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采用软磁非晶带材的巨型应力阻抗磁弹性传感器。

Giant Stress Impedance Magnetoelastic Sensors Employing Soft Magnetic Amorphous Ribbons.

作者信息

Beato-López Juan Jesús, Urdániz-Villanueva Juan Garikoitz, Pérez-Landazábal José Ignacio, Gómez-Polo Cristina

机构信息

Departamento de Ciencias, Universidad Pública de Navarra, 31006 Pamplona, Spain.

Institute for Advanced Materials and Mathematics INAMAT2, Universidad Pública de Navarra, 31006 Pamplona, Spain.

出版信息

Materials (Basel). 2020 May 8;13(9):2175. doi: 10.3390/ma13092175.

DOI:10.3390/ma13092175
PMID:32397310
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7254306/
Abstract

Soft magnetic amorphous alloys obtained via rapid quenching techniques are widely employed in different technological fields such as magnetic field detection, bio labeling, non-contact positioning, etc. Among them, magnetoelastic applications stand out due to excellent mechanical properties exhibited by these alloys, resulting from their amorphous structure, namely, their high Young modulus and high tensile strength. In particular, the giant stress impedance (GSI) effect represents a powerful tool to develop highly sensitive magnetoelastic sensors. This effect is based on the changes in the high-frequency electric impedance as the result of the variation in magnetic permeability of the sample under the action of mechanical stresses. In this work, the GSI effect is analyzed in two soft magnetic ribbons ((Co Fe) Si B and (Co Fe) Si B) for the subsequent development of two practical devices: (i) the characterization of the variations in the cross-section dimensions of irregularly shaped elements, and (ii) the design of a flow meter for measuring the rate of flow of water through a pipe.

摘要

通过快速淬火技术获得的软磁非晶合金被广泛应用于不同的技术领域,如磁场检测、生物标记、非接触定位等。其中,磁弹性应用因其非晶结构所展现出的优异机械性能而备受瞩目,这种结构赋予了合金高杨氏模量和高拉伸强度。特别是,巨应力阻抗(GSI)效应是开发高灵敏度磁弹性传感器的有力工具。该效应基于在机械应力作用下,样品磁导率变化导致高频电阻抗的变化。在这项工作中,对两种软磁带((Co Fe) Si B和(Co Fe) Si B)的GSI效应进行了分析,以用于后续两种实际装置的开发:(i)表征不规则形状元件横截面尺寸的变化;(ii)设计一种用于测量通过管道的水流流速的流量计。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/0341e0b7f45a/materials-13-02175-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/465ee9886af2/materials-13-02175-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/44d84371f9b4/materials-13-02175-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/ea042191adb9/materials-13-02175-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/3618af30c549/materials-13-02175-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/b9f04cdfc92d/materials-13-02175-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/55971a133cdb/materials-13-02175-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/1f19ad08f344/materials-13-02175-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/fd9dcfc1c735/materials-13-02175-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/0341e0b7f45a/materials-13-02175-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/465ee9886af2/materials-13-02175-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/44d84371f9b4/materials-13-02175-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/ea042191adb9/materials-13-02175-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/3618af30c549/materials-13-02175-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/b9f04cdfc92d/materials-13-02175-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/55971a133cdb/materials-13-02175-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/1f19ad08f344/materials-13-02175-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/fd9dcfc1c735/materials-13-02175-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5474/7254306/0341e0b7f45a/materials-13-02175-g009.jpg

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