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利用空间受限声致发光评估高静水压力下不同金属材料的空化侵蚀。

Cavitation erosion on different metallic materials under high hydrostatic pressure evaluated with the spatially confined sonoluminescence.

作者信息

Liu Yalu, Liu Huan, Luo Dehua, Wang Jie, Deng Chao, Zhang Mingjun, Li Chengyong, Song Dan, Li Faqi

机构信息

State Key Laboratory of Ultrasound in Medicine and Engineering, College of Biomedical Engineering, Chongqing Medical University, Chongqing 400016, China; National Engineering Research Center of Ultrasound Medicine, Chongqing 401121, China.

State Key Laboratory of Ultrasound in Medicine and Engineering, College of Biomedical Engineering, Chongqing Medical University, Chongqing 400016, China; Chongqing Key Laboratory of Biomedical Engineering, Chongqing Medical University, Chongqing 400016, China.

出版信息

Ultrason Sonochem. 2024 Jul;107:106920. doi: 10.1016/j.ultsonch.2024.106920. Epub 2024 May 23.

DOI:10.1016/j.ultsonch.2024.106920
PMID:38805885
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11154700/
Abstract

Cavitation erosion is a general phenomenon in the fields of aviation, navigation, hydraulic machinery, and so on, causing great damage to fluid machinery. With the vast requirements in deep ocean applications, it is urgent to study the mechanism of cavitation erosion and the cavitation erosion resistance of different materials under high hydrostatic pressure to predict and avoid the effect of cavitation erosion. In this work, the spatially confined cavitation bubble cloud associated with Gaussian-like intensity distribution sonoluminescence (SL) was produced by a spherically focused ultrasound transducer with two opening ends near metallic plates under different hydrostatic pressures (0.1, 3, 6, and 10 MPa). The cavitation erosion effects on copper, 17-4PH stainless steel and tungsten plates were studied. Through coupling analysis towards the SL intensity distribution, the macro/micro morphology of cavitation erosion, and the physical parameters of different metallic materials (hardness, yield strength, and melting point), it is found that with increasing hydrostatic pressure, the erosion effect is intensified, the depth of cavitation pits increases, the phenomenon of melting can be observed on materials with relatively low melting points, and the cavitation erosion experienced an evolution process from high-temperature creep to fracture. This work has also established a method for the evaluation of materials' cavitation erosion resistance with measurable SL intensity distribution, which is promising to promote the designing and selection of anti-cavitation materials in deep-sea applications.

摘要

空化侵蚀是航空、航海、水力机械等领域普遍存在的现象,会对流体机械造成严重损害。随着深海应用的大量需求,迫切需要研究空化侵蚀的机理以及不同材料在高静水压力下的抗空化侵蚀性能,以预测和避免空化侵蚀的影响。在这项工作中,通过一个两端开口的球形聚焦超声换能器,在不同静水压力(0.1、3、6和10MPa)下,在金属板附近产生了与高斯型强度分布声致发光(SL)相关的空间受限空化泡云。研究了空化侵蚀对铜、17-4PH不锈钢和钨板的影响。通过对SL强度分布、空化侵蚀的宏观/微观形态以及不同金属材料的物理参数(硬度、屈服强度和熔点)进行耦合分析,发现随着静水压力的增加,侵蚀作用增强,空化坑深度增加,在熔点相对较低的材料上可观察到熔化现象,并且空化侵蚀经历了从高温蠕变到断裂的演变过程。这项工作还建立了一种利用可测量的SL强度分布来评估材料抗空化侵蚀性能的方法,有望推动深海应用中抗空化材料的设计和选择。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/1dac391d933b/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/f7cc2eaf493f/ga1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/61dfc0c6128a/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/e1865e914811/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/8d957c62fc87/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/1d3d4a64aa62/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/937f8380d5f2/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/df8f57f07939/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/7eac848a2501/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/df8a2f165c70/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/1dac391d933b/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/f7cc2eaf493f/ga1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/61dfc0c6128a/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/e1865e914811/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/8d957c62fc87/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/1d3d4a64aa62/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/937f8380d5f2/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/df8f57f07939/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/7eac848a2501/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/df8a2f165c70/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/51c7/11154700/1dac391d933b/gr9.jpg

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