00:01
Okay, we're trying to probe the details of the nucleus.
00:08
The diameter of a nucleon is about 2 .4 times 10 to the minus 15 meters.
00:18
So we'd like the particle that we fire at this thing to be close to that diameter.
00:31
We're talking about 25 mev alpha particles and 25 mev protons.
00:39
So an energy of 25 meb.
00:43
Notice that this is not relativistic, which means that the momentum of each of these particles is just mv.
01:02
I can use my relationship between velocity and kinetic energy, v is the square root of k over 2m.
01:14
To write the momentum as the square root of 2m, i wrote the 2 at the wrong place here.
01:29
That's my mistake.
01:31
All right, this is our momentum, and we know that the debrogly wavelength of a particle is h over the momentum.
01:42
So in this case, h over root 2mk.
01:52
Keeping in mind that while we're not relativistic here, 25mev is much greater than the rest mass of either the proton or the alpha particle.
02:05
So we are able to say that the energy is all kinetic.
02:12
So now we just need to look at the de brogley wavelength of each of these particles.
02:20
And what we want, what our goal is, is for a wavelength that is approximately the size of the diameter of our nucleus.
02:35
Okay...