• R/Cv OK, so that means that this is really instead of -1 R over Cv. it's really gamma minus one.

    现在,变成了γ

    麻省理工公开课 - 热力学与动力学课程节选

  • I can't remember their names either, but their last names begin with "R" and "S" and "A".

    我也记不住他们的名字,但他们的姓氏是由“R”,“S”和“A”开头的。

    积极参与俱乐部活动 - SpeakingMax英语口语达人

  • He urged revival of the slave-trade in the late 1850s, and he developed a theory of what he called warranteeism--w-a-r-r-a-n-t-e-e-I-s-m.

    他促成了十八世纪五十年代后期,奴隶交易的复苏,还自己发明了一套理论,名为抵押品主义

    耶鲁公开课 - 美国内战与重建课程节选

  • So if we want to talk about the volume of that, we just talk about the surface area, which is 4 pi r squared, and we multiply that by the thickness d r.

    如果我们要讨论它的体积,我们要用的是表面面积,也就是4πr的平方,乘以厚度dr

    麻省理工公开课 - 化学原理课程节选

  • And so, you know from your Newtonian mechanics, as you were learning in 8.01, the dynamic force here mv^2/r is mv squared over r.

    在8。01节对牛顿动力学系统的学习中,我们可以知道这里的运动受力,就是。

    麻省理工公开课 - 固态化学导论课程节选

  • We take this Cv and put in the exponent here R right. And we put this R up in the exponent here.

    我们把这个Cv提出来,放在这里的指数上,好吧?然后把。

    麻省理工公开课 - 热力学与动力学课程节选

  • Mathematically, it's done by taking the expression for R and differentiating everything in sight that can be differentiated as vector t.

    从数学上看是这样的,写出 R 的表达式,并对所有可以进行矢量微分的部分,对时间 t 求微商

    耶鲁公开课 - 基础物理课程节选

  • Some languages like English has a-- have a distinction between 'l' and 'r.' Other languages do not.

    某些语言,如英语,在"l"和"r"之间是有差别的,其他语言则没有

    耶鲁公开课 - 心理学导论课程节选

  • If they quote the rate on the mortgage, call that r Traditionally you would be paying monthly.

    如果给定贷款利率,记为r,通常你是每月还款

    耶鲁公开课 - 金融市场课程节选

  • There's also this backslash R. Anyone know what backslash R is?

    这还有\r,谁知道\r代表什么?

    哈佛公开课 - 计算机科学课程节选

  • So kind of that strange cursive r, and our n final is 2, R so 1 over 2 squared minus n initial, so 1 over 3 squared.

    因为我们可以在这里用到它,这个有点奇怪的花体。

    麻省理工公开课 - 化学原理课程节选

  • 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

  • R And we abbreviate that by calling it r, l by two quantum numbers, and an l as a function of little r, radius.

    我们把它简称为,两个指定的量子数n和,它是半径小r的函数。

    麻省理工公开课 - 化学原理课程节选

  • At infinity, there's no stored potential energy, and it drops off more and more negative as one over R.

    在无限远处,没有储存的势能,并且它向负方向减少,当距离超过R时。

    麻省理工公开课 - 固态化学导论课程节选

  • a perfectly spherical shell dr at some distance, thickness, d r, dr we talk about it as 4 pi r squared d r, so we just multiply that by the probability density.

    在某个地方的完美球型壳层,厚度,我们把它叫做4πr平方,我们仅仅是把它,乘以概率密度。

    麻省理工公开课 - 化学原理课程节选

  • So, we can do that by using this equation, which is for s orbitals is going to be equal to dr 4 pi r squared times the wave function squared, d r.

    用这个方程,对于s轨道,径向概率分布,4πr的平方,乘以波函数的平方,这很容易理解。

    麻省理工公开课 - 化学原理课程节选

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