• An F is a failing grade worth zero toward a student's grade point average.

    VOA: special.2009.03.05

  • Change in entropy is greater than zero for an isolated system.

    对孤立系统,熵的变化是大于零的。

    麻省理工公开课 - 热力学与动力学课程节选

  • If this were to be an absolute zero Kelvin, then we could we can have something, T2 Sorry, it's T2.

    如果它等于绝对零度,我们可以,对不起,这是。

    麻省理工公开课 - 热力学与动力学课程节选

  • Tornadoes that cause only light damage are called an F-zero.

    VOA: special.2010.05.11

  • I have read an entire page full of words and given it zero because it is not on topic.

    我读到的是一整篇都是单词的文章,给了零分,因为跑题了。

    麻省理工公开课 - 固态化学导论课程节选

  • You've got a picture of somebody's face, it's a million pixels. Each pixel has a range of values from zero to 256. I want to hash a face with some function into an integer.

    你有一个人的脸部照片,它有一百万个像素,每个像素的值范围在0到256之间,我想用某个函数将一张脸部照片。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • Okay. How many people would say they were off by an average of zero to ten percent?

    多少人低估了,平均从0到10%

    耶鲁公开课 - 关于食物的心理学、生物学和政治学课程节选

  • So what we do is we pick an origin, call it zero, we put some markers there to measure distance, and we say this guy is sitting at 1,2,3,4,5.

    我们现在选择一个原点,称其为零点,我们做一些标记来测量距离,这个点在五个单位长度的地方

    耶鲁公开课 - 基础物理课程节选

  • So I said before when we were talking about single atoms, we always define the zero energy as when an electron was actually ejected, but now, when we talk about chemical reactions taking place, it's very, very rare that we're actually going to be talking about anything that gets to this point here.

    我之前说过,当我们讨论单个原子的时候,我们总是把零点能,定在电子被发射出去以后,但是现在,当我们讨论化学反应发生的时候,非常非常罕见出现,确实达到,这种程度的情况。

    麻省理工公开课 - 化学原理课程节选

  • So it does that for us so that you can get away with just knowing the address of the first byte and it will make sure that you know when to stop by including the special value so, in fact, get the string if you type in a three-letter word, we allocate four bytes no matter what because we need an additional byte 0 for this special sentinel value back slash zero at the very end.

    它为我们做了这些事情,这样我们就可以,通过第一个字节的地址,它还可以通过包含一个特殊的值,来保证在哪里停止,如果你输入了一个三个字母的单词,就可以获得那个字符串,不管怎样,我们分配四个字节,因为我们在末端需要一个额外的字节,来保存这个特殊的标志值--反斜杠。

    哈佛公开课 - 计算机科学课程节选

  • This is just an equality. I have a constant pressure dH process. This term here is equal to zero.

    这是一个等式,这是个恒压过程,这项等于零,这意味着。

    麻省理工公开课 - 热力学与动力学课程节选

  • And the temperature scale that turns out to be well-defined and ends up giving us the concept of an absolute zero is the ideal gas thermometer.

    比如理想气体温标,它有精确的定义,并能引出绝对零度的概念,今天我们就先来谈谈它。

    麻省理工公开课 - 热力学与动力学课程节选

  • B=0 There's going to be some temperature where B is equal to zero. In that case, your gas is going to look awfully like an ideal gas.

    在某个温度,这时,实际气体的表现,十分接近理想气体,高于这一温度它是正的。

    麻省理工公开课 - 热力学与动力学课程节选

  • This quantity is exactly zero for an ideal gas and we'll discover why eventually it has to do with what we mean by an ideal gas it turns out.

    对理想气体它是零,这点我们接下来会知道是,为什么,这与为什么我们叫它理想气体有关。

    麻省理工公开课 - 热力学与动力学课程节选

  • So let's look at an example of a zero-one knapsack problem.

    我们要像之前一样将其最优化,现在让我们来看一个0/1背包问题的例子。

    麻省理工公开课 - 计算机科学及编程导论课程节选

  • So, we just talked about the force law to describe the interaction between a proton and an electron. You told me that when the distance went to infinity, the force went to zero. What happens instead when the distance goes to zero? What happens to the force?

    我们刚刚讨论了描述质子,和电子之间相互作用力的定律,当距离变为无穷时,力变为零,那当距离变为,零时会发生什么?,这时候力是多少?

    麻省理工公开课 - 化学原理课程节选

  • 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

  • We could say an energy level diagram 0 This would be energy. Here is zero.

    我们可以画一个能量图,这是能量,这里是。

    麻省理工公开课 - 固态化学导论课程节选

  • 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

  • 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

  • dq=0 But if it's adiabatic, then dq is equal zero, du=dw and for an adiabatic process, then du is equal to dw.

    但如果它是绝热的,那么,因此对于绝热过程。

    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

  • I am going to say if that electron is to stay in its orbit, that is to say it doesn't flee the atom, it doesn't collapse under the nucleus then the sum of the forces on the electron must be zero No net force. And so that will be the sum of a dynamic force plus an electrostatic.

    如果电子会保持在它的轨道上运行,既不脱离原子的话,它就不会由于原子核对它的吸引力而被瓦解掉,电子所受的合力一定为零,由于没有合力,所以电子所受力为动态力和静电力的总和。

    麻省理工公开课 - 固态化学导论课程节选

  • It is. It's drawn like an array, it effectively is an array so bracket zero means go to the zero's location in that array, which happens to be F and do what with it?

    它看起来像个数组,实际上也是一个数组,所以【0】就是定位到那个数组的0的存储单元,对于f发生了什么?用它做什么?

    哈佛公开课 - 计算机科学课程节选

  • Going from two to three, that's an adiabatic expansion, so q is equal to zero in that step.

    从第二点到第三点,是绝热膨胀,因此q等于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • So this declares an integer, a variable of type int called I, 0 and initializes it to zero.

    所以这里声明了一个整型数,一个叫做I的整型变量,把它初始化为。

    哈佛公开课 - 计算机科学课程节选

  • 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

  • Now, for an ideal gas, du/dV under =0 constant temperature is equal to zero.

    对于理想气体,温度一定,时偏U偏V等于零。

    麻省理工公开课 - 热力学与动力学课程节选

  • Well, this question mark becomes an O, this question mark becomes an O, and then the loop terminates 0 1 2 because it's iterating from zero to N so that's zero, 1, 2 and the length of the string is 3 so the loop terminates, but I remember that I needed to have this special sentinel value so I'm just going to put it there manually.

    嗯,这个问号变成了,这个问号变成了0,然后循环结束了,以为迭代从0到N,那就是,字符串的长度是3,然后循环就结束了,但是我记得我需要这个特殊的标记值,所以需要手动的加上它。

    哈佛公开课 - 计算机科学课程节选

  • We're still going to be able to write that dq=0 it's an adiabat so that dq equals zero.

    绝热条件依然成立,于是。

    麻省理工公开课 - 热力学与动力学课程节选

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