What is Coulomb potential and energy?

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Discussion Overview

The discussion revolves around the concept of Coulomb potential and energy, particularly in the context of classical electrostatics and its application to atomic models. Participants explore the definitions and equations associated with Coulomb potential, potential energy, and the implications of treating atoms classically versus quantum mechanically.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question the equations for Coulomb potential and energy, noting discrepancies in their understanding.
  • There is a discussion about the definition of charge Q as Ze and its implications for calculating electric potential energy.
  • One participant suggests that the term "Coulomb" primarily refers to classical electrodynamics.
  • Another participant explains that for a one-electron atom, the classical treatment is more straightforward, while multi-electron atoms complicate the situation due to significant quantum effects.
  • Participants express uncertainty about the appropriateness of classical models for atoms with multiple electrons.

Areas of Agreement / Disagreement

Participants generally agree on the basic definitions of charge and potential energy but express differing views on the applicability of classical models to multi-electron atoms. The discussion remains unresolved regarding the accuracy of the equations presented and the implications of treating atoms classically.

Contextual Notes

There are limitations regarding the assumptions made about screening and quantum effects in multi-electron atoms, which are not fully explored in the discussion.

quietrain
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is it just potential and potential energy?

but if so, why is it given as

V(r) = - Ze2 / 4πεr ?
and
E = Z2e2 / 4πεr

i am having trouble understanding how come for potential V, Q = Ze2

while

for E, Q2 = Z2e2

thanks!
 
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If E is meant to denote the classical electrostatic field and V the classical electrostatic potential, then your equations look all wrong. Where did you get them?

The term "Coulomb potential" is essentially used to mean the potential that gives rise to a classical electrostatic force (quantum effects can be neglected). Van der Waals force potentials, covalent bond potentials, quantum wells, etc. are all electromagnetic potentials but are quantum in nature.
 
i got them off my notes, but they may be wrong

so is it right that charge Q = Ze?

so electric potential energy = kQQ/R = k(Ze)2/R ?

Ze is bascially the charge of the nucleus right? number of proton mulitply by electron charge e?

also, so the term "coulomb" refers to classical electrodynamics mainly?
 
quietrain said:
i got them off my notes, but they may be wrong

so is it right that charge Q = Ze?

Yes, if you are neglecting screening and quantum effects, then the total charge of a mass it the number of elementary charges (protons) times the charge of one element.

quietrain said:
so electric potential energy = kQQ/R = k(Ze)2/R ?

I think I see the problem. Coulomb Potential energy U = kQ1Q2/R where Q1 is the charge of the one particle and Q2 is the charge of the other. If you are treating a one-electron atom classically, then for the electron Q1 = -e and for the protons, Q2 = +Ze so that:

U = k(-e)(Ze)/R = - k Ze2/R

quietrain said:
Ze is bascially the charge of the nucleus right? number of proton mulitply by electron charge e?
Yes
quietrain said:
also, so the term "coulomb" refers to classical electrodynamics mainly?

Yes
 
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chrisbaird said:
If you are treating a one-electron atom classically, then for the electron Q1 = -e and for the protons, Q2 = +Ze so that:

U = k(-e)(Ze)/R = - k Ze2/R

ah i see... but why is an atom "one-electron" classically?
 
quietrain said:
ah i see... but why is an atom "one-electron" classically?

When you have an atom with more than one electron, the quantum effects become so strong that using a classical approach is rendered essentially useless. If you are going to use Coulomb's law to describe an atom (already a shaky proposition), it's best to keep to one-electron atoms. Even with the help of quantum theory, deriving the potential of a multi-electron atom is nontrivial. Sadly, most of the atoms we encounter in every day life are multi-electron, so the clean one-electron pictures are not entirely useful.
 
i see thank you very much
 

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