittle and ductile manners respectively e.g. spalling of limestone during UCS testing and crushing of mudstone during PL tests. Discontinuities also behave differently, vertical discontinuities exist within limestone, which are then ‘stepped’ through mudstone, taking the line of least resistance. GT1 is a hypothetical end member, included for completeness, comprised mostly of limestone. However, it must be emphasised that this GT1 was not observed in the field. The allocation of GTs to geological units within the BLI is shown in Fig. 11 with question marks denoting units that require visual verification. Justification is given in Appendix A.1.

Fig. 11
figure 11

Geological stratigraphy and corresponding GTs

Table 7 summarises the allocated geotechnical parameters and expected ground behaviour. Where possible, design values (and ranges) are obtained from laboratory results (excluding outliers), e.g. for GT1 (limestone) an average strength of PO and STM members is taken. Where laboratory results are missing or unrepresentative, values are estimated based on field observations, e.g. for the mudstone given the sampling bias.

Table 7 Geotechnical design parameters based of GTs

UCS is a required parameter for many PR prediction models. However, for heterogeneous conditions, there are no suggested guidelines on how to determine a single UCS value. However, the presented research work makes the following recommendation: the design value is determined by a weighted method based on percentage limestone. For example, in the case of 20% limestone and 80% mudstone the calculation is:

$$ {UCS}_{intact}=0.2\times {UCS}_{intact}(lmst)+0.8\times {UCS}_{intact}(mdst) $$
(5)

The limitations and further recommendations, when applying this to PR prediction, are discussed in the next section. The same system is also used for other parameters e.g. BTS and CAI.

The deformation modulus (Em) derived by RocData (by Rocscience) gives the rock mass stiffness and may also be used as a proxy for structure i.e. higher Em-values are correlated to higher limestone proportions, resulting in open folds with low amplitudes and minimal disturbance, and vice versa; as observed by Glen et al. (2005). It is important to understand how a cavity within the rock mass will behave without the support from the TBM. Therefore, potential failure mechanisms (Rock Mass Behaviour Type - RMBT) are also identified in Table 8 based on work by Marinos et al. (2019).

Tunnelling considerations and design analysis

The variation in geomechanical facies has an unknown but potentially large effect on AR. GT1 and GT4 represent the likely endmembers that could occur in the BLI. These are not necessarily ‘best’ and ‘worst’ cases, GT1 creates the most resistance to instantaneous PR, whilst GT4 would require the most support. The following analysis determines the difference in TBM performance between these GTs; hence, how sensitive to GT the design should be. Machine specifications are required for most PR models; therefore, hypothetical TBM specifications (Table 8). A 7.0 m EPB machine was selected for applicability in unstable (failure can occur) conditions and adaptability to changing geology.

Table 8 Hypothetical EPBM specifications

A quantitative estimate of PR was completed using the models outlined in Table 2 and parameters derived in Table 9. Each GT design parameter (Table 8) is kept constant, enabling comparison between models. Unless otherwise stated, uncertainty bounds are based on parameter ranges. The applied models were chosen based on industry recognition, the applicability to the geological formation and laboratory equipment availability. A sensitivity analysis for each model has been performed to determine which parameters are most influential shown in Figs. 12, 13, 14, 15 and 16.

Table 9 AR estimates using Barton’s model (2000)
Fig. 12
figure 12

Sensitivity analysis of the CSM model (Rostami and Ozdemir 1993)

Fig. 13
figure 13

Sensitivity analysis of the QTBM model (Barton 1999)

Fig. 14
figure 14

Sensitivity analysis of the Hassanpour et al. (2009) MRCI and GSI model

Fig. 15
figure 15

Sensitivity analysis of the Farrokh (2013) model

Fig. 16
figure 16

Sensitivity analysis of the Alber (2000) model

CSM model by Rotsami

The CSM model shows an increase in calculated PR, or, required thrust reduction to maintain a constant PR from GT1–GT4 (Figure 17a and b); this is partly expected due to decreasing percentages of limestone, limiting PR. However, unrealistically high values are calculated for GT3 and GT4; attributed to actual PR being limited by unconsidered technical issues. In reality, there is an upper PR limit of around 5m/h, as suggested by Barton (2000), as the operator would reduce the thrust to accommodate for poor ground conditions.

Fig. 17
figure 17

(a) PR prediction (CSM model); (b) Thrust per cutter with constant PR of 3.24m/h; (c) PR prediction (QTBM model); (d) Thrust cutter with constant PR of 5m/h; (e) PR prediction using the Farrokh and Hassanpour models; and, (f) Model by Alber. Error bars show the 90% and 10% percentiles of the model, based on the characteristic input parameters

QTBM model by Barton

Results from the QTBM model are shown in Fig. 17c and the Q-system was considered inapplicable to GT4 due to its very weak nature. Calculations apply σcm given that joints are mostly vertical so joint inclination (β) is around 90° and therefore ‘unfavourable’. Uncertainties shown account for variations in UCS, Q and quartz content only. Again, the predicted PR exceeds realistic values (Fig. 13). Similar overestimations were experienced by Hassanpour et al. (2016) when using the QTBM model, who attributed this to uncertain input parameters e.g. in situ stress. The sensitivity analysis shows cutter thrust is the most influential parameter; along with the Q-value if less than 5. Therefore, the change in predicted PR is largely related to Q-value in this study. The tangential (wall) stress was calculated using the Kirsch equations, assuming a k-value of 0.5 and a depth of 50m, for which the model is relatively sensitive. Maximum machine cutter thrust was used; this results in QTBM values being lower than 1, which is purely theoretical according to Barton (2000). In this circumstance, thrust is generally reduced particularly where faulting is encountered, to maintain a steady PR as shown in Fig. 17d.

Models by Farrokh and Hassanpour

The models by Farrokh and Hassanpour give similar results (Fig. 17e), which are all realistic giving PRs below 5m/h. The PR increases between GT1–4, associated with the reduced limestone proportion. These models include only RPM and cutter force as machine parameters. The Hassanpour (RMCI) and Farrokh models (Figs. 14 and 15) use only geological parameters derived from laboratory testing; this reduces uncertainty in parameter estimation and provides fewer sources of error. The Hassanpour (GSI) uses the flysch GSI system which is considered accurate for this rock mass. The sensitivity analysis shows these models are most sensitive to UCS, RPM and cutter thrust. For the Hassanpour’s (RMCI) model, PR is most sensitive to changes in UCS at high RQD values; whilst the Farrokh’s model shows the reverse. The high sensitivity to machine parameters demonstrates the importance of keeping these constant when comparing models.

Model by Alber

The model by Alber (2000) is the only one where the PR decreases between GT1-3 (Fig. 17f), resulting from reduced rock mass strength below 15 MPa and subsequent drop in achievable PR. In this sense, this model is perhaps the most realistic. The model is not applicable to rock masses with RMR-values below 25, i.e. GT4. The sensitivity analysis shows (Fig. 16) this model is mainly sensitive to changes in RPM and cutter thrust, though the trends are unclear due to the model’s accountability for reduced thrust.

Model comparison and discussion

A comparison between the models, given in Figure 18 shows large variation in PR prediction for each GT, highlighting the difficulties and inconsistency in predicting PR. The QTBM model infers that PR is not at all sensitive to the different GTs being limited solely by technical factors. Models by Hassanpour et al. 2009 and Farrokh (2013) best show the anticipated results, where PR is almost doubled between GT1–GT4, attributed to the reduced presence of strong limestone at the face. The model by Hassanpour (RMCI) is assumed to be the most accurate for these ground conditions. It should be noted that constant thrust was used to compare models and GTs; however, in practice, applied thrust varies according to ground conditions (Nelson 1983).

Fig. 18
figure 18

PR prediction model comparison, where PR is capped at 5m/h

Utilisation and advanced rate

Utilisation was calculated as a function of stress (tunnel depth) shown in Fig. 19, using Alber (2000). The tangential wall stress was calculated using the Kirsch equations, assuming a k-ratio of 0.5. As expected, GT4 has the lowest U-values, given the weaker rock mass requiring more support. That said, for a 50 m deep excavation, the U-value does not vary much (between 42.5 and 45%), showing that stress has a greater influence in UCS for this model. At higher stresses (e.g. 200m), the effect of UCS variation is notably more pronounced. This can then be applied to Eqs. 1 and 2 to determine the AR, using results from this section.

Fig. 19
figure 19

Utilisation determined by model from Alber. Error bars show the 75th and 25th percentiles from model

‘Average’ ground performance giving an m-value of −0.2 can be assumed, as significant grouting or very bad ground is not anticipated. This is applied to the PR from the Hassanpour (RMCI) model to estimate AR (Table 9).

Table 10 Summary of key activities during fieldwork

Concluding remarks

The principal aim of this research work is to propose a methodology, a modified approach, to preliminary assess TBM performance in heterogeneous rock masses based on primary collection data derived from field, in situ and lab testing using the existing empirical models. For this purpose, a desk study assessed the BLI formation in a lithological system consisting of mudstone and limestone layers. Based on the detailed fieldwork, the geological models for both the S. Wales and Somerset were developed. The BLI comprises varying proportions and thicknesses, of persistent, interbedded limestones and calcareous shale and mudstones. Intact rock strength, tensile strength and abrasivity were characterised by laboratory testing on collected samples confirming the expected strength difference between the mudstone/shales and limestone. Additionally, samples from S. Wales were found to be broadly stronger compared with those from Somerset. Abrasivity is determined to be negligible. From the above, a geotechnical model was developed based on which four ground types were determined, distinguished primarily by GSI and limestone percentage. Design values were obtained from laboratory results where possible but were otherwise estimated. Implications for TBM performance were assessed. For example, faulting is concluded to be manageable, with most faults unlikely to be recognised by a TBM. Percentage limestone has been identified to be critical for predicting PR, structural disturbance and tunnel convergence. The current PR models do not address the issue of parameter selection for heterogeneous rock masses comprising layers with different rock strengths. Therefore, a weighting system, proportional to the percentage of limestone present in the face, is proposed and applied to the selected PR models for the identified GTs. For the Hassanpour et al. (2009) and Farrokh (2013) models, PR decreases with increased limestone in the face, as expected. Whilst for the CSM and QTBM models, the TBM PR is found to be insensitive to ground type, limited instead by machine restrictions. It was established, from critical review that the Hassanpour et al. (2009) PR prediction models are most applicable to the BLI and consequently to similar heterogeneous lithologies. U is also estimated, employing models by Alber (2000) and Barton (2000), the latter was used to establish preliminary estimates of AR using PR values calculated by the Hassanpour’s RMCI model.

Overall, desk study, site reconnaissance, laboratory testing and development of the geological and geotechnical models have all been employed to characterise the rock mass of the BLI and estimate TBM performance. This reduces the risk of cost and time overruns; however, there is always uncertainty in geomaterial distribution (Yau et al. 2019, 2020). The employed methods are crucial, but ground investigation (i.e. boreholes) is still favoured to collecting data from exposures, however it is commonly absent. This work provides guidance on how primary collection dataset can add valuable insights to preliminary assess TBM performance in heterogeneous rock masses. It has been shown how every step of this work starting from field observations to lab testing to developing a geological and then geotechnical model can contribute in TBM assessment performance.

Finally, it should be noted that there is a gap in the literature for a more complex method to be developed, which should be verified by laboratory cuttability tests. Additional fieldwork and laboratory testing, incorporating a much larger suite of data, from all the stratigraphic zones within the BLI and comparison of results with borehole data, is recommended, for more detailed characterisation of the BLI. The variability of ground conditions has been simplified by the proposed ground types e.g. properties of PO and STM members are averaged to form GT2. The ground types could be further developed, and visual verification is still required for some geological zones. The weighted average method applied to input parameters for the PR models, is overly simple and it can be used at a preliminary design stage. Further work being considered by the authors includes extending this method to other sites showing natural lithological variations in stratigraphic sequences as well as assessments of how this proposed methodology could be adapted and applied to synthetic rock masses. It is recommended that a larger suite of samples is tested, covering additional localities/stratigraphic zones and comparisons made with borehole data. Testing to further characterise mudstone anisotropy is also suggested.