• So I went home to Alabama. Moments ago, at 2:25 P.M., as President Reaganwas leaving the...

    VOA: standard.other

  • And what I want to point out here is this angular dependence for the p orbitals for the l equals 1 orbital.

    这里我要指出的是,l等于1的p轨道随角度的变化。

    麻省理工公开课 - 化学原理课程节选

  • But other days I'll have class from 10 a.m to 6 p.m.

    但是其他时候,我会从早晨十点一直上课到下午六点。

    很好奇住宿生活 - SpeakingMax英语口语达人

  • "Friends,I interrupt the ball game, and I come to you with a heavy heart to make the announcement that at 6:45 p.m.tonight, Coach John Wooden passed away at Ronald Reagan UCLA hospital.

    VOA: standard.2010.06.05

  • P dV is equal to R dT. pV = RT for 1 mole, pdV=RdT so I just take dV here.

    对等压过程,那么。

    麻省理工公开课 - 热力学与动力学课程节选

  • 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

  • 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

  • And I'm going to rewrite it now with that P expanded out.

    我把它代入到这个表达式然后展开

    耶鲁公开课 - 博弈论课程节选

  • 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

  • Roughly speaking,the answer,presumably, on the physicalist view,is going to be something like-- if I'm alive when we've got a P-functioning body, roughly speaking,I die when that stops happening, when the body breaks and it stops functioning properly.

    粗略地说,从物理主义者角度看来,答案大概就是-,如果我有人格功能我就活着,粗略地说,那种人格功能停止时我就死了,当身体被破坏,机能停止时,我就死了。

    耶鲁公开课 - 死亡课程节选

  • I have two electrons now to occupy the p-orbitals.

    如果P轨道有分布了两个电子。

    麻省理工公开课 - 固态化学导论课程节选

  • It's reasonable because it's meant TMP for temporary purposes just to call it temp or T-M-P for short, X and I can define temp as -- why don't I set it as equal to X, initially, because now that I've stored X in a separate chunk of memory, I can now change its value and then I can say Y gets, not X, but temp, and so now I've actually swapped these values.

    这是合理的,因为它是为,暂时的目的,只要叫它Temp或简称它为,我可以定义temp为--为什么我不把它设定为等于,最初的,因为现在我把X存储在一个单独的内存块中,我现在可以改变它的值,然后我说Y等于,不是X,而是temp,所以现在我交换这些值。

    哈佛公开课 - 计算机科学课程节选

  • OK, now, if I actually do this, and I'm going to show you the example, I just, what did I type over there, I got p was a c point.

    传入了其他的参数,好,现在,如果我,实际上要做这个的话,我要给大家看个例子。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • If I want to get values back out, p I could in fact simply send to that instance a message, in this case I could say p dot x.

    我就是,我刚刚在这里输入的,我得到了一个c,point的实例,如果我想把值取出来,实际上我可以。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • And we can think about here we did get that energy for electron promotion that I mentioned before 2p where we moved the electron from the 2 s to the 2 p.

    我们可以考虑,我们从哪里,获得了能量使电子,从2s激发到。

    麻省理工公开课 - 化学原理课程节选

  • Some of you might be saying in your heads, wait a second, I happen to know, I happen to remember from high school, p have different energies then, for example, s orbitals.

    有些人,可能会心里想:,等等,我记得,高中的时候学过,轨道,that,p,orbitals,和s轨道,的能级是不同的。

    麻省理工公开课 - 化学原理课程节选

  • 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

  • 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

  • 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 if I take p times V to the gamma, anywhere on the path, it's going to be equal to the same relation This is going to be true for any point on the path.

    结果都,将等于,初态点的,只要在这条路径上。

    麻省理工公开课 - 热力学与动力学课程节选

  • If I'm not P-functioning, do we have to then say I'm dead?

    如果我没有人格功能性,可以说我死了吗?

    耶鲁公开课 - 死亡课程节选

  • And I can give a name to that, so c p 1 and c p 2 are both going to point to that.

    为这个实例分配了空间,现在它是空的,实际上也不完全是空的。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • I also want to assume for our present purposes that there's only pressure volume work going on, which is to say I want to put pdV p dV in here minus p dV for dw.

    同时假定,对于我们目前的目的而言,只有压强做功这就是说,我要把这里的dw替换为负。

    麻省理工公开课 - 热力学与动力学课程节选

  • So I changed the colors here to show that these are 2 p orbitals with an opposite phase or an opposite sign.

    我这里换了一种颜色,表示2p轨道,不同的相位或者是正负号。

    麻省理工公开课 - 化学原理课程节选

  • I'm pressing on the gas. So I expect that to be a positive number. The pressure is constant 0 p. The V goes from V1 to zero.

    我们对气体加压,所以这应该是一个正数,压强是常数,p,V从V1变成。

    麻省理工公开课 - 热力学与动力学课程节选

  • So instead of p, here I'm going to put nRT over V.

    于是把p写成。

    麻省理工公开课 - 热力学与动力学课程节选

  • So what we're going to do is take the equations for those two lines, so here's one of those equations and here's the other one, set the P in those equations equal to X, I've got two equations in one unknown, I'm sorry, I've got one equation and one unknown.

    接下来我们只需要,列出这两条线各自的方程,也就是这个方程和这个方程,把方程中的P换成X,我就得到了两个等式和一个未知数,错了,是一个等式和一个未知数

    耶鲁公开课 - 博弈论课程节选

  • And I know pdV what those turn out to be. It's minus S dT minus p dV.

    我们知道,这最终就是负SdT减去。

    麻省理工公开课 - 热力学与动力学课程节选

  • We can also look at them coming in from the side, and that's what I tried to depict here where you can actually see in pink is the p orbital.

    我们也可以看到它们从这个方向来,这就是我这里试图描绘的,你可以看到粉红色的p轨道。

    麻省理工公开课 - 化学原理课程节选

  • 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

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