(19)
(11) EP 0 439 337 A3

(12) EUROPEAN PATENT APPLICATION

(88) Date of publication A3:
06.11.1991 Bulletin 1991/45

(43) Date of publication A2:
31.07.1991 Bulletin 1991/31

(21) Application number: 91300505.4

(22) Date of filing: 23.01.1991
(51) International Patent Classification (IPC)5H01Q 17/00
(84) Designated Contracting States:
DE FR GB SE

(30) Priority: 25.01.1990 JP 15798/90
02.02.1990 JP 23818/90
08.06.1990 JP 150690/90
20.06.1990 JP 162403/90

(71) Applicants:
  • Naito, Yoshiyuki
    Yamato-Shi Kanagawa-Ken (JP)
  • Takahashi, Michiharu
    Yachiyo-Shi Chiba-Ken (JP)

(72) Inventors:
  • Naito, Yoshiyuki
    Yamato-Shi Kanagawa-Ken (JP)
  • Takahashi, Michiharu
    Yachiyo-Shi Chiba-Ken (JP)

(74) Representative: Palmer, Roger et al
PAGE, WHITE & FARRER 54 Doughty Street
London WC1N 2LS
London WC1N 2LS (GB)


(56) References cited: : 
   
       


    (54) Broad-band wave absorber


    (57) The present invention relates to a broad-band wave absorber wherein plates (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 tm is formed into cylindrical blocks of a height d (where d ≧ tm) 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 2tm, 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 radio-wave incidence direction, and the surfaces thereof of the dimensions 2tm and L being perpendicular to the radio-wave 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 ≧ d ≧ 2tm
    20tm ≧ b ≧ 2tm







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