And, in fact, if any electron comes in their midst, they'll capture it because the binding energy is so high.

事实上，如果电子从中间进来，它们会捕获它,因为束缚能是如此之大。

麻省理工公开课 - 固态化学导论课程节选

This is the remarkable thing about so many of Milton's similes: they're always bursting out of whatever critical or theological constraints that we work so hard to impose on them.

这是弥尔顿的比喻中的亮点：,它们总是能从我们强加的,无论多批判多神学的束缚中,挣脱出来。

耶鲁公开课 - 弥尔顿课程节选

And we know what that's equal to, this is something we've been over and over, ionization energy is simply equal to the negative of the binding energy.

而且你知道它等于什么，这是我们说过一遍又一遍的，电离能就等于,负的束缚能。

麻省理工公开课 - 化学原理课程节选

So I said that this technique was used to experimentally determine what the different binding energies or the different ionization energies are for the different states in a multielectron atom.

我说过，这项技术被用来,在实验上确定多电子原子的,各个不同态相应的束缚能,或者电离能。

麻省理工公开课 - 化学原理课程节选

And what we call the binding energy is this is what we saw on the last slide.

我们所说的束缚能,这个我们在上一张幻灯片中已经见过了。

麻省理工公开课 - 化学原理课程节选

And that's going to be equal to the negative the binding energy of 2 s in b, in neutral boron.

它应该等于中性硼原子中,2，s，电子的束缚能的负值。

麻省理工公开课 - 化学原理课程节选

So, what we call this is the third ionization energy, or the negative of the binding energy, again of the 2 s orbital, but now it's in boron plus 2 to we're starting with.

那么我们称它为第三电离能，或者负的束缚能，还是，2，s，轨道的，但现在我们是从正二价硼离子开始的。

麻省理工公开课 - 化学原理课程节选

And again, this is just the negative, the binding energy, when we're talking about the 2 p orbital.

再说一遍，这就是负的束缚能，当我们考虑，2，p，轨道的时候。

麻省理工公开课 - 化学原理课程节选

And what we say when we talk about the delta energy is I E 2 that this is going to be equal to i e 2, or the second ionization energy, or we could say the negative of the binding energy of a 2 s electron in b plus.

那么我们说,Δ，E，应该等于，或者说第二电离能，也就是正一价硼中，2，s，电子的,束缚能的负值。

麻省理工公开课 - 化学原理课程节选