00:01
So here we are given temperature, which is one nanocalcalfin in the size of the box that the particle is in.
00:09
That's one millimeter.
00:15
So it's this.
00:19
And this atom is subject to the eisenberg uncertainty principle, as everything is, which is delta x times delta p.
00:35
It's always bigger or equal than the blanks constant over two.
00:40
Okay, and delta b is just the mass times delta v.
00:48
Okay.
00:50
And now we wanna know the smallest range of speeds for sodium metham in this particular box.
01:01
So we can just calculate that the range of speeds, or the uncertainty in the speed, should i say, is always bigger than the plant's constant over two times.
01:19
Times the mass of sodium times this deltax, which really is d 'l.
01:32
Sodium's standard atomic weight is around 23 atomic mass units.
01:39
So we'll just take the, as an approximation, we'll take the mass of a proton and multiply it by, which is almost the mass of the neutron, will multiply it by 23.
01:52
23 to get the mass this one.
01:58
And so this is just the planx constant, which is 6 .63 times 10 to the minus 34.
02:07
We get 2 times 23 times the mass of a proton, which is around 1 .67 times 10 to the minus 27 kilograms.
02:20
And then the 1 millimeter, which is 10 to the minus 3 meters.
02:28
That's the uncertainty in the position.
02:31
And this gives around 8 .6 times 10 to the minus 6 meters per second.
02:48
So if we assume that the velocity, the medium, the average velocity is centered, is zero.
02:57
So the velocities will be centered around zero...