Parametric simulation of Induction Thermography for optimal cracks detection and characterization

Ghibaudo Olivier, Foucher Fabrice, Kalai Anouar
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Abstract

In the last few years, induction thermography has been identified as a non-destructive testing method for detecting and characterizing surface cracks in metals. The sample to be inspected is heated with a short induced electrical current pulse, and the infrared camera records the temperature distribution and transient temporal behavior at the surface during and after the heating pulse. In this work, 3D Finite element simulations, performed with the software FLUX©, were carried out to investigate how the thermal contrast depends on parameters such as excitation frequency, pulse duration, material parameters, crack depth and length. 1. Simulation description To compare the simulations with the experimental results, the modeled inductor is a realistic U-ferritic yoke surmounted by a copper winding. The two block samples involve two materials massively used in aeronautics: the first one is paramagnetic (nickel based superalloy INCONEL 718), the second one is ferromagnetic (low carbon steel 16CND13), which implies very different skin depths. The magnetic excitation frequency varies between 10 kHz and 600 kHz, and the step heating duration between 10 to 100 ms. Also, the length of the notch varies between 0.2 mm to 5 mm and the depth between 0.1 to 5 mm. A total of 360 configurations have been simulated. The multiphysical simulations take into account the non-linearity of the sample magnetic permeabilities, which makes it possible to calculate finely the total impedance of the inductor at each magnetic frequency. For a current imposed excitation through the inductor, this allows to normalize the observations with respect to the active and reactive power consumed by the inductor. (a) (b) (c) Fig. 1. (a) : Real inductor from Edevis©. (b) : schematic view of the problem : in green the ferrite of the inductor, in blue the plate sample, in red the defect (notch). (c) cross section of the mesh problem. (a) (b) (c) (d) Fig. 2. (a) : Simulation results : temperature distribution on the surface of Inconel sample at t=100 ms and fmag=100 kHz. (b) : without defect. (c) defect height=0.5 mm and length=2.5 mm. (d) : defect height=2 mm and length=2.5 mm. 10.21611/qirt.2020.076 15 Quantitative InfraRed Thermography Conference, 6 – 10 July 2020, Porto, Portugal 2 2. Signal analysis From the temperature distributions at each time step, the analysis of the differential thermal contrast between a defect situation and a defect-free situation, emphasizes the detectability of the defect as a function of the introduced parametric variations. The thermal-temporal extractions provided are used firstly to find the optimal excitation parameters (frequency of the induced currents, heating duration) which maximizes the thermal contrast, and on the other hand to define a methodology for sizing defects according to their lengths and depths. The optimum contrast calculated on the phase of the Fourier Transform (Pulse Phase Thermography PPT) provides credible but sensitive information related to the excitation parameters and the geometric parameters of the defects. In the final paper, two methods of analysis will be compared: the PPT and the wavelet pulsed phased thermography. Fig. 3. Temporal variation and phase of the Fast Fourier Transform for different excitation and defects parameters. The data are computed on a point localized at the surface nearby the orthogonal axis of the defect. The optimal analysis frequency of the FFT fopt wich maximize the differential contrast, varies with the step heating duration and the size of the defect. 10.21611/qirt.2020.076
感应热成像的参数化模拟,用于最佳的裂纹检测和表征
在过去的几年中,感应热成像已被确定为一种无损检测方法,用于检测和表征金属表面裂纹。用短脉冲感应电流加热待测样品,红外摄像机记录加热脉冲期间和之后样品表面的温度分布和瞬态时间行为。在这项工作中,使用FLUX©软件进行了三维有限元模拟,以研究热对比如何依赖于激励频率、脉冲持续时间、材料参数、裂纹深度和长度等参数。1. 为了将模拟结果与实验结果进行比较,模拟的电感器是一个真实的u -铁素体轭,上面有一个铜绕组。这两个块样品涉及航空领域大量使用的两种材料:第一个是顺磁性的(镍基高温合金INCONEL 718),第二个是铁磁性的(低碳钢16CND13),这意味着非常不同的蒙皮深度。磁激励频率在10khz ~ 600khz之间,步进加热时间在10 ~ 100ms之间。此外,缺口的长度在0.2毫米至5毫米之间变化,深度在0.1至5毫米之间变化。总共模拟了360种配置。多物理场模拟考虑了样品磁导率的非线性,从而可以精确地计算出电感器在各个磁频下的总阻抗。对于通过电感施加的励磁电流,这允许对电感消耗的有功和无功功率进行归一化观察。(a) (b) (c)图1(a):来自Edevis的真实电感©。(b):问题示意图:绿色为电感的铁氧体,蓝色为板样,红色为缺陷(缺口)。(c)网格问题的横截面。(a) (b) (c) (d)(a):仿真结果:t=100 ms, fmag=100 kHz时,Inconel试样表面温度分布。(b):无缺陷。(c)缺陷高度=0.5 mm,长度=2.5 mm。(d)缺陷高度= 2mm,长度=2.5 mm。10.21611/qirt.2020.076 15定量红外热成像会议,2020年7月6 - 10日,波尔图,葡萄牙2。信号分析从每个时间步长的温度分布,分析缺陷情况和无缺陷情况之间的热差对比,强调缺陷的可检测性是引入参数变化的函数。所提供的热时间提取首先用于找到最佳的激励参数(感应电流的频率,加热持续时间),使热对比度最大化,另一方面定义了根据其长度和深度确定缺陷尺寸的方法。根据傅里叶变换(脉冲相位热成像PPT)的相位计算的最佳对比度提供了与激励参数和缺陷几何参数相关的可靠而敏感的信息。最后,本文将比较两种分析方法:PPT和小波脉冲相控热成像。图3所示。不同激励和缺陷参数下快速傅里叶变换的时间变化和相位。数据是在缺陷正交轴附近的表面上的一个点上计算的。使差分对比度最大化的FFT fopt的最佳分析频率随阶跃加热时间和缺陷的大小而变化。10.21611 / qirt.2020.076
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