• No, the most immediately shocking aspect of the poem was its style, and we have to look at the actual poetic form by which this poem is constructed because the poetic form is absolutely integral to its meaning.

    不是这样的,此诗最先让人感到震惊的是它的格式,我们需要看一下这首诗遵循的诗体,因为诗体与其意是一体的。

    耶鲁公开课 - 弥尔顿课程节选

  • We want to integrate. So let's take the integral of both sides, going from the initial point to the final point.

    分别从初态,到末态做积分,消去微分。

    麻省理工公开课 - 热力学与动力学课程节选

  • And if it is going to be a standing wave then this must be an integral number of wavelengths.

    如果这有个驻波的话,那么周长就是个整数。

    麻省理工公开课 - 固态化学导论课程节选

  • Just take a look: if this is 9, 5 divided by 9 is always going to be 0 point something, and if you thus have two integers and you're rounding down, which is what happens when you do integral math we're using this operator, I'm going to get zero times whatever.

    稍微看一看:如果这是9,5除以9会得到,0点几,如果你用两个整型数,你舍去小数,这就是当你们,用整型数使用这个操作的所发生的事情,我将得到数值0乘以任何一个数字。

    哈佛公开课 - 计算机科学课程节选

  • So there are two components integral and inseparable in the concept of holiness: initial assignment of holy status by God and establishment of rules to preserve that holy status, and secondly, actualization of that holiness by humans through the observance of the commandments and rules that mark that thing off as holy.

    因此在神圣这一概念中,有两个组成部分,一个是上帝最初形成的神圣状态,和为了保持这个神圣状态而建立的规则制度,第二个是,人们通过遵守戒律,而将神圣现实化到生活中,将神圣的事物标记出来。

    耶鲁公开课 - 旧约导论课程节选

  • We know that charge is equal to the integral of current times the time. And he knows the current, he knows how much time and then he weighs this.

    我们知道电量等于电流,对时间的积分,他知道电流,他也知道时间,然后他测量这个。

    麻省理工公开课 - 固态化学导论课程节选

  • The reason for inexact doesn't mean it's a crummy measurement, t means that it's path dependent, and so the value of this integral depends on how you get from one to two.

    这是因为它是,与积分路径有关的,因此这里的积分值,取决于从一端到二端的,具体路径。

    麻省理工公开课 - 热力学与动力学课程节选

  • Even if the thing that you really want is an integral that would be difficult to evaluate.

    即使需要计算的,是一个很难的积分。

    麻省理工公开课 - 热力学与动力学课程节选

  • And so just like here, w2 now q2 is minus w2, that's integral going from three to four p dV.

    就跟这儿一样,现在是q2等于负,等于从第三点到第四点过程的pdv的积分。

    麻省理工公开课 - 热力学与动力学课程节选

  • I'm going from V2 to V2 dv - what do you think this integral is? Right, W1 so this is easy part, zero here.

    这样才保证了过程的可逆性,下面来计算,路径1的功。

    麻省理工公开课 - 热力学与动力学课程节选

  • du So, we can also write delta u as integral from 1 to 2 of du.

    我们也可以将Δu写成,从1到2的积分。

    麻省理工公开课 - 热力学与动力学课程节选

  • And, if you ever get confused, the way to remember these is that you know energy is the integral of a force moving through a distance.

    如果你感到很困惑的话,可以这么来记,能量是在沿力的方向进行路径积分。

    麻省理工公开课 - 固态化学导论课程节选

  • Going around in a cycle the integral of dq over T is less than or equal to zero.

    对一个循环过程作dq除以T的积分,小于等于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • V1 This first integral is zero V1 to V1, then I get minus p2 times V2 minus V1 or p2 times V1 minus V2. Again, 0 a positive number.

    先保持体积为,对pdV积分1,然后对p2dV从V1到V2积分,第一部分积分为。

    麻省理工公开课 - 热力学与动力学课程节选

  • /T We've got Cv integral from T1 to T2, dT over T is equal to minus R from V1 to V2 dV over V.

    左边是Cv乘以,从T1到T2对dT积分。

    麻省理工公开课 - 热力学与动力学课程节选

  • So, if you're doing physics, x2 work is the integral of force, dx, x1 to x2.

    如果你正在干活,功就是力的积分,从x1,到。

    麻省理工公开课 - 热力学与动力学课程节选

  • So it's nR integral from V1 to V2 dV over V.

    即nR除以V乘以dV从V1到V2的积分。

    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

  • 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

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