And the complete description, as I said, n l m is from n l and m.

我说过完整的描述，需要。

麻省理工公开课 - 化学原理课程节选

An electron. So now we have the complete description of an electron within an orbital.

电子，现在我们有了一个,轨道上的电子的完备描述。

麻省理工公开课 - 化学原理课程节选

So, kinematics is a complete description of the present.

运动学是对现在的完整描述

耶鲁公开课 - 基础物理课程节选

So, we have now a complete description of a wave function that we can talk about.

所以我们现在得到了，波函数,的完整描述。

麻省理工公开课 - 化学原理课程节选

So this is our complete description of the ground state wave function.

所以这是我们,对基态波函数的完整描述。

麻省理工公开课 - 化学原理课程节选

So we can completely describe an orbital with just using three quantum numbers, but we have this fourth quantum number that describes something about the electron that's required for now a complete description of the electron, and that's the idea of spin.

所以我们可以用３个,量子数完全刻画轨道，但我们有这第四个量子数,来完整的,描述电子，这就是自旋的概念。

麻省理工公开课 - 化学原理课程节选

So let's just think exactly what this means, and that means that if we take away function and we define it in terms of n, l and m sub l, what we're defining here is the complete description of an orbital.

让我们来考虑一下这是什么意思，这是说如果我们不考虑波函数,而是用ｎ，ｌ，ｍ下标ｌ来定义它，我们定义的,是一个轨道的完整描述。

麻省理工公开课 - 化学原理课程节选