Abstract
The rheological properties of three Na-activated, trioctahedral Mg-bentonites (hectorite clay from the CMS Source Clay Project repository, saponite clay from Spain and stevensite clay from Rhassoul, Morocco) and a sepiolite clay from Greece were examined after dynamic ageing at temperatures up to 230°C. The 5% w/v suspensions were prepared by dispersing the clay mineral samples in distilled water. The suspensions underwent dynamic, thermal ageing for 16 h before determination of the viscosity, filtration loss, filter cake thickness and pH and the concentration of dissolved Na+ and Mg2+. Thermal ageing contributed to the dispersion of clay particles, with a direct effect on plastic and apparent viscosity, introducing pseudoplastic behaviour. With the exception of the stevensite clay at 230°C that displayed limited dissolution at 230°C and partial conversion to kerolite, the clays were stable at high temperatures. The Na-activation of all clays except for stevensite was not adversely affected by thermal ageing. Thermal ageing of stevensite at 230°C facilitated Na exchange and yielded suspension with high viscosity and low filtrate loss. Only the suspensions of hectorite and those of stevensite aged at 230°C met with American Petroleum Institute specifications. The thermal behaviour and rheological properties of the clays might be interpreted according to the intrinsic properties of the clay minerals, such as layer charge and charge distribution.
Drilling fluids are an integral part of the oil and gas extraction process because they seal and support the walls of the well from the water of the surrounding formations by increasing the hydrostatic pressure inside the well (McKee & Geehan, 1989). In addition, they serve as coolants and lubricants for the drilling bits whilst transporting the fragmented rock to the surface, and they protect the drilling equipment from corrosion (McDonald et al., 2007; Temraz & Hassanien, 2016).
A drilling fluid consists of a fluid phase, in which one or several solid phases are dispersed. The fluid phase can be aqueous (water-based muds; WBMs), oily (oil-based muds; OBMs), gaseous or emulsions (Vryzas & Kelessidis, 2017; Zhang et al., 2020). The solid phases consist of a series of different materials that regulate the rheological properties of the suspension, the most important of which are clay mineral nanoparticles (mainly Na-smectite in the form of Na-bentonite, sepiolite and palygorskite; Güven, 1992; Neaman & Singer, 2000a,b; Christidis, 2011; Zhang et al., 2020). The main clay material used in drillings is Na-bentonite (Gautam et al., 2018). Smectites, the main mineral of bentonites, are characterized by flaky crystals, with a particle size of <0.5 μm, whilst carrying a negative electrical charge located in octahedral and/or tetrahedral sites (Odom, 1984; Meunier, 2005). By contrast, palygorskite and sepiolite form fibrous crystals of <2 μm in size, which are not characterized by significant layer charge (Meunier, 2005). These properties contribute to the formation of stable, non-Newtonian, viscous fluids (Lagaly, 1989; Christidis & Scott, 1996; Christidis, 1998; Neaman & Singer, 2000a,b). Additives, namely polymers (xanthan gum, polyanionic cellulose, etc.; Bavoh et al., 2022), weighting agents (barite, hematite, etc.; Bageri et al., 2021) and nanoparticles (including magnetite, sepiolite, etc.; Gerogiorgis et al., 2015; Al-Malki et al., 2016), are incorporated into the suspensions, improving their performance.
To date, research studies in this area have focused on understanding the rheological properties of Na-bentonites for application in the drilling industry. These studies involve almost exclusively dioctahedral smectites with octahedral charge, mainly montmorillonite (Brandenburg & Lagaly, 1988; Christidis & Scott, 1996; Christidis, 1998; Christidis et al., 2006; Kelessidis et al., 2007b; Kelessidis & Maglione, 2008; Vryzas & Kelessidis, 2017; Vryzas et al., 2017) and mixtures of palygorskite or sepiolite with dioctahedral smectite (Chemeda et al., 2014; Al-Malki et al., 2016). In addition, substantial work has been carried out in the last two decades relevant to the rheological behaviour of water-based and oil-based sepiolite drilling fluids (for a review, see Zhang et al., 2020). Sepiolite enhances the performance of drilling fluids functioning as thixotropic and thickening agents (Alvarez, 1984) and augments their gel strength, plastic viscosity (PV) and yield point (YP; Abdo et al., 2016).
Most studies on the rheological properties of water-based and oil-based drilling fluids, prepared with various types of clays, have been performed at room temperature and after ageing at room temperature (Brandenburg & Lagaly, 1988; Christidis & Scott, 1996; Christidis, 1998; Neaman & Singer, 2000a; Christidis et al., 2006; Kelessidis et al., 2007b; İşçi & Turutoğlu, 2011; Chemeda et al., 2014; Al-Malki et al., 2016; Zhuang et al., 2018; Echt & Plank, 2019). Studies on the effects of temperature on the rheological properties of clay suspensions at high temperatures and pressures are less common and have focused mainly on montmorillonite suspensions (Hiller, 1963; Alderman et al., 1988; Briscoe et al., 1994; Santoyo et al., 2001; Kelessidis et al., 2007a,c; Mohammed, 2017; Vryzas et al., 2017), especially Wyoming montmorillonite.
By contrast, studies on the rheological properties of clays with trioctahedral clay minerals, both bentonites and sepiolite, used as drilling fluid additives both at ambient conditions and at elevated temperatures and pressures are limited. Güven et al. (1988) studied the rheological properties of clays rich in saponite, sepiolite and Wyoming montmorillonite at a temperature range of 149–316°C and reported high stability and viscosity of the saponite-based fluid when interacting with electrolytes. The rheological behaviour of a series of dioctahedral smectites and hectorite at room temperature was reported by Christidis et al. (2006), and Xiong et al. (2019a,b) observed excellent dispersibility and stability of laponite, the artificial counterpart of hectorite, at high temperatures, making it a potential candidate for drilling in high-temperature environments. Laponite is not pure hectorite but a mixture of hectorite and stevensite with ~25% non-swelling disordered talc (kerolite) layers (Christidis et al., 2018). Laponite was also tested as additive in bentonite suspensions and was reported to be successful at temperatures as high as 150°C (Li et al., 2022). Mixtures of clays containing montmorillonite/saponite or sepiolite/saponite retain and even enhance the advantages of these trioctahedral clay minerals in various applications, including drilling fluids (Güven et al., 1987, 1992; Miles, 2011).
Τrioctahedral smectites, namely hectorite, stevensite and saponite (the main constituents of Mg-bentonites), are 2:1 clay minerals, with their octahedral sites occupied by Mg2+ cations (Brigatti et al., 2013). Partial substitution of Li+ for Mg2+ yields the octahedral sheet of hectorite and introduces a negative layer charge (Meunier, 2005). The layer charge of stevensite originates from a small number of vacancies in the octahedral sheet (Brindley, 1984; Christidis & Mitsis, 2006). In the case of saponite, Si4+ cations are substituted by Al3+ cations in the tetrahedral sheet. In contrast to other smectites, saponite may have a positive octahedral charge due to the replacement of the structural Mg2+ cations by Al3+ or Fe3+, which partially balances the negative tetrahedral charge (Christidis, 2011; Madejová et al., 2017). Sepiolite is a trioctahedral clay mineral with a fibrous structure (Newman & Brown, 1987), its octahedral sheets being continuous in one dimension, forming a ribbon-like structure. The layout of sepiolite tetrahedral sheets consists of inverted tetrahedra in every two or three rows. The above characteristics result in the formation of channels with dimensions 4.0 Å × 9.5 Å (Brigatti et al., 2013). In this contribution, new data are provided on the rheological properties of Mg-bentonites with saponite-, hectorite-, stevensite- and sepiolite-rich clay suspensions and on the ability of these clays to form filter cakes both at ambient temperature and after ageing (hot rolling) at elevated temperatures up to 230°C. The study particularly examines the importance of the intrinsic characteristics of the clays to rheological behaviour at these temperatures. Temperatures in excess of 120°C are encountered in oil drillings below 3000 m in depth, as well as in geothermal drillings of high enthalpy at shallow depths. Therefore, this work will be useful for predicting the behaviour of drilling fluids made from trioctahedral phyllosilicates in high-temperature settings, especially considering that the published information on natural Mg-clays is very limited and that the application of synthetic Mg-clay minerals such as laponite is an expensive solution for drilling fluid applications.
Materials and methods
Materials
Four Mg-rich clays were used in this study: three Mg-bentonites and one sepiolite sample (Table 1). The bentonites include SHCa-1 from Hector, CA, USA (CMS Source Clay Project), a saponite-rich bentonite from Vicalvaro Basin, Madrid, Spain, and a stevensite-rich bentonite from Jbel Ghassoul, Morocco (Benhammou et al., 2009), known as Rhassoul or Ghassoul clay, supplied by Dr K. El Ass. The sepiolite sample comes from the rims of magnesite veins in the ophiolite complex of Euboea Island, Greece, and it was collected by the lead author.
Characterization methods
The bulk mineralogy of the samples was determined using X-ray diffraction (XRD), with a Bruker D8 Advance diffractometer equipped with a LynxEye silicon strip detector, using Ni-filtered Cu-Kα radiation (35 kV, 35 mA), 0.298° divergence and anti-scatter slits, a step size of 0.019°2θ and counting time of 1 s per strip step (total time = 63.6 s per step), in the 2θ range of 4–70°2θ. Data were evaluated using EVA® software provided by Bruker. Quantitative analysis was performed with the BGMN computer code (Autoquan© software package version 2.8) on random powder samples, prepared by grinding with an agate pestle and mortar and mounted by careful side loading on Al-holders to avoid a preferred orientation.
Thermogravimetric and differential thermogravimetric (TG-DTG) analyses of the <2 μm fractions of clay samples were performed with a Perkin Elmer TGA-6 Thermal Analyser at the Laboratory of Solid Fuels Beneficiation and Technology of the School of Mineral Resources Engineering, Technical University of Crete. The clay fractions were separated according to Stokes’ law after dispersion of bulk samples in distilled water. Analyses were performed in an inert atmosphere (N2) in the temperature range 40–900°C with a heating rate of 10°C min–1.
The major elemental composition of the clay samples was determined using energy-dispersive X-ray fluorescence (ED-XRF) spectroscopy with a Bruker S2 Ranger ED-XRF spectrometer on fusion beads using an 1:1 mixture of Li-tetraborate and Li-metaborate as the flux. The Li contents of hectorite and stevensite were determined using flame atomic emission spectrometry (FAES) with a Perkin Elmer Analyst 100 FAES device. The SDC-1 standard was used as a Li-rich reference sample. Prior to Li analysis, the samples were dissolved with a mixture of HCl, HNO3 and HF acid solutions. The loss on ignition (LOI) was calculated by heating the samples at 1000°C. The cation-exchange capacity (CEC) of the clays was determined after saturation with 1 M ammonium acetate with a Kjeldahl microsteam distillator and titration with 0.05 N H2SO4.
Rheological properties
Viscosity
The materials were used without any prior purification. They were dried at 105°C and ground to pass through a 75 μm sieve. The bentonite samples were rendered Na-homoionic via the addition of optimal amounts of Na2CO3 determined from free swelling tests (c.f. Christidis et al., 2006). The suspensions were prepared according to the American Petroleum Institute (API) specifications (API 13A, 2010), except for the concentration of the suspension (5% instead of 6.42% w/v), by adding the ground clay and the optimal amount of Na2CO3 in distilled water. The suspensions were stirred for 20 min and then were aged for 16 h at various temperatures (see below). Therefore, the bentonites used for rheological tests were Na-saturated. Activation was not performed on the sepiolite samples. The properties determined were apparent viscosity (AV), PV, yield stress and 10 min gel strength. The rheological properties of the samples were determined with a Grace 3500a Couette-type viscometer on clay suspensions in distilled water.
Dynamic thermal ageing was performed by transferring the agitated suspensions in stainless steel autoclaves (FANN Instrument Company, Houston, TX, USA). Ageing was performed at room temperature (25°C), 100°C, 149°C, 176°C and 230°C. After completion of each thermal ageing cycle, the suspensions were cooled down and stirred for 5 min and their pH values were recorded. pH acts as a stabilization factor for suspensions. In general, alkaline conditions promote stabilization, as clay particles acquire negative overall charges and repel each other (Tombácz et al., 1990; Tombácz & Szekeres, 2004). At acidic pH values, the protons are adsorbed by the active edges of the clay mineral particles, whereas their edge charges become initially neutral and then positive (isoelectric point; van Olphen, 1977). The optimum pH for common drilling fluids ranges between 9 and 10 (Gamal et al., 2019). The rheological experiments after ageing at 100°C and 149°C were performed in duplicate to estimate the repeatability of the measurements.
The rheological data were analysed using M3600 software and plotted on shear stress vs shear rate charts (rheograms). The obtained curves corresponded to the Power Law, Herschel & Bulkley and Bingham Plastic rheological models, and the curves were fitted to the experimental data using an optimization routine written in MATLAB. The Herschel & Bulkley model looks identical to the Power Law model, with the difference being the presence of a yield stress parameter in the former model (Cheremisinoff, 1986). As the rheograms showed the existence of yield stress, the τ0 parameter was constrained to >0 in the Herschel & Bulkley model and all parameters were allowed to vary in the positive range.
Filtrate loss
The filtrate loss determination is a simulation of the fluid loss due to filtering of the drilling fluid through the surrounding drilling wall. A low-pressure–low-temperature (LPLT) filter press (FANN Instrument Company) was used for the experiments. CO2 was used as the pressure medium, and this was set at 6.9 atm (~100 psi). The API specifications set the limit of fluid loss for WBMs at 15 mL for a 30 min test run (API 13A, 2010). The filtrate loss volume collected during the first 7.5 min at 6.9 atm was not taken into account (API 13A, 2010). The expelled leachates were stored for further chemical analysis via flame absorption atomic spectrometry (FAAS) for their Na and Mg contents. The solids of those samples aged at 230°C were dried at 70°C and subsequently examined by XRD to trace possible mineralogical changes during thermal ageing using the same experimental setup described for the original materials.
Filter cake thickness
The thickness of the filter cake was measured with a calliper on the filter paper. In normal drilling operations, the cake also includes aggregated clay particles and other particles (i.e. cuttings, weighting agents, etc.) of different sizes, which reduce the permeability of the cake (Kelessidis et al., 2006; van Oort et al., 2016). In such cakes, the migration of the finer clay particles into the remainder of the pores and the saturation of the latter with the drilling fluid lead to even better sealing performance.
Results
Mineralogy of the trioctahedral clays
The bulk mineralogical composition of the Mg-clays is listed in Table 2. The samples have variable clay mineral contents. SHCa-1 consists mainly of hectorite and calcite, with minor quartz, dolomite and plagioclase and trace analcime. The stevensite clay consists almost exclusively of smectite (97.1%), with traces of dolomite and K-feldspar. The Spanish saponite sample consists mainly of smectite, with minor illite, quartz, K-feldspar and plagioclase. Finally, the sepiolite sample consists almost exclusively of sepiolite (97.5 wt.%), with minor brucite and trace dolomite. All clay minerals display 060 diffraction at 1.525–1.528 Å, confirming the trioctahedral nature of the smectites and the sepiolite.
After thermal ageing at 230°C, the Mg-clays displayed minor changes. The main modifications included the almost total dissolution of dolomite in hectorite, stevensite and sepiolite (Fig. 1a,b). In principle, the Mg-clay minerals were not affected by thermal ageing, with the exception of stevensite, in which the 001 diffraction maximum was split into two components: one at ~13–14 Å and a minor one at 10–10.5 Å. In addition, the Na-exchange was not complete, as is indicated by the location of the 001 diffraction maximum, which is centred at 13–14 Å. Saponite displayed a second 001 component in the form of a shoulder centred at ~12.8 Å, indicative of partial Na-exchange during ageing. The impact of Na-exchange on rheological behaviour after thermal ageing is addressed in the ‘Discussion’ section.
CEC determination
The CEC of clay minerals is a result of the permanent electric charge due to isomorphic substitutions in the tetrahedral and octahedral sheets (Johnston & Tombácz, 2002). Additionally, the exposed active edges of the crystals introduce a pH-dependent electric charge, which contributes up to 5% to the overall charge and consequently increases CEC (Grim, 1962). Smectites acquire CEC values of between 80 and 150 cmolc kg–1 of dry clay (Bergaya & Vayer, 1997; Grim, 1968). The stevensite clay is the only bentonite sample that has a CEC value within the accepted CEC range. Hectorite contains only 48.5% smectite, which explains its reduced CEC. Contrary to expectations, saponite has the lowest CEC, even though it contains 85.4% smectite. Sepiolites present lower CEC values than bentonites, as expected.
Chemical composition of the trioctahedral clays
The chemical composition of the studied clays is listed in Table 3 and is in accordance with the majority of trioctahedral phyllosilicates. MgO is the most abundant constituent after SiO2 in all of the samples, except for hectorite. Hectorite has a high CaO content and LOI and lower SiO2 and MgO contents compared to the other samples due to the presence of abundant calcite and the lower Mg-smectite content. Minor Li2O is present in hectorite and trace Li2O (380 ppm) is present in stevensite. The presence of Li is associated with octahedral substitutions of Li for Mg, and its presence in stevensite indicates the existence of trace hectorite layers in the sample. Saponite is richer in Al2O3 and K2O than its counterparts, which is in accordance with the tetrahedral Al in the mineral and the presence of illite and plagioclase impurities. Saponite also has a greater Fe2O3 content, linked to octahedral substitutions. Finally, sepiolite contains small amounts of NiO, which is in accordance with the origin of the material in ophiolite rocks.
TG-DTG analysis
The TG-DTG tests provide information regarding the dehydration and dehydroxylation temperatures of the clay minerals (Sainz-Diaz et al., 2001). Trioctahedral smectites dehydroxylate at higher temperatures (~800°C) compared to their dioctahedral counterparts (<700°C; Wolters & Emmerich, 2007). The TG and DTG curves of the <2 μm clay fractions are shown in Fig. 2. All samples show a main weight loss event due to removal of adsorbed water at between 100°C and 150°C (Fig. 2a,b). Stevensite expels crystalline water in four distinct stages: at ~320°C, 400–500°C, 600°C and 800°C (Fig. 2b). The main dehydroxylation event is observed at 800°C. Hectorite also displays three water loss events associated with dehydroxylation, at ~660°C, ~760°C and ~835°C, in accordance with Guggenheim & Koster van Groos (2001). The latter thermal event might receive contribution from trace fine-grained calcite, which might also participate in the clay fraction. Considering that the weight loss of hectorite at ~835°C, due to decomposition of calcite, is ~0.20%, it follows that the calcite content in the clay fraction would be ~0.45%. The saponite sample shows two endothermic events: a minor one at 500°C and a major one at >800°C (Fig. 2b). The event at 500°C is attributed to the presence – in minor concentration – of illite (Table 2), and possibly to minor stevensite layers that might be present in the sample. The sepiolite sample displays five endothermic events in addition to a low-temperature one (at ~100°C), namely at ~310°C, ~490°C and 550°C (doublet) and at 650°C and 800°C. The event at 490°C is associated with the dehydroxylation of minor brucite, and that at 650°C is associated with minor dolomite (Fig. 1 & Table 2). Finally, the events at 310°C, 550°C and 800°C are due to gradual dehydroxylation of sepiolite, with the event at 800°C receiving contribution from decarbonation of the CaCO3 component of dolomite (Fig. 1 & Table 2). Thermal analysis results show that the maximum ageing temperature of the fluids is considerably lower than the temperatures of weight loss due to dehydroxylation of all of the trioctahedral smectites and sepiolite. Therefore, the thermal ageing is not expected to have caused dehydroxylation of the trioctahedral clay minerals, and any changes in the rheological properties of the suspensions at high temperatures, especially the ones at 230°C, are not related to structural changes to the clay minerals.
Rheological properties
Rheograms, rheological models and representative rheological parameters
Previous work has shown that bentonite-based suspensions display remarkable rheological performance up to 120°C (250°F), but at higher temperatures the addition of rheological additives, namely lignite and xanthan gum, has been recommended (Kelessidis et al., 2006).
The rheograms of the different suspensions are shown in Fig. 3, the evolution of viscosity with ageing temperature is shown in Figure 4 and the main rheological parameters are summarized in Table 4. Hectorite suspensions became more viscous with increasing temperature (Figs 3a & 4). The rheological model that describes the flow behaviour of the hydrated suspension (i.e. without thermal ageing) is the Power Law. Thermal ageing introduced pseudoplastic flow behaviour, which is described by the Herschel & Bulkley model. The Power Law and Herschel & Bulkley models describe pseudoplastic fluids, as n < 1. Gel formation was spontaneous at temperatures >149°C, which is an indication of the extensive delamination of hectorite particles that led to sharp increases in PV and AV. The gel was completely broken down when shear stress was applied.
Saponite suspensions presented inferior rheological performance to hectorite (Fig. 3b). Viscosity increased after thermal ageing up to 149°C and decreased at higher temperatures (Table 4), suggesting that the dispersions collapsed at high temperatures. The API standards determine the acceptable AV limit at 15 cP (i.e. 15 mPa⋅s; Temraz & Hassanien, 2016), so saponite suspensions at 100°C and 149°C comply with the API specifications, although the suspension concentration was 5% instead of 6.42%. At room temperature, saponite dispersion is described by the Bingham Plastic model. After thermal ageing, all suspensions could be described by the Herschel & Bulkley model (Table 4).
The stevensite suspensions were completely inert at temperatures <176°C, with shear stress values being close to the detection limit of the viscometer (5 dyn cm–2) for the suspensions aged at 25°C and 100°C (Figs 3c & 4). However, the suspensions did not show evidence of collapse. The formation of a suspension with high PV and AV and a YP at 230°C (Figs 3c & 4 & Table 4) was an unexpected result, which suggests possible delamination of stevensite particles and the formation of particle networks.
In the sepiolite suspensions, higher temperatures facilitated hydration of particles, leading to augmented rheological behaviour (Altun et al., 2010). Indeed, the viscosity increased gradually with the temperature of ageing, although the viscosity of the suspensions after ageing up to 149°C is very low (Figs 3c & 4 & Table 4). Despite the profound increase of viscosity, sepiolite does not comply with API specifications because it formed thin suspensions that, however, did not collapse or aggregate. Sepiolite consists of fibrous crystals, whereas the smectites in bentonites form mostly flake/platelet-like crystals (Christidis, 2011). The latter introduce greater hydrodynamic drag and thus contribute to the formation of viscous suspensions. Sepiolite displays plastic flow behaviour at temperatures >176°C (Fig. 3c & Table 4).
Table 4 summarizes the YP values and YP/PV ratios of the suspensions, as well as the τ0, K and n values for the Herschel & Bulkley model corresponding to the yield stress, the consistency index and the flow-behaviour index of the suspension. These parameters were obtained both from the curve-fitting Herschel & Bulkley model and from the logarithmic form of the Herschel & Bulkley equation, namely log(t – t0) = logK + nlog(γ). YP is affected by the particle interactions via van der Waals attractive forces (Vryzas et al., 2016). The maximum acceptable value for YP is 18 lb 100 ft–2 (~8.6 Pa) according to API 13A (2010). The YP/PV ratio expresses the pseudoplastic (shear thinning) behaviour of the suspension (Safi et al., 2016), and the maximum acceptable value is 3 (API 13A, 2010). Both of the aforementioned limits apply to bentonite muds. Distinct limits for sepiolite dispersions are not available. The YP/PV ratios of all suspensions conform to the API specifications, although the solid content was 5% instead of 6.42%.
The YP during the experiments varies amongst the materials. In general, the YP of the suspensions increases with temperature, with a more profound effect occurring in the case of hectorite (Fig. 5). A similar trend was observed for dioctahedral Wyoming montmorillonite for ageing temperatures up to 80°C (Vryzas et al., 2017). In fact, gel formation in hectorite suspensions was pronounced at temperatures >149°C, with the YP exceeding the maximum acceptable limit (i.e. ~8.6 Pa). The same applies to the stevensite suspension aged at 230°C. The remaining stevensite suspensions yielded low or undetectable YPs. Saponite and sepiolite muds exhibited low YPs and compliance with the API regulations (minimum YP of 1.5 Pa); thus, the YPs of these suspensions would not undermine their ability to transport fragmented rock during drilling operations.
The τ0, K and n parameters for the suspensions of the different Mg-clays at the various temperatures display certain trends (Table 4). In hectorite, the yield stress (τ0) and flow-behaviour index (n) values increase with increasing ageing temperature, whereas the consistency index (K) shows the opposite trend. Similarly to hectorite, the K parameter of saponite decreases gradually with increasing ageing temperature, whereas the τ0 and n parameters are maximal after ageing at 149°C and decrease at greater ageing temperatures, similarly to what occurs in the viscosity of the suspensions (Fig. 5). The stevensite suspensions displayed gradual increases in τ0 and K with increasing temperature, whereas n did not display a clear trend. Finally, sepiolite suspensions displayed gradual increases in τ0 and K and a gradual decrease in n with increasing temperature (Table 4). In conclusion, all clay suspensions displayed an increase in τ0 with increasing temperature, but sepiolite suspensions displayed the opposite trends with respect to the consistency index and flow-behaviour index trends compared with their hectorite and saponite counterparts, at least at high ageing temperatures for which sepiolite data are available. The trends for τ0, K and n observed for hectorite and saponite suspensions with increasing temperature are in agreement with those found in similar studies with suspensions of bentonites with dioctahedral smectites (Vryzas et al., 2017). By contrast, the trends for τ0, K and n observed for stevensite suspensions are in general agreement with bentonite suspensions based on dioctahedral smectites, which contained laponite as an additive (Li et al., 2022). However, laponite is not a pure phase but a mixture of 50% hectorite layers with 25% stevensite and 25% kerolite layers (Christidis et al., 2018).
pH measurements
pH plays a key role in the performance of a multiphase fluid. Acidic conditions do not favour a bentonite-based suspension because the negative overall surface charge of the smectite particles is gradually neutralized and thus the electric double layer (EDL) is compressed (Park & Seo, 2011). This causes flocculation and sedimentation of particles. On the other hand, alkaline conditions contribute to the efficient dispersion of clay particles, as the net surface charge, which consists of the permanent and pH-dependent edge charges, is negative, and the EDLs expand and repel each other (Tombácz & Szekeres, 2004). The pH values obtained after ageing at various temperatures are listed in Table 5. The pH of suspensions increased with increasing ageing temperature in all of the trioctahedral clays (Fig. 6a & Table 5). The rheological parameters (PV, AV, YP) are improved at pH values >10 (Alaskari & Teymoori, 2007), which is also the case for most of the suspensions prepared in this study. In particular, PV displays a well-expressed exponential increase with increasing pH, except for the sepiolite suspension aged at 230°C (Fig. 6b).
The hectorite suspensions are typical examples of the influence of alkaline pH on rheological properties, as the rheological behaviour was improved considerably compared to that of the remaining clay minerals (Fig. 6b). The same applies to the stevensite suspension at 230°C. Saponite suspensions became more alkaline with increasing temperature, and despite their collapse at 176°C (sharp decrease of the viscosity in Fig. 6b), the pH continued to increase. The pH of the sepiolite suspensions ranged between 6.2 and ~9.0, increasing sharply at 230°C (Fig. 6a), and the PV increased sharply at 176°C and remained constant at greater temperatures (Fig. 6b).
Filtration loss and filter cake thickness
The stevensite and sepiolite suspensions did not comply with the maximum acceptable filtration loss of 15 mL according to the API 13A (2010) regulations for water-based drilling fluids (Fig. 7a). However, the hectorite and saponite muds did not produce large filtrate volumes. In fact, increasing temperature contributed to the reduction of filtration loss. Saponite suspensions collapsed at 176°C and 230°C, leading to extensive particle precipitation, which nevertheless did not significantly increase filtrate loss (Fig. 7a). The remaining filter cakes became thicker with increasing temperature for both saponite and hectorite suspensions. The thicker the filter cake, the more difficult it was for the fluid to penetrate it.
Stevensite suspensions expelled large volumes of fluid, far beyond the accepted limit. However, after a thermal ageing cycle at 230°C, the dispersion became viscous and the filtration loss complied with the API 13A specification, forming a thick filter cake (>3 mm). The sepiolite also displayed high filtration loss at all temperatures, indicating gel structures with open pores. In contrast to the smectite suspensions, the performance of sepiolite became poorer with increasing temperature. The filter cakes of the sepiolite suspensions were thin, acquiring a maximum thickness of 2.25 mm at a 25°C ageing temperature (Fig. 7b).
A well-defined overall negative exponential trend holds between the filtrate loss and thickness of the filter cakes (Fig. 8), indicating an association of high filter losses with thin filter cakes, as is to be expected. Maximum filter cake thickness/minimum filtrate loss was observed at greater ageing temperatures, with the sepiolite suspensions deviating from the overall trend. In general, a filtrate loss of <15 ml was observed in filter cakes thicker than ~3 mm, except for in the saponite suspension aged at 25°C (Fig. 8).
Chemical composition of the filtrates
Table 6 lists the concentrations of Na+ and Mg2+ cations of the filtrates. The Na+ and Mg2+ concentrations were used to assess the extent of cation exchange on bentonites after alkaline activation. In addition, the magnesium content was used to monitor possible decomposition of the smectite and sepiolite particles during thermal ageing.
The various bentonites display differing trends with respect to the Na content of the filtrates. The Na content of the hectorite filtrates increases with increasing temperature, reaching a plateau at >176°C, whereas the Na content in the saponite decreases slightly, and in the stevensite filtrates it decreases significantly, especially after ageing at 230°C. The high Na content of the stevensite suspensions indicates that ageing up to 149°C does not facilitate Na-exchange, which begins at 176°C and is more effective at 230°C. The effective Na-exchange at 230°C is reflected in the improved rheological properties. However, the relatively low Na+ content of the hectorite suspensions indicates successful cation exchange during activation, which is in accordance with the superior rheological properties of the suspensions. Finally, the saponite filtrates also have relatively high Na contents, suggesting incomplete cation exchange.
Similarly, the Mg content of the filtrates varies amongst the various clay suspensions. The hectorite filtrates display rather constant and high Mg concentrations up to 176°C, which increases further after thermal ageing at 230°C, although the amount of Mg2+ remains essentially constant at ~0.6 meq throughout the whole ageing temperature range, because the filtrate volume decreases (Fig. 7a). Ion exchange (i.e. Na for Mg), although it might take place to some extent, is not considered the main driving force for the Mg2+ contents in the hectorite filtrates because of the rather high Mg/Na meq ratios (Table 6). By contrast, the saponite and sepiolite filtrates display low Mg contents. Finally, the stevensite filtrates have moderate Mg concentrations that increase after ageing at 176°C and especially at 230°C. However, the total amount of Mg in meq in the stevensite filtrates tends to decrease with increasing ageing temperature because the filtrate volume decreases considerably (Fig. 7a & Table 6). Similarly to the hectorite suspensions, ion exchange is not the main driving force of the Mg2+ content in stevensite because of the high Mg/Na meq ratios (Table 6). By contrast, the Na for Mg-exchange in saponite might be the dominant mechanism controlling the concentrations of these ions in the filtrates due to the rather high Na/Mg meq ratios (Table 6).
The Mg content displays a positive trend with the pH of the filtrates for the hectorite and the stevensite suspensions (Fig. 9), suggesting a contribution of dissolved Mg to the alkalinity of the suspensions. The saponite and sepiolite suspensions do not follow this trend due to their low Mg contents. The increase in Mg concentration in the hectorite and stevensite suspensions with temperature is in accordance with the increase in the pH of the filtrates with temperature (Fig. 6a & Table 5).
Discussion
Response of the trioctahedral clays to high-temperature ageing
The present study showed that the different trioctahedral clay minerals display different rheological properties and that the filtrate compositions can also vary significantly after thermal ageing. The Na+ and Mg2+ contents of the filtrates are controlled by ion exchange and the structural stability of the trioctahedral clay minerals. Considering the Mg content of the filtrates after thermal ageing as a proxy for the stability of the clay minerals, when the Mg content exceeds the Na content, sepiolite displayed greater thermal stability than the trioctahedral smectites, and saponite had the greatest thermal stability amongst all of the trioctahedral smectites (Table 6). However, hectorite filtrates had high Mg2+ contents that tended to remain constant up to 176°C, increasing slightly after ageing at 230°C (Table 6). The high Mg2+ contents, even at ambient temperature, suggest that the Mg content of the filtrates might not result mainly from the dissolution of smectite but rather from the dissolution of other Mg-bearing phases, such as dolomite, or from the dissolution of soluble Mg salts. Indeed, the XRD results showed that dolomite dissolved after thermal ageing of the hectorite. Therefore, hectorite displayed very good thermal stability at high temperatures that is comparable to that of saponite.
The low Mg content of the saponite filtrates might be also attributed – at least partially – to Na-for-Mg exchange. In any case, saponite displayed inferior rheological properties at high temperatures compared to the other trioctahedral smectites, and its suspensions collapsed at temperatures >149°C (Fig. 5 & Table 4). By contrast, both hectorite and stevensite suspensions, with greater Mg contents, yielded viscous suspensions at high temperatures. The Na and Mg contents of the stevensite filtrates might also indicate limited Na-for-Mg exchange, as noted above. However, the existence of octahedral vacancies in the stevensite structure due to the lack of octahedral Mg suggests that Mg was not exchangeable and that the Mg2+ in the filtrates was probably due to modifications of the stevensite structure, except for the dissolution of dolomite. The appearance of a diffraction maximum at 10–11 Å (Fig. 1b), which might be attributed to kerolite layers, is in accordance with such a modification. This complex behaviour suggests that rheological properties at high temperatures might not be associated only with the stability of the crystal structure and particle morphology of the different trioctahedral clay minerals. Two additional parameters are considered further: the role of Na-exchange (Na-activation) and the intrinsic properties of clay mineral particles related to their crystal structure.
Na-exchange was relatively effective in hectorite, the filtrates of which showed low Na contents that slightly increased with increasing ageing temperature. This is also indicated in the d001 of hectorite after thermal ageing (13–14 Å; Fig. 1b). The presence of Mg ions in the suspension due to dissolution of dolomite explains the incomplete Na-exchange in hectorite. A possible negative influence of temperature on Na-for-Ca/Mg exchange (e.g. Deist & Talibudeen, 1967) is not considered important because the exchange was not complete at room temperature in all filtrates, except for those of hectorite; instead, it was effective in stevensite at 230°C (Table 6). In addition, the saponite filtrates had high Na contents at all ageing temperatures, with a tendency to decrease slightly with increasing temperature, especially at 230°C, and low Mg contents. The lack of a particular trend in the Na content of filtrates with temperature suggests that Na-exchange might be controlled by the intrinsic properties of the individual smectites rather than temperature. The intrinsic properties considered in this study are layer charge and charge localization.
Layer charge affects ion exchange in both univalent and bivalent cations (Maes & Cremers, 1977a,b; Shainberg et al., 1987). The selectivity for K over Ca or Na increases with increasing layer charge in natural smectites (Shainberg et al., 1987) and in smectites with reduced layer charge (Maes & Cremers, 1977a,b). By contrast, in natural smectites, the layer charge does not affect Ca-for-Na exchange (Shainberg et al., 1987). Layer charge seems to affect ion exchange by means of steric effects associated with swelling of the smectite layers (Verburg & Baveye, 1994; Laird et al., 1995). However, the preference for a particular cation is associated more with partition of the cation between the aqueous solution and the smectite surface than the selectivity of the surface for a particular cation (Teppen & Miller, 2006; Rotenberg et al., 2009). Yet, although stevensite has lower layer charge than hectorite and saponite, and therefore Na-exchange should have been facilitated, this was not observed in the present study (Table 6).
Charge localization and the source of charge are different in the various trioctahedral smectites. Hectorite and stevensite have octahedral layer charge, whereas saponite has tetrahedral layer charge. In addition, the source of charge in hectorite and saponite stems from substitutions within the octahedral sheet (Li for Mg) and the octahedral sheet (Al for Si), respectively, whereas the layer charge of stevensite is due to octahedral vacancies (Brigatti et al., 2013). The surfaces of smectite with tetrahedral charge are more hydrophilic compared to their counterparts with octahedral charge due to the control of the tetrahedral Al on the maxima and minima of the potential curves on the surface of smectite, which affect the hydrophobicity of the surface (Bleam, 1990; Szczerba et al., 2020).
Nevertheless, charge localization does not explain the behaviour of stevensite, which displayed enhanced Na-for-Ca exchange only after thermal ageing at 230°C. Indeed, although stevensite and hectorite bear octahedral charge, they displayed different responses in terms of Na-exchange at all temperatures except for 230°C. In both minerals, dissolution of dolomite released Mg2+ cations into the solution. The different response of stevensite to thermal ageing compared to hectorite is attributed to the particular nature of this mineral. Most stevensites are actually mixed-layer phases, consisting of a swelling phase (stevensite ss) and non-swelling kerolite (Eberl et al., 1982; Jones & Weir 1983). Although the Moroccan stevensite used in this study does not show evidence of mixed layering (e.g. Christidis & Koutsopoulou, 2013), the small ratio of vacant octahedra, which contribute to the layer charge, to the occupied octahedra (~1:27; c.f. Rhouta et al., 2008) suggests that the uncharged non-swelling kerolite domains (talc-like), which have hydrophobic surfaces, promoted particle aggregation. At high temperatures, stevensite showed evidence of discrete kerolite-like layers (Fig. 1b). The appearance of discrete kerolitic domains suggests that the charged domains might have been preferentially dissolved, enhancing particle disaggregation through separation of the charged from the uncharged domains and therefore improving the rheological properties at high temperatures.
Use of trioctahedral clays in high-temperature drilling muds
Due to their high dehydroxylation temperatures, trioctahedral clay minerals have greater thermal stability than their dioctahedral counterparts. Therefore, they are possible candidates for the formulation of drilling muds that are employed in high-temperature wells, provided that, in the case of smectites, the interlayer cation is Na. All smectites used in this study were Na-activated, but only hectorite muds developed satisfactory rheological properties, with the behaviour of the remaining clays being unpredictable. The inferior rheological properties of saponite might be attributed to the incomplete Na-exchange because they are expected to display a greater tendency for adsorbing hydrated cations and swelling, thus facilitating ion exchange, provided that they do not collapse. Yet, after ageing, the d001 of saponite was centred at 13–14 Å, and a minor shoulder indicative of Na layers appeared at ~12.8 Å (Fig. 1b). The incomplete Na-exchange in the saponite interlayer with respect to hectorite might reflect the influence of charge localization on the exchange. The saponite is dominated by a tetrahedral charge. Hence, it could be considered that this tetrahedral charge might hinder the Na-for-Ca exchange. Nevertheless, the concentration of Na2CO3 used to activate the clay was 6%, suggesting that only a fraction of the added Na was not exchanged. Therefore, the incomplete Na-exchange cannot explain the inferior rheological properties of saponite.
Although charge localization does not account for the observed incomplete Na-exchange in saponite, it might be considered for the interpretation of the rheological properties. Dioctahedral smectites with a tetrahedral charge have inferior rheological properties compared to their counterparts with an octahedral charge of similar magnitude located in octahedral sites (Christidis et al., 2006) because the tetrahedral charge will control the maxima of the potential curves on the surface of smectite (Bleam, 1990), which will lead to the aggregation of layers and thus to the suppression of the diffuse double layers. A similar behaviour is suggested for the trioctahedral smectites. Therefore, saponites are not expected to develop satisfactory rheological behaviour at any temperature, although the tetrahedral charge seems to provide greater thermal stability against dissolution in the temperature range considered in this study. Nevertheless, the rheological behaviour might be improved with the addition of suitable additives, but this is beyond the scope of this work.
Stevensite displayed differing rheological behaviour from hectorite, although they both have octahedral charge and the layer charge of stevensite is lower than that of hectorite (Christidis & Eberl, 2003; Rhouta et al., 2008). The small ratio of vacant octahedra, which are the source of the layer charge, to the occupied octahedra (~1:27; c.f. Rhouta et al., 2008) suggests that the uncharged non-swelling kerolite domains hinder Na-exchange. Inasmuch as the uncharged kerolite layers are expected to be hydrophobic, similarly to talc layers, they impede Na-exchange in the charged layers, causing limited swelling and thus inferior rheological properties. Dolomite dissolution hindered Na-exchange further. The preferential dissolution of the vacant octahedra compared to their occupied counterparts during high-temperature ageing facilitated particle separation and thus Na-exchange, thereby promoting Na-activation of the stevensite. Therefore, stevensite drilling fluids seem to be promising for high-temperature applications.
Hectorite suspensions presented superior rheological performance to all of the other examined clay minerals, even though the content of hectorite in the sample was <50% and dolomite dissolution hindered Na-exchange. Thermal ageing increased the PV and AV of hectorite suspensions, which demonstrated plastic flow behaviour. The extensive gel formation of hectorite suspensions led to the YP being reached, which is associated with the hydration of clay particles and the electrostatic interactions amongst them. The YP is a function of the number and strength of particle–particle bonds (van Olphen, 1964; Neaman & Singer, 2000a). In addition, hectorite displayed very good thermal stability over the whole temperature range used in this study. Therefore, hectorite is an excellent material for the formulation of drilling fluids for high-temperature applications.
The rheological properties of sepiolite were inferior to those of its bentonite counterparts. The rheological performance of fibrous clays is connected to their fibre length, CEC (which is low) and specific surface area (Simonton et al., 1988; Neaman & Singer, 2000b). The silanol groups at the external sepiolite surfaces bind the fibrous sepiolite crystals, forming networks and thus affecting the AV and YP of sepiolite suspensions (Simonton et al., 1988). However, the sepiolite did not develop suspensions with acceptable rheological behaviour, and a similar rheological behaviour was observed in a preliminary study of a Spanish sepiolite (data not shown). Nevertheless, the thermal stability of sepiolite at high temperatures indicates that it might be rendered suitable for high-temperature drilling applications after the addition of suitable additives. More information regarding the structural characteristics (e.g. specific surface area, fibre length, etc.) and use of additives in this context is necessary to support this suggestion.
Conclusions
This study examined the influence of thermal ageing (up to 230°C) on 5% suspensions of Mg-bentonites containing trioctahedral smectites (hectorite, stevensite and saponite) after activation with Na2CO3 and a sepiolite clay, and it yielded the following conclusions.
In general, thermal ageing did not affect the thermal stability of the clays. Except for stevensite clay at 230°C, the clay minerals displayed minimal dissolution after thermal ageing. Hectorite and saponite displayed the best thermal stability at all temperatures, whereas stevensite crystals displayed dissolution features and partial conversion to kerolite after thermal ageing at 230°C. Thermal stability (recorded as resistance to dissolution), the response to Na-activation and the rheological properties of the clays are directly associated with the crystal structure: namely, layer charge and charge localization, the particle shape of the clay minerals present and the presence of Mg-accessory minerals that might dissolve during thermal ageing, such as dolomite.
Based on the rheological properties, the sepiolite clay is considered unsuitable for drilling fluids at high temperatures. The rheological properties were almost identical and inferior to bentonites, presenting a subtle, plastic flow behaviour at higher temperatures. Moreover, the filtrate loss volume exceeded 15 mL. In addition, the saponite clay is not recommended for drilling fluid applications as it collapses at greater temperatures. Moreover, it did not present acceptable YP and viscosity, and hence its lubricating, insulating and carrying performances do not meet API 13A specifications. Nevertheless, the sepiolite and saponite clay suspensions might meet API 13A specifications if the concentration of solids is raised to 6.42%.
The activation of the cation-exchange mechanism of stevensite clay at high temperatures makes it a suitable additive for drilling fluids in high-temperature operations such as high-enthalpy geothermal fields or deep oil well drilling. The intense gel formation leads to high YP values, which might cause malfunctions in the mud pumps. Consequently, the utilization of stevensite clays in drilling fluid applications is recommended, along with other viscosity- and gel formation-regulating agents.
The hectorite clay displayed excellent rheological properties that did not deteriorate with increasing temperature, although the hectorite content was low. Therefore, this hectorite clay is recommended for a wide range of drilling purposes. However, its concentration should remain low due to the development of viscous fluids with considerable amounts of gel, which might prove stressful to the pumping equipment.
Acknowledgements
This paper is a result of the diploma thesis of N. Athanasakis (mineral resources engineering MSc), carried out at the Mineral Resources Engineering Department, Technical University of Crete. Professor Dr G.E. Christidis was the supervisor and editor of this paper and Professor Dr D. Marinakis planned the rheological experiments.
Conflicts of interest
The authors declare none.