0:00
Hi there.
00:01
So for this problem, we are told that by applying the technique of separation of variables, we need to split the rigid rotator shorting hair equation of the problem 20 to obtain.
00:13
So for part a, we need to, at the time independent shortingher equation, that is the following, minus h square, and this divided by two times the moment of inertia.
00:30
And this the second derivative of the wave function that depends on fee with respect to, and then this is equal to the energy times the wave function.
00:52
Now, to solve the first part of this problem, we're going to let that the wave function that depends on fee and the time, and we can separate this in two functions, function that depends only on fee and the function that depends only on the time.
01:13
Now, substitute this into the energy equation of problem 7 .20 and divide by the wavelength to obtain the following.
01:25
So from this, we obtain minus h .r.
01:29
2 squared divided by two times the moment of inertia and this times the function, the temporal function.
01:37
And these times the second derivative of the fee function with respect to fee.
01:46
Let me put in here, fee, respect to fee.
01:53
Oh, well, we call it in, let's call it as the same as before, is this, okay.
02:00
So this will be equal to i times h part times the differential, the derivative of this...