00:01
The uncertainty in the position is approximately equal to the length, and we know that the average momentum is zero.
00:08
And this gives us the result that the square of the uncertainty in momentum is equal to the average of the momentum squared, based on how one defines uncertainty in quantum mechanics.
00:21
So we're going to use the heisenberg uncertainty principle to get an estimate of the energy of the particle.
00:29
The uncertainty principle is given as the product of the uncertainty in position and uncertainty momentum, and it's an inequality.
00:38
Their product is greater than or equal to h bar over 2.
00:42
Now, h bar is equal to plonks constant h divided by 2 pi, and it's important, it is very important to distinguish between h bar and h.
00:52
Because obviously you have this factor of 2 pi.
00:57
And so proceeding, we're going to go ahead and write the energy for a particle in a box as p squared over 2m.
01:08
And in order to approximate the energy, we can go ahead and talk about the average energy, and that we just put in brackets.
01:18
Now, these brackets that we use for averages really refer to expectations.
01:23
Values as defined in quantum mechanics.
01:26
And real quick, if you have an operator m, an expectation value for an operator is simply the integral over an interval, which in general might be from minus infinity to positive infinity, of the product of the wave functions complex conjugate with the operator and the wave function on the right.
01:52
So that's how you get an expectation value.
01:55
You can also define them over other intervals, but in general it's from minus infinity to positive infinity.
02:01
Having said that, the estimate that we're going to get for the energy is just going to be this average, and we're going to say that it's approximately equal to this, because after all, we're not working with anything exact here.
02:16
So making note of the observation up here that based on the average momentum being zero, we have this result for the screen...