What happens when electrons crash into their proton

In summary: I don't actually know what you're asking. In summary, the electron does not orbit the nucleus as expected and there are other forces at work to keep the atom together.
  • #1
Invinoveritas
9
0
Do they just destroy each other?
 
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  • #2
No, this doesn't actually happen. Electrons are often thought of orbiting a nucleus containing protons like planets orbit the sun. But this is not an accurate picture - that model does not account for observed results (or even close). In reality, electrons do not move to the proton (i.e. into the nucleus) as expected. Even though there is an attraction, there are also limits.

Things like the Pauli Exclusion Principle, the Schrödinger Equation and other elements of quantum mechanics yield different solutions than you would guess off hand. I would recommend that you google the subject and read up more. Then ask some questions based on that.

For example, look at the PhysicsForums FAQ, 2nd item:

WHY DON’T ELECTRONS CRASH INTO THE NUCLEUS IN ATOMS?

Contributed by Marlon and edited by ZapperZ

If one describes atoms using only the Coulomb forces, the electron and the nucleus will attract each other and no stable atoms could exist. Obviously this is not the case. Niels Bohr was the first (1913) to propose a better model, which consisted of electrons moving around the nucleus in circular orbits. Each orbit corresponds to a certain discrete energy level. This model is based upon the quantisation of the angular momentum.

Unfortunately, electrons moving in a circular orbit have an acceleration due to the centripetal force. In classical electromagnetic theory, an accelerated charged particle must emit EM-radiation due to energy conservation. Hence, the electron would lose energy and spiral down towards the nucleus. Again stable atoms could not exist. What is wrong now?

It turns out that the picture of electrons moving in circular orbits around the nucleus isn’t correct either(*). The solution here is the implementation of Quantum Mechanics via the Schrödinger Equation and the concept of wavefunction. By applying such formalism, the “electron” occupies a volume of space simultaneously, so that it is “smeared” in a particular geometry around the nucleus. While there are no more “orbits”, we do use the term “orbitals” to indicate the shape of such geometry. However, this term should not be confused to mean an orbiting electron similar to our planets in the solar system. By describing the system in terms of the QM wavefunction, it creates stable states for the nucleus+electrons system that matches very well with experimental observation of standard atomic spectra.

Since there are no more “orbits” in the conventional sense, the problem of electrons radiating due to an accelerated motion is no longer meaningful. It explains why we have stable atoms.

To read more in detail: http://scienceworld.wolfram.com/phys...rogenAtom.html (*) By saying that “an electron orbits the nucleus”, one is already implicitly assuming that one can track the position and momentum of that electron in an atom over a period of time. We have no such ability, and for those who know a bit about the Heisenberg Uncertainty Principle (HUP), one can already tell that such a statement violates this principle.
 
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  • #3
Google K orbital electron capture.
 
  • #4
The only case when atomic electrons interact with the nucleus is in a type of beta decay called K capture, when a proton in the nucleus does not have enough energy to decay to a neutron and a positron, but does have enough energy to decay to a neutronif it can capture an electron from the K shell. Beryllium-7 is an example.
 
  • #5
Bob S said:
The only case when atomic electrons interact with the nucleus is in a type of beta decay called K capture

Um...not exactly. An electron interacts electromagnetically with a nucleus, and there is a small correction to the atomic energy levels due to the electron spending a fraction of its time inside the nucleus.

Bob S said:
when a proton in the nucleus does not have enough energy to decay to a neutron and a positron, but does have enough energy to decay to a neutronif it can capture an electron from the K shell.

Not exactly. Na-22, for example can and does emit positrons but also has a 10% branching ratio for electron capture.


Bob S said:
Beryllium-7 is an example.

Yes, that is correct.
 
  • #6
Vanadium 50 said:
Um...not exactly. An electron interacts electromagnetically with a nucleus, and there is a small correction to the atomic energy levels due to the electron spending a fraction of its time inside the nucleus.

Do you have a ref. for that? I've never heard of such a correction being done.
Obviously there's an effect, since the nucleus is not the infinitesimal point charge it's usually modeled as, but it's still dang small. I can't imagine the effect being larger than something on the parts-per-million scale of the electronic energy. (and certainly smaller than the thermal energy at any reasonable temperature, making it physically insignificant)
 
  • #7
Is there another force that counteracts the force of charge trying to pull them together?
If not, then why the electron won't fall into the proton?
 
  • #8
feynmann said:
Is there another force that counteracts the force of charge trying to pull them together?
If not, then why the electron won't fall into the proton?

Gravitating a little closer to the OP question...

A free neutron decays into a proton, an electron and an anti nuetrino in about 10 minutes. A free neutron is free--it's not inside a nucleus. The resultant particles go buzzing off in all directions, each with some kinetic energy. So the opposite charges of the electron and positron are not enough to keep them bound together. It takes some energy to get them to stick together into one particle.

(Or maybe the question was 'why don't an electron and proton anihilate each other? But I think Invinoveritas was scared away by the 10 dollar words.)
 
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  • #9
Phrak said:
Gravitating a little closer to the OP question...

A free neutron decays into a proton, an electron and an anti nuetrino in about 10 minutes. A free neutron is free--it's not inside a nucleus. The resultant particles go buzzing off in all directions, each with some kinetic energy. So the opposite charges of the electron and positron are not enough to keep them bound together. It takes some energy to get them to stick together into one particle.

(Or maybe the question was 'why don't an electron and proton anihilate each other? But I think Invinoveritas was scared away by the 10 dollar words.)

Thank you for all your answers.

What if there was a way to increase gravity between the Proton and the Electron to the point it overcame the forces counteracting the forces keeping them apart.

Ideas on what would happen?
What would happen to the energy that was previously keeping them apart?

I apologize for the simple questions.
 
  • #10
Invinoveritas said:
Ideas on what would happen?

Except for the occurrence of electron capture, nothing. And depending on the nucleus, electron capture ranges from 'rare' to 'not even once in the lifetime of the universe'.

For an s-orbital electron, the nucleus (r=0) is in fact the most likely point in space to find the electron. (but not the most likely radius)

What would happen to the energy that was previously keeping them apart?

There's no energy keeping them apart. It's just that an electron that's close to the nucleus, like an object that's fallen towards the ground, has a high kinetic energy. But unlike an object falling to the ground, an electron can't 'discard' that energy. So if it's there, it's not going to stay there for long.

The 'problem' of electrons 'falling into the nucleus' predates quantum physics. Classically, an electron can emit its kinetic energy and 'should' fall into the nucleus and just sit there.
 
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  • #11
feynmann said:
Is there another force that counteracts the force of charge trying to pull them together?
If not, then why the electron won't fall into the proton?

This is what lead one to consider quantum mechanics: "why does not the electron fall into the proton?"

The easiest answer is that the form of the solutions to the Schrödinger Equation prevents this, only in the ground state, there is a non zero probability for the electron to be located at the origin (where the nucleus resigns) - we have to forget about that particles are tiny balls with classical forces acting between them.

Second is that from QM, we get something called the Heisenberg uncertainty relation, the electron can not be located at a specific position with 100% certainty, only with less. Thus one can only talk about a probability per unit time that an electron undergoes inverse beta decay with a proton in the nucleus.

So there is no additional force, we just have to forget about our classical, intuitive picture of particles as being tiny balls with classical forces acting on them.
 
  • #12
malawi_glenn said:
This is what lead one to consider quantum mechanics: "why does not the electron fall into the proton?"

The easiest answer is that the form of the solutions to the Schrödinger Equation prevents this, only in the ground state, there is a non zero probability for the electron to be located at the origin (where the nucleus resigns) - we have to forget about that particles are tiny balls with classical forces acting between them.

Second is that from QM, we get something called the Heisenberg uncertainty relation, the electron can not be located at a specific position with 100% certainty, only with less. Thus one can only talk about a probability per unit time that an electron undergoes inverse beta decay with a proton in the nucleus.

So there is no additional force, we just have to forget about our classical, intuitive picture of particles as being tiny balls with classical forces acting on them.


Thank you.
My entire understanding of an atom was very far off.



Please correct me if you have time.

Bohr's atom says that electrons must be in orbit around the nucleus but that this could not alone stabalize and atom.

"An accelerated electric charge radiates energy and a circular motion constitutes acceleration"

Classical physics (Maxwell's equation) says that the electron would radiate energy away and spiral into the nucleus.

I understood that the there were three basic forces involved in this "balance"

1. The gravity attracting the Proton and the election
2. The unlike charge attraction
3. The large atomic force counteracting the first two.

very wrong?
 
  • #13
well yes, since I just said that there is no additional 'force',

there are two forces involved, whereas gravity is 10^-19 times weaker than EM-force. The reason for the electron not spiralling down to the nucleus due to attractive EM-force is just the imposing of certain physical boundary conditions to the Schrödinger equation, which isthe "equation of motion" at quantum level.
 
  • #14
Vanadium 50 said:
Not exactly. Na-22, for example can and does emit positrons but also has a 10% branching ratio for electron capture..

What would you call copper-64? The only thing it doesn't do is capture positrons.
 
  • #15
malawi_glenn said:
well yes, since I just said that there is no additional 'force',

there are two forces involved, whereas gravity is 10^-19 times weaker than EM-force. The reason for the electron not spiralling down to the nucleus due to attractive EM-force is just the imposing of certain physical boundary conditions to the Schrödinger equation, which isthe "equation of motion" at quantum level.

To the OP: Not taking away from malawi_glenn's explanation, which is correct...

It may help you to replace your current picture of an electron and a proton being magnetically attracted with a more descriptive and accurate one: The attraction is for the electron to be pulled into an inner orbital of the proton (nucleus). I.e. the attraction is to pull the electron into a position which is a solution to the Schrödinger equation. The concept of the magnets makes you think that the attraction is absolute at any distance, and it is not.

In fact: if you could place an election inside the first orbital (which is conceivable), then the electron would tend to move AWAY from the proton (rather than towards it as you might otherwise expect). This makes sense in terms of the equations which *correctly* describe the electron and proton, but makes NO sense if you picture a couple of magnets. Orbitals are not orbits, and charged particles are not magnets. So ultimately, you must replace one model with another if you want to understand what is really going on at a deeper level.

By the way, the same analogy applies with Newtonian Gravity vs. Einsteinian Gravity. You replace one model (which is simple and easy to understand) with a better one (which is far more accurate when accuracy matters).
 
  • #16
malawi_glenn said:
well yes, since I just said that there is no additional 'force',

there are two forces involved, whereas gravity is 10^-19 times weaker than EM-force. The reason for the electron not spiralling down to the nucleus due to attractive EM-force is just the imposing of certain physical boundary conditions to the Schrödinger equation, which isthe "equation of motion" at quantum level.


Thank you.

I was just thinking about how great it would be if you could force an atom to collapse itself and release energy in that process.
 
  • #17
It's the energy inside an eletron that makes it get farther from the nucleos, right? Such can be proved because energized eletrons skip distances.
So, follow my though: if an eletron emit a foton with a energy difference equivalent it's orbit and de nucleos, it skips to the nucleos and thus collide with a proton.
There's only one way to evade that, that is considering that the nucleos canNOT be considered an eletrosphere, and if you prove that you solve the puzzle right?
Sorry if there any errors on my logic, I'm new to this area and would appreciate corrections.
Gedatsu.
 
  • #18
alxm said:
Do you have a ref. for that? I've never heard of such a correction being done.
Obviously there's an effect, since the nucleus is not the infinitesimal point charge it's usually modeled as, but it's still dang small. I can't imagine the effect being larger than something on the parts-per-million scale of the electronic energy. (and certainly smaller than the thermal energy at any reasonable temperature, making it physically insignificant)

I'm away from my textbooks, but I'm pretty sure it's a problem in Liboff and/or Schiff.

It is a small effect, but it's important in that it breaks the n-L degeneracy. Also, for muonic atoms, it's a larger effect.
 
  • #19
alxm said:
Do you have a ref. for that? I've never heard of such a correction being done.
Obviously there's an effect, since the nucleus is not the infinitesimal point charge it's usually modeled as, but it's still dang small. I can't imagine the effect being larger than something on the parts-per-million scale of the electronic energy. (and certainly smaller than the thermal energy at any reasonable temperature, making it physically insignificant)
Your estimation is in the right ballpark, but you are wrong that it can not be measured.
As a result, the total calculated hyperfine splitting now has a standard deviation slightly under 1 part-per-million, and is about 1 standard deviation away from the measured value.
Proton Structure Corrections to Hydrogen Hyperfine Splitting
Proton structure corrections to electronic and muonic hydrogen hyperfine splitting
 
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  • #20
Invinoveritas said:
Thank you.

I was just thinking about how great it would be if you could force an atom to collapse itself and release energy in that process.

You would then need energy to do that, and since atoms are weakly bound, you would not gain that much. The energies in atoms are of the order 10eV, whereas in nuclei the energies are of the order 1MeV, i.e 100 000 times bigger.
 
  • #21
See posts #3, 4, and 5 for correct discussion of electron capture by the nucleus; capture of atomic electrons by protons in the nucleus. Beryllium-7 and sodium-22 both exhibit K-capture. Perhaps the most interesting is copper-64 (an odd-odd nucleus), which has 3 decay modes, positron emission (beta+ decay), electron emission (beta- decay), and K-capture (electron capture).
 
  • #22
malawi_glenn said:
This is what lead one to consider quantum mechanics: "why does not the electron fall into the proton?"

The easiest answer is that the form of the solutions to the Schrödinger Equation prevents this, only in the ground state, there is a non zero probability for the electron to be located at the origin (where the nucleus resigns) - we have to forget about that particles are tiny balls with classical forces acting between them.

Second is that from QM, we get something called the Heisenberg uncertainty relation, the electron can not be located at a specific position with 100% certainty, only with less. Thus one can only talk about a probability per unit time that an electron undergoes inverse beta decay with a proton in the nucleus.

So there is no additional force, we just have to forget about our classical, intuitive picture of particles as being tiny balls with classical forces acting on them.

But how do we know Schrödinger Equation is correct. I guess the answer is that experiments confirm its predictions. So the reason to the OP, "why electrons won't crash to their proton" is that experiment show electrons won't crash to their proton
 
  • #23
feynmann said:
But how do we know Schrödinger Equation is correct. I guess the answer is that experiments confirm its predictions. So the reason to the OP, "why electrons won't crash to their proton" is that experiment show electrons won't crash to their proton


Well, one does not even know experiments to show this - IF electrons would do this, we would not have stable atoms in the universe and we would not be around to talk about these things ;-)
 
  • #24
malawi_glenn said:
You would then need energy to do that, and since atoms are weakly bound, you would not gain that much. The energies in atoms are of the order 10eV, whereas in nuclei the energies are of the order 1MeV, i.e 100 000 times bigger.


The idea was more of a what if.

It was my idea that an atom can only exist in a limited number of dimensions.

Based upon the idea that Gravity is so weak comparitively because it is a cross dimensional force. The more dimensions the greater the effect of gravity.

Once the number of dimensions became great enough, would the gravity between the components of the atom overcome the repellent factors and cause an atom implosion.

It would be electron proton fission.

Not to offend anyone here.
You are all much more educated than me... I am more of an idea rat.
 
  • #25
humanino said:
Your estimation is in the right ballpark, but you are wrong that it can not be measured.

Well I didn't say it couldn't be measured. I just said I didn't think it was very significant. At least not from a 'chemical' standpoint. Which is what I'm personally most interested in.
 

1. What is an electron-proton collision?

An electron-proton collision is a type of interaction between an electron and a proton, the two fundamental particles that make up an atom. This collision occurs when the electron and proton come into close proximity and are subjected to strong electromagnetic forces.

2. What happens when an electron crashes into its proton?

When an electron crashes into its proton, the two particles undergo a process known as scattering. This means that the electron and proton will deflect off of each other, changing the direction and energy of both particles.

3. How do electrons and protons interact during a collision?

During a collision, the negatively charged electron and positively charged proton will experience a strong attraction due to their opposite charges. This attraction causes the electron to move towards the proton, resulting in a close interaction between the two particles.

4. What are the effects of an electron-proton collision?

The effects of an electron-proton collision can vary depending on the energy and angle of the collision. In general, this type of collision can result in the creation of new particles, such as positrons or photons, and can also produce electromagnetic radiation.

5. Why do scientists study electron-proton collisions?

Scientists study electron-proton collisions to better understand the fundamental properties of matter and the forces that govern the behavior of particles at the subatomic level. These collisions can also provide insights into the structure of atoms and the nature of the universe.

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