• But we've defined the enthalpy of those elements in their stable state at room temperature and pressure as zero, right?

    但我们已经定义了这些,元素处于它们室温常压下,最稳定的状态时的焓为,对吧?

    麻省理工公开课 - 热力学与动力学课程节选

  • And that's consistent with other things that we've seen, Remember the whole thing about the perfect crystal at zero degrees Kelvin has zero entropy It's completely ordered.

    我们看到的其他东西自洽吗?,想想摄氏度下的,完美晶体的熵为,这是完全有序的。

    麻省理工公开课 - 热力学与动力学课程节选

  • So that should make sense, because we saw no energy difference between the actual atoms and the molecules.

    这很好理解,因为我们看到,原子分子的能量差为

    麻省理工公开课 - 化学原理课程节选

  • First of all, happiness is a positive sum game-- it's not a zero sum game.

    首先,快乐是正游戏-,不是零和游戏。

    哈佛公开课 - 幸福课课程节选

  • We've already talked about how security selection is a zero-sum game.

    我们已经讨论过,证券选择是个零和博弈

    耶鲁公开课 - 金融市场课程节选

  • In the language, if I can switch to the language of modern economics, one could say that for Thrasymachus politics is a zero-sum game.

    换个领域的词汇,让我用现代经济学的话来说,这可能将,Thrasymachus,式的政治,喻成一场零和游戏。

    耶鲁公开课 - 政治哲学导论课程节选

  • So, you remember from last time radial nodes are values of r at which the wave function and wave function squared are zero, so the difference is now we're just talking about the angular part of the wave function.

    你们记得上次说径向节点在,波函数波函数的平方,等于的r的处,现在的区别是我们讨论的是,角向波函数。

    麻省理工公开课 - 化学原理课程节选

  • SdT This has minus T dS minus S dT, but the dT part is zero because we're at constant temperature.

    这一项包含负的Tds,但是dT的部分等于,因为温度为常数。

    麻省理工公开课 - 热力学与动力学课程节选

  • We discovered that the quantity dA, under conditions of constant volume and temperature, dA TS And A is u minus TS.

    我们发现在恒定的体积温度下,亥姆赫兹自由能的变化,小于,is,less,than,zero。,亥姆赫兹自由能A等于内能u减去。

    麻省理工公开课 - 热力学与动力学课程节选

  • It's not even a zero-- or rather if I have less, you'll have less- that's a negative sum game-- or a zero sum game-- if I have more, you'll have less- it's a fixed pie.

    甚至不是一个…,或者我更少,你也会更少,那也是负游戏-,或零和游戏,我更多,你就会更少-,饼就那么大。

    哈佛公开课 - 幸福课课程节选

  • So dS for u and V fixed is greater than zero.

    所以当内能u体积V固定时,dS大于

    麻省理工公开课 - 热力学与动力学课程节选

  • That's the some of delta u in these two paths and if we look at delta u in just path A, it's zero.

    这是这两条路径△U的,如果我们要看路径A的△U,它也是

    麻省理工公开课 - 热力学与动力学课程节选

  • du=0 So du is equal to zero because dq and dw are both zero.

    因此,因为dqdw都等于

    麻省理工公开课 - 热力学与动力学课程节选

  • H We also saw that dS for constant H and p was greater than zero.

    我们同样可以看到如果保持自由焓,压强不变熵的变化dS也是大于的。

    麻省理工公开课 - 热力学与动力学课程节选

  • If security selection is a zero-sum game, the amount by which the winner wins equals the amount by which the loser loses -winners and losers being defined by performance after a security selection that has been made -well, that sounds like a zero-sum game.

    如果证券选择是一个零和博弈,赢方赚得的金额,等于输方赔付的金额,谁赢谁输取决于,双方投资在证券选择后的表现,这听起来确实像个零和博弈

    耶鲁公开课 - 金融市场课程节选

  • U It's u, because u is to q plus w right, heat and work, but it's adiabatic. So there's no heat, exchange with the environment, and it's constant volume, so there's no p dV work, right.

    什么是?是U,因为,等于q加w,热量功,但这是绝热的,所以系统与环境间没有热量交换;,同时它是灯体的,所以也没有pdV形式的功。

    麻省理工公开课 - 热力学与动力学课程节选

  • du/dV under constant temperature was equal to zero for an ideal gas. And by analogy, we expect the same thing to be true here, because enthalpy and energy have all this analogy going on here. So let's look at an ideal gas.

    偏U偏V在恒温下等于,可以类比,我们希望在这里也一样,因为焓能量有很强的类比性,让我们看看理想气体,【理想气体】

    麻省理工公开课 - 热力学与动力学课程节选

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