• The Federal Reserve suggested again that short-term interest rates are likely to remain near zero for some time.

    VOA: special.2009.01.31

  • If the time you are interested in is not zero, you're allowed to cancel it and get the time from here.

    如果你们关注的解不是零时刻,那么就可以忽略它,然后从这里解出时间

    耶鲁公开课 - 基础物理课程节选

  • It's not going to be zero this time because we have non zero heat exchange between the system and the environment, right.?

    热力学量,但是现在让我们看一下,我们的特殊函数,这次它不会是零,因为系统与外界的热量交换并不是零,对吧?

    麻省理工公开课 - 热力学与动力学课程节选

  • 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,波函数和波函数的平方,等于零的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

  • If there's no work to be done, 0 the running time is gonna be zero.

    如果并不需要做什么,那么其运行时间肯定为。

    哈佛公开课 - 计算机科学课程节选

  • And at the same time,we also need to cultivate the positive, to think more of the zero to the positive side of the equation as well.

    同时,我们还需要培养积极性,探究如何让我们从零点升到正直,该如何做。

    哈佛公开课 - 幸福课课程节选

  • Then it lands on your foot, because assuming the cannon is at zero height, the cannonball certainly comes out towards the enemy, but has no time of flight.

    然后它就会落在你的脚边,因为假设大炮的高度为 0,炮弹笔直地出膛打向敌人,却没有时间飞行

    耶鲁公开课 - 基础物理课程节选

  • And the mathematics of that equation involved a double derivative in time of x 0 plus some constant times x equals zero with some constraints on it.

    那个数学方程式,包括了x对时间的二阶导数,加上常数乘以x等于,还有一些限制条件。

    麻省理工公开课 - 固态化学导论课程节选

  • Let's create a graph here that on the x axis it's going to be time, so time zero will be when you first take in a food and then one hour later, two hours later will be shown as you go from left to right, and then we'll have blood glucose level up on the y axis.

    我们在这建立一个曲线图,X轴代表的是时间,所以零时间点是你第一次进食的时间,然后一小时以后,两小时以后,是从左到右呈现在图表上的,在Y轴上是你的血糖值

    耶鲁公开课 - 关于食物的心理学、生物学和政治学课程节选

  • And let's run in one more time zero.

    然后让我们在运行一次。

    哈佛公开课 - 计算机科学课程节选

  • For example, if you started here and you did all this and you came back here, the average velocity would be zero, because you start and end at the same value of x, you get something; 0 divided by time will still be 0.

    例如,如果你从这里开始运动,经过这个过程又回到这里,平均速度就是0,因为初态和末态的位移相同,你得到了什么呢,0除以时间还是0

    耶鲁公开课 - 基础物理课程节选

  • So that means that delta u isn't zero this time.

    U不再是零,它是理想气体。

    麻省理工公开课 - 热力学与动力学课程节选

  • So you should know that 0 any time m is equal to zero that it's the p z.

    所以当我们讨论p轨道时,只要m等于,它就是pz轨道。

    麻省理工公开课 - 化学原理课程节选

  • So, let's say we start off at the distance being ten angstroms. We can plug that into this differential equation that we'll have and solve it and what we find out is that r actually goes to zero at a time that's equal to 10 to the negative 10 seconds.

    也就大约是这么多,所以我们取初始值10埃,我们把它代入到,这个微分方程解它,可以发现,r在10的,负10次方秒内就衰减到零了。

    麻省理工公开课 - 化学原理课程节选

  • Last time we reach the third law which is telling us that we can't quite get to zero degrees Kelvin .but that as the temperature approaches zero degrees Kelvin, the absolute entropy of a pure substance in perfect crystalline form is zero.

    上次课我们得到了热力学第三定律,这个定律告诉我们我们无法,达到0K的温度,但是在我们接近绝对零度的过程中,以完美晶体形式存在的纯物质的绝对熵,也趋向于零。

    麻省理工公开课 - 热力学与动力学课程节选

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