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    • 11. 发明专利
    • Support structure for vertical wind turbine
    • 垂直风力发电机的支撑结构
    • JP2012167662A
    • 2012-09-06
    • JP2011046959
    • 2011-02-15
    • Kenichi Suzuki健一 鈴木
    • SUZUKI KENICHI
    • F03D11/04F03D3/06
    • Y02E10/74
    • PROBLEM TO BE SOLVED: To provide a highly durable support structure for a large vertical wind turbine that can endure an impact of an earthquake and wind.SOLUTION: Two wire cables are stretched between two towers, and the wires are nearly orthogonally crossed at a point near the maximum deflection point between the towers. A cable band for tying the two wire cables in a crossed state is provided at the crossing point, and suspension wire ropes hung from the cable band and at least three wire ropes for attitude stabilization with lower ends thereof connected to anchors on the ground are used to place a rotor in a state of being suspended in the air while stabilized in its attitude.
    • 要解决的问题:为能够承受地震和风力影响的大型垂直风力发电机提供高度耐用的支撑结构。

      解决方案:两根电缆在两个塔之间拉伸,并且电线在靠近塔之间最大偏转点附近的点几乎正交。 在交叉点设置用于将交叉状态的两条电缆捆绑的电缆带,并且使用从电缆带悬挂的悬挂绳索和用于姿态稳定的至少三根钢丝绳,其下端连接到地面上的锚固件 使转子处于悬挂在空气中的状态,同时稳定在其姿态。 版权所有(C)2012,JPO&INPIT

    • 12. 发明专利
    • Dispersion of magnetic material particle having metal chelate compound on surface
    • 表面金属化合物的磁性材料颗粒的分散
    • JP2006334562A
    • 2006-12-14
    • JP2005165737
    • 2005-06-06
    • Kenichi Suzuki建一 鈴木
    • SUZUKI KENICHISUZUKI EREMIYA
    • B01J20/281B01D15/08B01J20/26C07K1/22
    • PROBLEM TO BE SOLVED: To provide a metal chelate compound to be used as a carrier matrix suitable for metal chelate affinity chromatography or a magnetic material particle, a method for producing the metal chelate compound and an inexpensive metal chelate resin having extremely large bonding capacity.
      SOLUTION: Sylylpropylethylenediamine triacetic acid is hydrolyzed, which is then bonded to the surface of the magnetic material particle. A nickel atom is chelate-bonded to the resulting magnetic material particle. This vertical link is regarded as one unit of a nickel chelate resin. As one unit on the right-hand side and one unit on the left-hand side are shown in Figure 1, silicon atoms Si of two units are connected laterally to each other through a -O-Si-O- bond to make a structure stronger, so that the silicon atom is hardly exfoliated from the surface of the magnetic material particle. The inexpensive nickel chelate resin has high adsorptivity of histidine.
      COPYRIGHT: (C)2007,JPO&INPIT
    • 待解决的问题:为了提供用作适合于金属螯合亲和层析或磁性材料颗粒的载体基质的金属螯合化合物,制备金属螯合物的方法和具有极大值的便宜的金属螯合树脂 接合能力。 解决方案:将Sylylpropylethylenediamine三乙酸水解,然后将其粘合到磁性材料颗粒的表面。 镍原子与所得磁性材料颗粒螯合。 该垂直连接被认为是镍螯合树脂的一个单位。 作为右侧的一个单位,左侧的一个单元示于图1中,两个单元的硅原子Si通过-O-Si-O-键横向连接以形成结构 使得硅原子几乎不从磁性材料颗粒的表面剥离。 廉价的镍螯合树脂具有高的组氨酸吸附性。 版权所有(C)2007,JPO&INPIT
    • 15. 发明专利
    • Separating/purifying device and separating/purifying method for biological constituent substance, and separated/purified substance
    • 分离/净化装置和生物组分物质的分离/净化方法和分离/纯化物质
    • JP2005140501A
    • 2005-06-02
    • JP2003367637
    • 2003-10-28
    • Kenichi Suzuki建一 鈴木
    • SUZUKI KENICHI
    • G01N33/543C07K1/14C12N15/09
    • PROBLEM TO BE SOLVED: To improve dispersivity of a magnetic particle bonded to a biological constituent substance in a solution by demagnetizing residual magnetization of the magnetic particle attracted and captured by magnetic attraction force by use of an alternating magnetic field. SOLUTION: When demagnetizing a magnetic body, the alternating magnetic field is applied to the magnetic body, and intensity of the alternating magnetic field is gradually reduced to zero. Thereby, an area of a magnetization-magnetic field hysteresis curve (a B-H curve) of the magnetic body is reduced while the hysteresis curve draws hysteresis, finally an operation point thereof reaches a point of magnetization (B) = 0, a magnetic field (H) = 0 that is the origin of the hysteresis curve, and the magnetic body is demagnetized. COPYRIGHT: (C)2005,JPO&NCIPI
    • 解决的问题:通过使用交变磁场通过磁吸引力吸引和捕获的磁性颗粒的残余磁化的消磁来改善与溶液中的生物构成物质结合的磁性颗粒的分散性。 解决方案:当磁体退磁时,将交变磁场施加到磁体,交变磁场的强度逐渐减小到零。 由此,磁滞磁场曲线(BH曲线)的面积减小,磁滞曲线拉动滞后,最后到达磁化点(B)= 0,磁场( H)= 0,即磁滞曲线的原点,磁体被去磁。 版权所有(C)2005,JPO&NCIPI