• Now, the coefficient that relates the amount of heat in to the temperature change is obviously going to be different for these two cases.

    在这两个例子中,很显然联系热量和温度变化的系数,是不一样的。

    麻省理工公开课 - 热力学与动力学课程节选

  • Also, we need to know how much individual stocks are correlated with rm; we measure that by the regression coefficient.

    我们必须清楚,有多少个股与市场总体收益率相关;,我们用回归系数,即β系数来表示。

    耶鲁公开课 - 金融市场课程节选

  • And so instead of defining efficiency the way you've got it written there, I'm going to define what's called something different for a refrigerator which is called the coefficient of performance.

    现在我们不用,效率的那个定义,我给出一个,有关制冷机的,新的定义,叫做制冷系数。

    麻省理工公开课 - 热力学与动力学课程节选

  • And then the repulsive term, some positive coefficient r and r to a very high number.

    然后排斥力,一些正系数,以及具有很大数值的。

    麻省理工公开课 - 固态化学导论课程节选

  • When I give you multiple of i and another multiple of i, there's some has got as its coefficient the sum of the two coefficients.

    如果我给你两个不同 i 矢量的倍数,就可以得到某个矢量,且它的系数是这两个系数的和

    耶鲁公开课 - 基础物理课程节选

  • So this is just going to be T2 over T1 minus T2, that's our coefficient of performance.

    这就是我们的,制冷系数。

    麻省理工公开课 - 热力学与动力学课程节选

  • And if that's equal to zero, that means that the Joule-Thomson coefficient for an ideal gas is also equal to zero. We're going to actually prove this later in the course.

    说明理想气体的,焦耳-汤姆逊系数也等于0。,详细的证明过程,会在以后的课上给出。

    麻省理工公开课 - 热力学与动力学课程节选

  • And we saw that, you saw that the Joule coefficient for an ideal gas was zero.

    我们会发现,你们也会发现,理想气体的焦耳系数是零。

    麻省理工公开课 - 热力学与动力学课程节选

  • but right now you're going to have to take it for granted. So, if the Joule-Thomson coefficient is equal to zero, just like we wrote, du = Cv dT du = Cv dT for an ideal gas, we're going to dH = Cp dT have dH = Cp dT for an ideal gas as well.

    但是现在请你们应该把它看成理所当然的,所以,如果焦耳-汤姆逊系数等于零,就像我们写的,对于理想气体,我们也可以得到对于理想气体。

    麻省理工公开课 - 热力学与动力学课程节选

  • And so they defined them, p after many experiments, the limit of this 0 delta T delta p and the limit of delta p goes to zero as the Joule-Thomson coefficient.

    他们定义了这些量,以及它们的范围,ΔT比Δ,Δp的极限趋近于,叫做焦耳-汤姆逊系数。

    麻省理工公开课 - 热力学与动力学课程节选

  • It is defined as rho= That's the correlation coefficient.

    定义为,rho等于xy的协方差比xy各自的标准差的乘积,这就是相关系数

    耶鲁公开课 - 金融市场课程节选

  • Again, I'm not going to spend much time on this, of the ith asset is the regression coefficient when you regress the return on the ith asset on the return of the market portfolio.

    再强调一次,我不打算花太多时间在这个等式上面,但要注意的是当你想将市场组合收益,but,the,β,回归到第i资产收益中去,第i资产β系数是线性回归方程的,回归系数。

    耶鲁公开课 - 金融市场课程节选

  • The Joule-Thomson coefficient is equal to zero.

    焦耳-汤姆逊系数等于。

    麻省理工公开课 - 热力学与动力学课程节选

  • This is real, unlike the Joule coefficient which is very small so that most gases have tiny Joule coefficients. So if you do a Joule experiment, you hardly measure a temperature change. With real gases, here you do actually measure it. You can feel it with your finger on your bicycle tire.

    系数那样小以至于,大多数气体的焦耳系数,都很小,所以如果你做焦耳实验,很难测量出温度的变化,对于真实气体,你可以测量它,你能通过手指按在,自行车轮胎上来感觉到它。

    麻省理工公开课 - 热力学与动力学课程节选

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