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Pole-changing, three-phase, alternating current motor or generator for three pole-numbers

机译:用于三个极数的变极三相交流电动机或发电机

摘要

986,379. Winding layouts for dynamo-electric machines. NATIONAL RESEARCH DEVELOPMENT CORPORATION. April 4, 1963 [April 24, 1962], No. 15612/62. Heading H2A. In a system of pole-changing by poleamplitude modulation effected by applying a single pole-amplitude modulation wave applied to the three-phase winding as a whole two modulated pole-numbers are obtained, one by the use of a modulation wave having an odd number of cycles, and another by the use of a modulation wave having an even number of cycles. Each phase winding is divided into four sections and the winding is connected in four-parallel star for one pole number (preferably the lowest), in series-parallel star for the intermediate pole number, and in series star or delta for the third pole number (preferably the highest). Fig. 7a shows an 8-pole, 120 degrees spread winding in 18 slots, the coil grouping per phase being alternately one and two coils per pole-pair, and the original phase sequence A, C, B. The modulation operator M-M indicates those coils under this operator which are reversed, and shows a 7-cycle modulation wave which transforms the winding to 6-poles. Fig. 7c shows a 6-cycle modulation wave applied to the same winding to produce 4-poles. In each modulated condition the phase sequence becomes A, B, C. Fig. 7f (not shown) shows how a 9-cycle modulation gives 10 poles. It is also described (Fig. 7d, also not shown) how these winding transformations are related to 4/6 pole transformation of the same winding by a single-cycle modulation, and the whole inter-relationship of the four pole numbers is set out in diagrammatic form in Fig. 6a (not shown). The correct slots to reverse are determined by slot-star diagrams Figs. 7b, 7e, not shown) showing the phaseangle of each slot with respect to the modulated pole-number.
机译:986,379。发电机的绕组布局。国家研究开发公司。 1963年4月4日[1962年4月24日],编号15612/62。标题H2A。在通过施加单极性振幅调制波而施加到三相绕组的整体通过极性振幅调制来改变极点的系统中,获得了两个调制极数,其中一个是通过使用具有奇数的调制波来实现的。一个周期,另一个是通过使用具有偶数个周期的调制波。每个相绕组分为四个部分,绕组以一个极数(最好是最低极)的四平行星形连接,中间极数以串联-并联星形连接,第三极数以串联星号或三角形连接。 (最好是最高的)。图7a显示了一个8极,120度扩展绕组,分布在18个槽中,每个相的线圈组交替为每个极对一对和两个线圈,以及原始相序A,C,B。调制运算符MM表示线圈在此运算符下反转,并显示7周期调制波,该波将绕组转换为6极。图7c示出了施加到相同绕组以产生4极的6周期调制波。在每个调制条件下,相位序列变为A,B,C。图7f(未显示)显示了9周期调制如何产生10个极点。还描述了(图7d,也未显示)这些绕组变换如何通过单周期调制与同一个绕组的4/6极变换相关,并且列出了四个极数的整体相互关系以图6a中的示意图的形式(未示出)。正确的反向时隙由时隙星形图确定。图7b,7e(未示出)示出了相对于调制极数的每个缝隙的相位角。

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