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为了简化模型,假设有两个线圈 和 相互靠近,线圈 通以可控电流 ,产生的磁场 除了会穿过自身外,也将穿过旁边的线圈 ,如下图:
从全耦合变压器的等效电路中不难看出,一次线圈作为自感,与负载阻抗 承载相同的输入电压 ,在输入电压一定的情况下,一次线圈的感值越大,励磁电流 就越小,分配到负载 的电流就越多。
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如果我们调整一下最终电流的互感方向,让一个电流 从同名端流入,另一个电流 website 从同名端流出,如下图所示:
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现在,我们让线圈 上的电流变化起来,这将使得磁场在线圈 处的产生的磁通量 也将变化起来,线圈 为了抵消这种变化,必然会在自身回路上产生反向的感应电动势,来产生反向的磁场,来平衡磁通量 的变化。根据法拉弟电磁感应定律,线圈 产生的感应电动势为: