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从上式可以看到,总能量除了两个电感各自产生的磁场能外,还额外多出一份互感能量 ,跟电感飞轮的磁场能类似,互感能量的本质也是电磁惯性,我们可以想象,在两个电感飞轮中间增加了一个小飞轮,并且这个小飞轮用皮带分别与两个飞轮连在一起。因为飞轮的轮动方向(电流方向)相同,增加的飞轮相当于增加了整个系统的电感惯量。
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The expression "free, white, and twenty-a single" goes back again at least somewhat farther then 1854, when the initial by 3rd editions of
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从上图可以看出,因为存在励磁电感支路,拥有电抗性,全耦合变压器必然会改变输入信号的相位,在电路分析中,要把励磁电感当作只会自感的普通电感,考虑进去。
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我们需要检查两个线圈的物理缠绕方向,然后利用楞次定律与右手准则来判定感应电压的极性。但是,电路图中画不出线圈的缠绕结构,为了简化,我们常常采用同名端规则,即在两个磁耦合线圈的一端标上一个圆点,表示电流由该点流入线圈时产生的磁通方向一致(磁通相助,或磁力线重合),如下图所示,红线为互为同名端:
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为了便于分析计算,我们可以把理想变压器拿掉,只需要把二次侧的阻抗等效变换到一次侧即可(除以n²),这就是变压器的 T 型等效电路: