P: I left my briefcase here, now it has gone.
我刚才把公文包忘在了这里，现在找不到了。
So for example I defined p, remember back over here, as a Cartesian point, but I can actually ask for its polar form.
我可以要求返回它的极坐标形式，这里对我是可访问的，好，这很棒，请再记另外一个为什么。
So here is an ellipse, A here is P and here is A.
所以，这是一个椭圆轨道，这是P，这是。
这里疼。
So it's along the bond axis and it's between a carbon s p 2 hybrid, and then the hydrogen is just a 1 s orbital that we're combining here.
所以它是沿着键轴方向的,而且这里是一个碳sp2杂化轨道，和一个氢的1s轨道的结合,在这里我们可以合并他们。
This point, p, was there, and the amount by which the things have moved can be measured either here or here.
这是点P，移动的总量，可以认为是这到这。
We want to do that because we have too many variables here. We've already got dV p we'll get rid of p as an additional variable and replace it with V which is already in here.
我们之所以要那么做,是因为这儿有太多变量了,我们已经有了dV，我们要把,作为额外的变量消去，用已存在的V代换它。
I also want to assume for our present purposes that there's only pressure volume work going on, which is to say I want to put pdV p dV in here minus p dV for dw.
同时假定,对于我们目前的目的而言，只有压强做功这就是说,我要把这里的dw替换为负。
So that's why we see the 2 p here, 1206 the 2 s is 12 06, and it makes sense that what we see as the greatest ionization energy, which is also the smallest kinetic energy is that 1 s orbital.
这就是为什么我们看到，2，p在这里，2，s对应,那么我们看到对应最高的电离能，同时也对应最低的动能的,应该就是，1，s，轨道。
p And we're going to put a little p here, because it's in terms of the partial pressures.
在这里写一个小，因为这是压强的函数。
Sigma2s sigma2s sigma2px and now we have sigma 2 p x how many electrons here?
有两个电子，So，，sigma，2，s，has，two，electrons，星有两个电子，sigma，2，s，star，with，two，electrons，现在我们有,这里有几个电子？
Q Here is a valid argument form. If P then Q. P therefore Q.
这里有一个有效的论点形式，如果P，那么Q，P所以。
So the G. O. P. argument here is exactly like claiming that my mortgage payments, which I'll have to make no matter what we do tonight, are a cost of going out for dinner.
因此，共和党在这方面的论调就好比说，无论我晚上干什么都必须缴纳的房贷金，就是我们晚上出去吃饭的费用。
P: Yes I'll be here for three to five years.
是的，我要在这儿呆三至五年。
Among the early exponents was Duane Beeson, seen here on the wing of his only P-51B, 43-6819, nicknamed BEE, in the spring of 1944.
杜安•比森是第4大队早期的王牌飞行员之一，在这张摄于1944年春的照片中，他站在自己驾驶过的唯一一架P-51B型机“蜜蜂”（P-51B43-6819）的机翼上。
What we are saying here is if Q is necessary for P so if Q isn't the case then P isn't the case either.
我们说的，如果Q对于P来说是必须的，所以如果Q不是这样，P也不是这样。
P This is point p, and here is the center of the rod.
这是点，这是杆子的中心。
So, maybe my point, P, now, is here.
点P，现在在这。
P So here at the bottom, at this point P, there is a loop.
在底部，点，有一个环。
And if you count the number of equations, p-1 the number of equals signs here, that's p minus one.
如果你数一下方程的数量，也就是这里等号的数量，结果是。
What premise would you like me to put in here in order to make this argument invalid? Not p. yea?
什么前提放在这里好呢？，来使论点无效？非p，对？
So if we say that we have a 2 p orbital here, that means that we can have 2 how many different complete orbitals have a 2 for an n, and a p as its l value?
如果我们说这里有一个“2p“轨道，那就意味着我们有,多少完全不同的轨道对于n有一个,而且对于l值有一个p？
A piece of graffiti on the wall read, P. MOYO WAS HERE FOR STANDING.
看守所的墙上有一处涂鸦写着“停下来，墨约站在这里。”
So again, looking at the shapes, now we're just combining two, we've got these two equal hybrid orbitals plus these 2 p orbitals here.
同样，我们看它的形状，现在我们仅仅结合两个轨道，我们得到这两个杂化轨道,和两个p轨道。
Here, we compared Germany's Messerschmitt ME-109 to the Allied planes, America's P-40 and the British Spitfire.
这张图片里，将德国梅塞施米特的ME- 109和盟军飞机，美国的P -40和英国的喷火式战斗机进行比较。
We can fill right up our table just like we did before, but now we have included our 2 p z orbital here.
我们可以像以前一样填充表格，但现在我们包括了2pz轨道。
You can get this information using vmstat -p ALL, as seen here in Listing 4.
可以使用vmstat- P ALL获得此信息，见清单4。
So if we write the electron configuration you see that this is the electron configuration here, 1s22s22p 1 s 2, 2 s 2, 2 p 6, 3s1 and now we're going into that third shell 3 s 1.
现在我们来到第三层,你们会看到3s1价电子之间的区别，电子构型是，现在我们来到第三层。
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。
It is this that allows us to do the trick of printing out the parameter "p" and then passing it to the "rest" function to continue the computation, seen here in the definition of the "Bind" method.
这样话，就可以让我们能取巧打印出参数“p”并接着把它传递给“rest”函数继续进行计算。
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