• 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

  • 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

  • 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

  • But it doesn't actually cost as much energy as you might think, because in this s orbital here we have a paired electron situation where we're moving up to a p orbital where the electron is no longer paired, so it won't feel quite as much electron repulsion, but nonetheless, this is going to cost us energy.

    但它消耗的并没有,你们想象的那么多,因为s轨道里我们电子是配对的,当我们把,电子移到p轨道,电子不再配对,所以它不会感受到那么多的电子排斥,但尽管如此,这个过程还是要消耗能量的。

    麻省理工公开课 - 化学原理课程节选

  • 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

  • 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

  • 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

  • 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

  • STUDENT: from the T delta V p to the delta p here?

    学生:,从TΔV到这里的Δ

    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

  • 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

  • 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 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

  • 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

  • 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

  • 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

  • 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

  • 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

  • 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

  • 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

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