会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 1. 发明授权
    • Spliced portion housing structure for optical fiber in optical submerged
repeater
    • 光接收式中继器光纤接头部分外壳结构
    • US4505540A
    • 1985-03-19
    • US340350
    • 1982-01-18
    • Kahei FurusawaMakoto NunokawaYoshihiro EjiriHitoshi YamamotoYoshihiko YamazakiKoichi Tatekura
    • Kahei FurusawaMakoto NunokawaYoshihiro EjiriHitoshi YamamotoYoshihiko YamazakiKoichi Tatekura
    • G02B6/24G02B6/44H02G15/08H02G15/14G02B5/14G02B7/26
    • G02B6/4448
    • A spliced portion housing structure for an optical fiber in an optical submerged repeater, characterized in that, in order to splice together in a joint ring an optical fiber and a power-supplying feeder from the optical submerged repeater to an optical fiber and a power-supplying feeder of a tail cable from a cable coupling of an optical submarine cable, respectively, a joint chamber is provided on an end plate of a housing of the optical submerged repeater in such a manner that the end plate forms a part of the joint chamber; the optical fiber and the power-supplying feeder from the submerged repeater are introduced into the joint chamber through a first feedthrough provided in the end plate for hermetically introducing the optical fiber and the power-supplying feeder; the tail cable from the cable coupling is hermetically introduced into the joint chamber through a second feedthrough provided in the wall of the joint chamber so that the tail cable is insulated from the joint chamber, the optical fibers and the feeders pulled into the joint chamber from both of the first and second feedthroughs are respectively spliced together while being isolated from each other and housed in the joint chamber; the optical fiber spliced portion is fixed to a cage mounted in the joint chamber; and the joint chamber is formed to have a water pressure resisting and airtight structure.
    • 一种用于光学浸没式转发器中的光纤的接合部分壳体结构,其特征在于,为了将接头环中的光纤和从所述光学浸没式中继器馈送到光纤的功率供给馈送器连接在一起, 分别从光学海底电缆的电缆耦合器供给尾缆的馈线,接合室设置在光学浸没式中继器的壳体的端板上,使得端板形成接头室的一部分 ; 来自浸没式中继器的光纤和供电给料器通过设置在端板中的用于气密地引入光纤和供电馈送器的第一馈通引入接头室; 来自电缆耦合器的尾部电缆通过设置在接头室的壁中的第二馈通气密地引入接头室,使得尾部电缆与接头室绝缘,光纤和馈线从接头室中拉出 第一和第二馈通两者分别拼接在一起,同时彼此隔离并容纳在关节室中; 光纤接合部固定在安装在接头室内的保持架上; 并且所述接合室形成为具有耐水压力和气密结构。
    • 3. 发明授权
    • Method and apparatus for measuring distribution of elongation in an
optical cable
    • 测量光缆伸长分布的方法和装置
    • US4595284A
    • 1986-06-17
    • US564534
    • 1983-12-22
    • Koichi TatekuraKiyofumi MochizukiYoshihiro Ejiri
    • Koichi TatekuraKiyofumi MochizukiYoshihiro Ejiri
    • G01B11/16G01M11/00G01S11/12G02B6/00G01N21/84
    • G01M11/30G01B11/18G01S11/12
    • Elongation distortion at any location of an optical fiber cable is measured by using the principle of the stimulated Raman effect in which a stokes beam with a little frequency difference from that of a pumping beam is generated when a pumping beam and a seed beam with the same frequency as that of the stokes beam meet in a Raman material like an optical fiber cable. Due to the fact that the group refractive index of an optical fiber cable for a pumping beam is different from that for a stokes beam, elongation of a cable is measured by observing time difference of the arrival of pumping beam and stokes beam. The location that the pumping beam meets with the stokes beam can be adjusted merely by shifting the pumping pulse, then, elongation distortion at any location can be measured. According to the invention, the pumping pulse is applied to the cable to be tested from both the ends of the cable with one of the pumping pulse delayed according to the desired location for meeting of two pulses. At one end of the cable, the arrival time t.sub.1 and t.sub.2 is observed, where t.sub.1 is the arrival time of the stokes pulse and t.sub.1 +t.sub.2 is the arrival time of the pumping pulse. The distribution of elongation (d.DELTA.z/dz) is obtained by calculating the equations z=k.sub.1 t.sub.1 -k.sub.2 t.sub.2, and .DELTA.z=k.sub.3 t.sub.2 -k.sub.4 t.sub.1, where k.sub.1, k.sub.2, k.sub.3 and k.sub.4 are constants, z is the length between the end and the location to be tested, and .DELTA.z is the elongation of the cable of the length z.
    • 通过使用受激拉曼效应的原理来测量光纤电缆的任何位置处的伸长失真,其中当具有相同的泵浦光束和种子光束时,产生具有与泵浦光束的频率差小的频率差的斯托克斯光束 频率与斯托克斯光束的频率在像光纤电缆那样的拉曼材料中相遇。 由于用于泵浦光束的光纤电缆的组折射率与斯托克斯光束的折射率不同,所以通过观察泵浦光束和斯托克斯光束到达的时间差来测量电缆的伸长率。 可以仅通过移动泵浦脉冲来调节泵浦梁与斯托克斯梁相遇的位置,然后可以测量任何位置处的伸长失真。 根据本发明,泵浦脉冲从电缆的两端施加到要测试的电缆,其中一个泵浦脉冲根据期望的位置延迟以满足两个脉冲。 在电缆的一端,观察到到达时间t1和t2,其中t1是斯托克斯脉冲的到达时间,t1 + t2是泵浦脉冲的到达时间。 通过计算公式z = k1t1-k2t2和DELTA z = k3t2-k4t1获得伸长分布(d DELTA z / dz),其中k1,k2,k3和k4是常数,z是端部和 要测试的位置,DELTA z是长度为z的电缆的伸长率。