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李涛等:含水率对放矿松动体形态的细观影响 ·671· 化的临界值. characteristics of an isolated extraction zone in caving mining Chin J Eng,2015,37(9):1111 4结论 (孙浩,金爱兵,高永涛,等.崩落法采矿中放出体流动特性 的影响因素.工程科学学报,2015,37(9):1111) (1)处于非饱和状态的崩落矿岩散体为固一液一 [7]Chen Q F,Chen Q L,Zhong J Y,et al.Flow pattern of granular 气三相耦合场,其细观力学特性主要取决于矿岩含 ore rock in a single funnel under a flexible isolation laver.Chin I 水率. Eng,2016,38(7):893 (2)基于非牛顿流体格子波尔兹曼法一离散元 (陈庆发,陈青林,仲建宇,等。柔性隔离层下单漏斗散体矿 岩流动规律.工程科学学报,2016,38(7):893) 法耦合修正方程建立自然崩落法放矿模型,ω=0时 8] Chen Q F,Chen Q L,Zhong J Y,et al.Evolution law of interface 模型计算结果的拟合优度接近于1,验证了计算模 morphology of flexible isolation layer under ore drawing from single 型的准确性及可靠性,同时也为放矿理论研究提供 funnel.Chin J Nonferrous Met,2016,26(6):1332 了一种新的研究手段. (陈庆发,陈青林,仲建宇,等。单漏斗放矿柔性隔离层界面 (3)不同含水率时,矿岩细颗粒流的速度分布 形态演化规律.中国有色金属学报,2016,26(6):1332) [9]Wu A X,Sun Y Z.Granular Dynamic Theory and its Application. 均呈沿放矿口轴线逐渐向两侧减小的趋势,且放矿 Beijing:Metallurgical Industry Press,2007 口处颗粒流动速度最大:含水率由0至15%逐渐增 [10]Campbell C S.Granular material flows-n overview.Pouder 大时,放矿场内颗粒流动速度呈现先减小后增大的 Technol,2006,162(3):208 趋势. [11]Ketterhagen W R,Curtis J S,Wassgren C R,et al.Modeling (4)在不同含水率情况下,Hz均随矿岩放出质 granular segregation in flow from quasi-hree-dimensional,wedge- 量分数的增加而增大,在矿岩放出质量分数为0~ shaped hoppers.Pouder Technol,2008,179(3):126 [12]Wang H J,Yin S H,Wu A X,et al.Experimental study of the 15%时,H增长率呈指数形式增长,随后呈线性形 factors affecting the ore flow mechanism during block caving. 式增长;在同等矿岩放出量时,放矿松动体高度随含 China Unir Min Technol,2010,39(5):693 水率的增大呈先增大后减小的趋势 (王洪江,尹升华,吴爱祥,等。崩落矿岩流动特性及影响因 (5)含水率对放矿松动体形态影响显著.在同 素实验研究.中国矿业大学学报,2010,39(5):693) 等矿岩放出质量分数情况下,随着含水率ω的增 [13]Zhang C Y,Cao P,Fan X,et al.Hopper discharge experiment for high viscosity bauxite flow and micromechanics research.Rock 大,放矿松动体先逐渐变为细长型再逐渐恢复,且放 Soil Mech,2012,33(6):1653 矿松动体形态变化的含水率临界值在10%左右. (张春阳,曹平,范祥,等.高黏性铝土矿放矿流动性试验与 微观力学研究.岩土力学,2012,33(6):1653) 参考文献 14]Pierce M E.A Model for Grarity Flow of Fragmented Rock in [Li T,Wu A X,Han B,et al.Discrete element method study on Block Caring Mines [Dissertation].Queensland:University of the percolation process of fine particles in ore drawing by the block Queensland,2010 caving method.Chin J Eng,2016,38(11):1509 15]Cundall PA.A computer model for simulating progressive large- (李涛,吴爱祥,韩斌,等.基于离散元理论的自然榭落法放 scale movements in block rock mechanics /Proceedings of the 矿细颗粒渗移过程研究.工程科学学报,2016,38(11): Symposium of the International Society of Rock Mechanics.Nancy, 1509) 1971:129 Melo F,Vivanco F,Fuentes C.Calculated isolated extracted and 6] Leonardi CR.Development of a Computational Framework Cou- movement zones compared to sealed models for block caving.t pling the Non-Neutonian Lattice Bolzmann Method and the Dis- Rock Mech Min Sci,2009,46(4):731 crete Element Method with Application to Block Caring [Disserta- B3]Castro R,Trueman R,Halim A.A study of isolated draw zones in tion].Swansea:Swansea University,2009 block caving mines by means of a large 3D physical model.Int I [17]Han K,Feng Y T,Owen D R J.Coupled lattice Boltzmann and Rock Mech Min Sci,2007,44(6):860 discrete element modelling of fuid-particle interaction problems 4]Vivanco F,Watt T,Melo F.The 3D shape of the loosening zone Comput Struct,2007,85(11-4):1080 above multiple draw points in block caving through plasticity model [18]Han Y H,Cundall P.Verification of two-dimensional LBM- with a dilation front.Int J Rock Mech Min Sci,2011,48 (3):406 DEM coupling approach and its application in modeling episodic [5]Zhu ZC,Wu A X,Xi Y.Analysis on influence of water content sand production in borehole.Petroleum,2017,3(2):179 on the flowing property of bulk ore-rock.Min Res Dev,2006,26 [19]MeMinn J.Identifying soils by a triangle based on unified soil (6):23 classification system /Papers on Soils 1959 Meetings.West (朱志根,吴爱祥,习泳.含水量对矿岩散体流动特性影响分 Conshohocken,1960:369 析.矿业研究与开发,2006,26(6):23) 220]Sun QC,Wang GQ.Introduction to the Mechanics of Granular 6]Sun H,Jin A B,Gao Y T,et al.Influencing factors on the flow Material.Beijing:Science Press,2009李 涛等: 含水率对放矿松动体形态的细观影响 化的临界值. 4 结论 ( 1) 处于非饱和状态的崩落矿岩散体为固--液-- 气三相耦合场,其细观力学特性主要取决于矿岩含 水率. ( 2) 基于非牛顿流体格子波尔兹曼法--离散元 法耦合修正方程建立自然崩落法放矿模型,ω = 0 时 模型计算结果的拟合优度接近于 1,验证了计算模 型的准确性及可靠性,同时也为放矿理论研究提供 了一种新的研究手段. ( 3) 不同含水率时,矿岩细颗粒流的速度分布 均呈沿放矿口轴线逐渐向两侧减小的趋势,且放矿 口处颗粒流动速度最大; 含水率由 0 至 15% 逐渐增 大时,放矿场内颗粒流动速度呈现先减小后增大的 趋势. ( 4) 在不同含水率情况下,HIMZ均随矿岩放出质 量分数的增加而增大,在矿岩放出质量分数为 0 ~ 15% 时,HIMZ增长率呈指数形式增长,随后呈线性形 式增长; 在同等矿岩放出量时,放矿松动体高度随含 水率的增大呈先增大后减小的趋势. ( 5) 含水率对放矿松动体形态影响显著. 在同 等矿岩放出质量分数情况下,随着含水率 ω 的增 大,放矿松动体先逐渐变为细长型再逐渐恢复,且放 矿松动体形态变化的含水率临界值在 10% 左右. 参 考 文 献 [1] Li T,Wu A X,Han B,et al. Discrete element method study on the percolation process of fine particles in ore drawing by the block caving method. Chin J Eng,2016,38( 11) : 1509 ( 李涛,吴爱祥,韩斌,等. 基于离散元理论的自然崩落法放 矿细颗粒渗移过程研究. 工 程 科 学 学 报,2016,38 ( 11 ) : 1509) [2] Melo F,Vivanco F,Fuentes C. Calculated isolated extracted and movement zones compared to scaled models for block caving. Int J Rock Mech Min Sci,2009,46( 4) : 731 [3] Castro R,Trueman R,Halim A. A study of isolated draw zones in block caving mines by means of a large 3D physical model. Int J Rock Mech Min Sci,2007,44( 6) : 860 [4] Vivanco F,Watt T,Melo F. The 3D shape of the loosening zone above multiple draw points in block caving through plasticity model with a dilation front. Int J Rock Mech Min Sci,2011,48( 3) : 406 [5] Zhu Z G,Wu A X,Xi Y. Analysis on influence of water content on the flowing property of bulk ore-rock. Min Res Dev,2006,26 ( 6) : 23 ( 朱志根,吴爱祥,习泳. 含水量对矿岩散体流动特性影响分 析. 矿业研究与开发,2006,26( 6) : 23) [6] Sun H,Jin A B,Gao Y T,et al. Influencing factors on the flow characteristics of an isolated extraction zone in caving mining. Chin J Eng,2015,37( 9) : 1111 ( 孙浩,金爱兵,高永涛,等. 崩落法采矿中放出体流动特性 的影响因素. 工程科学学报,2015,37( 9) : 1111) [7] Chen Q F,Chen Q L,Zhong J Y,et al. Flow pattern of granular ore rock in a single funnel under a flexible isolation layer. Chin J Eng,2016,38( 7) : 893 ( 陈庆发,陈青林,仲建宇,等. 柔性隔离层下单漏斗散体矿 岩流动规律. 工程科学学报,2016,38( 7) : 893) [8] Chen Q F,Chen Q L,Zhong J Y,et al. Evolution law of interface morphology of flexible isolation layer under ore drawing from single funnel. Chin J Nonferrous Met,2016,26( 6) : 1332 ( 陈庆发,陈青林,仲建宇,等. 单漏斗放矿柔性隔离层界面 形态演化规律. 中国有色金属学报,2016,26( 6) : 1332) [9] Wu A X,Sun Y Z. Granular Dynamic Theory and its Application. Beijing: Metallurgical Industry Press,2007 [10] Campbell C S. Granular material flows-an overview. Powder Technol,2006,162( 3) : 208 [11] Ketterhagen W R,Curtis J S,Wassgren C R,et al. Modeling granular segregation in flow from quasi-three-dimensional,wedge￾shaped hoppers. Powder Technol,2008,179( 3) : 126 [12] Wang H J,Yin S H,Wu A X,et al. Experimental study of the factors affecting the ore flow mechanism during block caving. J China Univ Min Technol,2010,39( 5) : 693 ( 王洪江,尹升华,吴爱祥,等. 崩落矿岩流动特性及影响因 素实验研究. 中国矿业大学学报,2010,39( 5) : 693) [13] Zhang C Y,Cao P,Fan X,et al. Hopper discharge experiment for high viscosity bauxite flow and micromechanics research. Rock Soil Mech,2012,33( 6) : 1653 ( 张春阳,曹平,范祥,等. 高黏性铝土矿放矿流动性试验与 微观力学研究. 岩土力学,2012,33( 6) : 1653) [14] Pierce M E. A Model for Gravity Flow of Fragmented Rock in Block Caving Mines [Dissertation]. Queensland: University of Queensland,2010 [15] Cundall P A. A computer model for simulating progressive large￾scale movements in block rock mechanics / / Proceedings of the Symposium of the International Society of Rock Mechanics. Nancy, 1971: 129 [16] Leonardi C R. Development of a Computational Framework Cou￾pling the Non-Newtonian Lattice Boltzmann Method and the Dis￾crete Element Method with Application to Block Caving [Disserta￾tion]. Swansea: Swansea University,2009 [17] Han K,Feng Y T,Owen D R J. Coupled lattice Boltzmann and discrete element modelling of fluid-particle interaction problems. Comput Struct,2007,85( 11-14) : 1080 [18] Han Y H,Cundall P. Verification of two-dimensional LBM-- DEM coupling approach and its application in modeling episodic sand production in borehole. 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