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    • 12. 发明授权
    • Separator for fuel cell and fuel cell
    • 燃料电池和燃料电池分离器
    • US08455156B2
    • 2013-06-04
    • US12741803
    • 2008-11-04
    • Yoshinori YamamotoHiroya NakajiHitoshi HamadaToshiyuki SuzukiHaruyuki Aono
    • Yoshinori YamamotoHiroya NakajiHitoshi HamadaToshiyuki SuzukiHaruyuki Aono
    • H01M8/02
    • H01M8/0254H01M8/0258H01M8/0267H01M8/241H01M8/2457H01M2008/1095
    • A separator has a concavo-convex structure formed in mutually reversed shapes on two opposite sides thereof to define flow paths of different fluids on the respective two sides. The concavo-convex structure includes multiple first projections formed and protruded on one side of the two opposite sides and arranged at intervals having a preset regularity. The concavo-convex structure also includes multiple second projections formed and protruded on the other side of the two opposite sides in a specific area corresponding to an area for formation of the multiple first projections on the one side and arranged at intervals having a preset regularity. The concavo-convex structure further includes reinforcing elements protruded on the one side. Each of the reinforcing elements is formed as a convex in a specific shape of connecting multiple positions where the first projections are expected to be formed according to the preset regularity, while avoiding positions corresponding to the second projections formed on the other side. This arrangement effectively prevents a potential trouble caused by deformation of the separator due to a pressure difference between the flow pressures of the respective fluids flowing on the respective sides of the separator.
    • 分离器具有在其两个相对侧上以相互反转的形状形成的凹凸结构,以限定相应两侧上不同流体的流动路径。 凹凸结构包括在两个相对侧的一侧上形成和突出的多个第一突起并以预定的规则间隔布置。 凹凸结构还包括在对应于一侧上形成多个第一突起的区域的特定区域中在两个相对侧的另一侧上形成和突出的多个第二突起,并且以预定的规则间隔布置。 凹凸结构还包括在一侧突出的增强元件。 每个加强元件形成为具有预定规则性地预期形成第一突起的多个位置的特定形状的凸起,同时避免与形成在另一侧上的第二突起相对应的位置。 这种布置有效地防止了由于在分离器的各个侧面上流动的各个流体的流动压力之间的压力差引起的分离器变形引起的潜在故障。
    • 15. 发明授权
    • Air conditioner and coating composition
    • 空调和涂料组成
    • US08171750B2
    • 2012-05-08
    • US12490880
    • 2009-06-24
    • Reiji MoriokaYoshinori YamamotoYasuhiro Yoshida
    • Reiji MoriokaYoshinori YamamotoYasuhiro Yoshida
    • F25D17/06
    • C09D5/1625C08K3/36C08L27/12C09D7/62C09D7/67C09D7/68F24F1/0007F24F2003/1664F28F19/04F28F21/067
    • Disclosed is an air conditioner coated by the coating composition to the resin-made components where due formation occurs upon the cooling operation, provides the antifouling performance against various stains, restrains enlargement of droplet, and provides an excellent long-term durability (sticking property and peeling off property) all at the same time. The air conditioner of the present embodiment forms a coating film 103 to surfaces of resin-made components and resin-made components installed to a rear flow side of the heat exchanger, includes the silica ultrafine particles 101 and the fluororesin particles 102, and provides, within the coating film 103, a silica film 104 comprising the silica ultrafine particles and the fluororesin particles 102 partially exposed from a surface of the silica film 104 in dots, and an exposed area of the silica film 104 is greater than an exposed area of the fluororesin particles 102.
    • 本发明公开了一种由涂料组合物涂布到制冷部件上的空调机,在冷却运转时发生适当形成,提供防污性能,抑制液滴的扩大,提供优异的长期耐久性(粘着性和 剥离财产)全部在同一时间。 本实施方式的空调装置在安装于热交换器的后流侧的树脂成分和树脂成分的表面上形成涂膜103,其包含二氧化硅超微粒子101和氟树脂粒子102, 在涂膜103内,包含二氧化硅超细颗粒的二氧化硅膜104和从二氧化硅膜104的表面部分露出的氟树脂颗粒102,并且二氧化硅膜104的暴露面积大于 氟树脂颗粒102。
    • 17. 发明授权
    • Optical glass for precision molding having high refractive index
    • 具有高折射率的精密模塑用光学玻璃
    • US07943540B2
    • 2011-05-17
    • US11905925
    • 2007-10-05
    • Yoshinori Yamamoto
    • Yoshinori Yamamoto
    • C03C3/253C03C3/14C03C3/15C03C3/155C03C3/068
    • C03C3/253C03C3/155
    • An optical glass for precision molding having a high refractive index (nd) and a low yield temperature (At). The optical glass comprises, as glass components in wt %, 64 to 83% of Bi2O3; 4 to 17% of B2O3; 0 to 12% of GeO2 (wherein the total of B2O3 and GeO2 is 10 to 20%); 0 to 7% of La2O3; 0 to 7% of Gd2O3 (wherein the total of La2O3 and Gd2O3 is 1 to 13%); 0 to 4% of ZrO2; 0 to 5% of Ta2O5; 0 to 15% of ZnO; 0 to 2% of Sb2O3; and 0 to 1% of In2O3. The optical glass has optical constants, that is, a refractive index (nd) of 2.05 to 2.25 and an Abbe number (vd) of 15 to 22, and a yield temperature (At) of 510° C. or less.
    • 具有高折射率(nd)和低屈服温度(At)的精密模塑用光学玻璃。 光学玻璃包含以重量%计的玻璃组分为64%至83%的Bi 2 O 3; 4〜17%的B2O3; 0〜12%的GeO2(其中B2O3和GeO2的总量为10〜20%); 0〜7%的La2O3; 0〜7%的Gd2O3(其中La2O3和Gd2O3的总量为1〜13%); 0〜4%的ZrO2; 0〜5%Ta2O5; 0〜15%的ZnO; 0〜2%的Sb2O3; 和0〜1%的In2O3。 光学玻璃的光学常数,即折射率(nd)为2.05〜2.25,阿贝数(vd)为15〜22,屈服温度(At)为510℃以下。
    • 19. 发明授权
    • Brillouin spectral measuring method and Brillouin spectral measuring apparatus
    • 布里渊光谱测量方法和布里渊光谱测量仪器
    • US07576840B2
    • 2009-08-18
    • US11913244
    • 2007-04-16
    • Yoshinori Yamamoto
    • Yoshinori Yamamoto
    • G01L1/24G01N21/00G01B9/02G02B6/00
    • G01B11/16G01D5/35364G01D5/3538G01K11/32G01K2011/322G01M11/083
    • The present invention relates to a Brillouin spectrum measuring method and measuring apparatus that have a structure for more accurately measuring the parameters of Brillouin spectra at predetermined sections of an optical fiber. The measuring method comprises an optical fiber section including first and second optical fibers that are serially connected via a connection portion. The first and second optical fibers have a Brillouin spectrum for which the difference between the peak frequencies in a predetermined temperature and predetermined strain-applied state for which the respective usage environments are assumed is equal to or more than a predetermined frequency difference. In the measuring method, a Brillouin spectrum which is obtained in accordance with pumping light supplied to the optical fiber section is measured, and a point of connection between the first and second optical fibers is specified on the basis of the measurement data for the measured Brillouin spectrum.
    • 本发明涉及一种布里渊频谱测量方法和测量装置,其具有用于更精确地测量光纤预定部分的布里渊频谱参数的结构。 该测量方法包括:光纤部分,包括通过连接部分串联连接的第一和第二光纤。 第一光纤和第二光纤具有预定温度下的峰值频率与假设各个使用环境的预定应变状态之间的差异等于或大于预定频率差的布里渊频谱。 在测量方法中,测量根据提供给光纤部分的泵浦光获得的布里渊光谱,并且基于所测量的布里渊的测量数据来指定第一和第二光纤之间的连接点 光谱。