利用热电耦合技术表征金属中夹杂物

A. Nayfeh, H. Carreon, P. Nagy
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引用次数: 1

摘要

最近发现,当试样受到定向加热或冷却时,利用高灵敏度磁力计探测受影响区域周围的弱热电电流,可以以完全非接触的方式,通过热电测量无损地检测夹杂物和其他类型的不均匀性。本文提出了能够预测在外部热激励下包裹体周围热电电流产生磁场的理论模型。我们研究了要检测的磁信号如何取决于(i)宿主和包裹体的相关物理性质,(ii)包裹体的大小,(iii)磁力计的极化,(iv)磁力计与样品的上升距离,以及(v)方向和(vi)施加在样品上的外部加热或冷却强度。本文对所提出的分析模型进行了数值计算,并与实验结果进行了比较。实验结果是通过测量在外部热激励下,在传感器与试样表面之间不同的升力距离下,铜中破裂球形锡夹杂周围的热电电流产生的磁场而得到的。包裹体直径为2.4 ~ 12.7 mm,离矿距离为12 ~ 20 mm。样品中相当适中的0.7°C/cm温度梯度产生的峰值磁通密度范围为1至250 nT,可通过商用磁通门磁强计轻松测量。实验结果与我们的分析预测非常吻合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the Exploitation of Thermoelectric Coupling for Characterization of Inclusions in Metals
It was recently discovered that inclusions and other types of inhomogeneities can be nondestructively detected by thermoelectric measurements in an entirely non-contact way by using high-sensitivity magnetometers to sense the weak thermoelectric currents around the affected region when the specimen is subjected to directional heating or cooling. This paper presents theoretical models capable of predicting the magnetic field produced by thermoelectric currents around inclusions under external thermal excitation. We investigated how the magnetic signal to be detected depends on (i) the relevant physical properties of the host and the inclusion, (ii) the size of the inclusion, (iii) the polarization of the magnetometer, (iv) the lift-off distance of the magnetometer from the specimen, and the (v) direction and (vi) strength of the external heating or cooling applied to the specimen. The presented analytical model is numerically evaluated for comparison to experimental results that were obtained by measuring the magnetic field produced by thermoelectric currents around surface-breaking spherical tin inclusions in copper under external thermal excitation for different lift-off distances between the sensor and the surface of the specimen. The diameter of the inclusions and the lift-off distance varied from 2.4 to 12.7 mm and from 12 to 20 mm, respectively. A fairly modest 0.7 °C/cm temperature gradient in the specimen produced peak magnetic flux densities ranging from 1 to 250 nT, that could be easily measured by a commercial fluxgate magnetometer. The experimental results were found to be in very good agreement with our analytical predictions.
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