• All right, so you can't get perfect efficiency, 0 but at least if you were able to go to zero degrees Kelvin, then you'd be all set.

    好吧,你得不到完美的效率,但至少如果能把温度降到,那你就万事俱备了。

    麻省理工公开课 - 热力学与动力学课程节选

  • If you could get to zero degrees Kelvin, you'd get perfect efficiency, 0 but you can't get to zero degrees Kelvin, you can't. Even if you have an infinite amount of resources, you can't get there.

    如果能达到,你就能获得完美的效率,但你得不到,得不到,即使你有无穷多的资源,你也做不到。

    麻省理工公开课 - 热力学与动力学课程节选

  • So, it turns out that we have zero nodes that we're dealing with when we're talking about a 3 d orbital.

    所以结果是,3d轨道没有节点。

    麻省理工公开课 - 化学原理课程节选

  • That's going to presumably be given--mathematically if we gave it a number, we'd slap a zero on that.

    如果用数学解释,给它一个数字,给它一个零。

    耶鲁公开课 - 死亡课程节选

  • 5 So similarly would there be the number 65 next to this then the corresponding number for V-I-D and then there's generally a special character at the end that looks like a zero that says end of string here.

    同样,A就是,接着再填上V-I-D对应的ASCII码,在最后还有添上一个特殊的字符,有点像0,代表这是该字符串结束。

    哈佛公开课 - 计算机科学课程节选

  • I can write this as d less than zero.

    我可以把这个写成的d小于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • But in sigma orbitals, you have no nodal planes along the bond axis, so if we had a nodal plane here, we'd see an area where the wave function was equal to zero.

    但在sigma轨道里,沿着轴向是没有节点平面的,如果我们有个节点,我们就会看到某个地方波函数等于0。

    麻省理工公开课 - 化学原理课程节选

  • We can look at the 2 p, which should have one radial node, and we just figured it out for the, excuse me, 3d for the 3 p has one radial node, and for the 3 d here, we should have zero radial nodes, we just calculated that.

    我们看2p,它有一个节点,我们已经知道对于,不好意思,是3p有一个节点,对于,它应该没有径向节点,我们刚刚算过这个。

    麻省理工公开课 - 化学原理课程节选

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