• The song was a million-selling hit on the R&B charts in the 1960s, and over the years, it became Taylor's most-requested show tune.

    VOA: standard.2009.06.18

  • 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

  • And we can simplify this expression as saying negative e squared over 4 pi, epsilon nought r squared. Epsilon nought is a constant, it's something you might see in physics as well.

    也会遇到它,在这里,你可以就把它,理解为一个转换系数,我们需要做的。

    麻省理工公开课 - 化学原理课程节选

  • And we plug in our values and end up with mv squared mv^2/r-Ze^2/ over r minus Ze squared over And I am going to call this equation two.

    我们最后的结果,就是,我把这称为方程式二。

    麻省理工公开课 - 固态化学导论课程节选

  • Were going to make it for a mole of gas, T1 so it's R times T1, V and then we'll have dV over V.

    假设是有一摩尔气体,那么就是R乘以,然后有dv除以。

    麻省理工公开课 - 热力学与动力学课程节选

  • You might want to say in the real world, if you go to a movie theater for this R-rated movie, "Are you 18 and over or are you with a parent?"

    在现实世界中,你可能想说,如果你去电影院看R级电影,“你有18岁吗?,或者你跟随你的父母亲来的吗?“

    哈佛公开课 - 计算机科学课程节选

  • The most important result from last time was that if you took this r, and you took two derivatives of this to find the acceleration, d^2 r over dt^2, try to do this in your head.

    上节课最重要的结论,就是如果你把 r 写成这样,对 r 求两次导就能得到加速度,d^2 r / dt^2,心算一下

    耶鲁公开课 - 基础物理课程节选

  • 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

  • And then we can take the derivative with respect to temperature, it's just R over molar volume minus b.

    这样我们求,压强对温度的偏导数,结果等于R除以摩尔体积V杠减去b的差。

    麻省理工公开课 - 热力学与动力学课程节选

  • So, for example, if I have a sodium ion over here, and I have a chloride ion over here, where the distance from center to center r I'm denoting as r, this is nucleus to nucleus separation.

    所以,比如这有一个钠离子,和一个氯离子,它们中心与中心间的距离,我把它设为,这是原子核和原子和的间距。

    麻省理工公开课 - 固态化学导论课程节选

  • And that's going to be equal to negative z effective squared times r h over n squared.

    有效的z的平方,乘以RH除以n的平方。

    麻省理工公开课 - 化学原理课程节选

  • p1V1/R That p2 V2 over R, and then I have p1 V1 over R, the R's cancel out.

    就是p2V2/R除以,两个R消掉了。

    麻省理工公开课 - 热力学与动力学课程节选

  • If you get them backwards, logr you will integrate one over r and will get log r.

    如果你逆推的话,对1/r积分得到。

    麻省理工公开课 - 固态化学导论课程节选

  • One over R to the sixth will come in, and then jump off precipitously.

    /R的六次方会出现,然后陡然减少。

    麻省理工公开课 - 固态化学导论课程节选

  • So we know that we can relate to z effective to the actual energy level of each of those orbitals, and we can do that using this equation here where it's negative z effective squared r h over n squared, we're going to see that again and again.

    我们知道我们可以将有效电荷量与,每个轨道的实际能级联系起来,我们可以使用方程去解它,乘以RH除以n的平方,它等于负的有效电荷量的平方,我们将会一次又一次的看到它。

    麻省理工公开课 - 化学原理课程节选

  • We also know how to figure out the energy of this orbital, and we know how to figure out the energy using this formula here, which was the binding energy, -Rh which is negative r h, we can plug it in because n equals 1, so over 1 squared, and the actual energy is here.

    我们知道如何算出,这个轨道的能级,而且我们知道如何,用这个公式,算出能量,也即是结合能,等于,我们把n等于1代进来,所以除以1的平方,这就是能量。

    麻省理工公开课 - 化学原理课程节选

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