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
    • 2. 发明授权
    • Broad-band wave absorber
    • 宽带波吸收器
    • US5276448A
    • 1994-01-04
    • US875200
    • 1992-04-24
    • Yoshiyuki NaitoMichiharu Takahashi
    • Yoshiyuki NaitoMichiharu Takahashi
    • H01Q17/00
    • H01Q17/008
    • The present invention relates to a broad-band wave absorber wherein beams (3) formed of a ferrite magnetic material are placed at an optimal spacing and are aligned in a lattice form in longitudinal and lateral directions on a conductive plate (2). A magnetic substance of a specific thickness t.sub.m is formed into cylindrical blocks of a height d (where d.gtoreq.t.sub.m) wherein an end surface thereof is polygonal, and the cylindrical blocks are provided with a radio-wave reflecting surface aligned in such a manner that this surface is perpendicular to the axial direction of the blocks, and the end surface of the blocks is approximately perpendicular to a direction from which radio waves are incident. The ferrite magnetic substance could also be formed into rectangular prisms of thickness 2t.sub.m, height d, and length in the longitudinal direction thereof L, with the prisms aligned at a spacing b on a radio-wave reflecting surface, the direction of the height dimension of the prisms being approximately parallel to a radiowave incidence direction, and the surfaces thereof of the dimensions 2t.sub.m and L being perpendicular to the radiowave incidence direction, forming a plane parallel to a magnetic field direction of incident radio waves and the dimension L, wherein the following relationships hold:L.gtoreq.d.gtoreq. 2t.sub.m 20t.sub.m .gtoreq.b.gtoreq. 2.sub.tm
    • 本发明涉及一种宽带波吸收体,其中由铁氧体磁性材料形成的光束(3)以最佳间距放置,并且在导电板(2)上沿纵向和横向以格子状排列。 将特定厚度tm的磁性物质形成为其端面为多边形的高度d(d> = tm)的圆柱形块,并且圆柱形块设置有以这种方式排列的无线电波反射表面 该表面垂直于块的轴向,并且块的端面大致垂直于无线电波入射的方向。 铁氧体磁性物质也可以形成为厚度为2tm,高度d,长度方向为L的矩形棱镜,棱镜以无线电波反射面上的间距b排列,高度方向 棱镜大致平行于无线电波入射方向,其尺寸2tm和L的表面垂直于无线电波入射方向,形成平行于入射无线电波的磁场方向的平面和尺寸L,其中以下 关系保持:L> = d> = 2tm 20tm> = b> = 2tm