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Optical fiber tension monitoring technique

机译:光纤张力监测技术

摘要

As an optical fiber (12) is being drawn, air (14) is directed at a portion of the fiber as a succession of air pulses, the pulses having a frequency near the natural frequency of the fiber portion. The frequency of the air pulses is then varied over a range of frequencies that includes the natural frequency of the fiber portion. When the air pulse frequency equals the natural frequency of the fiber portion, a resonance occurs which greatly amplifies the amplitude of the vibration of the fiber portion. The large deflection of the fiber that occurs at resonance is easy to detect, and the air pulse frequency which causes such maximum deflection is taken as being equal to the resonant frequency and therefore to the natural frequency of the fiber portion. Changes of the detected resonant frequency can be interpreted in a straightforward manner as changes in optical fiber tension which, in turn, are used to make compensatory changes of the temperature of the furnace (10).
机译:当拉出光纤(12)时,空气(14)作为一连串的空气脉冲被引向光纤的一部分,这些脉冲的频率接近光纤部分的固有频率。然后,空气脉冲的频率在包括纤维部分的固有频率的频率范围内变化。当空气脉冲频率等于纤维部分的固有频率时,会发生共振,从而大大放大纤维部分的振动幅度。谐振时发生的光纤的大挠度易于检测,并且将引起这种最大挠度的空气脉冲频率视为等于谐振频率,因此等于光纤部分的固有频率。所检测到的共振频率的变化可以以直接的方式解释为光纤张力的变化,而光纤张力的变化又被用于补偿炉子(10)的温度。

著录项

  • 公开/公告号US5316562A

    专利类型

  • 公开/公告日1994-05-31

    原文格式PDF

  • 申请/专利权人 AT&T BELL LABORATORIES;

    申请/专利号US19920909238

  • 发明设计人 DAVID H. SMITHGALL;ALAN T. WOODWARD;

    申请日1992-07-06

  • 分类号C03B37/023;

  • 国家 US

  • 入库时间 2022-08-22 04:31:41

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