00:01
Here, let's say that we're looking at states of the hydrogen atom where the angular momentum quantum number l is equal to two.
00:09
And so some things we're going to find out are what is the maximum angular momentum in the vertical direction that we can have given this restriction.
00:20
And what are the available angles between the l vector and its corresponding z axis, which looks sort of like this? so if you have z, this is the direction of z.
00:36
If you have some vector l, this is going to be the height of the vertical component here.
00:43
So l sub z.
00:45
So we're going to figure out l sub z max, the angles available.
00:50
And finally, we're going to compare that to l equals 3.
00:55
So this is what we have.
00:58
This is what we're going to find.
00:59
And okay, so starting with the vertical component, the max that we can have, we have to think about what l sub z is actually equal to l sub z is actually going to be equal to m subel, the magnetic quantum number, times h bar.
01:19
So what values for m subal do we have available, given that l is equal to two? we know that m subel has to be in the range from negative l to positive l.
01:31
So we're going to have negative 2 positive 2.
01:35
And those are integers.
01:37
So this means that the maximum of this range is going to be 2, which means that the maximum of the vertical component of angle of momentum is going to be 2 times h bar.
01:52
So that's our first result.
01:54
Next, we're going to be looking at the angles that are available to the system given what we know about the angular momentum quantum number l being two.
02:09
So given that this is true, there are five different values of m -sabell that we can have...