CN111460666B - Rock burst risk prediction method for typical rock burst mine - Google Patents
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Abstract
Description
技术领域Technical Field
本发明属于煤炭开采技术领域,尤其涉及一种典型冲击地压矿井的冲击地压危险性预测方法。The invention belongs to the technical field of coal mining, and in particular relates to a method for predicting rock burst hazard of a typical rock burst mine.
背景技术Background Art
冲击地压是一种严重的、破坏性强的矿井动力灾害,给煤矿生产安全和人员生命安全构成极大威胁。具有冲击地压煤层的矿井为冲击地压矿井,如矿井在达到一定开采深度后开始发生冲击地压,此深度称为本冲击地压矿井的临界深度,如开采深度达到此深度时继续开采将会有冲击地压发生的危险。临界深度值随地质条件不同而异,总体趋势为冲击地压危险性随开采深度增加而增大。对于不同的冲击地压矿井,定量判断冲击地压发生的临界深度对于冲击地压的危险性预测尤为重要,可以进行有效的防控。但是目前对深矿井的概念和临界深度问题没有取得共识,这给探讨矿山深部开采遇到的地质灾害等问题带来了不便,目前以深度区间的研究结果居多,对于典型冲击地压矿井的临界深度鲜有定量研究,因此,对于典型冲击地压矿井的冲击地压危险性预测缺少定量判断。Rock burst is a serious and destructive mine dynamic disaster, which poses a great threat to coal mine production safety and personnel life safety. A mine with rock burst coal seams is a rock burst mine. If the mine begins to experience rock burst after reaching a certain mining depth, this depth is called the critical depth of the rock burst mine. If the mining depth reaches this depth, there will be a risk of rock burst if mining continues. The critical depth value varies with different geological conditions. The overall trend is that the risk of rock burst increases with the increase of mining depth. For different rock burst mines, quantitative judgment of the critical depth of rock burst is particularly important for predicting the risk of rock burst, which can be effectively prevented and controlled. However, there is no consensus on the concept of deep mines and the critical depth issue, which brings inconvenience to the discussion of geological disasters encountered in deep mining. At present, most of the research results are based on depth intervals, and there is little quantitative research on the critical depth of typical rock burst mines. Therefore, there is a lack of quantitative judgment for the prediction of rock burst risk in typical rock burst mines.
发明内容Summary of the invention
针对现有技术存在的不足,本发明提供一种典型冲击地压矿井的冲击地压危险性预测方法,从而定量判断冲击地压发生的临界深度,准确预测典型冲击地压矿井的冲击地压危险性。In view of the deficiencies in the prior art, the present invention provides a method for predicting the rock burst hazard of a typical rock burst mine, thereby quantitatively determining the critical depth of rock burst occurrence and accurately predicting the rock burst hazard of a typical rock burst mine.
本发明的技术方案:The technical solution of the present invention:
一种典型冲击地压矿井的冲击地压危险性预测方法,包括如下步骤:A method for predicting rock burst hazard of a typical rock burst mine comprises the following steps:
步骤一:收集目标矿井数据,测试物理力学参数,并建立煤岩动力系统模型,通过构建矿井的地质动力环境体系判定典型冲击地压矿井;Step 1: Collect target mine data, test physical and mechanical parameters, and establish a coal-rock dynamic system model to determine typical rock burst mines by building a geological dynamic environment system for the mine;
步骤二:确定煤岩动力系统的能量特征;Step 2: Determine the energy characteristics of the coal-rock power system;
步骤三:计算煤岩动力系统总能量及基础能量;Step 3: Calculate the total energy and basic energy of the coal-rock power system;
步骤四:计算煤岩动力系统释放能量,结合步骤三所求结果推导计算典型冲击地压矿井的临界深度;Step 4: Calculate the energy released by the coal-rock power system, and derive the critical depth of a typical rock burst mine based on the results obtained in
步骤五:通过临界深度预测典型冲击地压矿井的冲击地压危险性。Step 5: Predict the rock burst hazard of typical rock burst mines by critical depth.
所述步骤一中构建矿井的地质动力环境体系判定典型冲击地压矿井的方法,具体包括以下步骤:The method for constructing a mine geological dynamic environment system to determine a typical rock burst mine in
(1)构建由目标矿井的构造凹地地貌条件、断块构造垂直运动条件、断块构造水平运动条件、断裂构造影响范围、构造应力、煤层开采深度、上覆坚硬岩层条件、本区及邻区冲击地压判据条件八个因素构成的地质动力环境评价体系;(1) Construct a geodynamic environment evaluation system consisting of eight factors: the geomorphological conditions of the target mine's structural depression, the vertical movement conditions of the fault block structure, the horizontal movement conditions of the fault block structure, the influence range of the fault structure, the tectonic stress, the coal seam mining depth, the overlying hard rock conditions, and the rock burst judgment criteria of the area and the adjacent areas;
(2)将地质动力环境评价指标体系中各项评价指标值ai划分为四个等级,根据每项评价指标对矿井地质动力环境的影响程度逐一评判,对矿井地质动力环境无影响的评价指标ai的评价指数为0、影响程度弱时ai的评价指数为1、中等影响时ai的评价指数为2、有强烈影响时ai的评价指数为3;具体为:(2) The evaluation index values ai in the geological dynamic environment evaluation index system are divided into four levels, and each evaluation index is judged one by one according to the degree of influence of each evaluation index on the mine geological dynamic environment. The evaluation index ai with no influence on the mine geological dynamic environment is 0, the evaluation index ai with weak influence is 1, the evaluation index ai with medium influence is 2, and the evaluation index ai with strong influence is 3; specifically:
①井田构造凹地地貌特征:① Geomorphic characteristics of the well field structural depression:
其中,C—构造凹地的反差强度;Where, C—contrast intensity of structural depression;
△h—构造凹地最高与最低高程的差值,km;△h—the difference between the highest and lowest elevations of the structural depression, km;
△l—构造凹地的宽度,km;△l—width of structural depression, km;
A、B—权重系数;山地地貌:A=0.25,B=0.75,丘陵地貌:A=0.5,B=0.5,平原地貌:A=0.75,B=0.25;A, B—weight coefficients; mountainous landform: A=0.25, B=0.75, hilly landform: A=0.5, B=0.5, plain landform: A=0.75, B=0.25;
当C≥0.75时,评价指数a1为3;当0.5≤C0.75时,评价指数a1为2;当0.25≤C<0.5时,评价指数a1为1;当C<0.25时,评价指数a1为0;When C≥0.75, the evaluation index a1 is 3; when 0.5≤C0.75, the evaluation index a1 is 2; when 0.25≤C<0.5, the evaluation index a1 is 1 ; when C<0.25, the evaluation index a1 is 0;
②断块构造垂直运动条件:②Conditions for vertical movement of fault-block structures:
目标矿井的断块垂直运动速度为V1,当垂直运动速率V1≥8mm/yr时,评价指数a2为3;当垂直运动速率V1>5mm/yr时,评价指数a2为2;当垂直运动速率V1<-3mm/yr时,评价指数a2为1;当垂直运动速率-3mm/yr≤V1≤5mm/yr时,评价指数a2为0;The vertical movement speed of the fault block in the target mine is V 1 . When the vertical movement speed V 1 ≥8mm/yr, the evaluation index a 2 is 3; when the vertical movement speed V 1 >5mm/yr, the evaluation index a 2 is 2; when the vertical movement speed V 1 <-3mm/yr, the evaluation index a 2 is 1; when the vertical movement speed -3mm/yr≤V 1 ≤5mm/yr, the evaluation index a 2 is 0;
③断块构造水平运动条件:③Conditions for horizontal movement of fault block structures:
目标矿井的断块垂直运动速度为V2,当水平运动速率V2>10mm/yr时,评价指数a3为3;当垂直运动速率5mm/yr≤V2≤10mm/yr时,评价指数a3为2;当垂直运动速率2mm/yr≤V2<5mm/yr时,评价指数a3为1;当垂直运动速率V2<2mm/yr时,评价指数a3为0;The vertical movement speed of the fault block in the target mine is V 2 . When the horizontal movement speed V 2 >10 mm/yr, the evaluation index a 3 is 3; when the vertical movement speed is 5 mm/yr≤V 2 ≤10 mm/yr, the evaluation index a 3 is 2; when the vertical movement speed is 2 mm/yr≤V 2 <5 mm/yr, the evaluation index a 3 is 1; when the vertical movement speed V 2 <2 mm/yr, the evaluation index a 3 is 0;
④断裂构造影响范围条件④Conditions of the influence range of fault structure
b=±(K·10h)b=±(K·10h)
式中:b—断裂构造影响范围宽度,km,当断裂影响范围边界在井田边界外时,b取正值,当断裂影响范围边界跨入井田边界内部时,b取负值;Where: b is the width of the influence range of the fault structure, km. When the boundary of the influence range of the fault is outside the boundary of the well field, b takes a positive value; when the boundary of the influence range of the fault crosses into the boundary of the well field, b takes a negative value.
K—活动性系数(K=1,2,3),断裂活动性强时K=3、断裂活动性中等时K=2、断裂活动性弱时K=1;K—activity coefficient (K=1, 2, 3), when the fault activity is strong, K=3, when the fault activity is medium, K=2, when the fault activity is weak, K=1;
h—断裂垂直落差,m;h—vertical height of the fracture, m;
当b≤0.5时,评价指数a4为3,当0.5<b≤2时,评价指数a4为2,当2<b≤5时,评价指数a4为1,当b>5时,评价指数a4为0;When b≤0.5, the evaluation index a4 is 3, when 0.5<b≤2, the evaluation index a4 is 2, when 2<b≤5, the evaluation index a4 is 1, and when b>5, the evaluation index a4 is 0;
⑤构造应力条件⑤ Tectonic stress conditions
构造应力对冲击地压危险性评价指标用应力集中系数K表示,当K>2时,评价指数a5为3,当1.2<K≤2时,评价指数a5为2,当0.8<K≤1.2时,评价指数a5为1,当K≤0.8时,评价指数a5为0;The evaluation index of tectonic stress on rock burst danger is expressed by stress concentration coefficient K. When K>2, the evaluation index a5 is 3; when 1.2<K≤2, the evaluation index a5 is 2; when 0.8<K≤1.2, the evaluation index a5 is 1; when K≤0.8, the evaluation index a5 is 0;
⑥开采深度条件⑥ Mining depth conditions
当开采深度h>800m时,评价指数a6为3,当600m<h≤800m时,评价指数a6为2,当400m<h≤600m时,评价指数a6为1,当开采深度h≤400m时,评价指数a6为0;When the mining depth h>800m, the
⑦上覆坚硬岩层条件⑦ Overlying hard rock conditions
覆坚硬厚岩层距煤层距离为d,当覆坚硬厚岩层距煤层距离d≤20m,评价指数a7为3;当覆坚硬厚岩层距煤层距离20m<d≤50m,评价指数a7为2;当覆坚硬厚岩层距煤层距离50m<d≤100m,评价指数a7为1;当覆坚硬厚岩层距煤层距离d>100m,评价指数a7为0;The distance between the overlying hard and thick rock layer and the coal seam is d. When the distance between the overlying hard and thick rock layer and the coal seam is d≤20m, the evaluation index a7 is 3; when the distance between the overlying hard and thick rock layer and the coal seam is 20m<d≤50m, the evaluation index a7 is 2; when the distance between the overlying hard and thick rock layer and the coal seam is 50m<d≤100m, the evaluation index a7 is 1; when the distance between the overlying hard and thick rock layer and the coal seam is d>100m, the evaluation index a7 is 0;
⑧本区及邻区判据的评价⑧ Evaluation of the criteria for this area and neighboring areas
本区及邻区同一煤层冲击地压发生次数为n,当n≥3时,评价指数a8为3,当2≤n<3时,评价指数a8为2,当n=1时,评价指数a8为1,当n=0时,评价指数a8为0;The number of rock bursts in the same coal seam in this area and the adjacent areas is n. When n≥3, the evaluation index a8 is 3; when 2≤n<3, the evaluation index a8 is 2; when n=1, the evaluation index a8 is 1; when n=0, the evaluation index a8 is 0;
(3)将步骤(2)中得的到各项评价指标值ai进行加和得到综合评价指数 (3) Add the values of each evaluation index a i obtained in step (2) to obtain a comprehensive evaluation index
(4)将步骤(3)中综合评价指数进行归一化处理,得到目标矿井地质动力环境综合评价指标值 (4) Normalize the comprehensive evaluation index in step (3) to obtain the comprehensive evaluation index value of the target mine geological dynamic environment
(5)根据步骤(4)中的标矿井地质动力环境综合评价指标值N划分目标矿井的类型,具体为:当0.5<N≤1时,将目标矿井定义为典型冲击地压矿井,其中0.5<N≤0.75时,目标矿井为具有中等冲击地压的地质动力环境,0.75<N≤1时,目标矿井为具有强冲击地压的地质动力环境;当0.25<N≤0.5时,将目标矿井定义为非典型冲击地压矿井,目标矿井为具有弱冲击地压的地质动力环境;当0≤N≤0.25时,将目标矿井定义为无冲击地压矿井,目标矿井为具有无冲击地压的地质动力环境。(5) The target mine is classified into types according to the comprehensive evaluation index value N of the geological dynamic environment of the target mine in step (4), specifically: when 0.5<N≤1, the target mine is defined as a typical rock burst mine, wherein when 0.5<N≤0.75, the target mine is a geological dynamic environment with moderate rock burst, and when 0.75<N≤1, the target mine is a geological dynamic environment with strong rock burst; when 0.25<N≤0.5, the target mine is defined as an atypical rock burst mine, and the target mine is a geological dynamic environment with weak rock burst; when 0≤N≤0.25, the target mine is defined as a non-rock burst mine, and the target mine is a geological dynamic environment with no rock burst.
所述步骤一中的数据及参数包括应力集中系数、由微震监测系统监测到的煤岩动力系统的释放能量、泊松比、弹性模量、煤岩体的容重、煤岩体的埋藏深度、抗拉强度、抗压强度。The data and parameters in step one include stress concentration factor, released energy of the coal-rock dynamic system monitored by the microseismic monitoring system, Poisson's ratio, elastic modulus, bulk density of the coal-rock mass, burial depth of the coal-rock mass, tensile strength, and compressive strength.
所述步骤二中用煤岩动力系统的能量密度来反映能量特征,具体为:In
(1)自重应力场下煤岩动力系统的能量特征(1) Energy characteristics of coal-rock dynamic system under self-weight stress field
式中:EZ为自重应力场下煤岩动力系统能量密度,J/m3,μ为泊松比;E为弹性模量,Pa;γ为煤岩体的容重,N/m3;H为煤岩体的埋藏深度,m;Where: E Z is the energy density of the coal-rock dynamic system under the self-weight stress field, J/m 3 , μ is Poisson's ratio; E is the elastic modulus, Pa; γ is the bulk density of the coal-rock mass, N/m 3 ; H is the burial depth of the coal-rock mass, m;
(2)构造应力场下煤岩动力系统的能量特征(2) Energy characteristics of coal-rock dynamic system under tectonic stress field
式中:EG为构造应力场下煤岩动力系统能量密度,J/m3;μ为泊松比;E为弹性模量,Pa;γ为煤岩体的容重,N/m3;H为煤岩体的埋藏深度,m;k1、k2、k3为应力集中系数。Where: EG is the energy density of the coal-rock dynamic system under tectonic stress field, J/ m3 ; μ is Poisson's ratio; E is the elastic modulus, Pa; γ is the bulk density of the coal-rock mass, N/ m3 ; H is the burial depth of the coal-rock mass, m; k1 , k2 , k3 are stress concentration coefficients.
所述步骤三中煤岩动力系统能量分别为:The energy of the coal-rock power system in
(1)自重应力场条件下煤岩动力系统的能量(1) Energy of coal-rock dynamic system under self-weight stress field conditions
(2)构造应力场条件下煤岩动力系统的能量(2) Energy of coal-rock dynamic system under tectonic stress field conditions
所述步骤四中煤岩动力系统释放能量为:The energy released by the coal-rock power system in
式中:v0为破碎煤岩体抛出的平均初速度,m/s;ρ为破碎后被抛出的煤岩体的平均密度,kg/m3;σc为煤体单轴抗压强度,MPa;Where: v 0 is the average initial velocity of the crushed coal-rock mass, m/s; ρ is the average density of the coal-rock mass thrown out after crushing, kg/m 3 ; σ c is the uniaxial compressive strength of the coal mass, MPa;
结合步骤三的计算结果推导出典型冲击地压矿井的临界深度为:Combined with the calculation results of
根据临界深度预测冲击地压危险性,当开采深度达到临界深度时,继续开采将会有冲击地压发生的危险。The risk of rock burst is predicted based on the critical depth. When the mining depth reaches the critical depth, continued mining will lead to the risk of rock burst.
本发明的有益效果是:冲击地压矿井由于诱发原因不同,冲击显现形式和程度不同,危险性大小也是不同的,如果笼统地、无差别地定义为“冲击地压矿井”,会为防治和管理工作带来更多的难度。”将冲击地压矿井划分为“典型冲击地压矿井”和“非典型冲击地压矿井”两种类型,定量计算典型冲击地压矿井的临界深度,准确预测冲击地压的危险性,实现煤矿冲击地压的有效防控。本发明通过收集目标矿井数据、测试物理力学参数,建立煤岩动力系统模型,并通过构建矿井的地质动力环境体系判定典型冲击地压矿井,针对典型冲击地压矿井分别分析了自重应力场下、构造应力场下煤岩动力系统的能量特征,并分别确定了相应的计算方法,计算煤岩动力系统能量,在此基础上推导计算出典型冲击地压矿井的临界深度,确定煤岩动力系统能量演化与冲击地压动力显现的关系,并进行了准确性验证,本方法可定量计算出典型冲击地压矿井的临界深度,从而准确预测冲击地压发生的危险性,即当开采深度达到临界深度时冲击地压开始发生,应停止开采或采取有效防控措施,本发明能够为煤矿冲击地压的有效防控提供依据。The beneficial effects of the present invention are as follows: due to different inducing causes, impact manifestation forms and degrees of impact in impact mines are different, and the degree of danger is also different. If it is defined as "impact mine" in general and indiscriminately, it will bring more difficulties to prevention, control and management work. Rock burst mines are divided into two types: "typical rock burst mines" and "atypical rock burst mines", the critical depth of typical rock burst mines is quantitatively calculated, the danger of rock burst is accurately predicted, and effective prevention and control of rock burst in coal mines is achieved. The present invention collects target mine data, tests physical and mechanical parameters, establishes a coal-rock power system model, and determines a typical rock burst mine by constructing a geological dynamic environment system of the mine. The energy characteristics of the coal-rock power system under the self-weight stress field and the tectonic stress field are analyzed for typical rock burst mines, and the corresponding calculation methods are determined respectively to calculate the energy of the coal-rock power system. On this basis, the critical depth of the typical rock burst mine is derived and calculated, the relationship between the energy evolution of the coal-rock power system and the manifestation of rock burst power is determined, and the accuracy is verified. The method can quantitatively calculate the critical depth of the typical rock burst mine, thereby accurately predicting the danger of rock burst, that is, when the mining depth reaches the critical depth, rock burst begins to occur, and mining should be stopped or effective prevention and control measures should be taken. The present invention can provide a basis for the effective prevention and control of rock burst in coal mines.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
图1为一种典型冲击地压矿井的冲击地压危险性预测方法流程图;FIG1 is a flow chart of a method for predicting rock burst hazard in a typical rock burst mine;
图2为本发明中的煤岩动力系统与冲击地压显现关系模型示意图;FIG2 is a schematic diagram of a model showing the relationship between the coal-rock power system and rock burst pressure in the present invention;
图3为本发明中的煤岩动力系统立体模型示意图;FIG3 is a schematic diagram of a three-dimensional model of a coal-rock power system in the present invention;
图4为本发明中的煤岩动力系统能量来源示意图;FIG4 is a schematic diagram of energy sources of the coal-rock power system of the present invention;
图5为本发明中实施例提供的某矿井A01综放面冲击地压发生临界深度计算结果折线图;FIG5 is a line graph showing the calculation results of the critical depth of rock burst at the fully mechanized caving face of a certain mine A01 provided in an embodiment of the present invention;
其中,1动力核区,2破坏区,3损伤区,4影响区。Among them, 1 is the power core area, 2 is the destruction area, 3 is the damage area, and 4 is the impact area.
具体实施方式DETAILED DESCRIPTION
为了更好的解释本发明,以便于理解,下面结合附图,通过具体实施方式,对本发明的技术方案和效果作详细描述。In order to better explain the present invention and facilitate understanding, the technical solutions and effects of the present invention are described in detail below through specific implementation modes in conjunction with the accompanying drawings.
如图1所示,一种典型冲击地压矿井的冲击地压危险性预测方法,具体包括以下步骤:As shown in FIG1 , a method for predicting rock burst hazard of a typical rock burst mine specifically includes the following steps:
步骤一:收集目标矿井数据,测试物理力学参数,并建立煤岩动力系统模型,通过构建矿井的地质动力环境体系判定典型冲击地压矿井;为冲击地压提供能量及受到影响的煤岩体构成了“煤岩动力系统”,在不同地质动力环境和开采条件下,煤岩体积聚能量和释放能量的形式不同,冲击地压显现特征不同。自然地质条件下,煤岩动力系统处于平衡状态;在采掘活动扰动下,煤岩体应力升高、能量积聚,当超过煤岩体的强度极限时,引起系统结构失稳,能量释放,可能发生冲击地压。为了描述煤岩动力系统与冲击地压显现关系,构建“煤岩动力系统与冲击地压显现关系模型”,如图2所示,根据能量积聚程度和影响范围等特征,可将煤岩动力系统划分为“动力核区”、“破坏区”、“损伤区”、“影响区”,即图2中所示的动力核区1、破坏区2、损伤区3、影响区4四个区域,煤岩动力系统的能量集中在“动力核区”内,煤岩动力系统“动力核区”是冲击地压发生的动力源,煤岩动力系统立体模型如图3所示,由中心位置向外依次为动力核区1、破坏区2、损伤区3、影响区4。当冲击地压发生时,煤岩动力系统释放的能量是由“动力核区”提供,煤岩动力系统总能量由基础能量与释放能量构成。“动力核区”的半径如下式所示:Step 1: Collect target mine data, test physical and mechanical parameters, and establish a coal-rock dynamic system model. Determine typical rock burst mines by constructing the geological dynamic environment system of the mine; the coal and rock mass that provide energy for rock burst and are affected constitute the "coal-rock dynamic system". Under different geological dynamic environments and mining conditions, the coal and rock mass accumulate and release energy in different forms, and rock burst characteristics are different. Under natural geological conditions, the coal-rock dynamic system is in a state of equilibrium; under the disturbance of mining activities, the stress of the coal and rock mass increases and energy accumulates. When it exceeds the strength limit of the coal and rock mass, it causes the system structure to become unstable, energy is released, and rock burst may occur. In order to describe the relationship between the coal-rock dynamic system and rock burst, a "coal-rock dynamic system and rock burst relationship model" is constructed, as shown in Figure 2. According to the characteristics of energy accumulation degree and influence range, the coal-rock dynamic system can be divided into "dynamic core area", "destruction area", "damage area" and "influence area", namely the four areas of
式中,R为煤岩动力系统“动力核区”半径,m;k1、k2、k3为应力集中系数。k1为最大主应力与垂直应力的比值;k2为中间应力与垂直应力的比值;k3为最小主应力与垂直应力的比值;△U为由微震监测系统监测到的煤岩动力系统的释放能量,J。μ为泊松比;E为弹性模量,Pa;γ为煤岩体的容重,N/m3;H为煤岩体的埋藏深度,m。Where R is the radius of the "dynamic core area" of the coal-rock dynamic system, m; k1 , k2 , and k3 are stress concentration coefficients. k1 is the ratio of the maximum principal stress to the vertical stress; k2 is the ratio of the intermediate stress to the vertical stress; k3 is the ratio of the minimum principal stress to the vertical stress; △U is the released energy of the coal-rock dynamic system monitored by the microseismic monitoring system, J. μ is Poisson's ratio; E is the elastic modulus, Pa; γ is the bulk density of the coal-rock mass, N/ m3 ; H is the burial depth of the coal-rock mass, m.
根据地质动力环境评价方法,可将冲击地压矿井分为典型冲击地压矿井和非典型冲击地压矿井两类,冲击地压的发生是地质动力环境与开采扰动共同作用的结果,也是煤岩动力系统能量的积聚与释放的动态过程。当煤岩动力系统积聚的能量能够支撑冲击地压发生,在开采活动诱发下就会发生冲击地压的矿井为典型冲击地压矿井;当煤岩动力系统积聚的能量不能够支撑冲击地压发生,需要其他工程条件补充能量,在开采活动诱发下才有可能发生冲击地压的矿井为非典型冲击地压矿井。According to the geological dynamic environment assessment method, rock burst mines can be divided into two categories: typical rock burst mines and atypical rock burst mines. The occurrence of rock burst is the result of the combined effect of the geological dynamic environment and mining disturbance, and is also a dynamic process of energy accumulation and release of the coal-rock dynamic system. When the energy accumulated in the coal-rock dynamic system can support the occurrence of rock burst, the mine that will experience rock burst under the induction of mining activities is a typical rock burst mine; when the energy accumulated in the coal-rock dynamic system cannot support the occurrence of rock burst, other engineering conditions are needed to supplement the energy, and the mine that may experience rock burst only under the induction of mining activities is an atypical rock burst mine.
通过构建地质动力环境评价体系判定典型冲击地压矿井的方法,具体包括以下步骤:The method for determining a typical rock burst mine by constructing a geological dynamic environment evaluation system specifically includes the following steps:
(1)构建由目标矿井的构造凹地地貌条件、断块构造垂直运动条件、断块构造水平运动条件、断裂构造影响范围、构造应力、煤层开采深度、上覆坚硬岩层条件、本区及邻区冲击地压判据条件八个因素构成的地质动力环境评价体系;(1) Construct a geodynamic environment evaluation system consisting of eight factors: the geomorphological conditions of the target mine's structural depression, the vertical movement conditions of the fault block structure, the horizontal movement conditions of the fault block structure, the influence range of the fault structure, the tectonic stress, the coal seam mining depth, the overlying hard rock conditions, and the rock burst judgment criteria of the area and the adjacent areas;
(2)将地质动力环境评价指标体系中各项评价指标值ai划分为四个等级,根据每项评价指标对矿井地质动力环境的影响程度逐一评判,对矿井地质动力环境无影响的评价指标ai的评价指数为0、影响程度弱时ai的评价指数为1、中等影响时ai的评价指数为2、有强烈影响时ai的评价指数为3;具体为:(2) The evaluation index values ai in the geological dynamic environment evaluation index system are divided into four levels, and each evaluation index is judged one by one according to the degree of influence of each evaluation index on the mine geological dynamic environment. The evaluation index ai with no influence on the mine geological dynamic environment is 0, the evaluation index ai with weak influence is 1, the evaluation index ai with medium influence is 2, and the evaluation index ai with strong influence is 3; specifically:
①井田构造凹地地貌特征:① Geomorphic characteristics of the well field structural depression:
其中,C—构造凹地的反差强度;Where, C—contrast intensity of structural depression;
△h—构造凹地最高与最低高程的差值,km;△h—the difference between the highest and lowest elevations of the structural depression, km;
△l—构造凹地的宽度,km;△l—width of structural depression, km;
A、B—权重系数;山地地貌:A=0.25,B=0.75,丘陵地貌:A=0.5,B=0.5,平原地貌:A=0.75,B=0.25;A, B—weight coefficients; mountainous landform: A=0.25, B=0.75, hilly landform: A=0.5, B=0.5, plain landform: A=0.75, B=0.25;
当C≥0.75时,评价指数a1为3;当0.5≤C0.75时,评价指数a1为2;当0.25≤C<0.5时,评价指数a1为1;当C<0.25时,评价指数a1为0;When C≥0.75, the evaluation index a1 is 3; when 0.5≤C0.75, the evaluation index a1 is 2; when 0.25≤C<0.5, the evaluation index a1 is 1 ; when C<0.25, the evaluation index a1 is 0;
②断块构造垂直运动条件:②Conditions for vertical movement of fault-block structures:
目标矿井的断块垂直运动速度为V1,当垂直运动速率V1≥8mm/yr时,评价指数a2为3;当垂直运动速率V1>5mm/yr时,评价指数a2为2;当垂直运动速率V1<-3mm/yr时,评价指数a2为1;当垂直运动速率-3mm/yr≤V1≤5mm/yr时,评价指数a2为0;The vertical movement speed of the fault block in the target mine is V 1 . When the vertical movement speed V 1 ≥8mm/yr, the evaluation index a 2 is 3; when the vertical movement speed V 1 >5mm/yr, the evaluation index a 2 is 2; when the vertical movement speed V 1 <-3mm/yr, the evaluation index a 2 is 1; when the vertical movement speed -3mm/yr≤V 1 ≤5mm/yr, the evaluation index a 2 is 0;
③断块构造水平运动条件:③Conditions for horizontal movement of fault block structures:
目标矿井的断块垂直运动速度为V2,当水平运动速率V2>10mm/yr时,评价指数a3为3;当垂直运动速率5mm/yr≤V2≤10mm/yr时,评价指数a3为2;当垂直运动速率2mm/yr≤V2<5mm/yr时,评价指数a3为1;当垂直运动速率V2<2mm/yr时,评价指数a3为0;The vertical movement speed of the fault block in the target mine is V 2 . When the horizontal movement speed V 2 >10 mm/yr, the evaluation index a 3 is 3; when the vertical movement speed is 5 mm/yr≤V 2 ≤10 mm/yr, the evaluation index a 3 is 2; when the vertical movement speed is 2 mm/yr≤V 2 <5 mm/yr, the evaluation index a 3 is 1; when the vertical movement speed V 2 <2 mm/yr, the evaluation index a 3 is 0;
④断裂构造影响范围条件④Conditions of the influence range of fault structure
b=±(K·10h)b=±(K·10h)
式中:b—断裂构造影响范围宽度,km,当断裂影响范围边界在井田边界外时,b取正值,当断裂影响范围边界跨入井田边界内部时,b取负值;Where: b is the width of the influence range of the fault structure, km. When the boundary of the influence range of the fault is outside the boundary of the well field, b takes a positive value; when the boundary of the influence range of the fault crosses into the boundary of the well field, b takes a negative value.
K—活动性系数(K=1,2,3),断裂活动性强时K=3、断裂活动性中等时K=2、断裂活动性弱时K=1;K—activity coefficient (K=1, 2, 3), when the fault activity is strong, K=3, when the fault activity is medium, K=2, when the fault activity is weak, K=1;
h—断裂垂直落差,m;h—vertical height of the fracture, m;
当b≤0.5时,评价指数a4为3,当0.5<b≤2时,评价指数a4为2,当2<b≤5时,评价指数a4为1,当b>5时,评价指数a4为0;When b≤0.5, the evaluation index a4 is 3, when 0.5<b≤2, the evaluation index a4 is 2, when 2<b≤5, the evaluation index a4 is 1, and when b>5, the evaluation index a4 is 0;
⑤构造应力条件⑤ Tectonic stress conditions
构造应力对冲击地压危险性评价指标用应力集中系数K表示,当K>2时,评价指数a5为3,当1.2<K≤2时,评价指数a5为2,当0.8<K≤1.2时,评价指数a5为1,当K≤0.8时,评价指数a5为0;The evaluation index of tectonic stress on rock burst danger is expressed by stress concentration coefficient K. When K>2, the evaluation index a5 is 3; when 1.2<K≤2, the evaluation index a5 is 2; when 0.8<K≤1.2, the evaluation index a5 is 1; when K≤0.8, the evaluation index a5 is 0;
⑥开采深度条件⑥ Mining depth conditions
当开采深度h>800m时,评价指数a6为3,当600m<h≤800m时,评价指数a6为2,当400m<h≤600m时,评价指数a6为1,当开采深度h≤400m时,评价指数a6为0;When the mining depth h>800m, the
⑦上覆坚硬岩层条件⑦ Overlying hard rock conditions
覆坚硬厚岩层距煤层距离为d,当覆坚硬厚岩层距煤层距离d≤20m,评价指数a7为3;当覆坚硬厚岩层距煤层距离20m<d≤50m,评价指数a7为2;当覆坚硬厚岩层距煤层距离50m<d≤100m,评价指数a7为1;当覆坚硬厚岩层距煤层距离d>100m,评价指数a7为0;The distance between the overlying hard and thick rock layer and the coal seam is d. When the distance between the overlying hard and thick rock layer and the coal seam is d≤20m, the evaluation index a7 is 3; when the distance between the overlying hard and thick rock layer and the coal seam is 20m<d≤50m, the evaluation index a7 is 2; when the distance between the overlying hard and thick rock layer and the coal seam is 50m<d≤100m, the evaluation index a7 is 1; when the distance between the overlying hard and thick rock layer and the coal seam is d>100m, the evaluation index a7 is 0;
⑧本区及邻区判据的评价⑧ Evaluation of the criteria for this area and neighboring areas
本区及邻区同一煤层冲击地压发生次数为n,当n≥3时,评价指数a8为3,当2≤n<3时,评价指数a8为2,当n=1时,评价指数a8为1,当n=0时,评价指数a8为0;The number of rock bursts in the same coal seam in this area and the adjacent areas is n. When n≥3, the evaluation index a8 is 3; when 2≤n<3, the evaluation index a8 is 2; when n=1, the evaluation index a8 is 1; when n=0, the evaluation index a8 is 0;
(3)将步骤(2)中得的到各项评价指标值ai进行加和得到综合评价指数 (3) Add the values of each evaluation index a i obtained in step (2) to obtain a comprehensive evaluation index
(4)将步骤(3)中综合评价指数进行归一化处理,得到目标矿井地质动力环境综合评价指标值 (4) Normalize the comprehensive evaluation index in step (3) to obtain the comprehensive evaluation index value of the target mine geological dynamic environment
(5)根据步骤(4)中的标矿井地质动力环境综合评价指标值N划分目标矿井的类型,具体为:当0.5<N≤1时,将目标矿井定义为典型冲击地压矿井,其中0.5<N≤0.75时,目标矿井为具有中等冲击地压的地质动力环境,0.75<N≤1时,目标矿井为具有强冲击地压的地质动力环境;当0.25<N≤0.5时,将目标矿井定义为非典型冲击地压矿井,目标矿井为具有弱冲击地压的地质动力环境;当0≤N≤0.25时,将目标矿井定义为无冲击地压矿井,目标矿井为具有无冲击地压的地质动力环境。(5) The target mine is classified into types according to the comprehensive evaluation index value N of the geological dynamic environment of the target mine in step (4), specifically: when 0.5<N≤1, the target mine is defined as a typical rock burst mine, wherein when 0.5<N≤0.75, the target mine is a geological dynamic environment with moderate rock burst, and when 0.75<N≤1, the target mine is a geological dynamic environment with strong rock burst; when 0.25<N≤0.5, the target mine is defined as an atypical rock burst mine, and the target mine is a geological dynamic environment with weak rock burst; when 0≤N≤0.25, the target mine is defined as a non-rock burst mine, and the target mine is a geological dynamic environment with no rock burst.
步骤二:针对典型冲击地压矿井,确定煤岩动力系统的能量特征;在煤岩动力系统中,能量因素对冲击地压的发生起着控制作用,并影响整个煤岩动力系统的稳定性。煤岩动力系统能量主要来源于两个方面:一是自然地质动力条件,主要是构造应力(包括自重应力);二是采掘工程效应,即采动应力。煤岩动力系统处于大地构造环境和现代应力场中,具有能量积聚的动力条件,通过采掘等工程活动使得系统的应力叠加、能量积聚,当积聚的能量超过了煤岩体的强度极限时,系统结构失稳,能量释放大于104J~106J时,发生冲击地压等矿井动力灾害,如图4所示。可以说,没有构造运动,就不具备冲击地压发生的地质动力环境,就没有煤岩动力系统的形成,也就没有冲击地压的发生的能量条件。Step 2: Determine the energy characteristics of the coal-rock dynamic system for typical rock burst mines; in the coal-rock dynamic system, the energy factor plays a controlling role in the occurrence of rock burst and affects the stability of the entire coal-rock dynamic system. The energy of the coal-rock dynamic system mainly comes from two aspects: one is the natural geological dynamic conditions, mainly tectonic stress (including self-weight stress); the other is the mining engineering effect, that is, mining stress. The coal-rock dynamic system is in the geotectonic environment and modern stress field, and has the dynamic conditions for energy accumulation. Through mining and other engineering activities, the system's stress is superimposed and energy accumulates. When the accumulated energy exceeds the strength limit of the coal-rock mass, the system structure becomes unstable. When the energy release is greater than 10 4 J to 10 6 J, rock burst and other mine dynamic disasters occur, as shown in Figure 4. It can be said that without tectonic movement, there is no geological dynamic environment for rock burst to occur, there is no formation of the coal-rock dynamic system, and there is no energy condition for the occurrence of rock burst.
煤岩动力系统的总能量由自重应力场下能量、构造应力场下能量和采动应力场下能量组成,具体如下式所示:The total energy of the coal-rock dynamic system is composed of the energy under the self-weight stress field, the energy under the tectonic stress field and the energy under the mining stress field, as shown in the following formula:
U=UZ+UG+UC (2)U=U Z + UG + UC (2)
式中:U为煤岩动力系统的总能量,J;UZ为自重应力场下煤岩动力系统能量,J;UG为构造应力场下煤岩动力系统能量,J;UC为采动应力场下煤岩动力系统能量,J。Where: U is the total energy of the coal-rock dynamic system, J; U Z is the energy of the coal-rock dynamic system under the deadweight stress field, J; UG is the energy of the coal-rock dynamic system under the tectonic stress field, J; UC is the energy of the coal-rock dynamic system under the mining stress field, J.
煤岩动力系统的总能量包括基础能量和释放能量,为了方便对比分析和计算,用煤岩动力系统的能量密度来反映能量特征,典型冲击地压矿井的能量密度主要源于构造应力场,在构造应力场条件下煤岩动力系统积聚的能量已经能够支撑冲击地压发生,此时采掘工程活动等对于冲击地压发生的贡献仅考虑其诱发作用,因此典型冲击地压矿井的临界深度在构造应力场条件下开展研究。由于地应力测量得到的应力值包含自重应力场下的应力,所以构造应力场条件下计算出的能量也包含自重应力场的能量,自重应力场下煤岩动力系统的能量为基础能量,构造应力场下煤岩动力系统的能量定义为总能量。The total energy of the coal-rock dynamic system includes basic energy and released energy. In order to facilitate comparative analysis and calculation, the energy density of the coal-rock dynamic system is used to reflect the energy characteristics. The energy density of a typical rock burst mine mainly comes from the tectonic stress field. Under the conditions of the tectonic stress field, the energy accumulated in the coal-rock dynamic system can already support the occurrence of rock burst. At this time, the contribution of mining engineering activities to the occurrence of rock burst only considers its inducing effect. Therefore, the critical depth of a typical rock burst mine is studied under the conditions of the tectonic stress field. Since the stress value obtained by the geostress measurement includes the stress under the self-weight stress field, the energy calculated under the tectonic stress field also includes the energy of the self-weight stress field. The energy of the coal-rock dynamic system under the self-weight stress field is the basic energy, and the energy of the coal-rock dynamic system under the tectonic stress field is defined as the total energy.
煤岩动力系统能量的计算由能量密度对“动力核区”的体积积分得到,由式(1)可知,煤岩动力系统释放的能量不同,“动力核区”的半径不同,进而体积不同。煤岩动力系统能量密度统一计算公式如式(3)所示:The energy of the coal-rock power system is calculated by integrating the energy density with the volume of the "power core area". From formula (1), it can be seen that the energy released by the coal-rock power system is different, the radius of the "power core area" is different, and then the volume is different. The unified calculation formula for the energy density of the coal-rock power system is shown in formula (3):
式中,Eε为煤岩动力系统的能量密度,J/m3;σ1、σ3为侧向应力,MPa;σ2为自重应力,MPa。Where, Eε is the energy density of the coal-rock dynamic system, J/m 3 ; σ 1 and σ 3 are lateral stresses, MPa; σ 2 is the self-weight stress, MPa.
(1)自重应力场下煤岩动力系统的能量特征(1) Energy characteristics of coal-rock dynamic system under self-weight stress field
在自重应力场下,应力值大小与埋藏深度和容重相关。以单位体积煤岩体为研究对象,自重应力场下能量密度表示式(4)所示。由式(4)可以看出,在自重应力场下,根据金尼克假说,煤岩动力系统的能量仅考虑自重应力的影响,侧向应力在数值上等于自重应力与侧压系数的乘积,煤岩动力系统内积聚的能量随着开采深度的增大而增加。研究中将自重应力场条件下煤岩动力系统的能量定义为煤岩动力系统的基础能量。Under the self-weight stress field, the stress value is related to the burial depth and bulk density. Taking the unit volume of coal rock as the research object, the energy density under the self-weight stress field is expressed as shown in formula (4). It can be seen from formula (4) that under the self-weight stress field, according to the Kinnick hypothesis, the energy of the coal rock dynamic system only considers the influence of the self-weight stress, and the lateral stress is numerically equal to the product of the self-weight stress and the lateral pressure coefficient. The energy accumulated in the coal rock dynamic system increases with the increase of mining depth. In this study, the energy of the coal rock dynamic system under the self-weight stress field is defined as the basic energy of the coal rock dynamic system.
式中,EZ为自重应力场下煤岩动力系统能量密度,J/m3。Where E Z is the energy density of the coal-rock dynamic system under the self-weight stress field, J/m 3 .
(2)构造应力场下煤岩动力系统的能量特征(2) Energy characteristics of coal-rock dynamic system under tectonic stress field
在构造应力场条件下,煤岩动力系统的能量来源于构造应力场。煤岩体中积蓄的能量与三向应力σ1、σ2、σ3相关,以单位体积煤岩体作为研究对象,其能量密度可由式(3),进一步由式(5)~(7)推导得到,如公式(8)所示。由式(8)可以看出,在构造应力场条件下,煤岩动力系统系统内积聚的能量随着构造应力增加而升高。Under the condition of tectonic stress field, the energy of coal-rock dynamic system comes from tectonic stress field. The energy accumulated in coal-rock mass is related to triaxial stress σ 1 , σ 2 , σ 3. Taking unit volume of coal-rock mass as the research object, its energy density can be derived from formula (3) and further from formula (5) to (7), as shown in formula (8). It can be seen from formula (8) that under the condition of tectonic stress field, the energy accumulated in coal-rock dynamic system increases with the increase of tectonic stress.
σ1=k1γH (5)σ 1 =k 1 γH (5)
σ2=k2γH (6)σ 2 = k 2 γH (6)
σ3=k3γH (7)σ 3 = k 3 γH (7)
式中,EG为构造应力场下煤岩动力系统能量密度,J/m3。Where EG is the energy density of the coal-rock dynamic system under tectonic stress field, J/m 3 .
步骤三:计算煤岩动力系统的总能量及基础能量Step 3: Calculate the total energy and basic energy of the coal-rock power system
煤岩动力系统划分为“动力核区”、“破坏区”、“损伤区”和“影响区”4个区域,只有当采掘工程活动进入到“动力核区”、“破坏区”和“损伤区”这三个区域,才会具备不同程度和破坏形式冲击地压的发生危险。当采掘工程进入到“影响区”范围内时,动力显现主要以“煤炮”的形式表现出来;当采掘工程进入到“损伤区”范围内时,动力显现主要以“压出、倾出”等形式表现出来;当采掘工程进入到“破坏区”范围内时,动力显现则表现为“冲击地压”;当采掘工程进入“动力核区”范围内时,则会产生“强冲击地压”。因此,对于典型冲击地压矿井,其煤岩动力系统能量是将各应力场下的能量密度对“动力核区”的体积积分得到。The coal-rock dynamic system is divided into four areas: "dynamic core area", "destruction area", "damage area" and "influence area". Only when the mining project enters the "dynamic core area", "destruction area" and "damage area", will there be the danger of rock burst with different degrees and forms of damage. When the mining project enters the "influence area", the dynamic manifestation is mainly in the form of "coal cannon"; when the mining project enters the "damage area", the dynamic manifestation is mainly in the form of "pressing out, pouring out" and so on; when the mining project enters the "destruction area", the dynamic manifestation is "rock burst"; when the mining project enters the "dynamic core area", it will produce "strong rock burst". Therefore, for a typical rock burst mine, the energy of its coal-rock dynamic system is obtained by integrating the energy density under each stress field over the volume of the "dynamic core area".
(1)自重应力场条件下煤岩动力系统的能量(1) Energy of coal-rock dynamic system under self-weight stress field conditions
自重应力场条件下煤岩动力系统的能量是式(4)所示能量密度的体积积分,计算方法如下式(10)所示:The energy of the coal-rock power system under the condition of self-weight stress field is the volume integral of the energy density shown in formula (4), and the calculation method is shown in the following formula (10):
计算结果如式(11)所示,式(11)所示即为构造应力场下的煤岩动力系统的基础能量:The calculation results are shown in formula (11), which is the basic energy of the coal-rock dynamic system under the tectonic stress field:
(2)构造应力场条件下煤岩动力系统的能量(2) Energy of coal-rock dynamic system under tectonic stress field conditions
构造应力场条件下煤岩动力系统的能量是式(9)所示的能量密度的体积积分,计算方法如式(12)所示:The energy of the coal-rock dynamic system under tectonic stress field conditions is the volume integral of the energy density shown in formula (9), and the calculation method is shown in formula (12):
计算结果如式(13)所示,式(13)所示即为构造应力场条件下煤岩动力系统的总能量:The calculation results are shown in formula (13), which is the total energy of the coal-rock dynamic system under the tectonic stress field:
由于构造断块间的相互作用和岩石力学性质的差异,在井田范围内会自然形成高应力区、应力梯度区和低应力区。在高应力区内,岩体在较高的应力作用下,积聚的弹性能与正常应力区相比有较大幅度提高,部分岩体已经达到稳态向非稳态转变的临界,最容易导致巷道破坏发生;在应力梯度区内,应力和变形模量都有较大幅度的增长,岩石的脆性增大、破坏强度降低,容易形成地质构造,在构造应力的作用下容易导致巷道破坏;位于低应力区的岩石,其特性变化程度不大,不易产生能量的积聚,巷道破坏的危险性最低。一般情况下,当应力集中系数K>1.2时,与之对应的主应力等值线圈定的范围为高应力区;当K<0.8时,与之对应的主应力等值线圈定的范围为低应力区;应力梯度区通常位于应力正常区与高应力区之间。位于不同应力区的系统能量使用相应的应力值和应力集中系数计算即可。Due to the interaction between structural fault blocks and the difference in rock mechanical properties, high stress areas, stress gradient areas and low stress areas will naturally form within the well field. In the high stress area, the elastic energy accumulated by the rock mass under higher stress is significantly increased compared with the normal stress area. Some rock masses have reached the critical transition from steady state to unsteady state, which is most likely to cause tunnel damage; in the stress gradient area, the stress and deformation modulus have increased significantly, the brittleness of the rock increases, the destructive strength decreases, and it is easy to form geological structures, which are easy to cause tunnel damage under the action of tectonic stress; the rock located in the low stress area has a small degree of change in characteristics, is not easy to produce energy accumulation, and has the lowest risk of tunnel damage. In general, when the stress concentration coefficient K>1.2, the corresponding range of the principal stress contour line is the high stress area; when K<0.8, the corresponding range of the principal stress contour line is the low stress area; the stress gradient area is usually located between the normal stress area and the high stress area. The system energy located in different stress areas can be calculated using the corresponding stress value and stress concentration coefficient.
步骤四:计算煤岩动力系统释放能量,结合步骤三所求结果推导计算典型冲击地压矿井的临界深度,确定煤岩动力系统能量演化与冲击地压动力显现的关系:煤岩动力系统的释放能量等于总能量与基础能量的差值,冲击地压显现强度与煤岩动力系统释放能量正相关。研究表明,破碎煤岩体抛向自由空间的初速度是冲击地压发生与否的一项重要指标,当初速度小于1m/s时,不可能发生冲击地压;当初速度大于10m/s时,则发生冲击地压的可能性较高。冲击地压发生时,所需能量既要满足单位煤岩体发生破碎需要消耗的能量,又要满足煤岩体发生冲击地压需要聚积的最小动能,当单位煤岩体聚积的弹性能超过二者之和时,冲击地压就可能发生。因此,冲击地压发生时,煤岩动力系统释放能量的能量密度计算结果可用公式(15)表示,此时煤岩动力系统释放能量的计算结果可用公式(16)表示:Step 4: Calculate the energy released by the coal-rock dynamic system. Combined with the results obtained in
式中,Emin为冲击地压发生时,煤岩动力系统释放能量的能量密度,J/m3;v0为破碎煤岩体抛出的平均初速度,m/s;ρ为破碎后被抛出的煤岩体的平均密度,kg/m3;σc为煤体单轴抗压强度,MPa。冲击地压发生时,煤岩动力系统释放的能量可用下式表示:Where, Emin is the energy density of the energy released by the coal-rock dynamic system when rock burst occurs, J/ m3 ; v0 is the average initial velocity of the crushed coal-rock mass, m/s; ρ is the average density of the coal-rock mass thrown out after crushing, kg/ m3 ; σc is the uniaxial compressive strength of the coal mass, MPa. When rock burst occurs, the energy released by the coal-rock dynamic system can be expressed by the following formula:
式中,US为冲击地压发生时,煤岩动力系统释放的能量,J。Where US is the energy released by the coal-rock dynamic system when rock burst occurs, J.
典型冲击地压矿井开始发生冲击地压时,释放能量为构造应力场能量与基础能量的差值,即:When rock burst occurs in a typical rock burst mine, the released energy is the difference between the tectonic stress field energy and the basic energy, that is:
UG-UZ=US=△U (17)U G -U Z =U S =△U (17)
带入式(11)、(13)、(16)得到的H值定义为Hmin,即典型冲击地压矿井的临界深度:Substituting into equations (11), (13), and (16), the H value is defined as H min , which is the critical depth of a typical rock burst mine:
步骤五:通过临界深度预测典型冲击地压矿井的冲击地压危险性:根据临界深度预测冲击地压危险性,当开采深度达到临界深度时,继续开采将会有冲击地压发生的危险,应立即停止开采或采取有效的防控措施。Step 5: Predict the rock burst hazard of typical rock burst mines through critical depth: Predict the rock burst hazard based on the critical depth. When the mining depth reaches the critical depth, there will be a risk of rock burst if mining continues. Mining should be stopped immediately or effective prevention and control measures should be taken.
将上述一种典型冲击地压矿井的冲击地压危险性预测方法在某典型冲击地压矿井进行应用,进行该方法的准确性验证:The rock burst hazard prediction method of a typical rock burst mine is applied in a typical rock burst mine to verify the accuracy of the method:
首先分别从某矿井的构造凹地地貌特征、断块构造垂直运动条件、断块构造水平运动条件、断裂构造影响范围条件、构造应力条件、开采深度条件、上覆坚硬岩层条件、本区及邻区判据的评价这八个因素对井田冲击地压的地质动力环境进行分析和评估,构建地质动力环境评价体系,判断典型冲击地压矿井:Firstly, the geodynamic environment of rock burst in the mine field is analyzed and evaluated from eight factors, including the geomorphological characteristics of the structural depression of a mine, the vertical movement conditions of the fault block structure, the horizontal movement conditions of the fault block structure, the influence range of the fault structure, the structural stress conditions, the mining depth conditions, the overlying hard rock conditions, and the evaluation of the criteria of the area and the neighboring areas. A geodynamic environment evaluation system is constructed to judge the typical rock burst mine:
(1)井田构造凹地地貌特征(1) Geomorphic characteristics of the structural depression in the well field
经过计算,该井田的构造凹地的反差强度为0.62,评价指数为2,属于中等危险程度。After calculation, the contrast intensity of the structural depression in the well field is 0.62, and the evaluation index is 2, which is a medium-risk level.
(2)断块构造垂直运动条件(2) Conditions for vertical movement of block structures
根据该矿的地理位置与华北板块内部升降运动的相对关系,矿井位于冀辽上升区,上升速度为3mm/a,地处冀辽上升区和下辽河下降区的升降断块带上,即断块相对运动剧烈区,两断块相对运动2.5mm/a,表明该矿井的垂直运动速率为5.5mm/a。根据地质动力环境评价指标,该矿井评价指数为2,属于中等危险程度。According to the relative relationship between the mine's geographical location and the internal uplift movement of the North China Plate, the mine is located in the Ji-Liao uplift area, with an uplift speed of 3 mm/a. It is located in the uplift fault block belt of the Ji-Liao uplift area and the Xia Liaohe downlift area, that is, the area of intense relative movement of the fault blocks. The relative movement of the two fault blocks is 2.5 mm/a, indicating that the vertical movement rate of the mine is 5.5 mm/a. According to the geological dynamic environment evaluation index, the mine has an evaluation index of 2, which is a medium-risk level.
(3)断块构造水平运动条件(3) Conditions for horizontal movement of block structures
该矿井所处区域断块以垂直升降运动为主,水平运动速率为0,根据地质动力环境评价指标,该矿井处于水平断块运动平稳区,评价指数为0,无危险。The blocks in the area where the mine is located mainly move in vertical up and down motion, and the horizontal movement rate is 0. According to the geological dynamic environment evaluation indicators, the mine is in a stable area of horizontal block movement, the evaluation index is 0, and there is no danger.
(4)断裂构造影响范围条件(4) Conditions of the influence range of fault structure
根据浑河断裂的观测资料,1962年~1982年断裂的上盘下降的平均速率为1.0mm/a,历史地震震级为4级,综合考虑判别浑河断裂为弱活动断裂,取K=1。该矿F1断层最大落差约1200m,则其影响宽度为:According to the observation data of Hunhe Fault, the average rate of the upper wall of the fault from 1962 to 1982 was 1.0mm/a, and the historical earthquake magnitude was 4. Taking comprehensive consideration, the Hunhe Fault was judged to be a weakly active fault, and K = 1 was taken. The maximum drop of the F1 fault in the mine is about 1200m, so its affected width is:
b=K·10h=1×10×1200=12000mb=K·10h=1×10×1200=12000m
F1断裂位于该井田内,因此根据断裂构造影响范围条件判断,该矿井评价指数为3,属于强危险程度。The F1 fault is located within the mining area. Therefore, based on the influence range of the fault structure, the mine evaluation index is 3, which is a highly dangerous level.
(5)构造应力条件(5) Tectonic stress conditions
结合本矿地应力实测数据,矿井开采深度均在400m以上,最大主应力σ1=34.95MPa,垂直主应力σv=21.80MPa,最大水平应力与垂直应力的比值为1.60,介于1.2与2之间,因此根据构造应力条件判断,该矿井评价指数为2,属于中等危险程度。Combined with the measured data of ground stress in this mine, the mining depth of the mine is above 400m, the maximum principal stress σ1 = 34.95MPa, the vertical principal stress σv = 21.80MPa, and the ratio of the maximum horizontal stress to the vertical stress is 1.60, which is between 1.2 and 2. Therefore, according to the structural stress conditions, the evaluation index of the mine is 2, which is of medium risk.
(6)开采深度条件(6) Mining depth conditions
该矿井目前的开采深度大于830m,因此根据开采深度条件判断,该矿井评价指数为3,属于强危险程度。The current mining depth of the mine is greater than 830m. Therefore, based on the mining depth conditions, the mine evaluation index is 3, which is a highly dangerous level.
(7)上覆坚硬岩层条件(7) Overlying hard rock conditions
该矿井顶板岩层均为岩性软弱的页岩层,相当于坚硬岩层距离煤层距离大于100m,因此根据上覆坚硬岩层条件判断,该矿井评价指数为0,无危险。The roof rock layers of the mine are all soft shale layers, which is equivalent to the hard rock layers being more than 100m away from the coal seams. Therefore, based on the conditions of the overlying hard rock layers, the mine evaluation index is 0, which means there is no danger.
(8)本区及邻区判据的评价(8) Evaluation of the criteria for this area and neighboring areas
该矿井的两个相邻矿井均有冲击地压发生,且历史发生次数均在5次以上,因此根据本区及邻区判据的评价结果,该矿井评价指数为3,属于强危险程度。Both of the two adjacent mines of this mine have experienced rock bursts, and the number of such incidents in history is more than five times. Therefore, according to the evaluation results of this area and neighboring areas, the evaluation index of this mine is 3, which is a highly dangerous level.
综上所述,通过综合指标判断,该冲击地压矿井的综合评价指数为0.625,大于0.5,属于典型冲击地压矿井的范围。In summary, judging by comprehensive indicators, the comprehensive evaluation index of this rock burst mine is 0.625, which is greater than 0.5 and falls within the range of typical rock burst mines.
上述的典型冲击地压矿井煤岩物理力学参数测试结果见表1,选取2011年1月至2013年11月的20次冲击地压的震源点深度,以及计算得到每一次冲击地压发生时煤岩动力系统的总能量、基础能量和释放能量见表2。The test results of the physical and mechanical parameters of coal and rock in the above-mentioned typical rock burst mines are shown in Table 1. The source depths of 20 rock bursts from January 2011 to November 2013 were selected, and the total energy, basic energy and released energy of the coal and rock dynamic system were calculated for each rock burst, as shown in Table 2.
表1某煤矿煤岩体物理力学性质参数测试结果汇总Table 1 Summary of test results of physical and mechanical properties of coal and rock mass in a coal mine
表2某煤矿部分冲击地压煤岩动力系统释放能量计算结果Table 2 Calculation results of energy released by the coal-rock dynamic system of some rock bursts in a coal mine
该矿井A01综放工作面位于-830m水平,地面标高+89.1m~+95.4m,井下标高-748.2m~-833.5m,工作面走向长度603m,倾斜长度163.5m,煤厚11.8m。该工作面从2014年6月23日至2015年1月29日共发生冲击地压和矿震(能量166J以上)58次,震源点深度为-584m~-874m,平均标高-804.93m。根据地应力测量结果,该工作面的k1值为1.97、k2值为1.00、k3值为0.79,根据式(18)所示的计算方法,该工作面的冲击地压发生临界深度为标高-754.54m,如图5所示的58组数据中,有54组数据在计算的临界深度以下,由此说明本发明所提供的方法可准确地预测典型冲击地压矿井的冲击地压危险性。The A01 fully mechanized caving working face of the mine is located at the -830m level, with a ground elevation of +89.1m to +95.4m, an underground elevation of -748.2m to -833.5m, a working face strike length of 603m, an inclined length of 163.5m, and a coal thickness of 11.8m. From June 23, 2014 to January 29, 2015, the working face experienced 58 rock bursts and mine shocks (energy above 16 6 J), with a focal depth of -584m to -874m and an average elevation of -804.93m. According to the ground stress measurement results, the k1 value of the working face is 1.97, the k2 value is 1.00, and the k3 value is 0.79. According to the calculation method shown in formula (18), the critical depth of rock burst in the working face is -754.54 m above sea level. Among the 58 sets of data shown in Figure 5, 54 sets of data are below the calculated critical depth, which shows that the method provided by the present invention can accurately predict the rock burst hazard of typical rock burst mines.
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