• "Petit" -- p-e-t-i-t comes from the French word for small.

    VOA: special.2009.08.31

  • pV=RT p plus a over v bar squared times v bar minus b equals r t. All right if you take a equal to zero, these are the two parameters, a and b. If you take those two equal to zero you have p v is equal to r t.

    我们就回到,也就是理想气体,状态方程,下面我们来看看,这个方程。

    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

  • "Haitian nationals will be able to remain in the United States legally, be able to obtain authorization to work legally in the United States, be eligible to obtain permission to travel outside the United States, and return to their T.P.S.status."

    VOA: special.2010.02.01

  • That's why we said on the personality theory,as we went ahead in time, once the P-functioning stops,I don't exist anymore.

    这就是为什么根据人格理论的说法,随着时间流逝,人格功能停止,我也不再存在。

    耶鲁公开课 - 死亡课程节选

  • U.S.State Department Spokesman P.J.Crowley says Amiri met with authorities while in this country, but wouldn't say if the Iranian gave up any secrets.

    VOA: standard.2010.07.13

  • In that case point p 1 doesn't correspond to this point, it actually corresponds to the point of radius 2 and angle 1, which is about here.

    基本上也就是说这是第一个点1,这是第二个点,把它们的值加到一起,然后我就得到了目标点,好,这听起来挺不错的。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • It's true for any gas, and if I remove this limit here, r t is equal to p v bar, I'm going to call that an ideal gas.

    这样的气体被称作理想气体,这就是理想气体的性质,理想气体的涵义是什么?

    麻省理工公开课 - 热力学与动力学课程节选

  • That's different when you have continuous values-- you don't have P because it's always zero.

    和离散型随机变量的分布不同的是,连续型随机变量的分布中,某一点的概率值始终是零

    耶鲁公开课 - 金融市场课程节选

  • Texts that insist on a central sanctuary are probably Josiah's time or later. And there are many sections of P that don't seem to assume a central sanctuary.

    一些章节坚持中心圣所,则可能在约西亚或之后时期,P资源中有很多部分,并没有呈现出一个中心圣所。

    耶鲁公开课 - 旧约导论课程节选

  • Again, so as we don't get confused, normally we use S for strategy, but let's use P since they're prices.

    为了避免混淆,通常我们用S表示策略,但是这次我们使用P,因为它代表价格

    耶鲁公开课 - 博弈论课程节选

  • Well, the initially tempting thing to say is not only aren't you broken, but you're actually engaged in P-functioning.

    首先要说的会是,不仅你没有被破坏,还有确实,拥有人格功能性。

    耶鲁公开课 - 死亡课程节选

  • Well,you can't tell by thinking about the normal case, because the B-functioning and the P-functioning stop at the same time.

    这从通常的例子中是研究不出来的,因为生理功能和人格功能同时结束。

    耶鲁公开课 - 死亡课程节选

  • But if death means permanent cessation of P-functioning, then it turns out the dead weren't really dead after all.

    但如果死亡指的是人格功能性的永久停止,那就说明死者并非死去。

    耶鲁公开课 - 死亡课程节选

  • It's somewhat different when we're talking about the p or the d orbitals, and we won't go into the equation there, but this will give you an idea of what we're really talking about with this radial probability distribution.

    当我们讨论p轨道或者,d轨道的时候会有些不同,我们那时不会给出方程,但它会给你们一个,关于径向概率,分布的概念。

    麻省理工公开课 - 化学原理课程节选

  • So the most basic answer that doesn't explain why is just to say well, the s orbital is lower in energy than the p orbital, but we now have a more complete answer, so we can actually describe why that is.

    所以最基本的答案是那没有解释,所以我们事实上可以描述,为什么是那样,但是我们现在有一个更复杂的答案,又是有效电荷量。

    麻省理工公开课 - 化学原理课程节选

  • If T is less than T inversion, you have the opposite case, and dT/dp is greater than zero.

    如果T比转变温度低,情况就相反,偏Tp大于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • TdS It comes from the fact that dq reversible is T dS, pdV and dw reversible is minus p dV.

    这个结论来自于:可逆过程下dq等于,做功dw等负的。

    麻省理工公开课 - 热力学与动力学课程节选

  • Remember, we didn't hybridize the 2 p y orbital, so that's what we have left over to form these pi bonds.

    记住,我们并没有杂化2py轨道,这是我们剩下的那个行成了π键。

    麻省理工公开课 - 化学原理课程节选

  • It can't just be a matter of not P-functioning.

    肯定不止和人格功能性有关。

    耶鲁公开课 - 死亡课程节选

  • But we don't have a P-functioning body.

    但这不是具有人类能力的肉体

    耶鲁公开课 - 死亡课程节选

  • du external dV minus T surroundings dS is less than zero.

    加上压强p,du,plus,p,乘以dV减去环境温度T乘以dS小于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • G P Thompson And it turns out that G.P. Thompson, and I'm sure this wasn't the case, but I like to think of it as a little bit of child rebelling against the father.

    结果是他的儿子,我确定不是那种情况,但是我们认为他在小时候,对他的父亲可能有一点叛逆。

    麻省理工公开课 - 化学原理课程节选

  • So the proposal that death is a matter of permanent cessation of P-functioning versus temporary, that doesn't seem like it's going to do the trick.

    所以说死亡只永久地,停止人格功能性的这个说法,也不是正确的。

    耶鲁公开课 - 死亡课程节选

  • So when I type, I'm sorry, I shouldn't say type, c point although I would have typed it, p dot x, here's what basically happens.

    处于特定点的实例的这个概念,我知道它来自于这个类,这个类,when,I,write,因此当我输入,抱歉,我不该说输入的,当我写,虽然我需要输入它,p,x的时候。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • Normally I couldn't do that Vdp because this term would have p dV plus V dp, but we've specified the pressure is constant, so the dp part is zero.

    一般情况下我不能这么写,因为这一项会包含pdV和,但是我们已经假定压强为常数,所以包含dp的部分等于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • I'm going to call it r. It's going to be the gas constant, and now I have r times t is equal to the limit, p goes to zero of p r.

    如果去掉p趋于0的条件,在有限压强下都,保持RT=pV的关系。

    麻省理工公开课 - 热力学与动力学课程节选

  • v We don't know what it is yet. In order to change this from a p to a V, you have to use the chain rule. So let's use the chain rule.

    为了把这里的p变成,我们需要利用链式法则,好,让我们使用链式法则。

    麻省理工公开课 - 热力学与动力学课程节选

  • We want a relationship in p-V space, not in T-V space. So we're going to have to do something about that. But first, it turns out that now we have this R over Cv.

    我们想要p-V空间中的结果,而不是T-V空间中的,因此需要做一些变换,先来看现在的关系,它跟R/Cv有关。

    麻省理工公开课 - 热力学与动力学课程节选

  • That's it. Again, these other p dxy dyz - or the d x y, d y z, those are going to be those more complicated linear combinations, you don't need to worry about them.

    同样,这些p轨道,或者,它们是一些,很复杂的线性组合,你们,不用管它。

    麻省理工公开课 - 化学原理课程节选

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