00:01
Here we're going to use some simple electrical ideas to figure out the energy as needed to ionize the hydrogen atom.
00:12
So these ideas are incorporated in what's called the bore model of hydrogen.
00:20
And much of that model is using classical dynamics and energy ideas.
00:27
So total energy of the electron is just its kinetic plus its potential energy.
00:37
And its potential energy is the electrical value for point charges.
00:45
And we know that both the electron and the proton, we know the charge on both of those.
00:52
The electron's negative e.
00:54
The proton is positive e.
00:56
And their separation were taken as a given as 0 .0529 nanometers.
01:05
So if we put all those numbers in, we calculate what appears to be a small energy, a negative energy, of course, as the two particles attract each other.
01:25
Now, to get the kinetic energy, we are going to need to use newton's second law in order to use f -equals m -a to determine the velocity of the electron.
01:43
So the force on the particle is the electrical or coulomb force.
01:52
I'll write that down.
01:56
And we are just finding the magnitude of the force.
01:59
It is going to change direction, always being directed towards the center of the orbit.
02:07
So we are going to set that force equal to the mass of the electron times its centripetal acceleration.
02:18
But the force we can calculate is k e squared over a squared.
02:30
And that turns out to be what appears to be a small force.
02:43
And now we are going to set that equal to mass times the centripetal acceleration.
02:52
And this is where numbers start to get a little bit crazy.
02:57
Mass of the electron is given in the data over to the left.
03:04
But we get a huge acceleration.
03:08
Any macroscopic object would be in bad shape with this acceleration...