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CN114458307A - A method for in situ acquisition of rock dynamic parameters - Google Patents

A method for in situ acquisition of rock dynamic parameters Download PDF

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CN114458307A
CN114458307A CN202111573863.4A CN202111573863A CN114458307A CN 114458307 A CN114458307 A CN 114458307A CN 202111573863 A CN202111573863 A CN 202111573863A CN 114458307 A CN114458307 A CN 114458307A
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李泽华
余德运
王仲琦
王洪强
杨恩
徐谦
张世青
王银涛
冯凯
吕智铭
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    • EFIXED CONSTRUCTIONS
    • E21EARTH OR ROCK DRILLING; MINING
    • E21BEARTH OR ROCK DRILLING; OBTAINING OIL, GAS, WATER, SOLUBLE OR MELTABLE MATERIALS OR A SLURRY OF MINERALS FROM WELLS
    • E21B49/00Testing the nature of borehole walls; Formation testing; Methods or apparatus for obtaining samples of soil or well fluids, specially adapted to earth drilling or wells
    • EFIXED CONSTRUCTIONS
    • E21EARTH OR ROCK DRILLING; MINING
    • E21BEARTH OR ROCK DRILLING; OBTAINING OIL, GAS, WATER, SOLUBLE OR MELTABLE MATERIALS OR A SLURRY OF MINERALS FROM WELLS
    • E21B47/00Survey of boreholes or wells
    • EFIXED CONSTRUCTIONS
    • E21EARTH OR ROCK DRILLING; MINING
    • E21FSAFETY DEVICES, TRANSPORT, FILLING-UP, RESCUE, VENTILATION, OR DRAINING IN OR OF MINES OR TUNNELS
    • E21F17/00Methods or devices for use in mines or tunnels, not covered elsewhere
    • E21F17/18Special adaptations of signalling or alarm devices
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    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • G06F30/23Design optimisation, verification or simulation using finite element methods [FEM] or finite difference methods [FDM]
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
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Abstract

本发明属于矿山爆破技术领域,公开了一种岩石动力学参数原位获取方法,包括如下步骤:根据钻机参数划分爆破工区内岩石分层的层位,并获取各层位的岩石物理力学参数;在爆破工区内进行微测井试验;根据各层位的岩石物理力学参数和微测井试验数据;在爆破工区内进行试炮激发试验;建立初始的有限元模型;获取最优的有限元模型;基于最优的有限元模型获取各层位的岩石动力学参数。本发明解决了现有技术存在的步骤复杂,精确性和实时性较低,时间成本投入过大以及工区岩体连续性被破坏的问题。

Figure 202111573863

The invention belongs to the technical field of mine blasting, and discloses a method for in-situ acquisition of rock dynamic parameters, comprising the following steps: dividing layers of rock layers in a blasting work area according to drilling rig parameters, and acquiring rock physical mechanics parameters of each layer; Carry out micro-logging test in the blasting work area; according to the rock physical and mechanical parameters and micro-logging test data of each layer; carry out the test shot excitation test in the blasting work area; establish the initial finite element model; obtain the optimal finite element model ; Obtain the rock dynamic parameters of each horizon based on the optimal finite element model. The invention solves the problems existing in the prior art that the steps are complicated, the accuracy and real-time performance are low, the time cost is too large, and the continuity of the rock mass in the work area is destroyed.

Figure 202111573863

Description

一种岩石动力学参数原位获取方法A method for in situ acquisition of rock dynamic parameters

技术领域technical field

本发明属于矿山爆破技术领域,具体涉及一种岩石动力学参数原位获取方法。The invention belongs to the technical field of mine blasting, and particularly relates to an in-situ acquisition method of rock dynamic parameters.

背景技术Background technique

常规的爆破作业中,通过取芯的方法获取岩体样本,在实验室中对岩体样本进行力学性能测试,获得岩石力学参数,这种方式在工程运用中,步骤复杂,精确性和实时性较低,并且时间成本投入过大。目前爆破岩石动力学参数自动识别方法有基于聚类分析和人工智能的方法,这两种方法都是基于样本数据库,通过构建自变量和因变量的函数关系,确定岩石动力学参数。这就涉及到基于样本数据库预测到的岩石动力学参数的准确性问题,岩石动力学参数是岩石内在物理力学特征,在动力学过程中表现出的特定属性,可以把岩体样本取样后带入实验室进行检测,进行力学测试后进行力学参数准确性验证,这个过程破坏了工区岩体连续性,且费时费力费事。并且随着精细爆破理念和电子雷管的发展,对爆破的设计和爆破全程精细控制要求越来越高,矿山岩石动力学参数是精细爆破设计的基础,跟随钻机钻孔过程中实时获取钻机参数以识别岩性,并对岩性数据分析进而反馈钻机,以优化钻机参数,以此循环,获取-计算-反馈-调整-获取,使爆破更加合理与经济。5G信息技术和随钻传感器的发展,让露天矿山爆破钻孔作业过程中,实时获取钻机数据成为现实。如何在钻机钻孔过程中实时获得岩石动力学参数并能够进行快速岩石动力学参数准确性验证,对爆破质量控制和爆破经济性具有重要意义。In conventional blasting operations, the rock mass samples are obtained by coring, and the mechanical properties of the rock mass samples are tested in the laboratory to obtain rock mechanical parameters. This method has complex steps, accuracy and real-time performance in engineering applications low, and the time cost is too high. At present, the automatic identification methods of blasting rock dynamic parameters include methods based on cluster analysis and artificial intelligence, both of which are based on sample databases, and determine rock dynamic parameters by constructing the functional relationship between independent variables and dependent variables. This involves the accuracy of the rock dynamic parameters predicted based on the sample database. The rock dynamic parameters are the inherent physical and mechanical characteristics of the rock, and the specific properties exhibited in the dynamic process can be taken into the rock samples after sampling. Testing in the laboratory, and verification of the accuracy of mechanical parameters after mechanical testing, this process destroys the continuity of the rock mass in the work area, and is time-consuming, labor-intensive, and labor-intensive. And with the development of fine blasting concept and electronic detonator, the requirements for blasting design and fine control of blasting process are getting higher and higher. Mine rock dynamic parameters are the basis of fine blasting design. Identify the lithology, analyze the lithology data and then feed back the drilling rig to optimize the drilling rig parameters. This cycle, acquisition-calculation-feedback-adjustment-acquisition, makes blasting more reasonable and economical. The development of 5G information technology and sensors while drilling has made real-time acquisition of drilling rig data a reality during blasting and drilling operations in open-pit mines. How to obtain the rock dynamic parameters in real time during the drilling process of the drilling rig and to be able to quickly verify the accuracy of the rock dynamic parameters is of great significance to the blasting quality control and blasting economy.

发明内容SUMMARY OF THE INVENTION

为了解决现有技术存在的步骤复杂,精确性和实时性较低,时间成本投入过大以及工区岩体连续性被破坏的问题,本发明目的在于提供一种岩石动力学参数原位获取方法。In order to solve the problems of complex steps, low accuracy and real-time performance, excessive time cost and damage to the continuity of the rock mass in the work area in the prior art, the present invention aims to provide an in-situ acquisition method of rock dynamic parameters.

本发明所采用的技术方案为:The technical scheme adopted in the present invention is:

一种岩石动力学参数原位获取方法,包括如下步骤:A method for in-situ acquisition of rock dynamic parameters, comprising the following steps:

根据钻机参数划分爆破工区内岩石分层的层位,并获取各层位的岩石物理力学参数;According to the drilling rig parameters, the rock layered layers in the blasting area are divided, and the rock physical and mechanical parameters of each layer are obtained;

在爆破工区内进行微测井试验,得到各层位的各第一监测点的微测井试验数据;Carry out micro-logging test in the blasting area, and obtain the micro-logging test data of each first monitoring point in each layer;

根据各层位的岩石物理力学参数和微测井试验数据,得到各层位的弹塑性参数;According to the petrophysical and mechanical parameters of each layer and the micro-logging test data, the elastic-plastic parameters of each layer are obtained;

在爆破工区内进行试炮激发试验,动态设置第二监测点并记录对应的监测振动数据;Carry out the test shot excitation test in the blasting work area, dynamically set the second monitoring point and record the corresponding monitoring vibration data;

根据试炮激发试验的爆源参数、第二监测点的位置数据、岩石分层的层位以及各层位的弹塑性参数,建立初始的有限元模型;According to the blast source parameters of the test shot excitation test, the position data of the second monitoring point, the layers of rock layers and the elastic-plastic parameters of each layer, the initial finite element model is established;

使用初始的有限元模型获取各第二监测点的计算振动数据,将计算振动数据与对应的监测振动数据进行对比分析,根据对比分析结果优化初始的有限元模型,得到最优的有限元模型;Use the initial finite element model to obtain the calculated vibration data of each second monitoring point, compare and analyze the calculated vibration data with the corresponding monitoring vibration data, and optimize the initial finite element model according to the comparative analysis results to obtain the optimal finite element model;

基于最优的有限元模型获取各层位的岩石动力学参数。The rock dynamic parameters of each horizon are obtained based on the optimal finite element model.

进一步地,根据钻机参数划分爆破工区内岩石分层的层位,并获取各层位的岩石物理力学参数,包括如下步骤:Further, according to the drilling rig parameters, the layers of the rock layers in the blasting work area are divided, and the rock physical and mechanical parameters of each layer are obtained, including the following steps:

获取钻头在不同深度处的钻机参数;Get the rig parameters of the drill bit at different depths;

根据获取的钻机参数划分爆破工区内岩石分层的层位;According to the obtained drilling rig parameters, the rock layers in the blasting area are divided;

根据钻机参数计算各层位的岩石物理力学参数。The rock physical and mechanical parameters of each horizon are calculated according to the drilling rig parameters.

进一步地,钻机参数包括钻头的转速、钻进速度、回转压差、风压、端阻以及摩阻比。Further, the drilling rig parameters include the rotational speed of the drill bit, the drilling speed, the rotary pressure difference, the wind pressure, the end resistance and the frictional resistance ratio.

进一步地,岩石物理力学参数包括岩石的密度、剪切模量以及屈服强度。Further, the rock physical and mechanical parameters include the density, shear modulus and yield strength of the rock.

进一步地,得到各层位的各第一监测点的微测井试验数据,包括如下步骤:Further, obtaining the micro-logging test data of each first monitoring point in each layer includes the following steps:

根据微测井试验要求,在不同深度的微测井中设置雷管;According to the requirements of micro-logging test, set detonators in micro-logging at different depths;

在微测井周围设置若干监测点;Set up several monitoring points around the micro-logging;

依次激发雷管,并记录各第一监测点的微测井试验数据。The detonators are activated in sequence, and the micro-logging test data of each first monitoring point is recorded.

进一步地,得到各层位的弹塑性参数,包括如下步骤:Further, obtaining the elastic-plastic parameters of each horizon includes the following steps:

根据各第一监测点的微测井试验数据获取对应的地震波经过时间数据,并根据地震波经过时间数据获取地震波在各层位的传播波速;The corresponding seismic wave transit time data is obtained according to the micro-logging test data of each first monitoring point, and the propagation wave velocity of the seismic wave in each horizon is obtained according to the seismic wave transit time data;

根据地震波在各层位的传播波速优化爆破工区内岩石分层的层位,得到岩石分层的优化后层位;According to the propagating wave velocity of seismic waves in each horizon, the rock layered layers in the blasting area are optimized, and the optimized rock layered layers are obtained;

根据各优化后层位的岩石物理力学参数和对应的微测井试验数据,获取各优化后层位的弹塑性参数。According to the rock physical and mechanical parameters of each optimized horizon and the corresponding micro-logging test data, the elastic-plastic parameters of each optimized horizon are obtained.

进一步地,弹塑性参数包括衰减系数和弹性模量。Further, the elastic-plastic parameters include attenuation coefficient and elastic modulus.

进一步地,动态设置第二监测点并记录对应的监测振动数据,包括如下步骤:Further, dynamically setting the second monitoring point and recording the corresponding monitoring vibration data includes the following steps:

保持药量不变,在各优化后层位进行试炮激发试验,记录各第二监测点的第一试炮激发数据;Keep the dose constant, carry out the test shot excitation test at each optimized horizon, and record the first test shot excitation data of each second monitoring point;

保持优化后层位不变,使用不同药量进行试炮激发试验,记录各第二监测点的第二试炮激发数据;Keep the optimized horizon unchanged, use different doses to conduct the test shot excitation test, and record the second test shot excitation data of each second monitoring point;

根据第一、二试炮激发数据以及岩石分层的优化后层位,动态设置第二监测点并记录对应的监测振动数据。According to the excitation data of the first and second test shots and the optimized horizon of rock stratification, the second monitoring point is dynamically set and the corresponding monitoring vibration data is recorded.

进一步地,建立初始的有限元模型,包括如下步骤:Further, establishing an initial finite element model includes the following steps:

根据岩石分层的优化后层位,建立岩石力学计算模型;According to the optimized horizon of rock stratification, establish rock mechanics calculation model;

基于岩石力学计算模型,将各优化后层位的弹塑性参数作为介质力学参数,并根据试炮激发试验的爆源参数和各第二监测点的位置数据,建立初始的有限元模型。Based on the rock mechanics calculation model, the elastic-plastic parameters of each optimized horizon are taken as the medium mechanics parameters, and the initial finite element model is established according to the blast source parameters of the test shot excitation test and the position data of each second monitoring point.

进一步地,得到最优的有限元模型,包括如下步骤:Further, obtaining the optimal finite element model includes the following steps:

使用初始的有限元模型获取当前第二监测点在当前优化后层位的计算振动数据,并将计算振动数据与对应的监测振动数据进行对比分析;Use the initial finite element model to obtain the calculated vibration data of the current second monitoring point at the currently optimized horizon, and compare and analyze the calculated vibration data with the corresponding monitored vibration data;

若对比分析结果为误差大于阈值,则调整当前优化后层位的弹塑性参数,重新获取该第二监测点的计算振动数据并重新进行对比分析,否则,更换至下一第二监测点进行对比分析;If the result of the comparative analysis is that the error is greater than the threshold, adjust the elastic-plastic parameters of the currently optimized horizon, re-acquire the calculated vibration data of the second monitoring point and perform the comparative analysis again, otherwise, change to the next second monitoring point for comparison analyze;

若当前优化后层位的所有第二监测点均进行分析比较,则将当前优化后层位的弹塑性参数作为下一优化后层位的介质力学参数,更换至下一优化后层位进行分析比较;If all the second monitoring points of the current optimized horizon are analyzed and compared, the elastic-plastic parameters of the current optimized horizon will be used as the media mechanics parameters of the next optimized horizon, and the analysis will be performed at the next optimized horizon. Compare;

若所有优化后层位的所有第二监测点均进行分析比较,则得到最优的有限元模型。If all the second monitoring points of all the optimized horizons are analyzed and compared, the optimal finite element model will be obtained.

本发明的有益效果为:The beneficial effects of the present invention are:

本发明提供一种不改变爆破工区现有岩层分布现状的岩石动力学参数原位获取方法,把钻孔作业中的钻机数据和岩层地震数据相结合的实时获取方法,简化了岩石动力学参数的获取步骤,提高了精确性和实时性,保证了工区岩体连续性,并且适用于无法使用实验室测试的情况,例如难以获得完整样本,凸显了原位获取岩石动力学参数的优越性。The present invention provides an in-situ acquisition method of rock dynamic parameters without changing the distribution status of existing rock formations in blasting work areas, and a real-time acquisition method combining drilling rig data and rock formation seismic data in drilling operations, which simplifies the analysis of rock dynamic parameters. The acquisition step improves the accuracy and real-time performance, ensures the continuity of the rock mass in the work area, and is suitable for situations where laboratory tests cannot be used, such as it is difficult to obtain a complete sample, which highlights the superiority of in-situ acquisition of rock dynamic parameters.

本发明的其他有益效果将在具体实施方式中进一步进行说明。Other beneficial effects of the present invention will be further described in the specific embodiments.

附图说明Description of drawings

图1是本发明中岩石动力学参数原位获取方法的方法流程图。Fig. 1 is a method flow chart of the method for in-situ acquisition of rock dynamic parameters in the present invention.

具体实施方式Detailed ways

下面结合附图及具体实施例对本发明做进一步阐释。The present invention will be further explained below with reference to the accompanying drawings and specific embodiments.

实施例1:Example 1:

如图1所示,本实施例提供一种岩石动力学参数原位获取方法,包括如下步骤:As shown in FIG. 1 , this embodiment provides an in-situ acquisition method for rock dynamic parameters, including the following steps:

根据钻机参数划分爆破工区内岩石分层的层位,并获取各层位的岩石物理力学参数,包括如下步骤:Divide the layers of rock layers in the blasting area according to the drilling rig parameters, and obtain the rock physical and mechanical parameters of each layer, including the following steps:

获取钻头在不同深度处的钻机参数,钻机参数包括钻头的转速、钻进速度、回转压差、风压、端阻以及摩阻比,本实施例中使用到了钻进速度、回转速度、回转压差、加压压力以及风压压力;Obtain the drilling rig parameters of the drill bit at different depths. The drilling rig parameters include the rotational speed of the drill bit, the drilling speed, the rotary pressure difference, the wind pressure, the end resistance and the friction resistance ratio. In this example, the drilling speed, the rotary speed, and the rotary pressure are used. difference, pressurized pressure and wind pressure;

根据获取的钻机参数划分爆破工区内30米深岩层的岩石分层的层位;According to the obtained drilling rig parameters, the rock layers of the 30-meter deep rock layer in the blasting work area are divided;

使用多元回归方法划分岩石分层的层位,其划分公式为:The multiple regression method is used to divide the layers of rock layers, and the division formula is:

C=-3.2v1-0.72v2+0.12p1+37.56p2+500p3+6.257C=-3.2v 1 -0.72v 2 +0.12p 1 +37.56p 2 +500p 3 +6.257

式中,C为岩石强度普氏系数;v1为钻进速度,单位为m/s;v2为回转速度,单位为r/s;p1为回转压差,单位为kPa;p2为加压压力,单位为kPa;p3为风压压力,单位为kPa;In the formula, C is the Platts coefficient of rock strength; v 1 is the drilling speed, in m/s; v 2 is the rotation speed, in r/s; p 1 is the rotary pressure difference, in kPa; p 2 is Pressurized pressure, the unit is kPa; p 3 is the wind pressure, the unit is kPa;

根据钻机参数回归得到的岩石分层的层位,一般使用普氏强度系数表征岩层分布,比如煤层岩石的普氏系数一般在2到5之间,砂岩一般在4到10之间,根据普氏系数差异将岩石分为3层;According to the layers of rock layers obtained by the regression of drilling rig parameters, the Platts strength coefficient is generally used to characterize the distribution of rock layers. For example, the Platts coefficient of coal seam rocks is generally between 2 and 5, and sandstone is generally between 4 and 10. The coefficient difference divides the rock into 3 layers;

根据钻机参数计算各层位的岩石物理力学参数,岩石物理力学参数包括岩石的密度、剪切模量以及屈服强度;Calculate the rock physical and mechanical parameters of each layer according to the drilling rig parameters. The rock physical and mechanical parameters include the density, shear modulus and yield strength of the rock;

在爆破工区内进行微测井试验,得到各层位的各第一监测点的微测井试验数据,包括如下步骤:Carry out a micro-logging test in the blasting work area to obtain the micro-logging test data of each first monitoring point in each layer, including the following steps:

根据微测井试验要求,将微测井从深到浅等分为三个区,从深到浅设置不同的雷管间隔,深区雷管间隔为2米,中区雷管间隔为1米,浅区雷管间隔为0.5米;According to the requirements of the micro-logging test, the micro-logging is divided into three areas from deep to shallow, and different detonator intervals are set from deep to shallow. The detonator interval is 0.5 meters;

在微测井周围设置十字形分布的第一监测点,单边设置10个传感器,传感器设置间隔是5米,传感器用于记录振动数据和地震波经过时间;The first monitoring point distributed in a cross shape is set around the micro-logging, and 10 sensors are set on one side, and the sensor installation interval is 5 meters. The sensors are used to record vibration data and seismic wave elapsed time;

从下到上依次激发雷管,并记录各第一监测点的微测井试验数据;Excite the detonators sequentially from bottom to top, and record the micro-logging test data of each first monitoring point;

根据各层位的岩石物理力学参数和微测井试验数据,得到各层位的弹塑性参数,包括如下步骤:According to the rock physical and mechanical parameters and micro-logging test data of each layer, the elastic-plastic parameters of each layer are obtained, including the following steps:

根据各第一监测点的微测井试验数据获取对应的地震波经过时间数据,并根据地震波经过时间数据获取第一监测点之间的地震波传播平均速度,即地震波在各层位的传播波速,公式为:The corresponding seismic wave transit time data is obtained according to the micro-logging test data of each first monitoring point, and the average seismic wave propagation speed between the first monitoring points is obtained according to the seismic wave transit time data, that is, the seismic wave propagation speed in each horizon, the formula for:

v=l/τv=l/τ

式中,v为两个第一监测点地震波传播平均速度;l为两个第一监测点之间的距离;τ为两个第一监测点的地震波经过时间间隔;In the formula, v is the average velocity of seismic wave propagation at the two first monitoring points; l is the distance between the two first monitoring points; τ is the time interval of the seismic waves passing through the two first monitoring points;

根据地震波在各层位的传播波速优化爆破工区内岩石分层的层位,得到岩石分层的优化后层位;According to the propagating wave velocity of seismic waves in each horizon, the rock layered layers in the blasting area are optimized, and the optimized rock layered layers are obtained;

各岩石分层的层位高度的获取公式为:The formula for obtaining the horizon height of each rock layer is:

Figure BDA0003424652180000071
Figure BDA0003424652180000071

式中,hi为第i个层位的高度;vi、vi+1为第i、i+1个层位的传播波速;τi为第i个层位的地震波经过时间间隔;In the formula, hi is the height of the ith horizon; vi and v i +1 are the propagating wave speeds of the ith and i+1 horizons; τ i is the time interval of the seismic wave passing through the ith horizon;

根据各优化后层位的岩石物理力学参数和对应的微测井试验数据,获取各优化后层位的弹塑性参数,弹塑性参数包括衰减系数和弹性模量,弹性模量的计算公式为:According to the rock physical and mechanical parameters of each optimized horizon and the corresponding micro-logging test data, the elastic-plastic parameters of each optimized horizon are obtained. The elastic-plastic parameters include attenuation coefficient and elastic modulus. The calculation formula of elastic modulus is:

Figure BDA0003424652180000072
Figure BDA0003424652180000072

式中,θ为弹性模量;C为岩石强度普氏系数;ρ为岩石密度开方数;In the formula, θ is the elastic modulus; C is the Platts coefficient of rock strength; ρ is the root of rock density;

在爆破工区内进行试炮激发试验,动态设置第二监测点并记录对应的监测振动数据,包括如下步骤:Carry out the test shot excitation test in the blasting work area, dynamically set the second monitoring point and record the corresponding monitoring vibration data, including the following steps:

保持药量为2kg的TNT炸药不变,在各优化后层位进行试炮激发试验,记录各第二监测点的第一试炮激发数据;Keep the TNT explosive with the dosage of 2kg unchanged, carry out the test shot excitation test at each optimized horizon, and record the first test shot excitation data of each second monitoring point;

保持优化后层位不变,使用依次为1kg、2kg、3kg的TNT炸药的不同药量进行试炮激发试验,记录各第二监测点的第二试炮激发数据;Keep the optimized horizon unchanged, use different doses of TNT explosives of 1kg, 2kg, and 3kg to carry out the test shot excitation test, and record the second test shot excitation data of each second monitoring point;

根据第一、二试炮激发数据以及岩石分层的优化后层位,动态设置第二监测点并记录对应的监测振动数据,第二监测点数量大于层位总数加2;According to the excitation data of the first and second test shots and the optimized horizon of the rock stratification, the second monitoring point is dynamically set and the corresponding monitoring vibration data is recorded. The number of the second monitoring point is greater than the total number of horizons plus 2;

根据试炮激发试验的爆源参数、第二监测点的位置数据、岩石分层的层位以及各层位的弹塑性参数,建立初始的有限元模型,包括如下步骤:According to the blast source parameters of the test shot excitation test, the position data of the second monitoring point, the layers of rock layers and the elastic-plastic parameters of each layer, an initial finite element model is established, including the following steps:

根据岩石分层的优化后层位,建立岩石力学计算模型;According to the optimized horizon of rock stratification, establish rock mechanics calculation model;

基于岩石力学计算模型,将各优化后层位的弹塑性参数作为介质力学参数,并根据试炮激发试验的爆源参数和各第二监测点的位置数据,建立初始的有限元模型;Based on the rock mechanics calculation model, the elastic-plastic parameters of each optimized horizon are taken as the medium mechanics parameters, and the initial finite element model is established according to the blast source parameters of the test shot excitation test and the position data of each second monitoring point;

使用初始的有限元模型获取各第二监测点的计算振动数据,将计算振动数据与对应的监测振动数据进行对比分析,根据对比分析结果优化初始的有限元模型,得到最优的有限元模型,包括如下步骤:Use the initial finite element model to obtain the calculated vibration data of each second monitoring point, compare and analyze the calculated vibration data with the corresponding monitoring vibration data, and optimize the initial finite element model according to the results of the comparative analysis to obtain the optimal finite element model, It includes the following steps:

使用初始的有限元模型获取当前第二监测点在当前优化后层位的计算振动数据,并将计算振动数据与对应的监测振动数据进行对比分析;Use the initial finite element model to obtain the calculated vibration data of the current second monitoring point at the currently optimized horizon, and compare and analyze the calculated vibration data with the corresponding monitored vibration data;

若对比分析结果为误差大于阈值3%,则调整当前优化后层位的弹塑性参数,重新获取该第二监测点的计算振动数据并重新进行对比分析,否则,更换至下一第二监测点进行对比分析;If the result of the comparative analysis is that the error is greater than the threshold value of 3%, adjust the elastic-plastic parameters of the currently optimized horizon, re-acquire the calculated vibration data of the second monitoring point and perform the comparative analysis again, otherwise, change to the next second monitoring point carry out comparative analysis;

若当前优化后层位的所有第二监测点均进行分析比较,则将当前优化后层位的弹塑性参数作为下一优化后层位的介质力学参数,更换至下一优化后层位进行分析比较;If all the second monitoring points of the current optimized horizon are analyzed and compared, the elastic-plastic parameters of the current optimized horizon will be used as the media mechanics parameters of the next optimized horizon, and the analysis will be performed at the next optimized horizon. Compare;

若所有优化后层位的所有第二监测点均进行分析比较,则得到最优的有限元模型;If all the second monitoring points of all the optimized horizons are analyzed and compared, the optimal finite element model will be obtained;

基于最优的有限元模型获取各层位的岩石动力学参数。The rock dynamic parameters of each horizon are obtained based on the optimal finite element model.

本发明提供一种不改变爆破工区现有岩层分布现状的岩石动力学参数原位获取方法,把钻孔作业中的钻机数据和岩层地震数据相结合的实时获取方法,简化了岩石动力学参数的获取步骤,提高了精确性和实时性,保证了工区岩体连续性,并且适用于无法使用实验室测试的情况,例如难以获得完整样本,凸显了原位获取岩石动力学参数的优越性。The present invention provides an in-situ acquisition method of rock dynamic parameters without changing the distribution status of existing rock formations in blasting work areas, and a real-time acquisition method combining drilling rig data and rock formation seismic data in drilling operations, which simplifies the analysis of rock dynamic parameters. The acquisition step improves the accuracy and real-time performance, ensures the continuity of the rock mass in the work area, and is suitable for situations where laboratory tests cannot be used, such as it is difficult to obtain a complete sample, which highlights the superiority of in-situ acquisition of rock dynamic parameters.

本发明不局限于上述可选的实施方式,任何人在本发明的启示下都可得出其他各种形式的产品。上述具体实施方式不应理解成对本发明的保护范围的限制,本发明的保护范围应当以权利要求书中界定的为准,并且说明书可以用于解释权利要求书。The present invention is not limited to the above-mentioned optional embodiments, and anyone can derive other various forms of products under the inspiration of the present invention. The above specific embodiments should not be construed as limiting the protection scope of the present invention, which should be defined in the claims, and the description can be used to interpret the claims.

Claims (10)

1. An in-situ acquisition method of rock kinetic parameters is characterized by comprising the following steps: the method comprises the following steps:
dividing the positions of rock layering in a blasting work area according to the parameters of the drilling machine, and acquiring the physical and mechanical parameters of rocks at each position;
carrying out a micro-logging test in the blasting work area to obtain micro-logging test data of each first monitoring point of each layer;
acquiring elastoplasticity parameters of each layer according to the rock physical mechanical parameters and the micro-logging test data of each layer;
carrying out a test-blasting excitation test in a blasting work area, dynamically setting a second monitoring point and recording corresponding monitoring vibration data;
establishing an initial finite element model according to the explosion source parameters of the test gun excitation test, the position data of the second monitoring point, the layer position of the rock layering and the elastoplasticity parameters of each layer position;
obtaining the calculated vibration data of each second monitoring point by using the initial finite element model, comparing and analyzing the calculated vibration data with the corresponding monitored vibration data, and optimizing the initial finite element model according to the comparison and analysis result to obtain an optimal finite element model;
and acquiring rock dynamics parameters of each layer based on the optimal finite element model.
2. The in-situ acquisition method of rock kinetic parameters according to claim 1, characterized in that: dividing the positions of rock layering in a blasting work area according to the parameters of a drilling machine, and acquiring the physical and mechanical parameters of rocks of all the positions, wherein the method comprises the following steps:
acquiring drilling machine parameters of a drill bit at different depths;
dividing the rock layering layer in the blasting work area according to the obtained drilling machine parameters;
and calculating the rock physical mechanical parameters of each layer according to the drilling machine parameters.
3. The in-situ acquisition method of rock kinetic parameters according to claim 2, characterized in that: the parameters of the drilling machine comprise the rotating speed, the drilling speed, the rotary pressure difference, the wind pressure, the end resistance and the friction-resistance ratio of the drill bit.
4. The in-situ acquisition method of rock kinetic parameters according to claim 3, characterized in that: the rock physical mechanical parameters comprise the density, the shear modulus and the yield strength of the rock.
5. The in-situ acquisition method of rock kinetic parameters according to claim 4, characterized in that: obtaining micro-logging test data of each first monitoring point of each layer, comprising the following steps:
arranging detonators in micro-logging wells at different depths according to the requirements of the micro-logging test;
arranging a plurality of monitoring points around the micro-logging;
and sequentially exciting the detonators and recording the micro-logging test data of each first monitoring point.
6. The in-situ acquisition method of rock kinetic parameters according to claim 5, characterized in that: obtaining elastic-plastic parameters of each layer, comprising the following steps:
acquiring corresponding seismic wave passing time data according to the micro-logging test data of each first monitoring point, and acquiring the propagation wave velocity of the seismic waves at each layer according to the seismic wave passing time data;
optimizing the layer position of the rock layering in the blasting work area according to the propagation wave velocity of the seismic waves at each layer position to obtain an optimized layer position of the rock layering;
and acquiring the elastoplasticity parameters of the optimized layers according to the rock physical and mechanical parameters of the optimized layers and the corresponding micro-logging test data.
7. The in-situ acquisition method of rock kinetic parameters of claim 6, characterized by comprising: the elastic-plastic parameters comprise attenuation coefficient and elastic modulus.
8. The in-situ acquisition method of rock kinetic parameters of claim 7, characterized by: dynamically setting a second monitoring point and recording corresponding monitoring vibration data, comprising the following steps:
keeping the dosage unchanged, performing a test firing excitation test on each optimized layer, and recording first test firing excitation data of each second monitoring point;
keeping the optimized layer constant, performing a test-gun excitation test by using different doses, and recording second test-gun excitation data of each second monitoring point;
and dynamically setting a second monitoring point and recording corresponding monitoring vibration data according to the first and second pilot gun excitation data and the optimized layer position of the rock layering.
9. The in-situ acquisition method of rock kinetic parameters of claim 8, characterized by: establishing an initial finite element model, comprising the following steps:
establishing a rock mechanics calculation model according to the optimized horizon of the rock layering;
and based on a rock mechanics calculation model, taking the elastoplasticity parameters of each optimized layer as medium mechanics parameters, and establishing an initial finite element model according to the explosion source parameters of the test gun excitation test and the position data of each second monitoring point.
10. The in-situ acquisition method of rock kinetic parameters of claim 9, characterized in that: obtaining an optimal finite element model, comprising the following steps:
using an initial finite element model to obtain the calculated vibration data of the current second monitoring point at the current optimized position, and comparing and analyzing the calculated vibration data with the corresponding monitored vibration data;
if the comparison analysis result is that the error is larger than the threshold value, adjusting the elastic-plastic parameters of the current optimized layer, re-acquiring the calculated vibration data of the second monitoring point and performing comparison analysis again, otherwise, replacing the second monitoring point with the next second monitoring point for comparison analysis;
if all the second monitoring points of the current optimized layer are analyzed and compared, the elastic-plastic parameters of the current optimized layer are used as the medium mechanical parameters of the next optimized layer, and the next optimized layer is replaced for analysis and comparison;
and if all the second monitoring points of all the optimized layers are analyzed and compared, obtaining the optimal finite element model.
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