• We are talking about probability, but what we're saying is that most probable radius is further away from the nucleus.

    我们说的是概率,也就是说它的最可能半径,离原子核更远。

    麻省理工公开课 - 化学原理课程节选

  • And then the potential energy, the energy is stored here due to the coulombic force of attraction between the electron and the nucleus.

    然后说势能,位能其实就是,由电子和原子核之间的库仑引力而形成的能量。

    麻省理工公开课 - 固态化学导论课程节选

  • So the probability of having an electron at the nucleus in terms of probability per volume is very, very high.

    在单位体积内发现,一个电子的概率非常非常大。

    麻省理工公开课 - 化学原理课程节选

  • One of the most obvious things about a red blood cell is it doesn't have nucleus, it has no nucleus.

    红细胞最为明显的不同就是,它是无核的,它没有细胞核

    耶鲁公开课 - 生物医学工程探索课程节选

  • And that's essentially what we saw people have more nucleus accumbens activation priority choice " they are more likely to choose that stock.

    这就是我们得到的结果,在作出选择时,受试者的伏隔核活动越多,他们就越有可能选择“股票。

    斯坦福公开课 - 7个颠覆你思想的演讲课程节选

  • Because what it tells is that we can figure out exactly what the radius of an electron and a nucleus are in a hydrogen atom.

    我们可以,准确的算出,氢原子中,电子。

    麻省理工公开课 - 化学原理课程节选

  • So I will take into account it that there is some contribution of both the nucleus and the electron.

    所以我将考虑,那是原子核与电子,共同作用的结果。

    麻省理工公开课 - 固态化学导论课程节选

  • So, what we're looking at here is the force when we have two charged particles, one positive one negative -- here, the nucleus and an electron.

    我们现在研究的是,一正一负俩个带电粒子之间的,作用力-在这里。

    麻省理工公开课 - 化学原理课程节选

  • But luckily for us, there's a classical equation of motion that will, in fact, describe how the electron and nucleus change position or change their radius as a function of time.

    但幸运的是,有一个,经典方程描述了电子和核子,位置或者它们直接的距离是,如何随时间变化的。

    麻省理工公开课 - 化学原理课程节选

  • But what's important is not where that most probable radius is when we're talking about the z effective it feels, what's more important is how close the electron actually can get the nucleus.

    但重要的不是,最可能半径,当我们谈论它感到的有效电荷量的时候,更重要的是,电子实际上。

    麻省理工公开课 - 化学原理课程节选

  • How far you are away from the nucleus in terms of a radius, they don't depend at all on those two angles, theta they're independent of theta phi and they're independent of phi.

    只和离核子的距离,也就是半径有关,它们和,另外两个角度无关,它们不决定于,也不决定于。

    麻省理工公开课 - 化学原理课程节选

  • So if you have some charge in the nucleus, but you also have repulsion with another electron, the net attractive charge that a given electron going to feel is actually less than that total charge in the nucleus.

    所以如果在原子核中,有一些电荷但是你也有来自,另一个电子的排斥力,那么一个给定电子的,吸引电荷感觉到的事实上,小于原子核中的总电荷。

    麻省理工公开课 - 化学原理课程节选

  • So, if I kind of circle where the probability gets somewhat substantial here, you can see we're much closer to the nucleus at the s orbital than we are for the p, then when we are for the d.

    我把概率,很大的地方圈出来,你们可以看到在s轨道上,比p轨道更接近原子核,最远是d轨道。

    麻省理工公开课 - 化学原理课程节选

  • So if you think of a shell, you can actually just think of an egg shell, that's probably the easiest way to think of it, where the yolk, if you really maybe make it a lot smaller might be the nucleus.

    可以把它想成,个蛋壳,这也许是,最简单的思考办法,蛋黄如果,缩小非常多倍的话,就可以想象成核子。

    麻省理工公开课 - 化学原理课程节选

  • So what this means is that unlike s orbitals, they don't have the exact same shape at any radius from the nucleus.

    这意味着和s轨道不同,它们在离原子核不同距离处的形状不是完全一样的。

    麻省理工公开课 - 化学原理课程节选

  • I said what hold the bonds together, what holds two atoms together is the attractive force we have between each electron and the other nucleus.

    我说过什么将它们结合在一起,将两个原子结合在一起的是一个吸引力,其中一个原子中的电子与另一个原子中的原子核之间。

    麻省理工公开课 - 化学原理课程节选

  • Because we know as we go to infinity, even though the density gets smaller and smaller and smaller, we still have electron density very far away from the nucleus.

    因为我们知道即使到了无穷远处,尽管电子密度会变得非常非常非常小,但我们仍然有一定的电子密度,无论离原子核多远。

    麻省理工公开课 - 化学原理课程节选

  • The bacterium doesn't have a nucleus, and in fact, they don't have very well formed organelles in general.

    细菌没有细胞核,实际上,细菌没有完善的细胞器

    耶鲁公开课 - 生物医学工程探索课程节选

  • Again we have the charge of the nucleus on plus 2, +2 but let's say this time the electron now is going to be very, very close to the nucleus.

    对于我们的氦原子,我们有一次得到了原子核电荷量为,但是我们说这次电子。

    麻省理工公开课 - 化学原理课程节选

  • So even if we strip an atom of all of its electrons, we still have that same amount of positive charge in the nucleus.

    所以即使把一个原子的所有电子都拿走,原子核还是带那么多的正电。

    麻省理工公开课 - 化学原理课程节选

  • That is why we don't worry about the motion of the nucleus 1 because the ratio of mass is about 2,000 to one.

    这就解释了为什么我们不担心,原子核运动起来,因为原子核和电子的质量比约为2000:

    麻省理工公开课 - 固态化学导论课程节选

  • So, essentially we're just breaking it up into two parts that can be separated, and the part that is only dealing with the radius, so it's only a function of the radius of the electron from the nucleus.

    所以本质上我们把它写成,两个可分离的部分,这部分,只与半径有关,它仅仅是,电子,到核子距离的函数。

    麻省理工公开课 - 化学原理课程节选

  • And so the other thing that we consider is the nucleus as being stationary.

    接下来我们讲的是,原子核是静止的。

    麻省理工公开课 - 固态化学导论课程节选

  • So where we had left off with was we'd fully discussed up to the point of considering homonuclear diatomic molecules, so molecules that both have the same nucleus.

    我们上次,讲到了我们,已经讨论过同核双原子分子,也就是有相同原子和的分子。

    麻省理工公开课 - 化学原理课程节选

  • So, the size still for an s orbital is larger than for a d orbital, but what we say is that an s electron can actually penetrate closer to the nucleus.

    轨道的尺寸比,p轨道还是要大,但我们说的是s轨道可以,穿透到更接近原子核的地方。

    麻省理工公开课 - 化学原理课程节选

  • We're going to be looking at the solutions to the Schrodinger equation for a hydrogen atom, and specifically we'll be looking at the binding energy of the electron to the nucleus.

    我们将研究下氢原子薛定谔方程的解,特别是电子和核子的结合能,我们将研究这部分。

    麻省理工公开课 - 化学原理课程节选

  • What I just spent many lectures discussing is the fact that we can not know how far away an electron is from the nucleus, so we can't actually know the radius of a certain atom.

    我花了这么多课时所讨论的正是我们,不可能知道电子离原子核有多远这一事实,因此我们不可能知道某个原子的半径。

    麻省理工公开课 - 化学原理课程节选

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