00:01
In this question, we want to construct a similar diagram to 44 .18, where we have various iz components with the same magnitude of nuclear spin i.
00:20
So in this case, we are given that the quantum number, the nuclear spin quantum number i is 5 over 2 and 4.
00:29
We have two different cases let's consider the first case first 5 over 2 over here the mi value can vary from plus 5 over 2 all the way down to minus 5 over 2 right in integer steps therefore the z component of the i just m i times h each bar right so these are the various iz components the overall magnitude of our nucleus spin will be equals to i times i plus 1 square root times hbar in this case is 5 over 2 times 7 over 2 square root times hbar which you'll div us with square root of 35 over 2 each bar now we can start to construct our figure so starting from the origin right it can a nuclear spin can point in three possible positive directions right they all have the same magnitude overall magnitude but they will have different z components something like this right where the z components over here i see this way it goes to 5 over 2 h bar the second one will be equals to 3 over 2 h bar and the third one will be equals to half each bar.
03:04
This would be the same for the negative side.
03:07
It's negative half.
03:09
Negative 3 over 2, and negative 5 over 2.
03:15
This will form a semicircle, because they have the same overall magnitude.
03:23
So they should have magnitude of square root 3 over 35.
03:33
Square root 35 over 2 times hbar.
03:40
Now we move on to the case where we have i equals to 4.
03:49
For i equals to 4 our mi value runs from plus 4 all the way to minus 4.
04:17
Same thing, the magnitude of the nuclear spin would be just i times i plus 1, square root times hbar...