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基于啁啾光纤布拉格光栅的冲击与爆轰速度测量系统的研制

Development of a Shock and Detonation Velocity Measurement System Using Chirped Fiber Bragg Gratings.

作者信息

Barbarin Yohan, Lefrançois Alexandre, Chuzeville Vincent, Magne Sylvain, Jacquet Laurent, Elia Thomas, Woirin Karol, Collet Christelle, Osmont Antoine, Luc Jérôme

机构信息

CEA, DAM, GRAMAT, BP 80200, F-46500 Gramat, France.

CEA, LIST, Laboratoire Capteurs Fibres Optiques, F-91191 Gif-sur-Yvette, France.

出版信息

Sensors (Basel). 2020 Feb 14;20(4):1026. doi: 10.3390/s20041026.

DOI:10.3390/s20041026
PMID:32074991
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7070336/
Abstract

Dynamic measurements of shock and detonation velocities are performed using long chirped fiber Bragg gratings (CFBGs). Such thin probes, with a diameter of typically 125 µm or even 80 µm can be directly inserted into high-explosive (HE) samples or simply glued laterally. During the detonation, the width of the optical spectrum is continuously reduced by the propagation of the wave-front, which physically shortens the CFBG. The light power reflected back shows a ramp-down type signal, from which the wave-front position is obtained as a function of time, thus yielding a detonation velocity profile. A calibration procedure was developed, with the support of optical simulations, to cancel out the optical spectrum distortions from the different optical components and to determine the wavelength-position transfer function of the CFBG. The fitted slopes of the X-T diagram give steady detonation velocity values which are in very good agreement with the classical measurements obtained from discrete electrical shorting pins (ESP). The main parameters influencing the uncertainties on the steady detonation velocity value measured by CFBG are discussed. To conclude, different HE experimental configurations tested at CEA () are presented: bare cylindrical sticks, wedges for shock-to-detonation transitions (SDT), spheres, a cast-cured stick around a CFBG, and a detonation wave-front profile configuration.

摘要

利用长啁啾光纤布拉格光栅(CFBG)对冲击速度和爆轰速度进行动态测量。这种细探针直径通常为125µm甚至80µm,可直接插入高爆炸药(HE)样品中,或简单地横向粘贴。在爆轰过程中,光谱宽度会因波前传播而持续减小,这实际上缩短了CFBG。反射回来的光功率呈现出一种下降型信号,从中可获得波前位置随时间的函数关系,从而得到爆轰速度分布。在光学模拟的支持下,开发了一种校准程序,以消除不同光学元件引起的光谱畸变,并确定CFBG的波长 - 位置传递函数。X - T图的拟合斜率给出的稳定爆轰速度值与通过离散电短路引脚(ESP)获得的经典测量值非常吻合。讨论了影响CFBG测量稳定爆轰速度值不确定性的主要参数。最后,展示了在法国原子能委员会(CEA)测试的不同高爆炸药实验配置:裸圆柱形药柱、用于激波到爆轰转变(SDT)的楔形体、球体、围绕CFBG的浇铸固化药柱以及爆轰波前分布配置。

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