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    • 5. 发明申请
    • Film and magnetic-recording medium using the same
    • 胶片和磁记录介质使用它
    • US20070082232A1
    • 2007-04-12
    • US10578921
    • 2004-11-11
    • Masanori SueokaAkimitsu Tsukuda
    • Masanori SueokaAkimitsu Tsukuda
    • B32B27/34B32B27/08G11B5/706C08G69/08
    • G11B5/73H05K1/0346H05K1/0393Y10T428/31681Y10T428/31725
    • A film and a magnetic-recording medium using the film, where the heat shrinkage ratio in the transverse direction of the film subjected to heat treatment under no tension for 30 min. at 180° C. is from 1.0 to 2.5%, and where the film satisfies the following equations (1)-(4) simultaneously, with αMD (×10−6/° C.) and αTD (×10−6/° C.) being coefficient of thermal expansion in the longitudinal and the transverse direction, respectively, and βMD (×10−6/% RH) andβTD (×10−6/% RH) being coefficient of hygroscopic expansion in the longitudinal and the transverse direction, respectively. In the film, by controlling the dimensional changes by temperature and humidity within specific ranges, it becomes possible to control the dimensional change and the difference in dimensional changes between the longitudinal and the transverse direction of the film used as a magnetic-recording medium to be extremely small. −10≦αMD≦10 (1), αMD−10≦αTD≦αMD−3 (2), −10≦βMD≦10 (3), βMD−10≦βTD≦βMD−3 (4)
    • 使用该膜的膜和磁记录介质,其中在无张力下进行30分钟热处理的膜的横向热收缩率。 在180℃下为1.0至2.5%,并且其中该膜同时满足以下等式(1) - (4),使用αMD(x10 -6 /℃)和αTD( 分别为纵向和横向的热膨胀系数和βMD(x10-6 /%RH)和βTD(x10)的热膨胀系数 分别为纵向和横向的吸湿膨胀系数。 在薄膜中,通过将温度和湿度的尺寸变化控制在特定范围内,可以将尺寸变化和用作磁记录介质的薄膜的纵向和横向之间的尺寸变化的差异控制为 非常小 -10 <=αMD<= 10(1),αMD-10 <=αTD<=αMD-3(2),-10 <=βMD= 10(3),βMD-10 <=βTD<=βMD-3 (4)
    • 6. 发明授权
    • Film and magnetic-recording medium using the same
    • 胶片和磁记录介质使用它
    • US07531252B2
    • 2009-05-12
    • US10578921
    • 2004-11-11
    • Masanori SueokaAkimitsu Tsukuda
    • Masanori SueokaAkimitsu Tsukuda
    • B32B13/04G11B5/71
    • G11B5/73H05K1/0346H05K1/0393Y10T428/31681Y10T428/31725
    • A film and a magnetic-recording medium using the film, where the heat shrinkage ratio in the transverse direction of the film subjected to heat treatment under no tension for 30 min. at 180° C. is from 1.0 to 2.5%, and where the film satisfies the following equations (1)-(4) simultaneously, with αMD (×10−6/° C.) and αTD (×10−6/° C.) being coefficient of thermal expansion in the longitudinal and the transverse direction, respectively, and βMD (×10−6/% RH) andβTD (×10−6/% RH) being coefficient of hygroscopic expansion in the longitudinal and the transverse direction, respectively. In the film, by controlling the dimensional changes by temperature and humidity within specific ranges, it becomes possible to control the dimensional change and the difference in dimensional changes between the longitudinal and the transverse direction of the film used as a magnetic-recording medium to be extremely small. −10≦αMD≦10 (1), αMD−10≦αTD≦αMD−3 (2), −10≦βMD≦10 (3), βMD−10≦βTD≦βMD−3 (4).
    • 使用该膜的膜和磁记录介质,其中在无张力下进行30分钟热处理的膜的横向热收缩率。 在180℃下为1.0至2.5%,并且其中膜与αMD(x10-6 /℃)和αTD(x10-6 /℃)同时满足以下等式(1) - (4) )分别为纵向和横向的热膨胀系数,βMD(x10-6 /%RH)和βTD(x10-6 /%RH)分别为纵向和横向的吸湿膨胀系数。 在薄膜中,通过将温度和湿度的尺寸变化控制在特定范围内,可以将尺寸变化和用作磁记录介质的薄膜的纵向和横向之间的尺寸变化的差异控制为 非常小 -10 <=αMD<= 10(1),αMD-10 <=αTD<=αMD-3(2),-10 <=βMD= 10(3),βMD-10 <=βTD<=βMD-3 (4)。
    • 7. 发明授权
    • Magnetic recording medium
    • 磁记录介质
    • US06468628B2
    • 2002-10-22
    • US09759332
    • 2001-01-16
    • Masanori SueokaAkimitsu TsukudaNobuaki Ito
    • Masanori SueokaAkimitsu TsukudaNobuaki Ito
    • G11B5733
    • G11B5/7315G11B5/64G11B5/70G11B5/7325G11B5/733G11B5/735Y10T428/24355Y10T428/24975Y10T428/31725
    • Disclosed is a magnetic recording medium having a magnetic layer directly formed on at least one surface of a base film that comprises, as the essential ingredient, an aromatic polyamide, in which the number of protrusions having a height of at least 10 nm on the surface of the magnetic layer, Na(10) (/mm2), the number of protrusions having a height of at least 50 nm thereon, Na(50) (/mm2), and the number of protrusions having a height of at least 10 nm on the surface of the base film coated with the magnetic layer, Na(10)′ (/mm2), all satisfy the following formulae: 2×104≦Na(10)≦2×107, 0≦Na(50)≦5×104, −0.9≦(Na(10)−Na(10)′)/Na(10)′≦0. The medium has, as the non-magnetic substrate (base film), a highly-tough, aromatic polyamide film, and the surface profile of its magnetic layer and that of its base film are specifically controlled.
    • 公开了一种磁记录介质,其具有直接形成在基膜的至少一个表面上的磁性层,所述磁性层包含作为必要成分的芳族聚酰胺,其中表面上具有至少10nm的高度的突起的数量 的磁性层的Na(10)(/ mm 2),其上具有至少50nm的高度的突起的数量为Na(50)(/ mm 2),并且具有至少10nm的高度的突起的数量 在涂覆有磁性层的基膜的表面上,Na(10)'(/ mm2)都满足下列公式:介质作为非磁性基材(基膜)具有高韧性,芳香性 聚酰胺薄膜及其磁性层的表面轮廓及其底膜的表面轮廓是特别受控制的。
    • 8. 发明授权
    • Aromatic polyamide film and magnetic recording medium using it
    • 芳香聚酰胺薄膜和使用它的磁记录介质
    • US06358619B1
    • 2002-03-19
    • US09331511
    • 1999-06-22
    • Masanori SueokaMitsuhiro HoriuchiAkimitsu Tsukuda
    • Masanori SueokaMitsuhiro HoriuchiAkimitsu Tsukuda
    • G11B566
    • B32B27/08B32B27/06G11B5/73G11B5/733Y10S428/90Y10T428/31725Y10T428/31739
    • The present invention is an aromatic polyamide film, which is a laminated film consisting of at least two layers, comprising an aromatic polyamide and 0.1 wt % to 10 wt % of at least one or more different polymers, being contained at least in the outermost layer (layer A) of the film, subject to the condition that the following formulae are satisfied 0.01≦t/d≦0.5 0.05≦s/L≦1 where d is the thickness of the layer A (&mgr;m); t, the circle equivalent diameter of the isles of the different polymer (&mgr;m); L, the major axis of the isles (&mgr;m); and s, the minor axis of the isles (&mgr;m). The aromatic polyamide film of the present invention is especially useful an a base film of a magnetic recording medium with high productivity since it is free from the wrinkling and weaving caused at the time of film winding and excellent in abrasion resistance on the film surface.
    • 本发明是一种芳族聚酰胺薄膜,其是由至少两层构成的层叠薄膜,其包含芳族聚酰胺和0.1重量%至10重量%的至少一种或多种不同的聚合物,至少在最外层 (A层),满足满足以下条件的条件,其中d是层A(mum)的厚度; t,不同聚合物(mum)的岛的圆当量直径; L,岛的主轴(妈妈); 和s,小岛的短轴(妈妈)。 本发明的芳香族聚酰胺薄膜特别适用于具有高生产率的磁记录介质的基膜,因为它没有在卷绕时引起的起皱和编织,并且在膜表面上具有优异的耐磨性。
    • 10. 发明授权
    • Aromatic polyamide and/or aromatic polyimide film and magnetic recording
medium having such a film as a base
    • 芳族聚酰胺和/或芳族聚酰亚胺膜和具有这种膜作为基材的磁记录介质
    • US5972474A
    • 1999-10-26
    • US805502
    • 1997-02-26
    • Toshihiro TsuzukiMasanori SueokaNobuaki Itoh
    • Toshihiro TsuzukiMasanori SueokaNobuaki Itoh
    • C08J5/18G11B5/73G11B5/733B32B3/10
    • C08J5/18G11B5/733C08J2377/10C08J2379/08Y10S428/90Y10T428/24355Y10T428/24372Y10T428/24992Y10T428/25Y10T428/265Y10T428/31725
    • An aromatic polyamide and/or aromatic polyimide film suitable as a support in a magnetic recording medium excellent in runnability and scratch resistance and good in S/N ratio comprises an aromatic polyamide and/or aromatic polyimide as a main component, with particles present in the film, which film has characteristics which satisfy the following formulae:10 nm.ltoreq.dmax.ltoreq.300 nm (1)3.ltoreq..rho.(dmax)/.rho.(dmin).ltoreq.100 (2)or10 nm.ltoreq.dmax.ltoreq.300 nm (3)3.ltoreq..rho.(dmax)/.rho.(d").ltoreq.100 (4).rho.(dmax)/.rho.(dmin)>100 (5)where dmax is the depth from a first surface of the film at which the particle density shows the first maximal value; dmin is the depth at which the particle density shows the first minimal or minimum value in a range from dmax to 1 .mu.m from the said first surface; the linear differential coefficient of the particle density distribution curve has an inflection point at which the quadratic differential coefficient of the particle density distribution curve ia a negative, which inflection point occurs at a depth d", deeper than dmax, and within a range between the depth at which .rho.(d) is 4/5 of .rho.(dmax), and dmin; and .rho.(d) is the particle density at each depth.
    • 适用作为运行性和耐刮擦性优异且S / N比良好的磁记录介质中的芳香族聚酰胺和/或芳香族聚酰亚胺膜包含作为主要成分的芳香族聚酰胺和/或芳香族聚酰亚胺, 薄膜,该膜具有满足以下公式的特性:10nm 100(5)其中dmax是 从粒子密度显示第一最大值的膜的第一表面的深度; dmin是从所述第一表面到dmax至1μm的范围内的颗粒密度显示第一最小值或最小值的深度; 粒子密度分布曲线的线性微分系数具有拐点,粒子密度分布曲线的二次微分系数曲线为负,拐点出现在比dmax更深的深度d“处,并且在 rho(d)的深度为+ E,fra 4/5 + EE的rho(dmax),dmin; rho(d)是每个深度处的粒子密度。