pV=RT dT here because the pressure is constant, dV=RdT/p so dV is equal to R over p dT.

因为对1摩尔气体有，于是。

麻省理工公开课 - 热力学与动力学课程节选

Remember, we don't do a one-to-one correlation, because p x and p y are some linear combination of the m plus 1 and m minus 1 orbital.

记住，我们不需要把它们一一对应，因为ｐｘ和ｐｙ轨道是,ｍ等于正负１轨道的线性组合。

麻省理工公开课 - 化学原理课程节选

All right, c p 1 dot y, x I've said assign that to the value 2, 2,0. So now c p 1 has inside of it an x and y value.

一个特定的版本，我现在命名了一个内置变量，并给它赋值了,我刚刚做的也就是给它。

麻省理工公开课 - 计算机科学及编程导论课程节选

V So this nR over V. And then, using the relation again, T we can just write this as p over T.

恒定温度下的dp/dT等于nR除以，再次利用状态方程，可以把它写成p除以。

麻省理工公开课 - 热力学与动力学课程节选

So it is very hard to understand P's silence in this regard, if it stems entirely from the post-exilic, priestly circles.

很难理解P资源在这一方面的缄默，如果它来源于流放后时期，牧师圈子。

耶鲁公开课 - 旧约导论课程节选

And so, if we look at our box notation, we've got three states in the p orbital.

因此，如果我们看看我们的盒子符号，在p轨道有三个状态。

麻省理工公开课 - 固态化学导论课程节选

He said he could do it if we could arrange to meet after 3:00 p.m., so I'm going to--on a Monday or a Wednesday, perhaps at 3:00 p.m. or later.

他说下午三点以后也许可以,所以我想安排在周一或周三,下午三点或更晚

耶鲁公开课 - 金融市场课程节选

And these shapes of p orbitals probably do look familiar to you, most of you, I'm sure, have seen some sort of picture of p orbitals before.

这些ｐ轨道的形状你们可以能已经很熟悉了，我相信大部分人，都看过ｐ轨道的图片。

麻省理工公开课 - 化学原理课程节选

Although they will be engaged in P-functioning later on, it's not true right now that they can engage in P-functioning.

虽然他们后来能够有人格功能性，但是现在却没有。

耶鲁公开课 - 死亡课程节选

OK, in fact if we look at this, if I say, print of p, it prints it out in that form.

好，实际上如果，我们来看看这个，如果我输入，p的显示。

麻省理工公开课 - 计算机科学及编程导论课程节选

If I do the following, and I say, I'm going to assign p 1 to be p 2.

现在我要去做一些改动，这是为了让大家,更好的理解这一点。

麻省理工公开课 - 计算机科学及编程导论课程节选

So, you turned in p-set 3 today, but we'll have the answers posted for you this afternoon, so you can start studying from p-set 3, even as early as tonight, if you want to, because those answers will be there for you.

今天大家应该要交第三次作业了，而我们会在今天下午将答案给大家贴出来，这样大家就可以尽快开始复习第三次作业的内容了，甚至今天晚上就可以开始，如果你需要的话，这些答案将会给你一些帮助。

麻省理工公开课 - 化学原理课程节选

px So we're talking about pi carbon 2 p x, 2px because it's the x axes combining to carbon 2 p x.

我们讨论的是π碳，因为它在x轴结合成碳。

麻省理工公开课 - 化学原理课程节选

So we're going to have to revise the P-functioning or the end of P-functioning theory of death.

我们要修改人格功能,或者人格功能的完结代表死亡这一说法。

耶鲁公开课 - 死亡课程节选

p We want p equal to p external for the entire expansion, p2 and p external is decreased steadily from p1 to p2.

在膨胀过程中保持p等于外部，外部p很快从p1衰减到。

麻省理工公开课 - 热力学与动力学课程节选

Remember the equation of state for Van der pV=nRT Waal's gas is not pV is equal to nRT, but p plus the attraction term.

记住范德瓦尔斯气体的状态,方程不是，而是p加上一个吸引项。

麻省理工公开课 - 热力学与动力学课程节选