• 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

  • which is f , divided by the value of the x-axis here.

    斜率,而f是p趋于0时pV的极限。

    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

  • The mean proportion-- The mean of x/n, is equal to p.

    事件发生频率的均值,即x/n的均值,就等于p

    耶鲁公开课 - 金融市场课程节选

  • 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

  • And what we see here is now when we're combining the p, we have our 2 p x and our 2 p y orbitals that are lower in energy, and then our pi anti-bonding orbitals that are higher in energy.

    这里我们看到,当我们结合p轨道时,在低能处我们有,2px和2py轨道,π反键轨道在更高的能级处。

    麻省理工公开课 - 化学原理课程节选

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