Electron Capture and Coulomb's Law

In summary, the conversation discusses the concept of electron capture in a proton-surfeited atom and the implications of Coulomb's law in this process. However, the participants come to the conclusion that classical views and laws cannot fully explain this process, as it occurs at a quantum level. The uncertainty principle and the limitations of Coulomb's law at high energies are also mentioned as factors that prevent the electron from approaching the proton infinitely. Additionally, the finite size of the proton is not a determining factor in this process.
  • #1
David Carroll
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Sorry for the brevity of the post, but eloquence has never been my strong point. Here's my question:

In a proton-surfeited atom, a proton captures an electron to form a neutron. Now, according to Coulomb's law, the magnitude of the electrostatic force field is equal to (kq1q2)/d2, where k is Coulomb's constant, q1 is the charge of the proton and q2 is the charge of the electron, and d is the distance between the proton and electron. Now, given that neither k, q1, nor q2 is changing, shouldn't the magnitude of the electrostatic force field approach infinity as the electron spirals toward the proton? Does it?
 
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  • #2
The events you describe happen at a quantum level where things are not as simple as looking at different forces acting on point particles.
 
  • #3
Ok. Thank you, Orodruin. So, the particles are treated as probability functions?

Wow, what was I thinking? Sorry, folks. Highly caffeinated and hardly slept. Forgive me.
 
  • #4
A fast answer: no.
The problem in your approach is that you are taking a classical view on the process of electron capture.
One very simplistic example to see that it's impossible to think of r->0 (that got in my mind right-away) is that if the energy of the particle goes way beyond some limit (eg twice the mass of the particle), you will get the creation of particles+antiparticles etc...I think this results in shielding the particle's charge (vacuum polarization).
Nevertheless, I am not sure if this explains why this is impossible, but it gives an idea.
The most precise answer for why this is impossible, is because of the quantum mechanics (so you don't have two balls that are at some distance D and go to some distance 0) as well as the interactions don't happen at points (there are intermediate W bosons, and you are in fact looking for the amplitudes for them to be mediated throughout the whole space).
 
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  • #5
So you implying that the electron has infinite velocity and kinetic energy when it collides with the proton?

Not sure what is the workaround this mini paradox, maybe that the proton can't be considered as a point particle because it is not an elementary particle like electron or quarks are.
 
  • #6
Delta² said:
So you implying that the electron has infinite velocity and kinetic energy when it collides with the proton?

I think it's better to say that the Coulomb's law is a result of the low-energetic QED ... at higher energies it's not applicable and you can't go the other way.

And in EC the electron "sees" the quarks since it interacts with them. The process is [itex] e u \rightarrow \nu_e d[/itex] (with a W-boson t-channel)
 
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  • #7
Is it that the uncertainty principle precludes this from happening because infinity is a definite momentum (or is it?) and zero is a definite position?
 
  • #8
David Carroll said:
Is it that the uncertainty principle precludes this from happening because infinity is a definite momentum (or is it?) and zero is a definite position?

This is again simplistic , but you could use that... in fact, some introductory books in elementary particles, prefer introducing the intermediate bosons with the uncertainty principle. It's way before reaching infinite, that you can get (as they say due to the uncertainty principle) extra particles appearing.

The thing is that once you take a limit, you cannot go from that limit and deduce how your initial theory works. Take for example the special relativity, the gamma factor: [itex]\gamma = \frac{1}{\sqrt{1- (u/c)^2}} [/itex], and the momentum [itex]\vec{p}= \gamma m \vec{u}[/itex]. In the low velocity limit ([itex]u \ll c[/itex]) the gamma factor goes to 1, and then the momentum is [itex]p=m u[/itex], how can you say that this holds when you let your velocity get large enough? You already left the SR...

The same is true for QED, you can only apply the coulomb's law at low energies [non-relativistic limit].
 
  • #9
Delta² said:
So you implying that the electron has infinite velocity and kinetic energy when it collides with the proton?

Not sure what is the workaround this mini paradox, maybe that the proton can't be considered as a point particle because it is not an elementary particle like electron or quarks are.
The finite size of the proton is irrelevant - you can ask the same question for positronium which is made out of two elementary particles. The answer is quantum mechanics in both cases.
 

1. What is electron capture?

Electron capture is a type of nuclear reaction in which an electron from the innermost shell of an atom is absorbed by the nucleus, causing a proton to be converted into a neutron.

2. How does electron capture affect the stability of an atom?

Electron capture can result in the formation of a more stable nucleus, as it reduces the number of protons and increases the number of neutrons. This can also result in the emission of gamma rays.

3. What is the role of Coulomb's Law in electron capture?

Coulomb's Law states that the force of attraction or repulsion between two charged particles is directly proportional to the product of their charges and inversely proportional to the square of the distance between them. In electron capture, this law explains the attraction between the positively charged nucleus and the negatively charged electron.

4. How is electron capture different from electron emission?

Electron capture involves the absorption of an electron by the nucleus, while electron emission involves the release of an electron from the nucleus. Electron capture results in a decrease in atomic number, while electron emission results in an increase.

5. What are the applications of electron capture?

Electron capture is commonly used in nuclear medicine for imaging and cancer treatment. It is also used in analytical techniques such as mass spectrometry to identify and quantify elements in a sample.

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