材料去除率光纤腐蚀传感器

A. Trego, E. Haugse, E. Udd
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引用次数: 8

摘要

光纤布拉格光栅传感器一般由写入低双折射光纤中的单个光栅组成。这些传感器反射光谱中峰值的波长位移可用于测量应变的单个分量或温度的变化[Lawrence, 1997]。光纤也有足够显著的双折射,以保持偏振状态沿长和通过许多匝。这种“保持偏振”的光纤通过几家公司和几种配置(包括不同的包层材料和波长移位)在商业上可用。光栅的长度通常约为3毫米至5米。Udd给出了光纤、布拉格光栅和双折射的详细解释[Udd, 1991]。当LED发出的光通过光纤时,只有与光栅周期一致的波长才会被反射回光源。所有其他的波长都会通过。当光纤在光栅位置沿其轴线拉伸时,反射光谱将发生位移。应变或温度在任何其他位置的变化对波长编码数据输出的影响可以忽略不计。当光纤布拉格光栅单轴传感器(以下称为光纤)横向应变时,根据Lawrence和Nelson定义的数学关系,波长将分成两个不同的峰值[Lawrence, Nelson等人,96]。利用这些光纤光栅,研制了一种测量材料腐蚀速率的腐蚀传感器。这种新开发的腐蚀传感器背后的原理是对已知负载的纤维进行预应力。载荷是通过在纤维周围施加压力的圆柱体诱导均匀的环向应力来施加的。这种诱导应力使反射光谱变宽,直到反射强度峰的分岔是可区分的。当外筒的材料被腐蚀掉时,施加的应力就会被解除。最后,当没有负载时,反射光谱将有一个以标称布拉格光栅波长为中心的单峰。如果使用维持偏振的三轴光栅,那么传感器将更加敏感,在每个波长范围内都有两个不同的峰值,这些峰值会发生移位。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Material removal rate fiber optic corrosion sensor
Fiber Bragg grating sensors generally consist of a single grating written in a low-birefringent optical fiber. The wavelength shift of the peak in the reflected spectrum from these sensors can be used to measure a single component of strain or a change in temperature [Lawrence, 1997]. Fibers are also available with a significant enough birefringence to maintain the polarization state along great lengths and through many turns. This 'polarization maintaining' fiber is commercially available through several companies and in several configurations (including different cladding material and wavelength shift). The grating usually extends approximately 3 mm - 5 m in length. Udd gives a detailed explanation of fiber optics, Bragg gratings and birefringence [Udd, 1991]. As light from an LED is passed through the fiber, only the wavelength consistent with the grating period will be reflected back towards the source. All other wavelengths will pass through. The reflected spectrum will shift as the fiber is strained along its axis at the grating location. Strain or temperature changes at any other location have negligible effect on the wavelength encoded data output. When the Fiber Bragg grating single-axis sensor (termed fiber hereafter) is strained transversely the wavelength will separate into two distinct peaks according to a mathematical relationship defined by Lawrence and Nelson [Lawrence, Nelson et al. 96]. Using these Fiber Bragg grating fibers a corrosion sensor which measures the rate of material was developed. The principle behind this newly developed corrosion sensor is to pre-stress the fiber with a known load. The load is applied by inducing a uniform hoop stress through pressure fitted cylinders around the fiber. This induced stress creates a broadening of the reflected spectrum until the bifurcation of the reflected intensity peaks is distinguishable. As the material from the outer cylinder corrodes away the applied stress will be relieved. Finally, when no load is achieved, the reflected spectrum will have a single peak centered around the nominal Bragg grating wavelength. If a polarizing-maintaining 3-axis grating is used then the sensor would be even more sensitive, having two distinct peaks in each wavelength regime which shift.
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