• z So, this is what we find the actual z effective is for an electron in the helium atom.

    所以这就是我们得到了实际有效的,对于一个氦原子的电子。

    麻省理工公开课 - 化学原理课程节选

  • But what you should be able to do is take a look at a list of answers for what we're saying z effective might be, and determining which ones are possible versus which ones are not possible.

    但是你们应该能够做到的,是看一下这个可能的,有效电荷量的答案列表,并且确定哪些是可能的,哪些是不可能的。

    麻省理工公开课 - 化学原理课程节选

  • So our minimum that we're going to see is that the smallest we can have for a z effective 1 is going to be equal to 1.

    所以我们能够看到的,最小的有效电荷量,等于。

    麻省理工公开课 - 化学原理课程节选

  • So again, when we check these, what we want to see is that our z effective falls in between the two extreme cases that we could envision for shielding.

    所以当我们再一次检查这些时,我们想看到的是,有效电荷量处于两种极端案例中,这两种极端案例。

    麻省理工公开课 - 化学原理课程节选

  • z So the main idea here is z effective is not z, so don't try to plug one in for the other, they're absolutely different quantities in any case when we're not talking about a 1 electron atom.

    所以这里主要的观点是有效的z不同于,所以不要尝试将一个插入到另一个,当我们不在讨论1个电子的原子时,它们在任何情况下是绝对不同的量子数。

    麻省理工公开课 - 化学原理课程节选

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