岩土力学 ›› 2023, Vol. 44 ›› Issue (S1): 186-196.doi: 10.16285/j.rsm.2022.0926

• 基础理论与实验研究 • 上一篇    下一篇

冲击荷载下全尾砂胶结充填体断裂特性与能耗特征分析

姜明归1, 2,孙伟1, 2,李金鑫1, 2,樊锴1, 2,刘增1, 2   

  1. 1. 昆明理工大学 国土资源工程学院,云南 昆明 650093; 2. 云南理工大学 云南省中?德蓝色矿山与特殊地下空间开发利用重点实验室,云南 昆明 650093
  • 收稿日期:2022-06-14 接受日期:2022-10-12 出版日期:2023-11-16 发布日期:2023-11-16
  • 通讯作者: 孙伟,男,1983年生,博士,教授,博士生导师,主要从事膏体充填及矿山废弃资源化方面的研究工作。E-mail:kmustsw@qq.com E-mail:2794004201@qq.com
  • 作者简介:姜明归,男,1997年生,博士研究生,主要从事膏体充填绿色开采等方面的研究工作。
  • 基金资助:
    国家自然科学基金(No. 51964023);云南省重大科技项目(No. 202202AG050014);云南省基础研究计划(No. 202101BE070001–038,No. 202201AT070146)

Analysis of fracture characteristics and energy consumption of full tailings cemented backfill under impact load

JIANG Ming-gui1,2, SUN Wei1,2, LI Jin-xin1,2, FAN Kai1,2, LIU Zeng1,2   

  1. 1. Faculty of Land and Resources Engineering, Kunming University of Science and Technology, Kunming, Yunnan 650093, China; 2. Yunnan Key Laboratory of Sino-German Blue Mining and Utilization of Special Underground Space, Kunming University of Science and Technology, Kunming, Yunnan 650093, China
  • Received:2022-06-14 Accepted:2022-10-12 Online:2023-11-16 Published:2023-11-16
  • Supported by:
    This work was supported by the National Natural Science Foundation of China (51964023), the Yunnan Major Scientific and Technological Projects (202202AG050014) and the Yunnan Fundamental Research Projects (202101BE070001-038, 202201AT070146).

摘要: 为研究冲击荷载作用下全尾砂胶结充填体断裂特性及能耗特征,借助分离式霍普金森压杆(split Hopkinson pressure bar,SHPB)试验系统,开展中等应变率下不同灰砂比充填体的单轴冲击试验。结果表明:灰砂比相同时,充填体的峰前应变能、吸收能、峰前应变能密度及吸能密度均随入射能的增加呈指数函数递增规律;当入射能小于16 J时,灰砂比为1︰6的充填体的吸能密度、峰前应变能密度、吸收能及峰前应变能比灰砂比1︰4与1︰8的更大;相同峰值强度、入射能、峰前应变能及吸收能下,充填体的断裂韧度均随灰砂比的增大而逐渐增大;充填体的断裂韧度随着动态峰值强度、吸能密度及峰前应变能密度的增加呈线性增长,而随着入射能、峰前应变能及吸收能的增加呈指数函数递增规律,灰砂比为1︰4的充填体断裂韧度随吸能密度、峰前应变能密度的增幅是灰砂比为1︰6和1︰8的2~3倍;基于应变能密度、能耗与应变的增长规律,可将充填体的损伤破坏演化过程划分为非线性压密、线弹性变形、弹塑性变形、峰后破坏4个阶段;通过对充填体试验结果回归分析,从能耗角度得出充填体断裂韧度的计算公式,可为井下充填体的稳定性分析提供参考。

关键词: 充填体, 断裂韧度, 能量耗散, 冲击荷载, 应变能密度, 吸能密度

Abstract: In order to study the fracture characteristics and energy consumption characteristics of the fully tailings cemented backfill under impact loading, uniaxial impact tests on fillers with different cement-sand ratios at moderate strain rates were carried out with the help of a split Hopkinson pressure bar (SHPB) test system. The results show that the pre-peak strain energy, absorbed energy, prepeak strain energy density and absorbed energy density of the backfill body all increase exponentially as increase of incident energy when the cement-sand ratio is the same. When the incident energy is less than 16 J, the absorbed energy density, pre-peak strain energy density, absorbed energy and pre-peak strain energy of the backfill body with the cement-sand ratio of 1:6 are greater than those of the cement-sand ratio of 1:4 and 1:8. The fracture toughness of the backfill body gradually grows with the increase of the cement-sand ratio for the same peak strength, incident energy, pre-peak strain energy and absorption energy. The fracture toughness of the backfill body increases linearly with the increase of dynamic peak strength, absorbed energy density and pre-peak strain energy density, and increases exponentially with the increase of incident energy, pre-peak strain energy and absorbed energy. The increase of fracture toughness with energy absorption density and pre-peak strain energy density of the filled body with cement -sand ratio of 1:4 is two to three times that of cement-sand ratios of 1:6 and 1:8. Based on the growth law of strain energy density, energy consumption and strain, the damage and failure evolution process of the backfill can be divided into four stages: nonlinear compression, linear elastic deformation, elasto-plastic deformation and post-peak damage. Through regression analysis of the backfill body test results, a calculation formula for the fracture toughness is derived from the perspective of energy consumption, which can provide a reference for the stability analysis of the underground backfill body.

Key words: back fill body, fracture toughness, energy dissipation, impact load, strain energy density, energy absorption density

中图分类号: TU 452
[1] 李晓锋, 李海波, 刘黎旺, 傅帅旸, . 冲击荷载作用下岩石动态拉伸破坏特征及细观机制[J]. 岩土力学, 2025, 46(8): 2387-2398.
[2] 姜立春, 李金柱, 李萍丰, 陈俊豪, . 顶板垮塌激励下多中段空区底板响应特征研究[J]. 岩土力学, 2025, 46(3): 916-929.
[3] 薛熠, 杨博鹍, 刘勇, 孙强, 张云, 曹正正, . 液氮循环冷冲击作用下高温花岗岩I型断裂特性研究[J]. 岩土力学, 2025, 46(2): 422-436.
[4] 张凌博, 孙宜松, 程星磊, 郭群录, 赵川, 刘京红. 基于损伤能量耗散的三维土体切削破坏面表征方法研究[J]. 岩土力学, 2025, 46(11): 3626-3636.
[5] 卢正, 李梦威, 唐楚轩, 胡智, 赵阳, 则志辉, 姚海林, . 考虑不同级配影响的填石路基压实质量评价研究[J]. 岩土力学, 2025, 46(11): 3346-3354.
[6] 郑可跃, 施成华, 娄义黎, 贾朝军, 雷明锋, 杨益, . 深部高地应力隧道开挖卸荷围岩能量计算方法及演化机制[J]. 岩土力学, 2025, 46(1): 165-177.
[7] 杨科, 于祥, 何祥, 侯永强, 张连富, . 不同含水状态矸石胶结充填体能量演化与损伤特性研究[J]. 岩土力学, 2025, 46(1): 26-42.
[8] 李顺群, 蔡田明, 张勋程, 张丙坤, 杨长松, 周光毅, 周燕, . 冲击荷载作用下非饱和场地的三维应力响应[J]. 岩土力学, 2024, 45(S1): 477-484.
[9] 王磊, 杨震宇, 陈礼鹏, 王勇, 张帅, 王安铖, 李伟利, . 不同超临界CO2浸蚀时间后冲击煤体能量演化与破坏特征[J]. 岩土力学, 2024, 45(8): 2251-2262.
[10] 王智德, 钱梦凡, 李杰, 司莹莹, 江俐敏, . 高应变率冲击荷载下节理花岗岩损伤机制研究[J]. 岩土力学, 2024, 45(7): 1917-1928.
[11] 金丹丹, 鲁先东, 王炳辉, 施展, 张雷, . 冲击荷载下含夹层饱和砂土孔压变化规律分析[J]. 岩土力学, 2024, 45(4): 1081-1091.
[12] 张宪尚, 文光才, 朱哲明, 隆清明, 刘杰, . 冲击荷载下充填节理岩体I型裂纹动态扩展特性研究[J]. 岩土力学, 2024, 45(2): 396-406.
[13] 徐文彬, 赵康奇, 张亚伦, 刘成保, 周磊, . 调控层胶结充填体三轴压缩力学性能及破坏特征研究[J]. 岩土力学, 2024, 45(12): 3658-3667.
[14] 乔兰, 尹雅, 李庆文, 苗淼, . 碳化硅增强相变充填体热力学性能研究[J]. 岩土力学, 2024, 45(12): 3624-3634.
[15] 贾鹏, 郤保平, 李晓科, 解瑾, 蔡佳豪, 高鹏利, . 花岗岩非稳态传热破坏过程能量演变规律研究[J]. 岩土力学, 2024, 45(10): 3013-3023.
Viewed
Full text


Abstract

Cited

  Shared   
  Discussed   
No Suggested Reading articles found!