• And for a couple of reasons, one this is the first P set where we're actually gonna give you code to work from.

    由于一些原因,这里是第一个习题集,在此我们提供了一些代码供大家参考。

    哈佛公开课 - 计算机科学课程节选

  • Well, presumably because whatever cognitive structures it takes in your brain to underwrite the ability to P-function, those cognitive structures have been broken, so they no longer work.

    大概是因为,无论你大脑中的什么认知结构,使得人格功能性成为可能,这种认知结构都被破坏了,它们不再继续工作。

    耶鲁公开课 - 死亡课程节选

  • I also want to assume for our present purposes that there's only pressure volume work going on, which is to say I want to put pdV p dV in here minus p dV for dw.

    同时假定,对于我们目前的目的而言,只有压强做功这就是说,我要把这里的dw替换为负。

    麻省理工公开课 - 热力学与动力学课程节选

  • So, it's very easy to calculate, however, the number of radial nodes, and this works not just for s orbitals, but also for p orbitals, or d orbitals, or whatever kind of work of orbitals you want to discuss.

    径向节点,的数量,这不仅对s轨道适用,对p轨道,d轨道,或者任何你们想讨论的轨道,都是适用的,它就等于。

    麻省理工公开课 - 化学原理课程节选

  • So, the work for this process is the integral, pdv or minus the integral, V1, V2, p dV.

    此过程中的做功等于负的积分,从v1到v2,外部。

    麻省理工公开课 - 热力学与动力学课程节选

  • So there's p v work and it's given by the integral minus p external dv or just the integral from one to two of dw.

    我们知道对于pv系统来说,功w可以写成黑板上的两种不同形式。

    麻省理工公开课 - 热力学与动力学课程节选

  • And it's p external and p external is zero, so there's no work.

    外部的p是零,所以结果是零,没有做功。

    麻省理工公开课 - 热力学与动力学课程节选

  • That's equivalent to doing the integral, and so, what we end up getting is that the reversible work v2 pdv is equal to minus integral V1, V2, p dV.

    这与刚才的积分过程效果相同,最后,我们得到的结论是可逆过程的功,是负的积分,从v1到。

    麻省理工公开课 - 热力学与动力学课程节选

  • 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.

    什么是零?是U,因为,等于q加w,热量和功,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

  • V Minus p2, V2. Minus p delta V. So the total work is the work from the left hand side plus the work on the right hand side, p1 V1- p2 V2 which is p1 V1 minus p2 V2.

    p2V2【w=-p2v2】,即负pΔ,所以全部的功就是,左边的功加上右边的功,等于。

    麻省理工公开课 - 热力学与动力学课程节选

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