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    • 13. 发明专利
    • ELECTROMAGNETIC WAVE SCREENING BREATHING HOLE
    • JPH08186394A
    • 1996-07-16
    • JP33787794
    • 1994-12-27
    • NEC CORPTOKIN CORP
    • HATAKEYAMA KENICHITOGAWA HITOSHI
    • F24F7/04H05K9/00
    • PURPOSE: To provide an electromagnetic wave screening breathing hole used for an electric dark room and an electromagnetic screening room for screening electromagnetic waves within a wide band from a low frequency to a mm-wave region. CONSTITUTION: In an electromagnetic wave screening breathing hole, a honeycomb screening material is provided in the entrance of the breathing hole and a pyramid or wedge-shaped electric wave absorbing material is fitted to the inner wall of the breathing hole. In the electric wave absorber, the view up to an exit is closed since the section entire region of the breathing hole is hidden by either absorbing body when viewed from the entrance surface of the breathing hole, and the installation position of the electric wave absorber is shifted in the depth direction of the breathing hole to secure the circulation of air. A length L of the breathing hole for fitting the electric wave absorbing body should be 2-3 wavelengths or longer. With this structure, an improved screening property can be achieved within a wide frequency range from a low frequency region to a mm-wave region.
    • 17. 发明专利
    • ELECTROMAGNETIC SHIELDING MATERIAL
    • JPH02250397A
    • 1990-10-08
    • JP7212389
    • 1989-03-23
    • NEC CORP
    • HATAKEYAMA KENICHISAWATO EIKICHI
    • H05K9/00
    • PURPOSE:To shield an electromagnetic wave which leaks out of a clearance section of a box body by providing a board of metal box body with a magnetic substance whose permeability has an incline which increases from an outer side of the box body toward an inner side thereof. CONSTITUTION:A metal box body board A which covers a metal box body B is provided with a magnetic substance D whose permeability has an incline which increases from an outer side of the box body toward an inner side thereof. Therefore, if a ratio of space occupied by the magnetic substance D is made larger inside the box body in correspondence with the clearance of an overlapped section C, the gradient of permeability at the clearance section can be acquired equivalently. As for an influence of the gradient of permeability concerning prevention of leakage from the clearance, strictly speaking, a propagation equation should be derived from the Maxwell's equations in a state where the permeability mu is a function of the position; however, it can be qualitatively explained by that the propagation velocity (v) is in inversely proportion to sq. rt. mu. Thereby, leakage of an electromagnetic wave from the clearance section of the box body can be restrained.