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SHUNT FOR MAGNETIC SYSTEMS USING PERMANENT MAGNETS

机译:使用永磁体的磁性系统应避开

摘要

1292073 Permanent magnets; transit-time tubes J A MELNIKOV 2 April 1970 15649/70 Headings H1D and H1P In a permanent magnet, e.g. for a magnetron or travelling wave-tube or for a magnetic focusing system, poles 1 co-operating with shielding yoke 3 are surrounded by annular discs 2 of magnetically soft material variably separated by ring 4 of high thermal expansivity, which shunt the magnet field so that variations of gap magnetic flux with temperature are compensated (Figs. 1a, 1b). The discs may have orthogonal projecting lugs sliding one over the other to provide a shunting flux path (Figs. 2a, 2b, not shown). A ring magnet 6 having end polepieces 7 (Figs. 3, 4) may be surrounded by annular magnetically soft discs 2 having studs 8 engaging inclined grooves of a split ring 9 of high thermal expansivity anchored at one end to the polepieces, so that the disc separation is varied with temperature to compensate flux variations. Two radially magnetized rings co-operating with a yoke (Figs. 5, 6, not shown) may have opposed hollow central polepieces containing elements of high thermal expansivity adjusting the spacing of conical spring steel discs from the magnetic rings, to compensate variations of gap flux. A focusing magnet (Figs. 7, 8) comprises an inner tube surrounded by ring magnets 6 and surrounding magnetically soft spaced discs 2, interconnected by a magnetically soft bar 16 terminating in an end member attached to a compensating pair of diametrically opposed bars 17 of high thermal expansivity; which expand and contract with temperature change, shifting the discs towards and away from the centres of the magnet rings, whereby changes of magnetic flux in the inner tube is compensated for temperature change. In a modification (Figs. 9, 10, not shown) magnetically soft rings surround each magnet circumferentially and fully or partly overlie adjacent polepieces whereby a portion of the flux is shunted. Diametrically opposed bars of highly thermal expansive material are arranged to traverse the rings with temperature changes over the magnets and polepieces to compensate the flux in the inner tube. The magnets may be ferrite.
机译:1292073永磁体;时移管J A MELNIKOV 1970年4月2日15649/70品目H1D和H1P在永久磁铁中,例如对于磁控管或行波管或磁聚焦系统,与屏蔽磁轭3配合使用的磁极1被软磁材料的圆盘2包围,该圆盘由高热膨胀率的环4可变地隔开,从而使磁场分流,间隙磁通量随温度的变化得到了补偿(图1a,1b)。圆盘可具有彼此垂直滑动的正交突出凸耳,以提供分流通量路径(图2a,2b,未示出)。具有端部极靴7(图3、4)的环形磁体6可以被环形软磁盘2围绕,该软磁盘2具有螺柱8,该螺柱8接合高热膨胀率的开口环9的倾斜槽,该斜槽的一端锚定到极靴,从而盘间距随温度变化以补偿通量变化。两个与磁轭配合的径向磁化环(图5、6,未显示)可以具有相对的中空中心极片,其中包含高热膨胀系数的元件,可调节锥形弹簧钢盘与磁环的间距,以补偿间隙的变化通量。聚焦磁体(图7、8)包括内管,该内管被环形磁体6围绕并且包围软磁间隔的盘2,该软磁盘由软磁棒16互连,该软磁棒终止于附接到一对成对的直径相对的棒17的端部构件中。高热膨胀率;它们随着温度变化而膨胀和收缩,使圆盘移向和移离磁环的中心,从而补偿了内管中磁通量的变化以适应温度变化。在一种改型中(图9、10,未示出),软磁环沿周向围绕每个磁体,并且全部或部分地覆盖在相邻的极靴上,由此一部分磁通被分流。沿直径方向相对的高热膨胀材料的条形布置成随着磁体和极靴上温度的变化而穿过环,以补偿内管中的通量。磁体可以是铁氧体。

著录项

  • 公开/公告号GB1292073A

    专利类型

  • 公开/公告日1972-10-11

    原文格式PDF

  • 申请/专利权人 JURY AFANASIEVICH MELNIKOV;

    申请/专利号GB19700015649

  • 发明设计人 JURY AFANASIEVICH MELNIKOV;

    申请日1970-04-02

  • 分类号H01F7/02;H01J23/087;H01J23/10;

  • 国家 GB

  • 入库时间 2022-08-23 08:04:18

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