• And one thing I want to tell you to start out with is something about this c h 3 group here.

    有一点需要告诉大家的是,从这个一个碳原子和三个氢原子的组合开始。

    麻省理工公开课 - 化学原理课程节选

  • Pressure has dropped out of the picture completely here. So there is no p dependence here.

    理想气体的H只是温度的函数,这对于真实气体来说是。

    麻省理工公开课 - 热力学与动力学课程节选

  • stdio h This file here is called standard I/O or stdio.h and this is just another text file someone else wrote many years ago and by using that line of code there, I'm telling the computer, give me acces to this code that this other person wrote that's in that file.

    在这里的头文件称为标准输入输出文件或,这是由某位前人编写的文本文件,我们只需要刚才所述的一行代码,就能告诉电脑,让我连接到,这个前人在那个文件中写的代码。

    哈佛公开课 - 计算机科学课程节选

  • So, the very important conclusion that nu Einstein made here is that energy is equal to nu h times nu, or that h times nu is an actual energy term.

    做出的重要结论就是能量,等于h乘以,或者说h乘以,是一个能量项。

    麻省理工公开课 - 化学原理课程节选

  • X This is H. We've got one "x" here.

    这是H,我们得到了一个。

    麻省理工公开课 - 固态化学导论课程节选

  • And there's actually a way that we can make predictions here, and what I'll tell you is molecular orbital theory predicts that h e 2 does not exist because it's not stabilized in terms of forming the molecule.

    其实我们有一种办法可以做出预测,我要告诉你们的是分子轨道,理论预测He2不存在,因为它形成分子不稳定。

    麻省理工公开课 - 化学原理课程节选

  • OK, delta H is delta of u plus pV. By definition that's how we define enthalpy up here.

    好,ΔH=Δ,根据定义,这就是我们。

    麻省理工公开课 - 热力学与动力学课程节选

  • du But here you've got pressure constant. du, T this is du, not H here. du/dT is only equal Cv to Cv when the volume is constant, not when the pressure is constant.

    这里是压强横笛,du,这是,不是H,偏U偏,只在体积恒定时等于,而不是压强恒定时。

    麻省理工公开课 - 热力学与动力学课程节选

  • So we are really looking at this reaction here H+ for ionization. It is H gas neutral goes to H plus in the gas phase plus the electron. And, furthermore, we can have multiple ionization energies.

    所以我们真正看到的是,电离,它是在气相中H变为,和电子的过程,还有,我们能电离能加倍。

    麻省理工公开课 - 固态化学导论课程节选

  • So here, I'm going to have delta H, is just the sum for all the products of delta heat of formation right? Here I'm going to put together all the products. So this is a positive heat of formation.

    所以这里△H就是所有生成物的,生成热的和,对吧?这里,我要把元素组合成所有这些,生成物,所以这里是正的生成热。

    麻省理工公开课 - 热力学与动力学课程节选

  • 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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