Effect of confining pressure unloading on strength reduction of soft coal in borehole ... · 2020....

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ORIGINAL ARTICLE Effect of confining pressure unloading on strength reduction of soft coal in borehole stability analysis Qingquan Liu 1,2,3 Yuanping Cheng 1 Kan Jin 1 Qingyi Tu 1 Wei Zhao 1 Rong Zhang 1 Received: 1 August 2016 / Accepted: 14 February 2017 Ó Springer-Verlag Berlin Heidelberg 2017 Abstract Underground borehole drilling usually causes instability in the surrounding coal due to in situ stress redistribution (including stress concentration and stress release). However, the mechanisms of unloading-induced coal strength reduction are still poorly understood. The primary objective of this study is to investigate the effect of confining pressure unloading on soft coal strength reduc- tion for borehole stability analysis. A series of mechanical tests were conducted on both the traditionally and newly reconstituted coal samples under two different experi- mental stress paths, including conventional uniaxial/triaxial compression and triaxial compression with confining pressure unloading. The unloading stress path was obtained by analyzing the stress redistribution around a borehole, to capture a more accurate coal mechanical response. According to our experimental results, plastic deformation generated before failure under the unloading stress path is smaller than that generated under the conventional loading stress path. Furthermore, the cohesion of the traditionally and newly reconstituted samples diminishes approximately by 44.77 and 29.66%, respectively, with confining pressure unloading, indicating that there is a significant reduction in coal strength due to confining pressure unloading. The mechanism for unloading-induced coal strength reduction comes from confining pressure unloading-induced increase in shear stress on the fracture surface and a decrease in shear strength. This effect increases the shear slipping potential, whose driving force generates tension fractures at both ends of the preexisting fractures. Keywords Soft coal Borehole stability Strength reduction Loading condition Unloading condition List of symbols P 0 Initial in situ stress (MPa) r r Tangential stress (MPa) r r p Tangential stress in the plastic zone (MPa) r r e Tangential stress in the elastic zone (MPa) r h Radial stress (MPa) r h p Radial stress in the plastic zone (MPa) r h e Radial stress in the elastic zone (MPa) r Distance from the center of a borehole (m) r a The borehole radius (m) R p The radius of the plastic zone (m) c Cohesion (MPa) u Internal friction angle (°) r Principal stress (MPa) s Shear stress (MPa) r p Peak strength (MPa) r 1 Compressive strength (MPa) r 3 Confining pressure (MPa) r 3 0 Initial confining pressure (unloading condition) (MPa) r 3 p Confining pressure measured at the peak strength (unloading condition) (MPa) e 1 p Axial strain measured at the peak strength w Fitting coefficient f Fitting coefficient & Yuanping Cheng [email protected] 1 National Engineering Research Center for Coal Gas Control, China University of Mining and Technology, Xuzhou 221116, China 2 State Key Laboratory of Coal Resources and Safe Mining, China University of Mining and Technology, Beijing 100083, China 3 School of Civil, Mining & Environmental Engineering, University of Wollongong, Wollongong, NSW 2522, Australia 123 Environ Earth Sci (2017)76:173 DOI 10.1007/s12665-017-6509-9

Transcript of Effect of confining pressure unloading on strength reduction of soft coal in borehole ... · 2020....

  • ORIGINAL ARTICLE

    Effect of confining pressure unloading on strength reductionof soft coal in borehole stability analysis

    Qingquan Liu1,2,3 • Yuanping Cheng1 • Kan Jin1 • Qingyi Tu1 • Wei Zhao1 •

    Rong Zhang1

    Received: 1 August 2016 /Accepted: 14 February 2017

    � Springer-Verlag Berlin Heidelberg 2017

    Abstract Underground borehole drilling usually causes

    instability in the surrounding coal due to in situ stress

    redistribution (including stress concentration and stress

    release). However, the mechanisms of unloading-induced

    coal strength reduction are still poorly understood. The

    primary objective of this study is to investigate the effect of

    confining pressure unloading on soft coal strength reduc-

    tion for borehole stability analysis. A series of mechanical

    tests were conducted on both the traditionally and newly

    reconstituted coal samples under two different experi-

    mental stress paths, including conventional uniaxial/triaxial

    compression and triaxial compression with confining

    pressure unloading. The unloading stress path was obtained

    by analyzing the stress redistribution around a borehole, to

    capture a more accurate coal mechanical response.

    According to our experimental results, plastic deformation

    generated before failure under the unloading stress path is

    smaller than that generated under the conventional loading

    stress path. Furthermore, the cohesion of the traditionally

    and newly reconstituted samples diminishes approximately

    by 44.77 and 29.66%, respectively, with confining pressure

    unloading, indicating that there is a significant reduction in

    coal strength due to confining pressure unloading. The

    mechanism for unloading-induced coal strength reduction

    comes from confining pressure unloading-induced increase

    in shear stress on the fracture surface and a decrease in

    shear strength. This effect increases the shear slipping

    potential, whose driving force generates tension fractures at

    both ends of the preexisting fractures.

    Keywords Soft coal � Borehole stability � Strengthreduction � Loading condition � Unloading condition

    List of symbols

    P0 Initial in situ stress (MPa)

    rr Tangential stress (MPa)rrp Tangential stress in the plastic zone (MPa)

    rre Tangential stress in the elastic zone (MPa)

    rh Radial stress (MPa)rhp Radial stress in the plastic zone (MPa)

    rhe Radial stress in the elastic zone (MPa)

    r Distance from the center of a borehole (m)

    ra The borehole radius (m)

    Rp The radius of the plastic zone (m)

    c Cohesion (MPa)

    u Internal friction angle (�)r Principal stress (MPa)s Shear stress (MPa)rp Peak strength (MPa)r1 Compressive strength (MPa)r3 Confining pressure (MPa)r30 Initial confining pressure (unloading condition) (MPa)

    r3p Confining pressure measured at the peak strength

    (unloading condition) (MPa)

    e1p Axial strain measured at the peak strength

    w Fitting coefficientf Fitting coefficient

    & Yuanping [email protected]

    1 National Engineering Research Center for Coal Gas Control,

    China University of Mining and Technology,

    Xuzhou 221116, China

    2 State Key Laboratory of Coal Resources and Safe Mining,

    China University of Mining and Technology, Beijing 100083,

    China

    3 School of Civil, Mining & Environmental Engineering,

    University of Wollongong, Wollongong, NSW 2522,

    Australia

    123

    Environ Earth Sci (2017) 76:173

    DOI 10.1007/s12665-017-6509-9

    http://crossmark.crossref.org/dialog/?doi=10.1007/s12665-017-6509-9&domain=pdfhttp://crossmark.crossref.org/dialog/?doi=10.1007/s12665-017-6509-9&domain=pdf

  • Abbreviations

    CMM Coal mine methane

    ISRM International Society for Rock Mechanics

    AE Acoustic emission

    UCS Unconfined compressive strength

    SEM Scanning electron microscope

    Introduction

    Capturing coal mine methane (CMM) by drainage bore-

    holes is not only important for improving safety in coal

    mines but also enables the beneficial recovery of a clean-

    burning fuel resource and reduction of greenhouse gas

    emissions (methane) at the same time (Karacan et al. 2011;

    Liu et al. 2014a, b). However, with increasing mining

    depth, soft coal seams are widely distributed under high

    in situ stress conditions in many Chinese coal mines,

    generating stability problems in drainage boreholes and

    further mitigating the effectiveness of CMM capture (Kang

    et al. 2010; Liu et al. 2014a, b).

    Stability of drainage borehole and other underground

    openings has drawn a lot of attention, leading to the

    development of various empirical, analytical and numerical

    methods for stability analysis and design (Meier et al.

    2015; Tao et al. 2012; Whittles et al. 2007; Zhang 2013).

    But proper estimation of in situ strength of coal is required

    to implement these approaches. In addition, coal strength

    also plays a significant role in various mining related

    engineering activities, including the evaluation of coal and

    gas outburst dangers, pillar design, hydraulic fracturing

    design (involving enhanced gas drainage), coalface sup-

    port, coal seam CO2 sequestration and other activities.

    The primary method for determining coal strength is by

    conducting a series of uniaxial/triaxial compressive tests in

    the laboratory, whose procedure has been standardized by

    the International Society for Rock Mechanics (ISRM).

    Because the ISRM suggested method provides us with a

    relatively straightforward standard to determine coal

    strength, many coal strength factors have been studied.

    Poulsen et al. (2014) reported that coal loses significant

    strength when it becomes water saturated due to its

    absorption of water. Ranjith et al. (2010) investigated the

    weakening effect of CO2 on Australian black coal by

    conducting acoustic emission and uniaxial tests, which

    have also been studied by a number of researchers (for

    example, Perera et al. 2013; Ranjith and Perera 2012; Viete

    and Ranjith 2006). Medhurst and Brown (1998) conducted

    a series of triaxial compression tests on samples with dif-

    ferent diameters to investigate scale effects on the

    mechanical behavior of coal, and based on these experi-

    mental results, Poulsen and Adhikary (2013) developed

    and calibrated a numerical Bonded Particle Model to study

    the scale effect on coal strength. Li et al. (2015)

    demonstrated that coal strength first increases and then

    decreases with increase in the loading rate during triaxial

    compression tests. Recently, due to innovations in tech-

    nologies for deep underground mining at great depths

    ([1000 m) or tunneling underneath mountains, effects ofhigh confining pressure and temperature on coal (rock)

    strength have drawn a lot of attention (Alshayea et al.

    2000; Brotóns et al. 2013; Cai and Kaiser 2014; Haimson

    and Chang 2000; Renshaw and Schulson 2007). Based on

    studies in excavation engineering, Kaiser and Kim (2015)

    reported that the strength characteristics of massive rock in

    the direct vicinity of excavation differ significantly from

    that which is remote with higher confinement. Further-

    more, Xu et al. (2011) reported that temperature generates

    a significant weakening effect on the compressive strength

    of coal.

    In addition to the above-mentioned factors on coal

    (rock) strength properties, it should be noted that stress

    path can also significantly impact coal (rock) strength.

    Underground coal or rock is under a three-dimensional

    stress equilibrium condition. However, excavation of an

    underground mine disturbs the original in situ stress state,

    leading to stress redistribution around the created under-

    ground cavity. With rock removal, the stress redistribution

    is characterized by the unloading process, under which the

    mechanical properties of rock (coal) are different from that

    of the loading process as the confining pressure is kept

    constant (Wu and Zhang 2004; Zhou et al. 2008). More-

    over, the unloading-induced stress release and its related

    deformation relaxation during excavation can drastically

    influence the stability of underground openings and might

    induce rock destruction or rock burst under the high in situ

    stress conditions (Tao et al. 2012; Zhao et al. 2014). Ding

    et al. (2016) investigated the mechanical behavior of

    sandstone under unloading conditions and found that its

    load bearing ability decreased gradually due to unloading

    of the confining pressure. Chen et al. (2016) reported that

    the volume deformation of halite under unloading condi-

    tions was greater than that under the triaxial loading con-

    ditions. To study rock burst processes, which usually occur

    on the underground excavation surface, He et al. (2010)

    conducted single-face dynamic unloading tests on lime-

    stone under true-triaxial conditions and showed that the

    acoustic emission (AE) energy release increases rapidly

    from the onset of unloading to sample failure.

    While rock strength has been widely studied, consider-

    ing the physical structural differences between rock and

    coal, insight into the unloading-induced strength reduction

    mechanism of coal is still poorly understood. Accordingly,

    an experimental study was undertaken in this paper to

    analyze and compare the strength characteristics of soft

    coal under triaxial loading and triaxial confining pressure

    unloading conditions, with the latter being called unloading

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  • condition in short in the following. The primary objective

    of this paper is to investigate the effect of confining pres-

    sure unloading on strength reduction of soft coal for

    borehole stability analysis. The principal features of this

    work include the attainment of the unloading path by

    analyzing the stress redistribution around a borehole and

    the mechanical tests on two types of reconstituted coal

    samples to capture a more accurate mechanical response in

    soft coal.

    Experimental procedures

    Coal sample preparation

    It is well known there are difficulties in cutting soft coal to

    a standard size, and the representativeness of a natural soft

    coal sample is poor due to the low cutting success rate.

    Moreover, the highly heterogeneous nature of coal some-

    times makes it difficult to interpret the results of laboratory

    experiments. Therefore, a homogeneous reconstituted coal

    sample with properties reproducible in the laboratory pro-

    vides significant advantages, especially in understanding

    the effects of various mechanical factors on the properties

    of coal (Jasinge et al. 2011b; Ranjith et al. 2012). However,

    while reconstituted coal samples have been widely used to

    investigate the mechanical and permeability properties of

    coal, there is still no standard particle size for their

    preparation. In general, reconstituted coal samples are

    made in the laboratory by compressing fine coal particles

    with some additives in a specially designed steel mold

    (Jasinge et al. 2011a). As there is no standard for coal

    particle size or additive, Xu et al. (2010) investigated the

    influence of varying the particle size on the mechanical

    properties of coal; Jasinge et al. (2009) made reconstituted

    coal samples with cement as an additive to study the

    geomechanical properties.

    In this paper, two types of reconstituted coal samples

    were prepared: a traditional sample and a reconstituted coal

    sample using a new method. The traditionally reconstituted

    sample was made in the laboratory by the following four

    steps: First, small coal blocks were crushed and sieved

    using a milling machine and a vibrating screen to select

    only coal particles of a small size (\1 mm). Second, thesieved fine coal particles were compressed using a spe-

    cially designed steel mold, with a diameter of 50 mm, and

    a mechanical servo press. The compression of coal parti-

    cles was stress-controlled with a loading rate of 300 N/s,

    and the compression was maintained for three hours when

    the load reached 100 MPa. Third, the coal sample was

    extruded from the steel mold and trimmed to an approxi-

    mate length of 100 mm using a diamond cutter. Fourth, the

    sample was polished with a grinder to a reasonable

    uniformity and smoothness in accordance with ISRM

    standards (Christiansson and Hudson 2003). Finally, the

    sample was dried in a vacuum oven at 60 �C for 24 h.The newly reconstituted samples were made from a

    mixture of naturally distributed small coal blocks and coal

    powder instead of crushed coal particles. The naturally

    distributed small coal blocks and coal powder were

    obtained from an underground coal mine using a number of

    specially designed core barrels at the same site. The

    preparation process for the newly reconstituted samples

    was the same as that for the traditionally reconstituted

    samples. The basic physical properties of both the tradi-

    tionally and newly reconstituted samples are listed in

    Table 1. As shown in Fig. 1, the internal structures of the

    two types of coal sample were examined optically using

    SEM (Scanning Electron Microscope, FEI QuantaTM 250)

    at various magnifications. It can be found there is little

    difference in sample mass between the newly and tradi-

    tionally reconstituted samples. The primary difference is in

    their source material.

    Testing facility

    As shown in Fig. 2, all the mechanical tests were con-

    ducted using a coupled ‘‘mechanical- permeability’’ sys-

    tem. The system primarily consists of two modules, i.e., the

    loading and fluid modules. The loading module is a

    hydraulic servo-controlled coal (rock) test system that can

    work independently to conduct uniaxial/triaxial compres-

    sion tests. When coupled with the fluid module, the

    Table 1 Physical parameters of coal samples

    Samples Diameter (mm) Length (mm) Mass (g)

    T1 50.6 103.0 248.42

    T2 50.8 102.6 249.13

    T3 50.8 102.4 248.85

    T4 50.8 103.6 251.03

    T5 51.0 103.5 253.32

    TX1 51.0 109.5 265.69

    TX2 51.1 109.8 268.56

    TX3 50.8 102.3 248.68

    TX4 50.8 104.5 254.04

    N1 50.5 102.8 257.25

    N2 50.2 103.1 254.83

    N3 50.5 102.0 255.11

    N4 50.8 102.2 258.46

    N5 50.5 103.5 259.02

    NX1 51.5 102.0 265.19

    NX2 50.8 103.1 261.07

    NX3 50.6 105.3 264.55

    NX4 50.8 104.1 263.61

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  • integrated system can be used to test both the coal per-

    meability and its mechanical properties when exposed to

    different gases (CH4, CO2, N2, He, etc.).

    The loading module consists of a loading frame, two oil

    hydraulic pumps (one for axial loading and another for con-

    fining pressure), a servo-system, a triaxial pressure cell, a

    Fig. 1 Photomicrographs of internal structures of traditional and newly reconstituted coal samples

    Fig. 2 Photograph andschematic diagram of the testing

    facility

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  • temperature control unit and a data measurement and

    recording unit. Based on the hardware, the loading module

    works in either a load-controlled mode or displacement-con-

    trolled mode with a seamless real-time changeover ability. In

    the load control mode, the designed maximum axial loading

    and confining pressures are 300 and 60 MPa, respectively. In

    the displacement control mode, the designed maximum dis-

    placement of the two oil hydraulic pumps is 230 mm. The

    control accuracies for the load-controlled mode and dis-

    placement-controlled mode are B±1 and B±0.5%, respec-

    tively. Using the temperature control unit, the temperature of

    the triaxial pressure cell can be controlled between ambient

    temperature and 90 �C with an accuracy B±0.2 �C. Whenconducting a mechanical test, the sample is placed inside the

    triaxial pressure cell on the base plate as shown in Fig. 3. The

    axial strain and radial deformation aremeasuredusing an axial

    strain gauge and a radial strain gauge and can be automatically

    recorded during experiments. The designed maximum

    deformation of the axial strain gauge and radial strain gauge is

    8 and 4 mm, respectively.

    Unloading path design and testing procedure

    It iswell known that accurate coalmechanical response can be

    captured only if the unloading path is accurately represented

    (Cai 2008). In this study, the unloading path was obtained by

    analyzing the stress redistribution around a borehole. A typi-

    cal stress redistribution around a borehole (when the initial

    in situ stress is P0, the hydrostatic pressure state) is shown in

    Fig. 4. Both the tangential stress (rr) and radial stress (rh)change with distance from the center of a borehole. The tan-

    gential stress is lower than the initial stress and increases with

    distance (r). The radial stress first increases from the residual

    coal strength to the maximum concentrated stress and then

    decreases with the distance (r) to the initial stress. The coal

    surrounding a borehole is characterized by elastic–plastic

    secondary stress distribution, and the thickness of the plastic

    zone is Rp - ra (Zhang et al. 2003). According to the Mohr–

    Coulomb Criterion, coal in the plastic zone fails to bear the

    maximumprinciple stress and loses its bearing strength. Thus,

    it can be concluded that with borehole drilling, the maximum

    principle stress increases prior to failure and the minimum

    principle stress decreases.

    The uniaxial test was performed on two samples (one

    traditional sample and one new sample); the triaxial tests

    (with confining pressures 2, 4, 6 and 8 MPa) were per-

    formed on eight samples (four traditional samples and four

    new samples). Conventional uniaxial and triaxial com-

    pression tests were conducted to obtain peak strengths,

    which was used to determine the unloading point. The

    Fig. 3 Photograph of a samplewith the sensors

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  • corresponding loading procedure was divided into two

    stages. In the first stage, the hydrostatic strength (confining

    pressure) was loaded at a rate of 10 N/s to some prede-

    termined values (i.e., 2, 4, 6 and 8 MPa; in the confining

    pressure-controlled mode). In the second stage, the axial

    strength was loaded at a rate of 50 N/s until failure

    occurred (in the axial load-controlled mode), while keeping

    the confining pressure constant.

    As shown in Fig. 5, the unloading path was designed

    based on stress redistribution characteristics, with the

    corresponding loading procedure divided into three stages.

    In the first stage, the hydrostatic strength was loaded at a

    rate of 10 N/s to predesigned values 2, 4, 6 and 8 MPa, in

    the confining pressure-controlled mode. In the second

    stage, the axial strength was loaded at a rate of 50 N/s until

    it reached the predesigned unloading point (80% of the

    corresponding peak strength), while keeping the confining

    pressure constant. In the third stage, the confining pressure

    was gradually unloaded at a rate of 10 N/s, and the axial

    strength was loaded at a rate of 50 N/s simultaneously until

    failure occurred. All conventional compression and

    unloading tests were conducted at 30 �C to avoid theinfluence of potential temperature fluctuations.

    Results and discussion

    The internal structures of the two types of samples are

    shown in the SEM images obtained by scanning the

    surfaces of the two types of coal samples (Fig. 1). There

    are numerous fractures present at different scales (ranging

    from 469 to 8009 magnification) found in the new type

    coal sample. In contrast, few microfractures were

    observed in the traditional coal sample (6009 and 12009

    magnifications). Based on the microscopic observations of

    internal structures, we conclude that the new type of

    reconstituted sample partially retained the structural

    characteristics of soft coal and is more representative of

    the natural ore body.

    Deviatoric stress–strain relationship under

    multi-triaxial loading conditions

    Ten conventional uniaxial and triaxial compression tests

    were conducted to determine the peak strengths of the two

    types of reconstituted coal samples. Of the ten tests, five

    were carried out on the traditionally reconstituted samples,

    and the other five on the newly reconstituted samples.

    Figure 6 shows the deviatoric stress–strain diagrams for the

    two types of reconstituted samples, tested under different

    confining pressures. As observed from the figures, the two

    types of samples have some similarities, such as their peak

    strength increasing with increasing confining pressure,

    unconfined compressive strengths (UCS) being far lower

    than the triaxial compression strength and undergoing

    through a significant plastic deformation before reaching

    the corresponding peak strengths. We therefore conclude

    that confining pressure helps to close the preexisting coal

    fractures, thereby inhibiting the generation of new fractures

    and the extension of initial ones. Moreover, confining

    pressure is also helpful in enhancing internal friction

    between mineral components, thus improving the bearing

    capacity of coal.

    Fig. 4 Illustration of elastic–plastic stress redistribution around aborehole (Liu et al. 2014a, b) (where s represents shear strength, rrepresents principal stress, rh

    p and rrp represent radial stress and

    tangential stress in the plastic zone, rhp and rr

    p represent radial stress

    and tangential stress in the elastic zone, ra is the borehole radius, Rp is

    the radius of the plastic zone)

    Fig. 5 Illustration of the confining pressure unloading stress path(where rp represents the peak strength, r3 represents the confiningpressure, r1 represents the compressive strength)

    173 Page 6 of 11 Environ Earth Sci (2017) 76:173

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  • However, there are still some differences between the

    two types of coal samples. The peak strength (rp), the axialstrain measured at the peak strength (e1

    p) and the corre-

    sponding confining pressure (r3) are summarized inTable 2. As indicated in Table 2, at the same confining

    pressure, the peak strength of the traditional sample is

    greater than that of the new sample and the axial strain (e1p)

    of the traditional sample is smaller than that of the new

    sample (except at a 8 MPa confining pressure).

    Preexisting fractures can strongly influence the

    mechanical properties of coal (Ding et al. 2016). The pri-

    mary reason for the observed differences is that the new

    samples can manage to maintain their preexisting soft coal

    fractures, while the preparation of traditional samples

    damaged the natural coal fractures (due to the crushing of

    the coal blocks). Thus, at the same confining pressure, the

    traditional sample can bear greater axial load than the new

    sample. With a lower bearing capacity, the new sample will

    generate plastic deformation even at a relatively low axial

    load.

    Based on the obtained peak strengths for the two

    types of samples, eight unloading tests were conducted

    with different initial confining pressures. Of the eight

    tests, four were carried on the traditionally reconstituted

    samples and the other four on the newly reconstituted

    samples. Figure 7 shows the deviatoric stress–strain

    diagrams for the two types of reconstituted samples,

    tested under different initial confining pressures. As

    observed in the figure, the peak strengths of the two

    types of samples also increase with increasing initial

    confining pressure; the peak strength of the traditional

    sample is also greater than that of the new sample under

    the same initial confining pressure. However, it is clear

    that the deviatoric stress–strain curves of the two types

    of samples obtained under the unloading stress path are

    quite different from those obtained under the conven-

    tional loading stress path. The initial confining pressure

    (r30), the peak strength (rp) and the corresponding con-

    fining pressure measured at the peak strength (r3p) are

    summarized in Table 3.

    As listed in Table 3, the peak strengths of the two types

    of samples are lower than that obtained under the con-

    ventional loading stress path. One reason for this result is

    that in the unloading path, the confining pressure measured

    at peak strength is lower than the corresponding initial

    confining pressure. In contrast, the plastic deformation

    generated at peak strength under unloading stress path is

    smaller than that generated under the conventional loading

    stress path, indicating that coal generates shear damage

    more easily under an unloading stress path.

    Fig. 6 Deviatoric stress versus strain for the coal samples obtained under conventional compression condition

    Table 2 Conventional uniaxial and triaxial compression testingresults

    Samples r3 (MPa) rp (MPa) e1p (91E-3)

    T1 0 1.66 16.3

    T2 2 13.72 30.8

    T3 4 21.90 38.8

    T4 6 28.57 50.7

    T5 8 36.14 97.2

    N1 0 0.95 24.0

    N2 2 11.64 35.9

    N3 4 19.56 53.2

    N4 6 27.17 64.6

    N5 8 33.76 79.6

    Environ Earth Sci (2017) 76:173 Page 7 of 11 173

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  • The strength reduction effect of confining pressure

    unloading

    It is difficult to produce tensile stress under the high

    compressive stress present in the earth; therefore, during

    deep drilling and geological faulting, shear failure pre-

    dominates (Maurer 1965). The Mohr–Coulomb strength

    criterion is one of the most widely used strength criterions

    in geomechanical engineering, which describes a linear

    relationship between normal stress and shear stress at

    failure. According to the Mohr–Coulomb criterion, the

    shear strength of coal (rock) is made up of two parts, a

    constant cohesion and a normal stress-dependent frictional

    component (internal friction angle) (Zhao 2000). In gen-

    eral, cohesion and the internal friction angle are indirect

    measurement parameters but can also be calculated using

    the statistics of uniaxial and triaxial compression test

    results. For an accurate regression analysis of the com-

    pression results, the Mohr–Coulomb criterion is translated

    into the following principal stress form (Li et al. 2007):

    r1 ¼ wþ fr3 ð1Þ

    where

    w ¼ 2c cosu1� sinu ð2Þ

    and

    f ¼ tan2 45� þ u2

    � �ð3Þ

    where w and f are fitting coefficients, c is cohesion, and uis internal friction angle.

    In particular, coal failure under uniaxial compression is

    due to shear dilatancy, rather than shear failure (Liu et al.

    2014a, b; Su et al. 2006). The uniaxial compression

    strength is far lower than the triaxial compression strength

    (as shown in Fig. 8) and will introduce some non-negligi-

    ble errors when calculating the shear strength parameters if

    incorporated. Thus, in this research, uniaxial compression

    strength was not incorporated in the regressive calculations

    of shear strength parameters.

    Fig. 7 Deviatoric stress versus strain for the coal samples obtained under confining pressure unloading condition

    Table 3 Triaxial confining pressure unloading testing results

    Samples r30 (MPa) r3

    p (MPa) rp (MPa)

    TX1 2 1.69 10.58

    TX2 4 3.02 17.04

    TX3 6 4.40 22.92

    TX4 8 5.75 27.56

    NX1 2 1.61 9.54

    NX2 4 3.66 15.01

    NX3 6 4.74 21.62

    NX4 8 6.31 26.13

    Fig. 8 Mohr–Coulomb circles of traditionally reconstituted coalsamples obtained under conventional compression condition

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  • As shown in Fig. 9, compressive strength increases with

    confining pressure, i.e., there is a clear enhancing effect of

    confining pressure on strength. The results also suggest that

    the strength criteria closely confirm the Mohr–Coulomb

    criterion, as linear r1–r3 curves are clearly observed.Natural coal (rock) is a heterogeneous material, and the

    strength test plots are usually scattered. This characteristic

    is significantly influenced by internal structures, which also

    depend on the confining pressure (You 2014). As the new

    coal sample partially maintains the structural characteris-

    tics of soft coal and the influence of confining pressure

    unloading, the compressive strengths test plots are a little

    scattered. The four linear r1–r3 curves represent fourexperimental conditions and are obtained by the linear

    least-squares regression method. The R-square of three

    linear regression results is higher than 0.99 and about 0.964

    for the new samples under the unloading condition, indi-

    cating that the standard errors in the four linear curves are

    low and the fitting results are reliable. By using Eqs. (1)–

    (3) and based on the linear regression results, cohesion and

    internal friction angle of the coal samples tested under two

    stress paths are calculated and listed in Table 4.

    As indicated in Table 4, for the conventional compres-

    sion stress path, the cohesions of traditionally and newly

    reconstituted samples are 1.72 and 1.18 MPa, respectively;

    for the triaxial unloading stress path, the cohesions of

    traditional and newly reconstituted samples are 0.95 and

    0.83 MPa, respectively. The cohesion of traditionally

    reconstituted samples is higher than that of the newly

    reconstituted samples under both loading and unloading

    stress paths. As cohesion represents the intermolecular

    force of coal, the comparison of cohesion between the two

    types of coal samples indicates that the preparation of

    traditional samples damaged the coal matrix (due to the

    crushing of the coal blocks), while the new type of samples

    maintained some of their internal structures.

    Furthermore, for both of the traditionally reconstituted

    sample and newly reconstituted sample, the cohesion

    obtained under the conventional compression stress path is

    higher than that obtained under the triaxial unloading stress

    path. Comparing the conventional compression stress path

    and triaxial unloading stress path, the cohesion of the tra-

    ditionally reconstituted sample and newly reconstituted

    sample reduced by 44.77 and 29.66%, respectively, with

    confining pressure unloading. These results show that there

    is a significant reduction effect of confining pressure

    unloading on coal strength.

    It is well known that during conventional compression, the

    process of shear failure consists initially of fracture closure

    followed by elastic deformation, then fracture initiation

    Fig. 9 Relationships between r1 and r3 obtained under multi-triaxial loading conditions

    Table 4 Computation results ofstrength parameters of the two

    types coal samples

    Samples Stress paths w (MPa) f c (MPa) u (�) R2

    Traditional samples Conventional compression 6.60 3.70 1.72 35.06 0.998

    Triaxial confining pressure unloading 3.91 4.21 0.95 38.03 0.992

    New samples Conventional compression 4.54 3.70 1.18 35.06 0.997

    Triaxial confining pressure unloading 3.18 3.65 0.83 34.74 0.964

    Environ Earth Sci (2017) 76:173 Page 9 of 11 173

    123

  • followed by fracture damage. This phenomenon is known as

    stable fracture growth; if the compressive load is removed

    generation of fracture growth will stop. Finally, unstable frac-

    ture growth occurs resulting in sample failure. However, con-

    fining pressure unloading leads to an increase in shear stress on

    the fracture surface and decrease in shear strength, thus

    increasing the potential of shear slipping whose driving force

    would generate tension fractures at both ends of the original

    fracture (Huang andHuang 2014). Thus, stable fracture growth

    transforms relatively quickly into unstable fracture growth,

    degrading the bearing capacity (cohesion) of coal.

    Conclusions

    Due to the poor representation of natural soft coal samples

    from the low cutting success rate, a new method has been

    developed to make reconstituted coal samples. This method

    partially maintains the structural characteristics of soft

    coal. By using both the traditionally and newly reconsti-

    tuted coal samples, a series of mechanical tests were con-

    ducted to investigate the effect of confining pressure

    unloading on strength reduction of soft coal in borehole

    stability. Based on the comparison and analysis of strength

    characteristics between conventional uniaxial/triaxial

    compression tests and triaxial unloading tests, some fun-

    damental conclusions can be drawn:

    1. To more accurately capture coal mechanical responses

    in borehole stability analysis, the unloading path was

    obtained by analyzing the stress redistribution around a

    borehole, which can be divided into three stages. The

    third stage was unique as the confining pressure was

    gradually unloaded at a rate of 10 N/s while loading

    the axial strength at a rate of 50 N/s until failure

    occurred.

    2. Because preexisting fractures can strongly influence

    the bearing capacity of coal, and the new samples

    maintain the preexisting fractures of soft coal, in

    conventional uniaxial/triaxial compression tests (at the

    same confining pressure), the traditional sample can

    bear a greater axial load than the new sample which

    generate plastic deformation even at a relatively low

    axial load.

    3. Before failure occurs, the plastic deformation gener-

    ated under the unloading stress path is smaller than that

    obtained under the conventional loading stress path,

    indicating that coal generates shear damage more

    easily under the unloading stress path.

    4. The cohesion (primary parameter) and internal friction

    angle are used to quantitatively evaluate the shear

    strength of coal. Comparing the conventional com-

    pression stress path and triaxial unloading stress path,

    the cohesions of the traditionally reconstituted sample

    and newly reconstituted sample degrade approximately

    by 44.77 and 29.66%, respectively, with confining

    pressure unloading. These results show that confining

    pressure unloading produces a significant reduction in

    coal strength, primarily because the confining pressure

    unloading leads to an increase in the shear stress on the

    fracture surface and decrease in shear strength. This

    effect increases the potential of shear slipping whose

    driving force could generate tension fractures at both

    ends of the preexisting fractures.

    Acknowledgements The authors are grateful to the financial supportfrom projects funded by Natural Science Foundation of Jiangsu

    Province (No. BK20160253), China Postdoctoral Science Foundation

    (No. 2016M590519), the State Key Laboratory of Coal Resources and

    Safe Mining (No. SKLCRSM16KFB01) and the Priority Academic

    Program Development of Jiangsu Higher Education Institutions and

    the Fundamental Research Funds for the Central Universities (No.

    2013QNA03).

    References

    Alshayea NA, Khan K, Abduljauwad SN (2000) Effects of confining

    pressure and temperature onmixed-mode (I–II) fracture toughness

    of a limestone rock. Int J Rock Mech Min Sci 37(4):629–643

    Brotóns V, Tomás R, Ivorra S, Alarcón J (2013) Temperature

    influence on the physical and mechanical properties of a porous

    rock: San Julian’s calcarenite. Eng Geol 167:117–127

    Cai M (2008) Influence of intermediate principal stress on rock

    fracturing and strength near excavation boundaries—insight

    from numerical modeling. Int J Rock Mech Min Sci

    45(5):763–772

    Cai M, Kaiser PK (2014) In-situ rock spalling strength near

    excavation boundaries. Rock Mech Rock Eng 47(2):659–675

    Chen J, Jiang D, Ren S, Yang C (2016) Comparison of the

    characteristics of rock salt exposed to loading and unloading

    of confining pressures. Acta Geotech 11(1):221–230

    Christiansson R, Hudson J (2003) ISRM Suggested Methods for rock

    stress estimation—Part 4: quality control of rock stress estima-

    tion. Int J Rock Mech Min Sci 40(7):1021–1025

    Ding QL, Ju F, Mao XB, Ma D, Yu BY, Song SB (2016)

    Experimental investigation of the mechanical behavior in

    unloading conditions of sandstone after high-temperature treat-

    ment. Rock Mech Rock Eng 49(7):2641–2653

    Haimson B, Chang C (2000) A new true triaxial cell for testing

    mechanical properties of rock, and its use to determine rock

    strength and deformability of Westerly granite. Int J Rock Mech

    Min Sci 37(1):285–296

    He MC, Miao JL, Feng JL (2010) Rock burst process of limestone and

    its acoustic emission characteristics under true-triaxial unloading

    conditions. Int J Rock Mech Min Sci 47:286–298

    Huang RQ, Huang D (2014) Evolution of rock cracks under

    unloading condition. Rock Mech Rock Eng 47(2):453–466

    Jasinge D, Ranjith PG, Choi SK, Kodikara J, Arthur M, Li H (2009)

    Mechanical properties of reconstituted Australian black coal.

    J Geotech Geoenviron Eng 135(7):980–985

    Jasinge D, Ranjith PG, Choi SK (2011a) Effects of effective stress

    changes on permeability of latrobe valley brown coal. Fuel

    90(3):1292–1300

    173 Page 10 of 11 Environ Earth Sci (2017) 76:173

    123

  • Jasinge D, Ranjith PG, Choi SK (2011b) Effects of effective stress

    changes on permeability of latrobe valley brown coal. Fuel

    90(3):1292–1300

    Kaiser PK, Kim BH (2015) Characterization of strength of intact

    brittle rock considering confinement-dependent failure pro-

    cesses. Rock Mech Rock Eng 48(1):107–119

    Kang HP, Zhang X, Si LP, Wu Y, Gao F (2010) In-situ stress

    measurements and stress distribution characteristics in under-

    ground coal mines in China. Eng Geol 116:333–345

    Karacan CÖ, Ruiz FA, Cotè M, Phipps S (2011) Coal mine methane:

    a review of capture and utilization practices with benefits to

    mining safety and to greenhouse gas reduction. Int J Coal Geol

    86(2):121–156

    Li HZ, Xia CC, Yan ZJ, Jiang K, Yang LD (2007) Study on marble

    unloading mechanical properties of Jinping hydropower station

    under high geostress conditions. Chin J Rock Mech Eng

    26(10):2104–2109

    Li HT, Jiang CX, Jiang YD, Wang HW, Liu HB (2015) Mechanical

    behavior and mechanism analysis of coal samples based on

    loading rate effect. J China Univ Min Technol 44(3):430–436

    Liu QQ, Cheng YP, Yuan L, Tong B, Kong SL, Zhang R (2014a)

    CMM capture engineering challenges and characteristics of

    in situ stress distribution in deep level of Huainan coalfield. J Nat

    Gas Sci Eng 20:328–336

    Liu QS, Liu KD, Zhu JB (2014b) Study of mechanical properties of

    raw coal under high stress with triaxial compression. Chin J

    Rock Mech Eng 33(1):24–34

    Maurer WC (1965) Shear failure of rock under compression. Soc

    Petrol Eng J 5(2):167–176

    Medhurst TP, Brown ET (1998) A study of the mechanical behaviour

    of coal for pillar design. Int J Rock Mech Min Sci

    35(8):1087–1105

    Meier T, Rybacki E, Backers T, Dresen G (2015) Influence of

    bedding angle on borehole stability: a laboratory investigation of

    transverse isotropic oil shale. Rock Mech Rock Eng

    48(4):1535–1546

    Perera MSA, Ranjith PG, Viete DR (2013) Effects of gaseous and

    super-critical carbon dioxide saturation on the mechanical

    properties of bituminous coal from the Southern Sydney Basin.

    Appl Energy 110:73–81

    Poulsen BA, Adhikary DPA (2013) A numerical study of the scale

    effect in coal strength. Int J Rock Mech Min Sci 63:62–71

    Poulsen BA, Shen B, Williams DJ, Huddlestone-Holmes C, Erarslan

    N, Qin J (2014) Strength reduction on saturation of coal and coal

    measures rocks with implications for coal pillar strength. Int J

    Rock Mech Min Sci 71:41–52

    Ranjith PG, Perera MSA (2012) Effects of cleat performance on

    strength reduction of coal in CO2 sequestration. Energy

    45(1):1069–1075

    Ranjith PG, Jasinge D, Choi SK, Mehic M, Shannon B (2010) The

    effect of CO2 saturation on mechanical properties of Australian

    black coal using acoustic emission. Fuel 89(8):2110–2117

    Ranjith PG, Shao SS, Viete DR, Jaysinge D (2012) Carbon dioxide

    storage in coal: reconstituted coal as a structurally homogeneous

    substitute for coal. Int J Coal Prep Util 32:265–275

    Renshaw CE, Schulson EM (2007) Limits on rock strength under high

    confinement. Earth Planet Sci Lett 258(1):307–314

    Su CD, Zhai XX, Li YM, Li SM, Liu ZY (2006) Study on

    deformation and strength of coal samples in triaxial compres-

    sion. Chin J Rock Mech Eng 25(S1):2963–2968

    Tao M, Li XB, Wu CQ (2012) Characteristics of the unloading

    process of rocks under high initial stress. Comput Geotech

    45:83–92

    Viete DR, Ranjith PG (2006) The effect of CO2 on the geomechanical

    and permeability behaviour of brown coal: implications for coal

    seam CO2 sequestration. Int J Coal Geol 66(3):204–216

    Whittles DN, Lowndes IS, Kingman SW, Yates C, Jobling S (2007)

    The stability of methane capture boreholes around a long wall

    coal panel. Int J Coal Geol 71(2):313–328

    Wu G, Zhang L (2004) Studying unloading failure characteristics of a

    rock mass using the disturbed state concept. Int J Rock Mech

    Min Sci 41(S1):419–425

    Xu J, Liu D, Peng SJ, Wu X, Lu Q (2010) Experimental research on

    influence of particle diameter on coal and gas outburst. Chin J

    Rock Mech Eng 29(6):1231–1237

    Xu J, Zhang D, Peng SJ (2011) Experimental research on influence of

    temperature on mechanical properties of coal containing

    methane. Chin J Rock Mech Eng 30(S1):2730–2735

    You MQ (2014) Effect of confining pressure on strength scattering of

    rock specimen. Chin J Rock Mech Eng 33(5):929–937

    Zhang JC (2013) Borehole stability analysis accounting for

    anisotropies in drilling to weak bedding planes. Int J Rock

    Mech Min Sci 60:160–170

    Zhang JC, Bai M, Roegiers JC (2003) Dual-porosity poroelastic

    analyses of wellbore stability. Int J Rock Mech Min Sci

    40(4):473–483

    Zhao J (2000) Applicability of Mohr–Coulomb and Hoek–Brown

    strength criteria to the dynamic strength of brittle rock. Int J

    Rock Mech Min Sci 37(7):1115–1121

    Zhao XG, Wang J, Cai M, Cheng C, Ma LK, Su R, Zhao F, Li DJ

    (2014) Influence of unloading rate on the strainburst character-

    istics of Beishan granite under true-triaxial unloading conditions.

    Rock Mech Rock Eng 47(2):467–483

    Zhou XP, Zhang YX, Ha QL (2008) Real-time computerized

    tomography (CT) experiments on limestone damage evolution

    during unloading. Theor Appl Fract Mech 50(1):49–56

    Environ Earth Sci (2017) 76:173 Page 11 of 11 173

    123

    Effect of confining pressure unloading on strength reduction of soft coal in borehole stability analysisAbstractIntroductionExperimental proceduresCoal sample preparationTesting facilityUnloading path design and testing procedure

    Results and discussionDeviatoric stress--strain relationship under multi-triaxial loading conditionsThe strength reduction effect of confining pressure unloading

    ConclusionsAcknowledgementsReferences