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显然，交变电流的频率越高，软磁的磁化频率也就越高，同一时间因为剩磁和纠磁花费的电能就越多，产生的热量就越大，磁滞损耗也就越大。

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 变压器是怎么传递能量的？为什么需要励磁电流？负载大小会改变相位吗？我能随意改变匝数吗？

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我们知道，变压器的铁芯采用的是软磁材料。当线圈产生的磁场撤去后（电流变为零），理想的软磁铁芯中的磁畴理应全部回归原来的杂乱无序状态，整体不带磁性。如下图，右边是（通电线圈产生）外磁场磁化后，软磁材料内部的磁畴结构，撤去外磁场后，理应回归到左边的初始结构。

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考虑到两个绕组的电感不可能无限大，我们先用全耦合变压器对上述电路进行建模，初级线圈的电感 即为励磁电感，用来建立初始的交变磁场。这样，后端我们就可以使用理想变压器符号，来实现电压和负载阻抗的变比，如下图：

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