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    • 8. 发明专利
    • METAL VAPOUR DISCHARGE LAMP
    • GB1292428A
    • 1972-10-11
    • GB2500071
    • 1971-04-19
    • JAPAN BROADCASTING CORPTOKYO SHIBAURA ELECTRIC CO
    • KAMEGAYA TAKEOIMAHORI YUTAKAOHTA AKIRAKANOH TADAOOHARA AKIO
    • H01J17/06H01J61/073
    • 1292428 Metal-vapour discharge lamps NIPPON HOSO KYOKAI and TOKYO SHIBAURA ELECTRIC CO Ltd 19 April 1971 [20 March 1970 27 March 1970] 25000/71 Heading H1D The production of radio frequency interference by a metal-vapour discharge lamp is minimized by the use of electrodes 11, heated by the discharge, which have an effective diameter De and Length L, in mm., satisfying for non-porous cathodes, the equations. 15#L/De# 46 and 1À7# Il 0À4 /De # 4 where Il is the lamp current, in amps, under running conditions, or, for a porous electrode having 5 to 30% porosity, the equations. 9#L/De#35 and 1#Il/De 0À5 #3À16 The effective diameter, De, relates to the cathode rod 11, upon which a coil 12 may or may not be wound, and, for a rod of non- uniform shape-e.g. tapered (Fig. 12, not shown) having an abrupt change between two uniform sections of different diameter (Figs. 13 and 14, not shown) or formed by two overlapping uniform rods (Fig. 15, not shown)- is equal to the width of a uniform figure having the same length and longitudinal cross-sectional area as the cathode; formulae for De appropriate to the above cases are given. The cathode is of conventional construction, the rod 11 being of tungsten, thallium-tungsten, or molybdenum, and optionally surrounded by a single or multiple coil 12 of similar material, the electron-emitting material-e.g. oxides of barium, strontuim, calcium, thorium, or double salts thereof or of barium and aluminium, being coated thereon or disposed between the turns of the coil and the rod or, in the case of the porous rod embodiment, being impregnated therein. As described, the electrodes are incorporated in a high pressure, double-walled, mercury lamp (Fig. 7, not shown), the filling of which also includes argon or a halogen. Restriction to the above numerical conditions is stated to ensure that the cathode is at a sufficiently high temperature to provide thermionic emission adequate for the discharge current, thereby avoiding the occurrence offield emission and the instabilities and associated noise stated to result therefrom, while the temperature is not sufficiently high to produce undue cathode evaporation and blackening of the arc tube.