{"title":"Challenges in contactless inductive flow tomography for Rayleigh--Bénard convection cells","authors":"","doi":"10.22364/mhd.58.1-2.3","DOIUrl":null,"url":null,"abstract":"Contactless inductive flow tomography (CIFT) can reconstruct the complex 3-dimensional flow structure of the large-scale circulation in liquid metal filled Rayleigh-Bénard (RB) convection cells. The method relies on the precise measurement of weak magnetic fields induced by currents in the conducting liquid arising from the fluid motion in combination with primary excitation fields. The velocity distribution is reconstructed from the magnetic field measurements by solving a linear inverse problem using the Tikhonov regularization and L-curve method. A number of technical challenges have to be overcome to reach the desired accuracy of the measurement signals. In this paper we will describe our design of a new CIFT set-up for a large RB vessel with a diameter of 320 mm and a height of 640 mm. We outline the major factors perturbing the measurement signal of several tens of nanoteslas and describe solutions to decrease mechanical drifts by thermal expansion to a sub-critical level to enable CIFT measurements for high-Rayleigh number flows. Figs 5, Refs 16.","PeriodicalId":18136,"journal":{"name":"Magnetohydrodynamics","volume":" ","pages":""},"PeriodicalIF":0.3000,"publicationDate":"2022-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Magnetohydrodynamics","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.22364/mhd.58.1-2.3","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"MECHANICS","Score":null,"Total":0}
引用次数: 2
Abstract
Contactless inductive flow tomography (CIFT) can reconstruct the complex 3-dimensional flow structure of the large-scale circulation in liquid metal filled Rayleigh-Bénard (RB) convection cells. The method relies on the precise measurement of weak magnetic fields induced by currents in the conducting liquid arising from the fluid motion in combination with primary excitation fields. The velocity distribution is reconstructed from the magnetic field measurements by solving a linear inverse problem using the Tikhonov regularization and L-curve method. A number of technical challenges have to be overcome to reach the desired accuracy of the measurement signals. In this paper we will describe our design of a new CIFT set-up for a large RB vessel with a diameter of 320 mm and a height of 640 mm. We outline the major factors perturbing the measurement signal of several tens of nanoteslas and describe solutions to decrease mechanical drifts by thermal expansion to a sub-critical level to enable CIFT measurements for high-Rayleigh number flows. Figs 5, Refs 16.
非接触式感应流动层析成像技术(CIFT)可以重建液态金属填充的rayleigh - b (RB)对流单元内复杂的大尺度循环三维流动结构。该方法依赖于精确测量由流体运动引起的导电液体中电流感应的弱磁场,并结合一次励磁场。利用Tikhonov正则化和l曲线法求解线性逆问题,重建了磁场测量的速度分布。为了达到所需的测量信号精度,必须克服许多技术挑战。在本文中,我们将描述我们为直径为320毫米,高度为640毫米的大型RB容器设计的新型CIFT装置。我们概述了干扰几十纳特斯拉测量信号的主要因素,并描述了通过热膨胀到亚临界水平来减少机械漂移的解决方案,以实现高瑞利数流的CIFT测量。图5,参考文献16。