1.江苏大学土木工程与力学学院,江苏 镇江 212013
2.江南大学机械工程学院,江苏 无锡 214122
3.中国地震局地球物理研究所,北京 100081
周恩全(1986—),男,副教授,博士。主要从事土动力学及环境岩土方面的研究工作。E-mail:enquan1986@126.com
收稿:2022-07-24,
修回:2022-09-17,
纸质出版:2024-04-25
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周恩全,姚缘,王龙等.基于粒间接触关系的饱和砂土液化特性研究[J].防灾减灾工程学报,2024,44(02):450-458.
ZHOU Enquan,YAO Yuan,WANG Long,et al.Study on Liquefaction Characteristics of Saturated Sand Based on Inter⁃particle Contact[J].Journal of Disaster Prevention and Mitigation Engineering,2024,44(02):450-458.
周恩全,姚缘,王龙等.基于粒间接触关系的饱和砂土液化特性研究[J].防灾减灾工程学报,2024,44(02):450-458. DOI: 10.13409/j.cnki.jdpme.20220724004.
ZHOU Enquan,YAO Yuan,WANG Long,et al.Study on Liquefaction Characteristics of Saturated Sand Based on Inter⁃particle Contact[J].Journal of Disaster Prevention and Mitigation Engineering,2024,44(02):450-458. DOI: 10.13409/j.cnki.jdpme.20220724004.
为了研究饱和砂土的液化机理,通过等体积加载的方式建立了循环荷载下饱和砂土动力响应的颗粒流计算模型,研究了饱和砂土在不同围压和加载幅值下的动力响应,探讨了颗粒间力链的发展特性,并从Shannon熵、Boltzmann熵以及Clausius熵的基本关系入手,建立基于粒间接触力链的饱和砂土颗粒熵计算方法,分析了颗粒熵发展特性。结果表明:饱和砂土初始总力链主要受围压的影响,围压越大,初始总力链越多;循环荷载下饱和砂土颗粒间力链总数逐渐降低,且强力链持续向中、弱力链转换;循环荷载下饱和砂土颗粒熵表现出先升高后降低的二阶段特性,围压和加载幅值对颗粒熵峰值无明显影响,各工况的颗粒熵峰值均为0.92;定义颗粒熵峰值为相变颗粒熵,相变颗粒熵时的饱和砂土表现出固液临界态的力学特征,指示了饱和砂土由固态向往返液化状态转变的临界点。
In order to study the liquefaction mechanism of saturated sand
a particle flow calculation model was developed to investigate its dynamic response under cyclic loading using isochoric loading. The study examined the dynamic response of saturated sand under different confining pressures and loading amplitudes
exploring the development characteristics of inter-particle force chains. Using the basic relationships of Shannon entropy
Boltzmann entropy
and Clausius entropy
a method for calculating particle entropy in saturated sand was established based on inter-particle force chains. The development characteristics of particle entropy in saturated sand were analyzed. The results showed that the total number of initial force chains in saturated sand was primarily influenced by confining pressure and increased with higher pressure. Under cyclic loading
the total number of force chains between saturated sand particles gradually decreased
with strong force chains transitioning to medium and weak force chains. The particle entropy of saturated sand exhibited a two-phase characteristic
initially increasing and then decreasing. Confining pressure and loading amplitude had no significant effect on the particle entropy peak value
which was 0.92 under different cases. The peak value of particle entropy was defined as the phase-change particle entropy. The saturated sand with phase-change particle entropy showed mechanical characteristics at the solid-liquid critical state
indicating the transition of saturated sand from a solid state to a cyclic liquefaction state.
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