针对混凝土、岩石等脆性材料,利用热传导和热-力耦合的相关理论,并结合材料在细观尺度上的损伤演化规律,提出了一种考虑损伤的热-力耦合模型,并在原有材料破坏过程分析系统RFPA(Realistic Failure Process Analysis)模型的基础上建立了...针对混凝土、岩石等脆性材料,利用热传导和热-力耦合的相关理论,并结合材料在细观尺度上的损伤演化规律,提出了一种考虑损伤的热-力耦合模型,并在原有材料破坏过程分析系统RFPA(Realistic Failure Process Analysis)模型的基础上建立了脆性材料热破裂过程分析的数值模拟方法。该方法考虑了脆性材料在细观层次上力学性质的非均匀性(包括强度、弹模、传导系数等),并通过统计分布函数建立了宏、细观力学性能之间的联系。对不同均匀程度材料的数值模拟结果表明:材料的非均匀性对热传导规律、热应力分布以及热破坏模式有较大的影响。材料热力学性质的非均匀性加剧了材料内部热应力分布的非均匀性,这是致使非均匀材料热破裂的一个重要因素。对稳态和瞬态热传导两种条件下的脆性介质破裂过程模拟分析表明,考虑瞬态热传导计算所得到的破裂区小于相同条件下稳态热传导所得到的结果,表明在热破裂过程分析中,应注重考虑瞬态热传导对破裂过程的影响。展开更多
The transient heat conduction in both armchair and zigzag-edged graphene ribbons pulsed by local heating with a duration of 1 ps was studied using nonequilibrium molecular dynamics simulations. The results show that t...The transient heat conduction in both armchair and zigzag-edged graphene ribbons pulsed by local heating with a duration of 1 ps was studied using nonequilibrium molecular dynamics simulations. The results show that the heat pulse excites two waves which indicates non-Fourier heat conduction. One of the two waves is a sound wave(first sound), which has macroscopic momentum and propagates at the speed of sound. The other is a thermal wave(second sound), whose propagation speed is 1=ffiffi3pof the sound velocity. The sound wave excited by the heat pulse is a longitudinal wave, whose energy is only transported in the longitudinal direction. The thermal wave excited by the heat pulse is generated by transverse lattice vibrations, with the energy only having the transverse component. The observed anisotropy of the transient heat conduction suggests that the system is in a non-equilibrium state during propagation of the heat pulse. Further statistical analyses show that the displacement of the heat pulse energy is related to the time as hr2 i / t1:80, which implies that heat transport is ballistic-diffusive transport in graphene. The higher proportion of the ballistic transport will lead to stronger heat waves. At the crest of the thermal wave, energy is transported ballistically, while in the diffusive region and during attenuation of the thermal wave,the energy is transported diffusively.展开更多
文摘针对混凝土、岩石等脆性材料,利用热传导和热-力耦合的相关理论,并结合材料在细观尺度上的损伤演化规律,提出了一种考虑损伤的热-力耦合模型,并在原有材料破坏过程分析系统RFPA(Realistic Failure Process Analysis)模型的基础上建立了脆性材料热破裂过程分析的数值模拟方法。该方法考虑了脆性材料在细观层次上力学性质的非均匀性(包括强度、弹模、传导系数等),并通过统计分布函数建立了宏、细观力学性能之间的联系。对不同均匀程度材料的数值模拟结果表明:材料的非均匀性对热传导规律、热应力分布以及热破坏模式有较大的影响。材料热力学性质的非均匀性加剧了材料内部热应力分布的非均匀性,这是致使非均匀材料热破裂的一个重要因素。对稳态和瞬态热传导两种条件下的脆性介质破裂过程模拟分析表明,考虑瞬态热传导计算所得到的破裂区小于相同条件下稳态热传导所得到的结果,表明在热破裂过程分析中,应注重考虑瞬态热传导对破裂过程的影响。
基金supported by the National Natural Science Foundation of China (51322603, 51136001, 51356001)the Science Fund for Creative Research Groups (51321002)+2 种基金the Program for New Century Excellent Talents in UniversityTsinghua University Initiative Scientific Research Programthe Tsinghua National Laboratory for Information Science and Technology of China
文摘The transient heat conduction in both armchair and zigzag-edged graphene ribbons pulsed by local heating with a duration of 1 ps was studied using nonequilibrium molecular dynamics simulations. The results show that the heat pulse excites two waves which indicates non-Fourier heat conduction. One of the two waves is a sound wave(first sound), which has macroscopic momentum and propagates at the speed of sound. The other is a thermal wave(second sound), whose propagation speed is 1=ffiffi3pof the sound velocity. The sound wave excited by the heat pulse is a longitudinal wave, whose energy is only transported in the longitudinal direction. The thermal wave excited by the heat pulse is generated by transverse lattice vibrations, with the energy only having the transverse component. The observed anisotropy of the transient heat conduction suggests that the system is in a non-equilibrium state during propagation of the heat pulse. Further statistical analyses show that the displacement of the heat pulse energy is related to the time as hr2 i / t1:80, which implies that heat transport is ballistic-diffusive transport in graphene. The higher proportion of the ballistic transport will lead to stronger heat waves. At the crest of the thermal wave, energy is transported ballistically, while in the diffusive region and during attenuation of the thermal wave,the energy is transported diffusively.
