When is a particles charge spread out?

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Discussion Overview

The discussion centers on the behavior of an electron's charge in quantum mechanics, particularly in relation to its position uncertainty and the implications for systems like hydrogen atoms and hydrogen molecules. Participants explore concepts such as charge density, wave functions, and the stability of molecular structures in quantum contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that an electron's charge can be spread out in regions of uncertainty, as seen in ground state hydrogen atoms.
  • Others argue that in certain configurations, such as with two protons and one electron, the electron's charge may not be evenly distributed, affecting the interactions between protons.
  • A participant references Heisenberg's uncertainty principle, suggesting that the electron appears more like a cloud when its position is uncertain.
  • One participant discusses the relationship between the square of the wave function and charge density, indicating that this relationship holds for both nonrelativistic and relativistic quantum mechanics.
  • Another participant mentions the stability of the H2 molecule, suggesting that the electron acts as a "glue" between the protons, which seems counterintuitive given their positive charges.
  • Some participants introduce the concept of overlap integrals and charge exchange integrals, questioning the familiarity of others with these terms.
  • A later reply challenges an earlier claim, stating that the charge density scales with the probability of finding the electron at a specific location, implying a more nuanced understanding of charge distribution.

Areas of Agreement / Disagreement

Participants express differing views on whether an electron's charge is always spread out or can be localized in certain situations. The discussion remains unresolved, with multiple competing perspectives on the nature of charge distribution in quantum systems.

Contextual Notes

Participants reference various quantum mechanics principles and models, but there are limitations in the assumptions made about charge distribution and the stability of molecular structures. Some mathematical steps and definitions remain unresolved.

box
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Correct me if I'm wrong but i think in quantum mechanics there are times when the charge of an electron is spread out in the area where its positon is uncertin, such has a ground state hydrogen atom. And there are times when even though the electrons position is unknown over a certin area the charge is not spread over the whole area but is modeled to be in a more certin spot. Such has when you have two protons and one electron that is equaly likely to be orbiting both of them, The protons don't repell each other because the electrons charge is only on one of them and not evenly spread between the two. So am I right in saying that sometimes an elecrons charge is spread out over the area were its position is uncertin and somtimes its not? If so what determines if its the former or the latter?
 
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aS PER hEISENBERG'S uNCERTAINITY pRINCIPLE , YOU CANNOT POSSIBLE DTERMINE THE VELOCITY AND POSITION OF AN ELECTRON simultaneously..

Imagine this , suppose you witness a fast moving electron and wth great precision you pin it up against the wall with a pin, before pinning it up , the electron was so fast that you couldnot determine its position and now you pinned it up in hope to determine the position correctly, now when you see the pinned-electron , it spreads itself and looks more like a cloud rather than a particle , this is what happens as per Heisenberg's..

More at :
http://www.doxlab.co.nr/
 
box said:
Correct me if I'm wrong but i think in quantum mechanics there are times when the charge of an electron is spread out in the area where its positon is uncertin, such has a ground state hydrogen atom. And there are times when even though the electrons position is unknown over a certin area the charge is not spread over the whole area but is modeled to be in a more certin spot. Such has when you have two protons and one electron that is equaly likely to be orbiting both of them, The protons don't repell each other because the electrons charge is only on one of them and not evenly spread between the two. So am I right in saying that sometimes an elecrons charge is spread out over the area were its position is uncertin and somtimes its not? If so what determines if its the former or the latter?

Ever heard of overlap integral,or charge exchange integral...?My guess is "no".

Daniel.
 
For nonrelativistic QM, the square of the electron's wave function times the electric charge is the spatial charge density, which in turn is determined by the specific dynamics of the electron's system. For relativistic QM the same is true -- up to a few technical matters.

There are no stable two-proton one or two electron systems. Replace a proton by a neutron, and you are talking helium city, a stable place.

Regards,
Reilly Atkinson
 
I think he meant a Hidrogen molecule.That's pretty stable.And it has no neutrons.


Daniel.
 
reilly said:
For nonrelativistic QM, the square of the electron's wave function times the electric charge is the spatial charge density,

This is what I guessed but when reading the Feynman lectures on physics vol 3 chapter 10 he talks about a two state system made up of two separated protons with one electron that's orbiting a different proton in each state. Now when you have a superposition of both states I would guesse the electrons charge would be spread out over both protons (it seemes to me your statement above says this) but then I would think the protons would repel each other. However Feynman says the protons don't repel because one proton is nutrual because of the electron orbiting it. (well they did repel or atract but not because both protons were positive)
Sorry if what I wrote dosn't make a lot of sense.
 
Since you're talkig about the H_{2} molecule,words won't do.Mathematics should come first.So how about you do some reading & caculations...?The proton may be screened,but not neutral.

Daniel.
 
Hello box,

it seems strange that a [itex]H_{2}^{+}[/itex] molecule exists, because as you mentioned one would think that the protons repel each other. However QM calculations indeed show that it is stable only because of that one electron.

Why is this so? You can think of the electron acting as glue between the protons (or as dextercioby said the proton's charge is screened by the electron's negative charge)
 
Edgardo said:
Hello box,

it seems strange that a [itex]H_{2}^{+}[/itex] molecule exists, because as you mentioned one would think that the protons repel each other. However QM calculations indeed show that it is stable only because of that one electron.

Why is this so? You can think of the electron acting as glue between the protons (or as dextercioby said the proton's charge is screened by the electron's negative charge)

And this is a good opportunity to add that that single electron in between the two H nucleus is actually in a Schrödinger Cat-type state where it is "localized" at BOTH nucleus simultaneously! [See? All of physics/QM are really connected!] The electron is being spread out over both nucleus in such a way that the overlap of its location from both nucleus causes a bonding state and an antibonding state of the ground state. This is something chemists have seen way before QM, but it had to wait till QM for there to be an explanation for the existence of such a state.

Zz.
 
  • #10
To answer the original question :
box said:
So am I right in saying that sometimes an elecrons charge is spread out over the area were its position is uncertin and somtimes its not?
No, that's not right. As explained previously, the charge density at some point [itex]\vec{r}[/itex] scales with the probability of finding the electron in the vicinity of [itex]\vec{r}[/itex].

[tex]\rho(\vec{r}) = e|\psi({\vec{r})|^2[/tex]
 

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