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Dynamic Ground Support in Underground Mines

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Research Article | Open Access

Volume 2021 |Article ID 6627520 | https://doi.org/10.1155/2021/6627520

Xiaowei Feng, Fei Xue, Tongyang Zhao, Wenjie Jiang, "Mechanical Modification of Resin Capsules by Adding Steel Particles", Shock and Vibration, vol. 2021, Article ID 6627520, 13 pages, 2021. https://doi.org/10.1155/2021/6627520

Mechanical Modification of Resin Capsules by Adding Steel Particles

Academic Editor: Nur Izzi Md. Yusoff
Received09 Dec 2020
Revised04 Feb 2021
Accepted16 Jun 2021
Published25 Jun 2021

Abstract

Five kinds of steel particles with sizes ranging from 0.6 mm to 2.2 mm with increments of 0.4 mm were mixed with mining resin materials, and the mixing ratio of the particles was also varied. By using this approach, the film gloving problem of coal mine bolting should be effectively solved due to the shredding effects of the particles during bolt rotation. The premise is that the mechanical behavior should not be weakened under such conditions. A total of 47 standard cylindrical specimens were manually prepared, which included pure resin specimens and specimens containing particles with different sizes and weights. First, the homogeneity of a prepared standard specimen was verified by computed tomography (CT) scanning technology. Second, the mechanical improvements provided by each type of particle were evaluated. Thirdly, the effectiveness of both the particle weight and particle size was comprehensively discussed, and the eventual recommendation was to set for the particle size and weight as 1.4 mm and 40 g, respectively, and the particles weight percentage was 7.27%. Finally, the failure patterns for all specimens were collected and comprehensively compared. Additionally, pullout tests were carried out to vindicate the recommended particle size and weight.

1. Introduction

A bolting system consists of a rebar inserted into a borehole and is simultaneously bonded with a rock mass by using a specific bonding material. Through the use of a bolting system, the deformation of a rock mass can be restrained, or a loose rock mass can be reinforced; eventually, the potential instabilities of rock masses can be largely prevented [13]. Bolting technologies are widely used in geotechnical and mining areas, and to the best of the author’s knowledge, bolting technology emerged over a hundred years ago in a slate quarry in North Wales in 1872 [4].

Currently, a bolting system uses either a resin cartridge or cementitious material to serve as an intermediary that can bond a bolt to the inner wall of a borehole. Consider that the reinforcement provided by the bolt can be classified as follows: (1) Continuously Mechanically Coupled (CMC); (2) Continuously Frictionally Coupled (CFC); and (3) Discretely Mechanically or Frictionally Coupled (DMFC) [5]. The classification is based on how the element load is transferred to the rock, and then the resin-bonded bolts belong to the CMC system. Nowadays, two-part polyester resin cartridges are extremely popular, especially in coal mines, because this resin system can achieve fantastic controlling effects of rock deformation when the resin cooperates appropriately with bolts and boreholes. The most obvious advantage of a resin cartridge is its fast-setting property, by which the fastest resin can set in less than or equal to 30 seconds [6]. Then, a rock mass can be reinforced immediately after excavation, which is particularly beneficial to the overall stability of an underground excavation. Additionally, the high early strength achieved by the resin is another advantage that can provide sufficient supporting effects to a rock mass, which is far beyond the corresponding property of a cementitious material.

Nevertheless, resin-based bolting systems still face challenges in practical applications. One noticeable problem is gloving, which is a phenomenon where the plastic cartridge of a resin capsule either partially or completely encases a certain length of a bolt, typically with a combination of mixed and unmixed resin filler and catalyst remaining within the cartridge [7, 8]. Gloving often leads to poor bearing strength in a bolting system due to the mixed or unbonded section along the bolt; as a result, the bolting system tends to exhibit premature failure. As early as 1987, Pettibone’s work indicated that resin properties alone could dramatically alter the extent of gloving [9]. In 2004, tests conducted by Campbell, Mould, and MacGregor testified that chamfered bolts, sinusoidal bolts, and offset nuts can reduce gloving and give the best results [10]. In 2005, Pastars and MacGregor concluded that the simulated gloved bolts provided only 10% of the load transfer of the nongloved test cases. In the same year, Compton and Oyler argued that there was no reduction in bond strength from gloving based on a comparison of standard 300 mm short encapsulation pull tests (SEPTs) and overcoring standard bolt pull tests.

More recently, in 2012, Peter Craig performed extensive in situ tests and indicated that SEPTs of gloved and nongloved bolts produced similar bond strength results; also, gloving could only be significantly reduced by a modified bolt end that nearly contacted the side of the bolt hole [11]. In 2016∼2017, Ma et al. and Aziz et al. noticed that the top parts of most bolts had the least bond strength due to film gloving and unmixed resin, and these authors proposed an overdrilled hole installation since it can mitigate capsule film gloving in the tops of bolts [12, 13].

In view of the short survey above, the main solutions for reducing gloving include improving the resin properties, modifying the bolt end, and overdrilling. By adding steel particles to resin, the mechanical properties of resin could be improved [14], and more importantly, all the gloving problems could also be simultaneously reduced due to the shredding effect during bolt installation process [15]. This work uses the following two guidelines, leaving opportunities for further detailed tests and verifications. (1) Steel wires that are 2 mm in diameter were manually cut to 2.0∼3.5 mm lengths, and the effects of various diameters and lengths were unknown. (2) Only 20∼40 steel particles were added into the resin for each specimen, and the effect of the weight ratio between steel particles and resin was unknown.

In this context, this study endeavors to investigate the effects of the size and weight of steel particles when mixed with the resin material. By adding specific steel particles into the resin, the strength of the modified resin was tested and analyzed, and the pullout tests on bolts boned by modified resin were carried out. Under the established results, possibility of adding particles to alleviate film gloving problems in actual bolting system in engineering environment could be achieved.

2. Materials and Methods

2.1. Brief Introduction of the Resin, Steel Particles, and Preparation Procedure

The resin capsule consisted of two separately packed internal areas and an outer packing film. One of the internal areas was filled with the resin and coagulation accelerator; the other area was filled with the curing agent. Under the rotation effect of the bolt, the film is shredded, and then these materials mix and eventually solidify in less than one minute. Solidification is extremely important to transfer the load between the bolt and rock mass; thus, tiny deformation of the rock mass can be detected and then restricted. The lengths and diameters of the resin capsules were 2300 mm and 50 mm, respectively. An actual photograph of the utilized resin capsule is shown in Figure 1(a).

The steel particles adopted in this test have various sizes: 0.6 mm, 1.0 mm, 1.4 mm, 1.8 mm, and 2.2 mm, as shown in Figure 1(b). Considering the appropriate thickness of the annulus between the bolt and the borehole, particles with sizes greater than 2.2 mm were not studied. Existing studies have already shown that the annulus thickness should be 3∼4 mm [16, 17], and excessively large particles are impractical, because they greatly increase the rotation resistance during the actual installation process, which slows the drill and lowers the installation speed.

The specimen preparation requires a proper mixture between the resin and steel particles, which was accomplished by using the following procedure:

First, the exact type of steel particle was chosen, and then the specific weight was measured on an electronic scale. Second, a knife was used to slit the packing film of the resin capsule to separately gather the resin and coagulation accelerator and the curing agent. Third, the two components of the resin capsule and the steel particles were manually mixed, and then the mixture was rapidly kneaded; it is extremely important to ensure the homogeneity of the mixture. A blender was not adopted because some preliminary trials have been conducted with several kinds of blenders, which showed that the resin compound could not be homogenously mixed with the steel particles with a blender. Simultaneously, the mixture process needed to be fast because the setting time was less than or equal to one minute. This procure normally required a relatively skilled operator. Fourth, the mixture was placed inside a standard 50 mm × 100 mm cylindrical mould, and the inner wall of the mould was waxed in advance for convenient demoulding. Demoulding could be performed roughly ten minutes later or after the temperature of the outer wall of the mould reached its regular temperature (the mixture process exhibited an exothermic reaction). The last step was machining. The semifinished specimens prepared in the fourth step generally could not guarantee precise standard 50 mm × 100 mm cylindrical specimens; hence, the demoulded specimens were further subjected to a machining procedure. Eventually, successfully prepared specimens were produced, and the top view and bottom view of a sample are shown in Figure 1(c).

By using the procedure mentioned above, a total of 47 specimens were prepared. The parameters, such as the particle size, particle weight, total weight, and density, are listed in Table 1. By careful inspection of these parameters, specimens with abnormal parameter values should be given additional attention in the analysis process, because some of them might lead to testing results that deviate from normal values.


No.Particle size (mm)Particle weight (g)IDTotal weight (g)Difference (g)RatioPercentage (%)

100R1411.11416.00∗0
2R2419.22
3R3417.66

40.680M0.6-80-1464.5348.530.6110.45
5120M0.6-120-1471.1855.180.4611.71
6160M0.6-160-1515.599.500.6219.30
7200M0.6-200-1531.86115.860.5821.78
8240M0.6-240-1555.91139.910.5825.17

9180M1.0-80-1455.0239.020.498.58
10M1.0-80-2470.4254.420.6811.57
11120M1.0-120-1493.0877.080.6415.63
12M1.0-120-2490.1974.190.6215.14
13160M1.0-160-1486.3670.360.4414.47
14M1.0-160-2518.79102.790.6419.81
15200M1.0-200-1543.81127.810.6423.50

161.440M1.4-40-1441.1925.190.635.71
17M1.4-40-2426.5310.530.262.47
18M1.4-40-3448.5932.590.817.27
1980M1.4-80-1466.9450.940.6410.91
20M1.4-80-2473.4157.410.7212.13
21M1.4-80-3483.2767.270.8413.92
22120M1.4-120-1511.3895.380.7918.65
23M1.4-120-2495.4179.410.6616.03
24160M1.4-160-1524.68108.680.6820.71
25M1.4-160-2537.42121.420.7622.59

261.840M1.8-40-1447.6931.690.797.08
27M1.8-40-2449.6333.630.847.48
28M1.8-40-3442.1126.110.655.91
2980M1.8-80-1476.2360.230.7512.65
30M1.8-80-2479.2863.280.7913.20
31M1.8-80-3459.4543.450.549.46
32120M1.8-120-1498.5382.530.6916.56
33M1.8-120-2496.6680.660.6716.24
34M1.8-120-3498.1982.190.6816.50
35160M1.8-160-1526.63110.630.6921.01

362.240M2.2-40-1429.7513.750.343.20
37M2.2-40-2442.5926.590.666.01
38M2.2-40-3442.3226.320.665.95
3960M2.2-60-1453.8537.850.638.34
40M2.2-60-2451.4435.440.597.85
41M2.2-60-3471.4455.440.9211.76
4280M2.2-80-1471.2155.210.6911.72
43M2.2-80-2481.7965.790.8213.66
44M2.2-80-3468.5252.520.6611.21
45120M2.2-120-1502.0786.070.7217.14
46M2.2-120-2508.4792.470.7718.19
47160M2.2-160-1497.781.700.5116.42

Average weight of R1∼3. Difference between the actual weight of each specimen and the average weight (416 g) of the resin specimen; taking M1.4-40-1 as an example, the difference is 441.19–416 = 25.19. Ratio between the actual particle weight and theoretical particle weight; taking M1.4-40-1 as an example, the ratio is 25.19/40 = 0.63. Percentage between the formerly mentioned “Difference” and “Total weight” in the table.

The seventh column (ratio) in Table 1 is extremely important, because it determines how many particles were added; theoretically, this ratio should be 1 if the measured particles were completely added and mixed. Nonetheless, after the demoulding procedure, the tops and bottoms of all the specimens were further ground to meet the guidelines of the testing method outlined by the International Society of Rock Mechanics (ISRM) [18], and then some parts at the top and bottom of each specimen were removed, causing a decrease in the number of particles and lowering the ratio to less than 1. To quantize the quality of the prepared specimens, a ratio of 0.6 was set as the critical value, and specimens with ratios less than 0.6 were regarded as abnormal, while specimens with ratios greater than 0.6 were regarded as normal. Based on this definition, the ratios of abnormal specimens are underlined in Table 1 for the convenience of mechanism interpretation in the following tests.

2.2. Testing Method

Uniaxial compressive strength (UCS) was selected as an index to evaluate the mechanical properties of the prepared specimens. It is important to note that the primary failure of resin in a practical bolting system is caused by shearing, which is the true reaction of resin within an engineering field environment; therefore, shearing is supposed to be a main factor that needs to be discussed. Nonetheless, it has been demonstrated that the UCS has a close relationship with shearing. The traditional Mohr–Coulomb shear strength criterion considers the strength to be linearly dependent on the normal stress on the shear plane [19], and the criterion for shear strength τ is τ = σntanϕ + c, where c is the cohesion, σn is the normal stress, and ϕ is the internal friction angle. Therefore, the evaluation of mechanical properties based on UCS can reflect the true behavior of resin in engineering fields. Basically, a resin specimen with a high UCS also has a high shear strength, and the corresponding modified resin capsule can also produce better reinforcing effects.

The tests were conducted by using an MTS testing system (Model 64.106/64.106 E). For the technical details regarding this machine, readers can refer to the author’s previous study [20]. The loading rate was 1 mm/min with a data sampling rate of 10 Hz, and the failure detection threshold was 70%. Note that the loading rate was comparatively different from the suggested testing standard [21] because the mechanical behavior of resin is prone to plasticity, unlike the brittleness exhibited by most rock masses.

3. Results and Discussion

3.1. Homogeneity Detection of the Prepared Specimens

Resin has a comparatively high viscosity, which makes the manual mixture of resin difficult in some instances. As previously mentioned, the mixture of the two parts of the resin must be fast, or premature solidification can easily occur, which will lead to inhomogeneous specimens. In this test, the admixture of the steel particles will make the viscosity of resin even greater; hence, a skilled preparation of the specimen is required.

It is also vital to ensure the distribution homogeneity of the particles in the prepared specimens; otherwise, pores, cracks, weak planes, or aggregations will lead to diverse testing results. In particular, the aggregation of steel particles must be avoided. To verify the homogeneity, an industrial computed tomography (CT) scan was conducted on specimen M1.8-120-1. CT-based homogeneity verification was not conducted on every specimen mainly because of cost limitations.

The scanning paths were divided into horizontal and vertical paths, and a total of 4921 image slices were obtained. Figures 2(a)2(c) show the extraction method and corresponding images. In Figure 2(a), the distance between the neighboring horizontal scanning slices was 10 mm, and the first slice was also 10 mm from the bottom. A total of 9 horizontal slices were then extracted and shown in Figure 2(b). Similarly, the distance between the neighboring vertical scanning slices was 5 mm, and the first slice was also 5 mm to the outer margin (Figure 2(a)). A total of 9 vertical slices were extracted and are shown in Figure 2(c).

Overall, the steel particles were distributed evenly in the specimen. Additionally, conspicuous pores/cracks and weak planes were barely noticed. By further referring to the three-dimensional rendered photograph in Figure 2(d), the homogeneity was further demonstrated.

3.2. Testing Results of the Pure Resin Specimens

The strengths of the resin specimens serve as a benchmark to evaluate the mechanical properties of the specimens mixed with steel particles. Figure 3 plots the curves of the three pure resin specimens (ID : R1∼3). All curves exhibit a concave trend in the beginning, which is followed by a linear response; afterwards, a convex trend continues until reaching the peak value. This type of developing trend is extremely familiar in rock mechanics, and the aforementioned process can be divided into three stages: elastic stage, stable crack growth stage, and unstable crack growth stage [22].

The peak points for resin R1∼3 are (30.83, 26.51), (25.19, 24.41), and (26.29, 23.85). Some representative parameters are collected in Table 2. In Table 2, E50 represents the secant elastic modulus, which indicates the ratio between the stress and strain at 50% of the peak stress value. The average stress, average modulus, and E50 of the pure resin specimens are 24.92 MPa, 0.92 GPa, and 1.08 GPa, respectively.


Specimen IDMillistrain at peak stressPeak stress (MPa)Ave. stress (MPa)E (GPa)Ave. E (GPa)Strain 50Stress 50E50 (GPa)

R129.8626.4824.920.890.9211.7113.241.13
R225.1924.410.9710.8712.211.12
R326.2923.850.9111.9011.931.00

Strain50 refers to the strain value when the stress reaches 50% of the peak stress value. Stress50 refers to 50% of the peak stress.
3.3. Testing Results for the Specimens with Particles

Figure 4 lists the strain-stress relationships for specimens mixed with particles, and the labels in the figure are sourced from Table 1. By referring to the specific parameters in Table 1, if the “Ratio” values for specimens are too small, then the results of the specimens will not be considered for plotting, for example, the ratios of 0.49, 0.44, and 0.26 for M1.0-80-1, M1.0-160-1, and M1.4-40-2, respectively.

Overall, A three-stage layout is evident in each curve. In the elastic stage, most particles suffer weak influences from rotation or shearing forces, and the bonding effects with the resin material are steady and compact. In the stable growth stage, a small number of steel particles begin to rotate and align with the direction of the inner regional shearing force, while most of the other particles can resist the rotation force and remain stationary. Accordingly, the bonding effects between some particles and the resin material may begin to deteriorate, and localized stresses tend to concentrate around the particle edges. In the unstable growth stage, the particles exhibit various kinds of movement, such as rotation, resin debonding, slippage, and distortion; the bonding effects between the particles and resin tend to be isolated or weakened. The process beyond the peak stress is mainly dominated by the movement of the macroscopic shearing planes or fracture planes.

For specimens with 0.6 mm particles in Figure 4(a), they exhibit greater strengths compared to those shown in Figure 3. The peak stress of M0.6-80-1 is 41.18 MPa, which is a 55.51% increase compared with the corresponding value (26.48 MPa) of R1 in Table 2. The elastic modulus of M0.6-80-1 reaches 1.96 GPa, which is also 2.02 times the corresponding value of R2 in Table 2. This enhancement is not limited to the largest value, and the remaining specimens with particle weights ranging between 120 g and 240 g also exhibit higher strengths than the pure resin specimens. The small particles can substantially increase the mechanical ability of a resin specimen, and the most noteworthy particle modification can produce a peak stress that is 55.51% greater than that of the pure resin specimen. However, an excessively large percentage of particles in a specimen will gradually weaken the mechanical behavior.

For specimens with 1.0 mm particles in Figure 4(b), the results show that 1.0 mm particles can also bring about strengthening effects to resin specimens, and the overall strength was increased with similar values. The exact weight of particles has a limited influence on the overall mechanical behavior of the specimens, and increasing the particle addition from 80 g to 200 g barely changes the peak stress values of the specimens. Moreover, the peak stress of M1.0-120-Ave. exhibits the lowest peak value among all the specimens; thus, the detailed mechanism for this finding needs to be discussed later with the complete consideration of the results from the other specimens.

For specimens with 1.4 mm particles in Figure 4(c), the “Ave. 40-1&40-3” and the “Ave. 160” attain the largest peak stresses, and their strain-stress relationships are also extremely similar. With regard to the behaviors along the linear sections of the curves, the specimens mixed with 40 g of particles normally exhibit comparatively higher stiffness values than the other specimens. When the elastic modulus is considered, the specimens mixed with 40 g of particles have a greater elastic modulus than the specimens mixed with 120 g of particles. Based on the tests conducted herein, it is certain that the mechanical properties of resin can be improved by adding steel particles. This trend seems to have no remarkable relationship with the particle size, while the relationship with the particle weight is obvious.

For specimens with 1.8 mm particles in Figure 4(d), the strength expresses a decreasing trend as the particle weight increases. The peak stress decreases from 40.73 MPa to 26.15 MPa as the particle weight increases from 40 g to 160 g, and both the elastic modulus and E50 exhibit roughly similar trends. It seems that when the particle size surpasses 1.8 mm, the mechanical properties tend to be weakened to some extent. However, the influence of the particle weight is still prominent, as can be noticed by the decreasing trend exhibited by the mechanical properties when the particle weight increases.

For specimens with 2.2 mm particles in Figure 4(e), the mechanical responses of the specimens containing 40 g, 60 g, and 80 g or particles are approximately the same, and this finding is especially prominent for the specimens containing 40 g and 80 g of particles. Nevertheless, the peak stresses of the specimens mixed with 120 g and 160 g of particles exhibited an evident decreasing trend. The highest E50 value was exhibited by the specimens containing 40 g of particles and attains the lowest E50 value exhibited by the specimens containing 160 g of particles. By overall comparison, it is also noticeable that increasing the particle size from 1.8 mm to 2.2 mm certainly cannot increase the strengths of the specimens. Therefore, particles larger than 1.8 mm will lower the strength, and this phenomenon becomes increasingly obvious when the particle size is 2.2 mm. Additionally, the decreasing trend of strength under the effect of increasing particle weight is also prominent.

Until the analysis right here, all of the aforementioned results still lack connection to each other, and it seems that some rules that are applicable to some type of specimens are not applicable to other specimens; thus, a more comprehensive and subtle discussion is required.

3.4. Effectiveness of the Particle Weight, Size, and Failure Patterns
3.4.1. Effectiveness of the Particle Weight

Figure 5 lists the relationships between particle weight and peak stress for the specimens conditioned by constant particle size. The evaluation criterion is that the effectiveness can be tested only if the peak stress and E50 under a specific particle weight can consistently reach a comparatively higher level than the alternatives.

Overall, the following main points can be established: (1) a decrease in the peak stress is frequently observed when the particle weight reaches 120 g, while the particle size is less than 1.4 mm, which creates a U-type shape along the particle weight-peak stress curve; (2) comparatively high values of peak stress and modulus are reached when the particle weight is 40 g; (3) setting the particle weight to 160 g can also lead to favorable values as long as the particle size is less than 1.4 mm.

3.4.2. Effectiveness of the Particle Size

The relationships between particle size and peak stress under different particle weights are plotted in Figure 6. By using the same approach as that described in Section 3.4.1., the curve with the highest peak stress in each group was selected and compared.

Overall, comparatively stronger combinations can be obtained when (1) the particle size is 1.4 mm and the particle weight is 40 g, (2) the particle size is 1.0 mm and the particle weight is 80 g, or (3) the particle size is 1.4 mm and the particle weight is 160 g. If the E50 is simultaneously incorporated for comparison, then the aforementioned first and third combinations can bring about the best mechanical responses.

3.4.3. Optimum Combination of Particle Size and Weight

In Figure 7, the peak stress and secant modulus (E50) of all valid specimens are summarized. The effects of particle weight on each type of particle can be summarized based on the fitted curve of each group; the group is divided by referring to the particle size.

For the peak stress (see Figure 7(a)), the M0.6-group and M1.8-group exhibited a decreasing trend as the particle weight increased; the M1.0-group and M1.4-group exhibited a concave trend as the particle weight increased; and the M2.2-group exhibited a convex trend as the particle weight increased.

For the secant modulus (see Figure 7(b)), the M0.6-group and M1.4-group exhibited a concave trend, and the M1.0-group behaved proportionally with the particle weight. Both the M1.8-group and M.2.2-group exhibited a decreasing trend with respect to the elastic modulus, while the secant modulus M.2.2-group exhibited a convex trend.

The conclusion extracted from Figure 7 is that the particle sizes of 1.0 mm and 1.4 mm are both favorable for the mechanical responses of the specimens, and this law is especially useful for specimens mixed with 1.4 mm particles. Additionally, a particle weight of 40 g is preferable, but sometimes a particle weight of 160 g can also lead to a considerable result.

Considering the rotation resistance of the bolt during actual installation in the engineering field, the shredding effects of particles should be simultaneously considered. Particles that are 1.0 mm are relatively small compared with the annulus thickness between a bolt and borehole, so the effective shredding on the plastic film may not be practical. In addition, 160 g particles can sometimes lead to excessively large rotation resistance because the viscosity of the resin capsule without particles is already large. Therefore, the optimum combination of particle size and weight is 1.4 mm and 40 g, respectively. It worth mentioning that all ratios in Table 1 should have been equal to 1 at the very beginning, and the reason for the inconsistency was interpreted in Section 2.1. Hence, the ratio should be adjusted accordingly. For example, for the M1.4-40-3 and M1.4-160-2, the percentage between the “difference” and the “total weight” in Table 1 is 7.27% and 22.59%, respectively.

3.4.4. Failure Patterns for All Specimens

Figure 8 presents the failure patterns of all specimens, and the number range corresponding to Table 1 in the block corresponds to a specific specimen photo in the figure. The failure patterns for the pure resin specimens are mainly dominated by tensile stress with approximate vertical major cracks distributed along the specimens. The failure patterns for the specimens mixed with 0.6 mm particles are mainly tension (M0.6-120-1), shearing (M0.6-160-1, M0.6-200-1, M0.6-240-1), and combined tension and shearing (M0.6-80-1). The failure patterns for the specimens mixed with 1.0 mm and 1.4 mm particles are mainly shearing and tension, and no rupture or splitting is observed after failure or during the postpeak force process.

Interestingly, the failure patterns of most specimens exhibit detached morphologies when the particle size is greater than 1.8 mm, as seen in No. 26-30, No. 32-35, No. 37-38, No. 43, and No. 46-47. The actual influencing factor should be the excessively large particles size, which weakens the bonding ability of the resin material and leads to a decrease in the cohesion force and shearing force. Then, the specimen tends to be crushed during the UCS test, and the shearing is the foremost factor causing the splitting of the specimens.

3.5. Verification Based on the Pullout Test

Considering the optimum combination of particle size and weight (1.4 mm, 40 g) and the particles weight percentage (7.27%) hereinbefore mentioned, additional pullout tests were conducted to further verify such a combination. Pullout test is a widely acknowledged method to examine the bearing capacity of a bolting system, whereby the rock mass is replaced by steel tube. In this test, all of the parameters regarding the coal mine bolt, steel tube, and resin annulus are annotated in Figure 9(a). The packing film of the resin capsule was removed before the test to erase the influence of the gloving; thus, the mechanical improvement of the particles could be independently evaluated. The internal wall of the steel tube was lathed to form rough thread; thereby, the bonding capacity along the resin-tube interface could be strengthened to avoid potential decoupling along this interface during pullout test. Furthermore, a 50 mm long steel rod was inserted into the steel tube end and was afterwards welded, and then 50 mm long at the far end of the steel tube was reserved for clamping of the MTS machine during the pullout test; thus, the movement of the bolt would not be restrained.

The relationship between displacement and load is plotted in Figure 9(b), and the bolt tensile behavior is also attached for reference. As can be clearly seen, bolting systems bonded by particles added resin express higher peak load than pure resin bonded bolting system, though the first linear increasing stage for all specimens shows no apparent difference. For resin-particles bonded No. 2 (1), the peak load is 141 kN (133 kN) with a displacement of 19 mm (18 mm), whilst, for resin bonded No.1, the values are 110 kN and 10 mm, respectively. A short summary can be drawn here: first, the peak load can be increased by 28% as least of particles are added into the resin material; second, the resin-particles bonded bolting systems can sustain a more stable postpeak loading state than the resin bonded bolting system can do. For instance, the load at a displacement of 50 mm for the resin bonded bolting system is 31 kN, whilst the value for the resin-particles bonded bolting system at a displacement of 50 mm is 90 kN at most. Undoubtedly, the advantages of the resin-particles bonded bolting system are proved; this is in line with another test conducted by Feng et al. [23].

Figure 9(c) exhibits the failure patterns of the resin bonded specimen (upper one) and resin-particles bonded specimen (lower one). Overall, the exposed bolts are not that different from one another, and scratches along the bolt-resin interface are clear. However, some particles can be observed on the surface of the lower one (enlarged view), and the exposed bolt area is larger than that of the upper one. The inner mechanism is that the particles are forced to slide during the pullout process of bolt, and the shearing force along the bolt-resin interface is the main power that actuate the particles to rotate and to crush the resin; therefore, the attached resin deposits on the lower one are not very compact. Nonetheless, it is because of the complex interlocking effects of these particles that the peak load of the system can be guaranteed, and the high postpeak load can be sustained; both properties are beneficial to the underground rock support, and the original intention of this study is somewhat achieved.

4. Discussion

A main research target in this study was the mechanical properties improvement of resin material after the adulteration of steel particles, with which the optimized particles size and mixture ratio could be determined. However, before drawing a conclusion, the following tips should be concerned. (1) Though the starting point of this study was to remove the gloving problem of bolting system by adding steel particles, the experiments were focused on the mechanical results of standard cylindrical specimens and prepared bolting systems; the main reason was the paper length consideration. Interesting readers can refer to another work of the authors for in-depth understanding of this methodology [23]. (2) The pullout tests were conducted by using steel tube to replace the actual rock, which was not the true reflection of the mechanical properties installed in in situ environment; therefore, the established results should be referred to with caution. Nonetheless, the effectiveness of the particles added bolting system was testified based on the pullout results.

Compared with the existing studies, the improvements are emphasized from following points. (1) The mechanical characteristics of cylindrical resin specimens with steel particles adulterated were analyzed, which were not discussed in the work performed by Cao et al. and Campbell, et al. [10, 15]. (2) Pullout tests on bolts bonded by particles-adulterated resin agent were conducted, which were also different with push test conducted by Chen et al. [24]. Normally, it was believed that pullout test was more reliable than the push test [25]. (3) The optimum combination of particle size and weight was defined to realize the optimum mechanical properties of resin-bonded bolt, which were also not extensively investigated in the existing studies in related with gloving problem, though they raised hypothesis that particles could be a solution to that problem [24, 26]. Last but not least, the numerical solution for fine particles in soil regarding slope failure or for sanding analysis by fluid flow model could also be referred to for numerical analysis on particles coupling mechanism in this study [27, 28], which could be investigated in the future.

5. Conclusions

(1)All specimens mixed with particles exhibited greater peak stresses and secant modulus than those of the pure resin specimens. Comparatively higher peak stresses are attained as the particle size varies between 1.0 mm and 1.4 mm. The secant modulus decreases as the particle size increases.(2)The optimum combination of particle size and weight in this study is 1.4 mm and 40 g, respectively; under these conditions, the percentage between the weight of added particles and the total weight of the specimen is 7.27%.(3)The failure patterns of the pure resin specimens are dominated by tension, and the failure patterns of the specimens mixed with particles are mainly tension, shearing, and combined tension and shearing.(4)Under the optimum combination of particle size (1.4 mm), weight (40 g), and particles weight percentage (7.27%), bolting systems were prepared to conduct pullout test. The pullout results indicate that the resin-particles bonded bolting system can have a higher peak load and a more stable postpeak loading state than the resin bonded bolting system can achieve. Therefore, the reliability of adding steel particles into resin capsules is defended, which provides the possibility for relevant field application in the future.

Data Availability

The raw data used to support the figures in this study are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Authors’ Contributions

Xiaowei Feng proposed the idea, performed the experiment, and wrote the manuscript. Tongyang Zhao conducted the experiment and the data analyses. Fei Xue and Wenjie Jiang helped perform the analysis with constructive discussions.

Acknowledgments

The authors would like to acknowledge the financial support from the National Natural Science Foundation of China (51804296), the China Postdoctoral Science Foundation (2019M661989), and the Natural Science Foundation of Zhejiang Province (LQ20E080006).

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Copyright © 2021 Xiaowei Feng et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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