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51.
The authors are concerned with the sharp interface limit for an incompressible Navier-Stokes and Allen-Cahn coupled system in this paper. When the thickness of the diffuse interfacial zone, which is parameterized by ε, goes to zero, they prove that a solution of the incompressible Navier-Stokes and Allen-Cahn coupled system converges to a solution of a sharp interface model in the L(L2) ∩ L2(H1) sense on a uniform time interval independent of the smal...  相似文献   
52.
In this paper, we present a unified finite volume method preserving discrete maximum principle (DMP) for the conjugate heat transfer problems with general interface conditions. We prove the existence of the numerical solution and the DMP-preserving property. Numerical experiments show that the nonlinear iteration numbers of the scheme in [24] increase rapidly when the interfacial coefficients decrease to zero. In contrast, the nonlinear iteration numbers of the unified scheme do not increase when the interfacial coefficients decrease to zero, which reveals that the unified scheme is more robust than the scheme in [24]. The accuracy and DMP-preserving property of the scheme are also veri ed in the numerical experiments.  相似文献   
53.
Based on the first-principles calculation, the effect of intercalated LiF on the contact characteristics of the interface between Au electrode and MoS2 layer is studied. It is found that adding LiF film can change the contact type between metal electrode Au and MoS2 layer from Schottky contact to ohmic contact, which is accompanied by interfacial charge transfer from LiF layer to MoS2 layer and the downward movement of d (dxy and dz2) orbital of Mo atom and p (px and py) orbital of S atom to Fermi level. And the interlayer spacing between LiF layer and Au electrode has a great impact on the interface contact characteristics. The electric field effect and stress effect of interface contact of Au, LiF and MoS2 (Au/LiF/MoS2)is more obvious than that of interface contact of Au and MoS2 (Au/MoS2). Au/LiF/MoS2 shows ohmic contact with the interlayer spacing between Au layer and LiF layer less than 3.05 Å and with the electric field less than 0.15 VÅ−1, respectively, while Au/MoS2 still shows N-type Schottky contact. These findings are helpful to control the contact resistance and have guiding significance for high performance MoS2 field effect transistor and other electronic components.  相似文献   
54.
We proposed absorbing interface conditions for the simulation of linear wave propagation on non-uniform meshes. Based on the superposition principle of second-order linear wave equations, we decompose the interface condition problem into two subproblems around the interface: for the first one the conventional artificial absorbing boundary conditions is applied, while for the second one, the local analytic solutions can be derived. The proposed interface conditions permit a two-way transmission of low-frequency waves across mesh interfaces which can be supported by both coarse and fine meshes, and perform a one-way absorption of high-frequency waves which can only be supported by fine meshes when they travel from fine mesh regions to coarse ones. Numerical examples are presented to illustrate the efficiency of the proposed absorbing interface conditions.  相似文献   
55.
运用基于密度泛函理论的第一性原理,研究掺杂W、Mo在镍基高温合金的沉淀强化γ′相分配差异的因素.通过VASP软件,建立γ′-Ni3(Al3/8Ti5/8)相的体系模型,选取非等效位置的不同阵点,计算W、Mo原子在不同位置的替代形成能,分析W、Mo在γ′相的占位倾向;计算掺杂W、Mo原子前后,界面的吸附能,研究掺杂W、Mo对相界的影响;计算W、Mo原子从γ向γ′相扩散,获得W、Mo扩散的路径与势垒.结果表明,W、Mo的掺杂优先替代γ′-Ni3(Al3/8Ti5/8)相5号Al原子,并提高相界的稳定性;分配的差异是W相比于Mo替代γ′相位置的Al原子更易形成空位,而γ相中的Ni原子较难形成空位,且逆扩散所需能量更多导致的.  相似文献   
56.
In periodontology and implantology, laser-induced cavitation has not yet been used to treat biofilm-related problems. In this study we have checked how soft tissue affects the evolution of cavitation in a wedge model representing periodontal and peri-implant pocket geometry. One side of the wedge model was composed of PDMS mimicking soft periodontal or peri-implant biological tissue, the other side was composed of glass mimicking hard tooth root or implant surface, which allowed observations of the cavitation dynamics with an ultrafast camera. Different laser pulse modalities, PDMS stiffness, and irrigants were tested for their effect on the evolution of cavitation in the narrow wedge geometry. The PDMS stiffness varied in a range that corresponds to severely inflamed, moderately inflamed, or healthy gingival tissue as determined by a panel of dentists. The results imply that deformation of the soft boundary has a major effect on the Er:YAG laser-induced cavitation. The softer the boundary, the less effective the cavitation. We show that in a stiffer gingival tissues model, photoacoustic energy can be guided and focused at the tip of the wedge model, where it enables generation of secondary cavitation and more effective microstreaming. The secondary cavitation was absent in severely inflamed gingival model tissue, but could be induced with a dual-pulse AutoSWEEPS laser modality. This should in principle increase cleaning efficiency in the narrow geometries such as those found in the periodontal and peri-implant pockets and may lead to more predictable treatment outcomes.  相似文献   
57.
Electrochemical interfaces are key structures in energy storage and catalysis. Hence, a molecular understanding of the active sites at these interfaces, their solvation, the structure of adsorbates, and the formation of solid-electrolyte interfaces are crucial for an in-depth mechanistic understanding of their function. Vibrational sum-frequency generation (VSFG) spectroscopy has emerged as an operando spectroscopic technique to monitor complex electrochemical interfaces due to its intrinsic interface sensitivity and chemical specificity. Thus, this review discusses the happy get-together between VSFG spectroscopy and electrochemical interfaces. Methodological approaches for answering core issues associated with the behavior of adsorbates on electrodes, the structure of solvent adlayers, the transient formation of reaction intermediates, and the emergence of solid electrolyte interphase in battery research are assessed to provide a critical inventory of highly promising avenues to bring optical spectroscopy to use in modern material research in energy conversion and storage.  相似文献   
58.
本文所提算法适用于二维和三维多介质流体力学两步欧拉数值方法中输运计算的混合网格(包括自由面网格)界面处理。在一个混合网格中,界面被近似地看作直线(二维)或平面(三维)。整个方法分为三步:(1)第一步,用混合网格周围的八个网格的介质面积份额(二维)或二十六个网格的介质体积份额(三维)确定界面的法线方向;第二步,用混合网格的本身的介质面积份额(二维)或体积份额(三维)确定界面的方程(位置);第三步,用此直线方程求出通过网格边界的流以及下一时刻网格的面积份额(二维)或体积份额(三维)。最后给出了用此方法所做的一些数值计算及与SLIC算法的比较。  相似文献   
59.
本文用云纹干涉法测取双材料高梁受集中载荷时沿x,y轴的位移场u,v.以其作为界面局部微区的边界条件,用有限元计算此微区内界面上的应力分量.与光弹性及全梁有限元法比较,发现局部杂交法的精度最高.  相似文献   
60.
在工程应用的很多摩擦对偶中,往往有一方是锐形的,因此,研究锐形滑块的滚动与滑动具有重要的实用意义。以锐缘硬质轮在挤压铝和软钢两种平面试样表面的滚动和滑动为研究对象,考察了两种摩擦过程中材料的受力状况和变形状况,结果表明,要在同种金属试样表面造成相同宽度的槽痕,滚动法所需要的垂直负荷比滑动法所需要的大,然而滚动法所需要的切向牵引力却比滑动法所需要的小.对两种摩擦过程中界面上的应力与材料的强度性能之关系的分析讨论指出,滚动试验中接触界面上的正应力相应于变形材料的屈服应力,因而滚动试验可以作为材料硬度的一种测量方法;滑动试验中接触界面上的剪应力相应于变形材料的流动剪应力;但滚动试验中界面剪应力与材料的流动剪应力之间,以及滑动试验中界面正应力与材料的屈服应力之间却都没有直线关系.  相似文献   
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