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首页> 外文期刊>Materials Science >METHODS OF PHYSICAL SIMULATION OF ELECTROCHEMICAL PROCESSES AT THE TIP OF A CRACK
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METHODS OF PHYSICAL SIMULATION OF ELECTROCHEMICAL PROCESSES AT THE TIP OF A CRACK

机译:裂纹尖端的电化学过程的物理模拟方法

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We analyze stresses and the degree of plastic deformation at the contours of cracks of two types, namely, a sharp crack and a crack with slip lines. We show that at the tip of a crack of the second type, at the contour of the bottom-walls of the crack galvanic couple, there appear two symmetric microgalvanic couples at the slip lines. Microinhomogeneities of a metal (grain bound-aries, nonmetallic inclusions, etc.) are submicrogalvanic couples whose activity increases due to inhomogeneity of microplastic deformations of their vicinities. We distinguished the mechanisms of corrosion-cyclic fracture and corrosion-static cracking. Under cyclic loading, breaking of grains occurs and grain boundaries and nonmetallic inclusions fail, which levels the influence of currents of submicrogalvanic couples on the growth rate of a crack. Under static loading, micro- and submicrogalvanic couples are permanently operating, the cold work of the surfaces of the metal of the walls of the crack is lower than that under cyclic loading, while the difference of potentials and the current of the bottom-walls of the crack galvanic couple are greater than those under cyclic loading. 'This explains both the phenomenon of branching and the higher growth rate of a crack of corrosion-static cracking with time. In addition to the electrode potential and pH of the medium, we propose to consider the following parameters as defining factors of the growth of a crack: currents of a galvanic couple, micro-, and submicrogalvanic couples and the time of repassivation of freshly formed metal surfaces appearing in the process of the growth of a crack. According to analysis of the literature data, these parameters cannot be experimentally determined. For this reason, we propose to use methods of simulation to investigate distributions of the potentials and currents of corrosion at the tip of a crack. We propose certain structures of physical and mechanoelectrochemical models of a crack and methods for measurement of distributions of the current density and the electrode potential at their surfaces.
机译:我们分析了两种类型的裂纹轮廓处的应力和塑性变形的程度,即尖锐裂纹和带有滑移线的裂纹。我们表明,在第二种裂纹的尖端,在裂纹电偶的底壁轮廓处,在滑移线上出现了两个对称的微电偶。金属的微不均匀性(晶粒边界,非金属夹杂物等)是亚微电流偶,其活动性由于其附近的微塑性变形的不均匀性而增加。我们区分了腐蚀循环断裂和腐蚀开裂的机理。在循环载荷下,会发生晶粒破裂,晶界和非金属夹杂物破裂,这会降低亚微电流偶对电流对裂纹扩展速率的影响。在静态载荷下,微和亚微电流耦合永久性地工作,裂纹壁的金属表面的冷作比循环载荷下的低,而电势和底壁电流的差裂纹电偶大于循环载荷下的偶电偶。 ``这既解释了分支现象,又解释了随着时间的推移,防腐蚀裂纹的裂纹增长率更高。除了介质的电极电势和pH值外,我们建议考虑以下参数作为定义裂纹扩展的因素:电流偶,微电流和亚微电流偶的电流以及新形成的金属的重新钝化时间表面在裂纹扩展过程中出现。根据文献数据的分析,这些参数不能通过实验确定。因此,我们建议使用模拟方法来研究裂纹尖端处的腐蚀电位和电流的分布。我们提出了裂纹的物理和机械电化学模型的某些结构,以及在其表面测量电流密度和电极电位分布的方法。

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