1. Introduction
Grouting technology refers to formulating suitable cementitious materials into a targeted slurry, which is then injected, either directly or indirectly, into the geotechnical body using pressurized equipment. This process aims to alter the mechanical distribution and structural composition of the geotechnical body. Subsequent solidification of the slurry with the existing formation creates a composite body, enhancing the physical and mechanical properties to achieve waterproofing and reinforcement objectives [
1]. Currently, grouting technology is extensively employed in managing water damage and reinforcing surrounding rock in mines, along with applications in tunnel and foundation engineering. This method plays a crucial and irreplaceable role in resource safety development, geological disaster management, and the reinforcement of underground surrounding rock [
2,
3,
4,
5,
6]. Current research on grouting technology primarily concentrates on grouting theory, materials, and techniques. These studies are particularly significant for advancing green, efficient, and safe practices, with a special emphasis on the development and improvement of grouting materials.
Grouting material constitutes a critical component of grouting technology and is a pivotal factor in determining the effectiveness of grouting [
7,
8]. Since the advent of grouting technology, a diverse range of grouting materials has emerged, primarily categorized into inorganic and organic types. Cement slurry, comprising primarily cement mixed with minor additives and water, represents the earliest and most prevalent inorganic grouting material. This mixture is prepared and injected in a single-fluid manner. The advantages of cement slurry include its abundant availability, low cost, high compressive strength, effective seepage resistance, non-toxicity, simplicity of the process and equipment, and ease of operation [
9,
10]. However, the disadvantages of cement slurry include a prolonged setting time, low initial strength, slow strength development, susceptibility to water separation, poor injectability, and vulnerability to being washed away by groundwater [
11]. Consequently, to enhance the performance of cement slurry in practical engineering applications, various modifiers—including quick-setting agents, early strength agents, suspending agents, lime, graphene oxide, and nano-additives—are commonly incorporated.
In recent years, extensive research has been conducted by scholars on the influence of various modifiers on the performance of cement-based grouting materials. Jia et al. [
12] incorporated polypropylene short fibers of 3 mm and 6 mm lengths into cement grouting materials and assessed their impact on fluidity, mechanical properties, drying shrinkage rate, and pore structure. The research revealed that polypropylene fibers enhance toughness, reduce water loss, and diminish drying shrinkage. Specifically, the use of 0.9 vol% 3 mm polypropylene fibers resulted in a 38% increase in the 28-day flexural strength of the grouting material and a 22% reduction in the drying shrinkage rate. Hu et al. [
13] incorporated two modifiers—early-strength and high-strength grouting modifiers—into cement-based grouting materials. They evaluated the impact of these modifiers on setting time, fluidity, plastic viscosity, and yield stress under varying water-to-cement ratios, ultimately focusing on the rheological properties of the materials. Cheng et al. [
14] incorporated varying amounts of graphene oxide into cement-based grouting materials and assessed the resultant changes in crystal structure, mechanical properties, and self-shrinkage characteristics of the modified materials. Yuan et al. [
15] introduced stabilizers and reinforcing agents into cement slurry, achieving a reduction in water separation rate from 21% to 5% for slurries with a 1:1 water–cement ratio. This modification maintained the compressive strength comparable to that of untreated slurries and significantly enhanced overall performance. Wang et al. [
16] developed a fast-hardening cementitious grouting material using sulphur–aluminate cement and investigated the influence of nano-SiO
2 on the fluidity and mechanical properties of the grouting materials across various water–cement ratios. The study found that adding 1.0% nano-SiO
2 increased the compressive strength of the grouting material by up to 44% without sacrificing fluidity. Shen et al. [
17] explored the impact of mineral admixtures—including fly ash, limestone powder, and silica fume—on the fluidity, rheological properties, and strength of cement-based grouting materials. Compared to pure cement grouting, the initial fluidity and 60 min fluidity of grouting materials with 40 wt% fly ash decreased by 35.5% and 53.8%, respectively.
Polycarboxylate superplasticizers are a type of admixture employed in concrete modification that disperses cement particles, reduces unit water consumption, and enhances the fluidity of the concrete mix. In recent years, advancements in the research and development of polycarboxylate superplasticizers have led scholars to explore their use in modifying grouting materials. Costa A. Anagnostopoulos [
18] utilized polycarboxylate superplasticizer (PCE) to modify cement slurry and investigated its effects on the rheological properties, mechanical strength, and water precipitation rate of the slurry through a series of experiments. The study found that the addition of PCE induced shear thickening in the slurry. For slurries with water–cement ratios of 0.4 and 0.5, the incorporation of PCE significantly increased the strength of the slurry stone body. However, in slurries with a water–cement ratio of 0.3, high doses of PCE reduced the early strength development and resulted in limited final strength growth. Puertas [
19] examined the impact of polycarboxylate (PC) admixtures on the mechanical, mineralogical, microstructural, and rheological properties of Portland cement slurries. The research demonstrated that PC admixtures delay the initial hydration reaction of cement, reduce the maximum yield stress of the slurry by 70%, and alter the microstructure of the slurry stone body, albeit with minimal effect on the strength of the stone body. Zhang et al. [
20] investigated the effect of polycarboxylate superplasticizers on the performance of a fine tailings filler slurry composed of cement and fine tailings. The study found that the addition of polycarboxylate superplasticizers induced shear thinning in the slurry, reducing the early strength of the slurry stone by 10.29% but ultimately increasing the strength by 10.51%. At present, there is still a lack of research and literature on the modification of grouting materials using polycarboxylate superplasticizers, especially in the quantitative analysis of the micropores and phase composition of slurry stone bodies. Further research is needed.
To enhance grouting efficiency, fluidity of cement slurry at low water–cement ratios, and slurry stability, and to offer scientific guidance on material proportioning, this study employs polycarboxylate superplasticizers BMC-L and BMC-S as modifiers in the development of new cement-based grouting materials. Utilizing indoor testing, this study tested the basic performance and mechanical performance of cement slurries across different formulations varying in water–cement ratios and polycarboxylate superplasticizer content, exploring the impact of polycarboxylate superplasticizers on the mechanical properties of cement-based grouting materials. Additionally, the study examines the evolution of the microscopic pore structure and phase composition of the slurry stone body with varying dosages of polycarboxylate superplasticizer. This provides a detailed analysis of the effects of the polycarboxylate superplasticizer on cement-based grouting materials at the microstructural level.
3. Results and Discussion
3.1. Slurry Density
Slurry density significantly influences the pumpability of cement slurry during the grouting process. Excessively high slurry density diminishes fluidity and pumpability, whereas excessively low density increases fluidity, potentially resulting in cement slurry loss and uneven deposition. A relative densitometer measured the density of each slurry test group, with results presented in
Figure 2. As illustrated in
Figure 2, slurry density exhibits minimal variation with increasing dosages of the two polycarboxylate superplasticizers. Notably, densities fluctuate slightly when the dosage is below 6‰; however, densities stabilize when the dosage exceeds 6‰. This phenomenon may be attributed to the full reaction between polycarboxylate superplasticizer and cement, reaching a saturation point at a dosage of 6‰. Additionally, the figure indicates that the water–cement ratio critically affects slurry density; a higher water–cement ratio correlates with lower density and better pumpability.
3.2. Slurry Funnel Viscosity
Viscosity is defined as the measure of internal friction experienced by molecules during liquid flow. In slurries, the magnitude of viscosity directly influences the diffusion radius and critically determines parameters such as grouting pressure and flow rate. As slurry viscosity increases, both its fluidity and diffusion radius decrease correspondingly.
Funnel viscosity for each test slurry was measured using a funnel viscometer, with results detailed in
Figure 3. As illustrated in
Figure 3, within the 0~6‰ dosage range of two types of polycarboxylate superplasticizers, an increase in dosage significantly reduces the slurry funnel viscosity, which does not follow a linear relationship. Notably, for a water–cement ratio of 0.5:1, the addition of the polycarboxylate superplasticizers resulted in a sudden change in funnel viscosity. When the dosage of polycarboxylate superplasticizer was increased from 6‰ to 14‰, there was negligible change in slurry funnel viscosity, indicating an effective incorporation range of 0~6‰ for the polycarboxylate superplasticizers used in this study. In this range, slurry funnel viscosity decreases with the increase of polycarboxylate superplasticizer content. Within this incorporation range, an increase in polycarboxylate superplasticizer content results in decreased slurry funnel viscosity. In addition, under identical conditions of water–cement ratio and polycarboxylate superplasticizer dosage, BMC-L exhibited lower slurry funnel viscosity compared to BMC-S, highlighting its superior efficacy in reducing viscosity. After adding polycarboxylate superplasticizer, the viscosity of the slurry significantly decreases. This may be because the adsorption layer formed by superplasticizer molecules on the surface of cement particles reduces direct contact between particles, thereby reducing the internal friction and cohesion of the mixture. This makes the cement slurry have lower viscosity and better fluidity at the same water content, which is helpful for pumping and construction of the slurry.
3.3. Slurry 2 h Water Separation Rate and Stone Rate
The water separation rate is a critical metric for assessing the stability and pumpability of slurry, significantly influencing the structure of the stone body and the efficacy of grouting reinforcement. A lower water separation rate reduces the tendency for segregation and delamination, enhancing the suitability of the slurry for pipeline transportation and its ability to fill fissures and pores effectively. The water separation rate over a specific duration indicates the slurry’s stability. A slurry that maintains a water separation rate of no more than 5% after standing for 2 h is considered stable.
The 2 h water separation rate for each test slurry was determined using a 100 mL measuring cylinder. After the test, the 2 h water separation rate of each group of slurry is 0, which indicates that the two polycarboxylate superplasticizers have almost no effect on the 2 h water separation rate of the slurry, and the slurry is a stabilized slurry after mixing polycarboxylate superplasticizer. Following complete solidification, the stone rate was measured.
Figure 4 illustrates the impact of varying dosages of polycarboxylate superplasticizers on the stone rate, showing an initial decrease followed by stabilization as the dosage increases. For a 0.6:1 water–cement ratio slurry, BMC-S more significantly reduces the stone rate than BMC-L. At a 0.5:1 water–cement ratio, the impact of polycarboxylate superplasticizers on the stone rate is comparable within the 0~6‰ range. Beyond this dosage, BMC-L is greater than BMC-S in reducing the stone rate. The reduction in slurry stone rate after the addition of polycarboxylate superplasticizer can be attributed to its effective dispersion effect, which diminishes aggregation among cement particles. This dispersion results from the unique molecular structure of the superplasticizers, particularly the side chains that form an adsorption layer on the cement particle surfaces, enhancing the repulsive forces between them.
3.4. Slurry Formulation Selection
To advance the study of how polycarboxylate superplasticizer affects the apparent viscosity of the slurry and the mechanical properties of the slurry stone body, a comprehensive analysis of density, funnel viscosity, 2 h water separation rate, and stone rate for each test slurry was conducted. The relatively optimal slurry formulations were selected for the subsequent slurry apparent viscosity test, uniaxial compression test, triaxial compression experiments, nuclear magnetic resonance test, and X-ray diffraction test.
The density of the tested slurries was more significantly influenced by the water–cement ratio compared to the dosage of the water-reducing agent. Comparative analysis was performed on slurry funnel viscosity across two water–cement ratios, two types of polycarboxylate superplasticizers, and various dosages. The effective dosage range for polycarboxylate superplasticizers was identified as 0~6‰. Notably, slurries with a 0.6:1 water–cement ratio and BMC-L superplasticizer exhibited lower funnel viscosities compared to others. A comparative analysis of the slurry stone rates revealed that mixtures with a 0.5:1 water–cement ratio and BMC-L superplasticizer generally exhibited higher stone rates than others. Within the dosage range of 0 to 6‰ for polycarboxylate superplasticizers, comparing slurry with water–cement ratios of 0.6:1 using BMC-L and 0.5:1 using both BMC-L and BMC-S, the stone rates are relatively similar.
Following a comparison of performance indices among the various slurry groups—distinguished by two water–cement ratios, two types of polycarboxylate superplasticizers, and varying dosages—the slurry formulation with a 0.6:1 water–cement ratio, BMC-L type superplasticizer, and water-reducing agent dosages of 0, 2‰, 4‰, and 6‰ was chosen for subsequent experimental investigations.
3.5. Apparent Viscosity of Slurry
The slurry outlined in
Section 3.4 is prepared, and its apparent viscosity is measured using a DHJ-5S/8S rotary viscometer produced by Ningbo Lawson Smarttech Co., Ltd. in Ningbo, China.
Figure 5 illustrates the relationship between the apparent viscosity of the slurry and the shear rate at various BMC-L dosages.
Figure 5 demonstrates that as the shear rate increases, the apparent viscosity of the slurry decreases, exhibiting “shear thinning” behavior where viscosity diminishes with higher shear rates. Compared to formulations without BMC-L, the addition of BMC-L significantly lowers the apparent viscosity of the cement slurry, with greater reductions observed at increasing dosages of BMC-L across various shear rates. At BMC-L dosages of 4‰ and 6‰, the shear rate–apparent viscosity curves nearly coincided, suggesting that at dosages ≥ 6‰, the slurry’s apparent viscosity reaches a minimally low level, beyond which further increases in BMC-L dosage minimally affect the viscosity.
3.6. Mechanical Properties of Slurry Stone Body
3.6.1. Uniaxial Compressive Strength
The uniaxial compressive strength of the slurry stone body is a crucial mechanical property that significantly influences slurry applications.
Figure 6 illustrates the relationship between the uniaxial compressive strength of the slurry stone body and the BMC-L dosage. It is observed that the uniaxial compressive strength of slurry stone bodies increases with the addition of BMC-L, with minimal strength gains at 3 days and significant increases at 7 and 28 days. At a BMC-L content of 6‰, the uniaxial compressive strengths at 7 and 28 days are 118.4% and 64% higher, respectively, than those of slurry without BMC-L. The increase in compressive strength of the slurry stone body is attributed to the use of polycarboxylate superplasticizers, which enhance the uniformity and density of the slurry. The hydration products formed after cement hydration, such as calcium silicate hydrates (C-S-H), are distributed more evenly throughout the slurry and fill its micropores, thus bolstering the mechanical properties of the stone body. Moreover, polycarboxylate superplasticizers delay the initial phase of cement hydration, moderating the dissolution and hydration reactions of cement particles. Consequently, the initial increase in strength of the slurry stone body is relatively modest but significantly greater in the later stages.
3.6.2. Stress–Strain Relationship
Figure 7 displays partial stress–strain curves for slurry stone bodies with varying dosages of BMC-L, subjected to triaxial compression under different confining pressures. As depicted in
Figure 7, the stress–strain curves of slurry stone bodies under various confining pressures follow a similar trend. Initially, stress increases with strain; upon reaching peak stress, it then decreases with further strain increase. Eventually, a sharp decline in stress indicates specimen failure.
The stress–strain relationship in slurry stone bodies with varying BMC-L dosages encompasses three distinct stages: (1) Elastic Deformation Stage: At the beginning of loading, the relationship between partial stress and strain is essentially linear. Axial strains primarily result from the compression of pore spaces between particles. With the axial loading, the particles are gradually compressed, and radial strain at this stage is smaller; (2) Plastic Deformation Stage: As axial and radial strains increase, the slope of the stress–strain curve decreases, indicating a nonlinear relationship and rapidly approaching peak stress. During this phase, internal particle compression and extrusion occur alongside local plastic deformation and cracking within the specimen; (3) Destruction Stage: the partial stress reaches the peak value, and the crack of the slurry stone body continues to expand. Finally, the stone body enters the destruction stage after rupture, and the curve shows a fluctuating downward state. Additionally, the figure illustrates that under a fixed confining pressure, the maximum partial stress in the slurry stone body increases with higher BMC-L dosages. Conversely, at a constant BMC-L dosage, the maximum partial stress escalates with rising confining pressure.
3.6.3. Shear Strength Parameters
To determine the shear strength parameters at various BMC-L dosages, the maximum partial stress served as the criterion for evaluating shear strength. With reference to the relevant triaxial compression test studies, the experimental results were solved by the programming solver tool of Excel 2016 [
22] to obtain the cohesion and internal friction angle of each group of specimens, and the collated results are shown in
Table 3.
The influence of BMC-L dosage on the cohesion and internal friction angle of the slurry stone body is illustrated in
Figure 8 and
Figure 9. As depicted in the figures, an increase in BMC-L dosage results in higher cohesion and internal friction angles. Specifically, cohesion escalated from 2.1 MPa to over 3 MPa, marking a maximum increase of 50.4%. Similarly, the internal friction angle rose from approximately 48 degrees to over 60 degrees, achieving a maximum increase of 29.8%. This indicates that BMC-L positively enhances the shear strength of the slurry stone body. This improvement is attributed to BMC-L’s role in dispersing cement particles and expanding their hydration reaction surface area, which facilitates the production of more cement hydration products, leading to a more uniform and denser structure.
3.6.4. Elastic Modulus
The elastic modulus of a slurry stone body characterizes its stiffness, representing the resistance of the stone body to deformation under load. This parameter is crucial for determining the bearing capacity and deformation resistance of the stone body. Referring to the related research, the elastic modulus E is calculated from the slope between the 30% and 70% strength peaks on the stress–strain curve and can be calculated using the following formula:
In the formula,
represents 70% maximum stress,
represents 30% maximum stress,
represents strain corresponding to 70% maximum stress, and
represents strain corresponding to 30% maximum stress. According to this formula, the elastic modulus of the slurry stone body with different BMC-L dosages under different confining pressures is obtained.
Figure 10 illustrates the relationship between the elastic modulus of the slurry stone body and varying dosages of BMC-L. The figure demonstrates that under all tested confining pressures, the elastic modulus increases with higher BMC-L dosages. This suggests that BMC-L improves the microstructure and stiffness of the slurry stone body, thereby increasing its resistance to compressive deformation. At a constant BMC-L dosage, the elastic modulus rises with increasing confining pressure. Notably, at a lower confining pressure (100 KPa), the increase in elastic modulus is relatively slow, whereas, at higher pressures (200 KPa and 300 KPa), it escalates more rapidly with additional BMC-L. This effect is attributed to higher confining pressures compacting the internal pores of the slurry stone body, resulting in a denser structure and, thus, a higher elastic modulus.
3.7. Pore Structure and Phase Composition of the Slurry Stone Body
3.7.1. Pore Structure
Recently, low-field nuclear magnetic resonance (NMR) has emerged in the geotechnical field as a rapid, non-destructive technology that provides an intuitive display of detection and can effectively characterize changes in the internal microscopic pore structure of rocks. In the natural state, the spin of the 1H nucleus is in a disordered state without magnetization. When the sample is placed in the test chamber of the nuclear magnetic resonance (NMR) instrument, the action of the main magnetic field will make the 1H nucleus magnetization phenomenon. The interaction between the spin magnetization of the 1H nucleus and the applied magnetic field will produce a signal that can be measured by the instrument, which is the prerequisite for the generation of NMR. The 1H nuclear proton leaps from a low-energy state to a high-energy state, a phenomenon known as NMR. It rotates along the direction of the applied magnetic field and releases energy to the outside world. The process of transition from a high-level state to a low-level state is called nuclear magnetic resonance relaxation. The transverse relaxation time decay, or T2 decay, contains the physical information of most porous samples, so T2 is the main target of rock NMR detection. According to the mechanism of nuclear magnetic resonance detection, the slurry stone body is subjected to vacuum-forced saturation to ensure that the water is fully filled with the internal pores of the slurry stone body. The T2 spectra of the slurry stone body are obtained by nuclear magnetic resonance test of the 1H nucleus in the water, and the internal pore characteristics and variation rules of the slurry stone body can be obtained by analyzing the T2 spectra.
The
T2 relaxation time is categorized into surface
T2 relaxation, free
T2 relaxation, and diffusion
T2 relaxation. For porous materials such as the slurry stone body, the relaxation time is mainly affected by the surface
T2 relaxation, and thus, the
T2 can be expressed according to the following formula [
23]:
In the formula,
T2 represents transverse relaxation time (ms),
represents the surface relaxation strength of
T2 (μm/ms),
S represents pore surface area (cm
2), and
V represents pore volume (cm
3). It can be seen that the transverse relaxation time
T2 is proportional to the pore-specific surface area (
S/
V) and the surface relaxation strength
, and Formula (2) can be further simplified to Formula (3):
In the formula,
r represents the pore radius (μm),
F2 represents the shape aggregation factor, taking value 3 for spherical pores and 2 for columnar pores, and
represents the surface relaxation strength of
T2 (μm/ms); the value can be referred to in
Table 4. Li et al. [
24] and Zhang et al. [
25] suggested a range of values for
from 0.01 to 0.15 μm/ms. In this paper, the value of 0.01 μm/ms is taken. This establishes a link between the transverse relaxation time
T2 and the pore radius
r. It can be seen that the larger the value of
T2, the larger the pore radius, and vice versa.
The pore structure of the slurry stone body includes pore distribution and pore aperture. Pore aperture directly influences the macroscopic strength of slurry stone bodies and is typically classified into micropores, mesopores, and macropores. Currently, there is no standard uniform method for this classification.
Table 5 summarizes commonly used methods for classifying pore apertures. It is evident that scholars vary in their definitions of micropores, mesopores, and macropores. In this study, pore apertures are classified according to Yan Jianping’s method: micropores are defined as pores smaller than 0.1 μm, corresponding to
T2 times less than 10 ms; mesopores range from 0.1 μm to 1 μm, with
T2 times between 10 ms and 100 ms; and macropores exceed 1 μm, corresponding to
T2 times greater than 100 ms.
Figure 11 displays the NMR
T2 spectra of slurry stone bodies with varying BMC-L contents, where the upper axis represents the converted pore radius. The figure shows that as BMC-L dosage increases, the NMR signal from the slurry stone body specimens decreases, suggesting a reduction in internal pore volume and overall porosity. There are two peaks in the
T2 spectra of the sample. The first peak
T2 from left to right is mainly between 0.05 and 7.5 ms, and the corresponding pore size is 0.005–0.75 μm, indicating that the first peak is in the range of micropore pores. The second peak
T2 is mainly in 7.5–68 ms, and the corresponding pore size is 0.075–0.68 μm, indicating that the second peak mainly contains micropores and mesopores, and the mesopores account for most of the pores. With the increase of BMC-L dosage, the peak area of the
T2 spectra curve of the sample decreases continuously, and both peaks shift to the left, indicating that the internal pores of the sample decrease and the pore radius decreases. This occurs because polycarboxylate superplasticizers render the cement slurry more uniform, allowing the cement hydration products to distribute more evenly. This uniform distribution effectively fills the micropores and microcracks within the slurry, thereby reducing both the porosity and pore radius of the slurry stone body.
3.7.2. Phase Composition
The X-ray diffraction (XRD) technique is a method to accurately identify the crystal structure and phase composition of materials by measuring the diffraction angle and intensity distribution of samples to X-rays. Widely utilized across various scientific and engineering disciplines, including physics, chemistry, and materials science, XRD has become an indispensable method for material structure analysis. The primary advantage of XRD is its capability to elucidate the crystal structure of a material and to identify and quantitatively analyze its phase composition. In cement-based material research, XRD is employed not only to determine the mineral composition of cement clinker but also to analyze the phase and structure of its hydration products. Consequently, XRD is pivotal in assessing the performance and optimizing formulations of cement-based materials.
To analyze the phase types and content changes in slurry stone bodies with varying BMC-L dosages, XRD was employed to test these variations. The XRD patterns of each slurry stone body are shown in
Figure 12. Different hydration products correspond to different diffraction angles, and the heights of the diffraction peaks correspond to different levels of hydration product content. According to
Figure 12, the hydration products remain consistent at BMC-L dosages of 0 and 2‰. At higher dosages of 4‰ and 6‰, a small quantity of kaolinite (Al
2Si
2O
5(OH)
4) begins to appear in the hydration products, as seen in
Figure 12c,d. This may be due to the fact that a higher dosage of superplasticizer enhances its dispersion effect, thereby facilitating more complete hydration.
To further investigate the variation in phase content of slurry stone bodies with BMC-L dosage, a quantitative analysis of their phase composition was conducted. The results of this analysis are presented in
Table 6 and
Figure 13.
Figure 13 illustrates that portlandite is the predominant phase in the slurry stone composition, followed by ettringite and calcium aluminum oxide carbonate hydrate. As BMC-L dosage increases, the proportions of portlandite, ettringite, calcium aluminum oxide carbonate hydrate, and calcium aluminum oxide carbonate hydroxide hydrate in the slurry stone body’s phase composition rise, while those of larnite, hatrurite, and quartz diminish. This trend suggests that BMC-L enhances hydration reactions; higher dosages result in more complete hydration and greater formation of hydration products.