Probability density versus radial distribution function

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Discussion Overview

The discussion revolves around the differences between the probability density and the radial distribution function in quantum mechanics, specifically in the context of the hydrogen atom's 1s orbital. Participants explore the implications of these concepts as they relate to electron density and the behavior of wave functions.

Discussion Character

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

Main Points Raised

  • One participant expresses confusion about how the radial distribution function can be zero at r=0 while the probability density is at a maximum there.
  • Another participant clarifies that the radial distribution function accounts for the volume element, which goes to zero at r=0, leading to its value being zero despite the probability density being non-zero.
  • A participant explains that the radial distribution function represents the probability of finding an electron in a spherical shell, not at a single point, which contributes to the confusion.
  • There is a discussion about the implications of the radial distribution function being zero at the origin, with one participant questioning how this relates to electron density within the nucleus.
  • Some participants discuss the concept of electron capture and whether the electron wave function penetrates the nucleus, with differing views on the implications for the hydrogen atom.
  • A participant raises a question about the meaning of negative values in radial wave function plots, leading to clarification that it is the square of the wave function that represents probability, which is always non-negative.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the radial distribution function and the behavior of the electron wave function, particularly regarding its penetration into the nucleus and the interpretation of negative values in wave function plots. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Some assumptions about the definitions of probability density and radial distribution function are not fully articulated, and there are unresolved questions about the behavior of wave functions at certain distances.

ishchayill
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Okay, this is a really basic question. I'm just learning the basics of QM now.

I can't wrap my head around the idea that the radial distribution function goes to zero as r-->0 but that the probability density as at a maximum as r-->zero. How can this be?

Thanks!
 
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What are you referring to exactly? The hydrogen ground state wave function? As you say, the probability density is a maximum at r=0. Perhaps the point you've missed is that the volume element (r^2 sin(theta))dr dtheta dphi goes to zero at r=0?
 
Ah, the 1s orbital. It's a common source of confusion, that.
Well, the radial wavefunction has a maximum at r=0. This is the point, i.e. infinitesimal volume element that has the highest probability. It's the volume of space the electron's most likely to be in.

The radial distribution function, on the other hand, is the sum of probabilities over a given r. It's not the probability of just one spot, but of every spot on the surface of an infinitesimally thin sphere of that radius. Since a sphere with zero radius has zero area, it means the radial distribution is 0 at r=0 no matter what the wave function's value there.

An analogy I once thought up: Imagine you paint a bunch of different-sized spheres, and where the thickness of the paint is e^{-r}.. The sphere with the thickest coat of paint is not the same thing as the sphere with the most paint on it!
 
Thank you. Yes, I'm referring to the 1s H-atom.

Mathematically it makes perfect sense: if r=0 then the radial distribution function is zero. So let's say we take a concentric sphere with the inner surface being the surface of the nucleus, and the outer surface at a distance dr from the surface of the nucleus. Saying that the radial distribution function is zero means that electrons will never be found within that volume. On the other hand, probability density (psi^2) tells us that there is some finite probability that an electron will be found in that very same region of space. Doesn't it?
 
It's only right at the origin that the radial distribution function goes to zero. Since the 1s wave function is spherically symmetric, the probability of finding the electron between r and r+dr is give by the expresssion: 4\pi r^2 \psi(r) \psi^*(r) dr. This will be nonzero (but very small) when r=r(nucleus), as you asked. The reason it will be very small is that the volume of space at r=r(nucleus) is very small. Try plotting the functions 4\pi r^2 \psi(r) \psi^*(r) and \psi(r) \psi^*(r), and I think you will see why it is this way.
 
So r=0 is defined as the center of the nucleus?
 
Yes. Where else would it be?
 
Okay, but then how can there be any electron density inside the nucleus?
 
Why can't the electron be inside the nucleus? Elementary particles appear to be pointlike as far down as we can measure. So even inside the nucleus it appears to be mainly empty space between the quarks and gluons that make it up. We know the electron definitely penetrates inside the nucleus because there are types of radioactive decay (called electron capture) where the nucleus basically captures one of the atomic electrons and transmutes into a nucleus with atomic number reduced by one.
 
  • #10
Electron capture occurs in large nuclei; however, the proton of the hydrogen atom cannot capture an electron yielding a free neutron.
 
  • #11
rlduncan said:
Electron capture occurs in large nuclei; however, the proton of the hydrogen atom cannot capture an electron yielding a free neutron.

No, of course not. I didn't mean to say that it could. I was just saying that this is evidence that the electron wave function does penetrate the nucleus. Do you think the electron wave function does not penetrate the nucleus of a hydrogen atom?
 
  • #12
If the radial wave function represents the probability that an electron will be contained within an infinitesimal volume at some specified radius, how can it be then that some plots of the radial wave functions have negative values, would this not imply a negative probability at these distances?

For example, what does the radial wave function tell us at the distances where minima occur in the 2s, 3s and 3p plots?

Thanks.:rolleyes:
 
  • #13
Scott Gray said:
If the radial wave function represents the probability that an electron will be contained within an infinitesimal volume at some specified radius, how can it be then that some plots of the radial wave functions have negative values, would this not imply a negative probability at these distances?

For example, what does the radial wave function tell us at the distances where minima occur in the 2s, 3s and 3p plots?

Thanks.:rolleyes:

It's not the wave function itself that represents the probability of finding the electron at a given location. It is the square of the wave function ψψ* . This quantity is always non-negative, although it can be zero.
 

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