{"title":"Functional Capabilities of Electromagnetic-Acoustic Transformations in Current Mode in the Metal Melt","authors":"V. N. Tsurkin, A. V. Ivanov","doi":"10.3103/S1068375522030139","DOIUrl":null,"url":null,"abstract":"<p>The paper deals with a symmetric problem on the basis of physically substantiated estimates of the processes of electromagnetic-acoustic transformations (EMAT) of energy during the flow of an electric current through a melt and the key parameters of the open problem of the system “Power source parameters–Parameters of the magnetic field and magnetic pressure of the skin layer–Parameters of acoustic disturbances.” When formulating the EMAT problem in technological applications, it was shown that the key parameter is the geometry of the container with the object of processing and the material of the mold. When solving the problem, it is the parameter of the skin layer and the time dependence of the discharge current. It was established that the part of energy during the formation of the magnetic pressure in the skin layer from the amount of the energy stored in the capacitor bank of the pulse current generator is approximately 10<sup>–4</sup>–10<sup>–2</sup>. The value of this part depends on the period of the discharge current and is proportional to the <span>\\(\\sqrt T \\)</span>. When acoustic disturbances propagate in the melt, the main share of energy losses is determined by the difference in the acoustic rigidity of the melt and the shape of materials. The frequency spectra of the pressure of sound waves at the parameters selected for the analysis can cover the range of up to hundreds kHz, which is a good reason for the realization of resonance effects and the active formation of dissipative structures. Attention is focused on the fact that the EMAT effects are manifested in the melt not only under the influence of an acoustic field but also under that of an electromagnetic one in the skin layer. They are separated in time, but the acoustic field can occupy the entire volume of the melt and its effect is longer in time.</p>","PeriodicalId":49315,"journal":{"name":"Surface Engineering and Applied Electrochemistry","volume":"58 3","pages":"239 - 247"},"PeriodicalIF":1.1000,"publicationDate":"2022-06-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Surface Engineering and Applied Electrochemistry","FirstCategoryId":"1085","ListUrlMain":"https://link.springer.com/article/10.3103/S1068375522030139","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ELECTROCHEMISTRY","Score":null,"Total":0}
引用次数: 0
Abstract
The paper deals with a symmetric problem on the basis of physically substantiated estimates of the processes of electromagnetic-acoustic transformations (EMAT) of energy during the flow of an electric current through a melt and the key parameters of the open problem of the system “Power source parameters–Parameters of the magnetic field and magnetic pressure of the skin layer–Parameters of acoustic disturbances.” When formulating the EMAT problem in technological applications, it was shown that the key parameter is the geometry of the container with the object of processing and the material of the mold. When solving the problem, it is the parameter of the skin layer and the time dependence of the discharge current. It was established that the part of energy during the formation of the magnetic pressure in the skin layer from the amount of the energy stored in the capacitor bank of the pulse current generator is approximately 10–4–10–2. The value of this part depends on the period of the discharge current and is proportional to the \(\sqrt T \). When acoustic disturbances propagate in the melt, the main share of energy losses is determined by the difference in the acoustic rigidity of the melt and the shape of materials. The frequency spectra of the pressure of sound waves at the parameters selected for the analysis can cover the range of up to hundreds kHz, which is a good reason for the realization of resonance effects and the active formation of dissipative structures. Attention is focused on the fact that the EMAT effects are manifested in the melt not only under the influence of an acoustic field but also under that of an electromagnetic one in the skin layer. They are separated in time, but the acoustic field can occupy the entire volume of the melt and its effect is longer in time.
本文在对电流通过熔体时能量的电磁-声转换过程进行物理上有根据的估计和“电源参数-蒙皮层磁场和磁压参数-声扰动参数”系统开放问题的关键参数的基础上,讨论了一个对称问题。在制定工艺应用中的EMAT问题时,指出关键参数是加工对象容器的几何形状和模具的材料。在解决问题时,它是蒙皮层的参数和放电电流的时间依赖性。确定了脉冲电流发生器电容器组中存储的能量在蒙皮层磁压形成过程中所占的能量部分约为10-4-10-2。该部分的值取决于放电电流的周期,并与\(\sqrt T \)成正比。当声扰动在熔体中传播时,能量损失的主要份额由熔体的声刚度和材料形状的差异决定。所选分析参数下的声波压力频谱可以覆盖高达数百kHz的范围,这是实现共振效应和主动形成耗散结构的一个很好的理由。重点讨论了熔体中EMAT效应不仅在声场的影响下表现出来,而且在蒙皮层的电磁场的影响下也表现出来。它们在时间上是分离的,但声场可以占据熔体的整个体积,其影响时间较长。
期刊介绍:
Surface Engineering and Applied Electrochemistry is a journal that publishes original and review articles on theory and applications of electroerosion and electrochemical methods for the treatment of materials; physical and chemical methods for the preparation of macro-, micro-, and nanomaterials and their properties; electrical processes in engineering, chemistry, and methods for the processing of biological products and food; and application electromagnetic fields in biological systems.