u0442u0440u0435u0445u0444u0430u0437u043du0430u00a0 u0434u0432u0443u0445u0441u043bu043eu0439u043du0430u00a0 u0434u0440u043eu0431u043du0430u00a0 (q = 4.5) u043fu043eu043bu044eu0441u043eu043fu0435u0440u0435u043au043bu044eu0447u0430u0435u043cu0430u00a0 against 2p1 / 2p2 = 2 / 1 phase wire connection schemes or / y / yy yy u0432u044bu043fu043eu043bu043du00a0u0435u043cu0430u00a0 at z = 6u04402q u043fu0430u0437u0430u0445 of Nu043au0433 = 6u04402 u043au0430u0442u0443u0448u0435u0447 for groups with a step out on u043fu0430u0437u0430u043c u0443u043fz / 2p1 at division of each phase in two parts, with the odd groups in one, even in the other and further the medium the points in each phase, u043eu0442u043bu0438u0447u0430u044eu0449u0430u00a0u0441u00a0 orderthe 2p1 / 2p2 = 3 / 2, 8 / 4, 12 / 6 concentric group of odd numbered coils are u043fu00a0u0442u0438u043au0430u0442u0443u0448u0435u0447u043du044bu0435 steps u0443u043fi = 11 - 2 (i - 1) numbers of turns (1 - x) wu043a coils with i = 1, 5 and (1 + x) wu043a coils with i = 3, and even che u0442u044bu0440u0435u0445u043au0430u0442u0443u0448u0435u0447u043du044bu0435 - 'u043fi = 10 - 2 (i - 1) with the number of cycles (1 + x) wu043a coils with i = 3, with wu043a u0432u0438u0442u043au0430u0445 other control groups, where z = 27 u0434u043bu00a0 2u04401 / 2u04402 = 4 / 2, z = 54 u0434u043bu00a0 2u04401 / 2u04402 = 8 / 4, z = 81 u0434u043bu00a0 2p1 / 2p2 = 12 / 6, (i = 1,...5 - the number of coils in the group u043du0430u0447u0438u043du0430u00a0 with the outside, 2wu043a - the number of turns of each groove in the value of x = 0.52.
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