00:01
In this exercise, we have to assume that the electron behaves like a standing wave inside a one -dimensional box of length l.
00:09
And in question a, we want to show that the momentum p of the electron can be written as n, h divided by 2l.
00:20
So the first thing i need to remember here is that for a standing wave, l, the length of the box, is equal to n times the way.
00:32
Wavelength of the wave divided by 2.
00:36
If you don't remember where that comes from, just notice that for the first standing wave possible for n equals 1 is this one that i'm drawing here.
00:53
Notice that the here you have l, that's the size of the box, but l is equal to one half the wavelength okay because the distance between two nodes is one half the wavelength okay so in this case l equals lambda over two for for n equals two the second possible sending wave is this one let me draw it a little better is this one when l this distance here is equal to lambda.
01:37
Okay.
01:37
So notice that our equation here, the equation for l that i just wrote as a function of n and lambda holds.
01:45
Okay...