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    • 81. 发明申请
    • ELECTROMAGNETIC CONTACTOR
    • 电磁接触器
    • US20120133462A1
    • 2012-05-31
    • US13138029
    • 2010-06-14
    • Yasuhiro NakaToshikatsu OhgamiKoji OkuboKoetsu TakayaKenji Suzuki
    • Yasuhiro NakaToshikatsu OhgamiKoji OkuboKoetsu TakayaKenji Suzuki
    • H01H36/00H01H5/00
    • H01H50/16H01H50/42H01H50/641H01H51/2209H01H2050/446
    • The electromagnetic contactor enables a reliable return to a pole open position without increasing the spring force of a return spring. In an electromagnetic contactor, an electromagnetic device having an exciting coil and a contact mechanism having a return spring are disposed in parallel, and the electromagnetic device and contact mechanism are linked by a drive lever. The electromagnetic device has a polarized electromagnet having a magnetic circuit that includes a permanent magnet generating a suction force that moves the contact mechanism to a pole open position side when the exciting coil is not energized. The drive lever is fixed to either one of the electromagnetic device or contact mechanism and contacts with the other with no gap at least when the contact mechanism is moved to the pole open position side. The return force of the contact mechanism is covered by the suction force of the permanent magnet.
    • 电磁接触器能够可靠地返回到极开放位置,而不增加复位弹簧的弹簧力。 在电磁接触器中,具有励磁线圈的电磁装置和具有复位弹簧的接触机构平行设置,电磁装置和接触机构通过驱动杆连结。 电磁装置具有具有磁路的极化电磁体,该磁路包括永久磁铁,当励磁线圈未通电时,该永磁体产生将接触机构移动到极开位置侧的吸力。 驱动杆固定到电磁装置或接触机构中的任一个,并且至少当接触机构移动到极开位置侧时与另一个无接触。 接触机构的返回力被永久磁铁的吸力所覆盖。
    • 89. 发明授权
    • Optical fiber preform and the method of producing the same
    • 光纤预制棒及其制造方法
    • US06827883B2
    • 2004-12-07
    • US10242609
    • 2002-09-13
    • Yukio KoumuraYasuhiro NakaNobuaki Orita
    • Yukio KoumuraYasuhiro NakaNobuaki Orita
    • G02B616
    • C03B37/027C03B37/01446C03B37/01466C03B2205/90Y02P40/57Y10T428/24926Y10T428/2495
    • An optical fiber preform (1) serving as a material of an optical fiber has a shoulder portion (12) thrusting beyond a middle portion (M) in a base end region (K) which is on the upper side when the optical fiber preform is suspended for a drawing process. The optical fiber preform (1) of this configuration can be easily produced by appropriately setting the heating condition, etc. for the sintering step in the production process. Thus, it is possible to omit the elongating step after the sintering step, thereby simplifying the production process. Further, in the prior-art technique, turbulence is generated in the gas flow in the furnace of the drawing apparatus toward the end of the drawing step, making it impossible to draw in a stable manner. In contrast, in this embodiment, due to the shoulder portion (12), there is a small gap between the inner wall surface of the furnace and the optical fiber preform; due to this small gap, the gas flow is regulated, and the drawing can be conducted in a stable manner even toward the end of the drawing step.
    • 用作光纤材料的光纤预制件(1)具有在光纤预制件是上侧时位于上侧的基端区域(K)中的超过中间部分(M)的肩部(12) 暂停绘制过程。 通过在生产过程中适当地设定烧结步骤的加热条件等,可以容易地制造这种结构的光纤预制件(1)。 因此,可以省略烧结步骤后的延伸工序,从而简化了制造工序。 此外,在现有技术中,在拉拔装置的炉内的气流中产生湍流,使得不可能稳定地绘制。 相反,在本实施方式中,由于肩部(12),炉内壁面和光纤预制体之间存在小间隙, 由于这种小的间隙,气流被调节,并且即使在拉拔步骤结束时也可以以稳定的方式进行拉伸。
    • 90. 发明授权
    • Method of measuring optical fiber drawing tension
    • 测量光纤拉伸张力的方法
    • US06816245B2
    • 2004-11-09
    • US10650050
    • 2003-08-28
    • Yasuhiro NakaHiroyuki Kobayashi
    • Yasuhiro NakaHiroyuki Kobayashi
    • G01N2100
    • G01L5/042
    • A method of measuring optical fiber-drawing tension, containing: measuring oscillation of an optical fiber when drawing; determining a fundamental oscillation frequency of the optical fiber based on peak frequencies contained in spectrum components of oscillation waveform; and converting the fundamental oscillation frequency into tension applied to the optical fiber being drawn; wherein the determination of the fundamental oscillation frequency is performed through specifying, as a harmonic oscillation series group, a group of peak frequencies containing at least two peak frequencies, in which an interval between zero (0) and first peak frequencies, an interval between first and second peak frequencies, . . . , and an interval between (n−1)th and nth peak frequencies (where n is a natural number) are equal to each other, from among the peak frequencies in the spectrum components, to carry out the method based on the peak frequencies in the specified harmonic oscillation series group.
    • 测量光纤拉伸张力的方法,包括:拉伸时测量光纤的振荡; 基于包含在振荡波形的频谱分量中的峰值频率来确定光纤的基本振荡频率; 并将基本振荡频率转换为施加到被拉伸的光纤上的张力; 其中基本振荡频率的确定是通过将​​谐波振荡系列组指定为包含至少两个峰值频率的一组峰值频率,其中零(0)和第一峰值频率之间的间隔是第一 和第二峰值频率。 。 。 ,并且从第(n-1)和第n峰值频率(其中n是自然数)之间的间隔从频谱分量的峰值频率中彼此相等,以基于频谱分量中的峰值频率执行该方法 指定谐波振荡系列组。