Probability wave peaks and quantum number

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Discussion Overview

The discussion revolves around the interpretation of quantum numbers, specifically the principal quantum number (n) and the azimuthal quantum number (l), in relation to the peaks of probability waves and their implications for electron energy levels in atoms. Participants explore concepts related to atomic wavefunctions, energy states, and the relationship between quantum numbers and electron probability distributions.

Discussion Character

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

Main Points Raised

  • Some participants suggest that the principal quantum number (n) represents the number of peaks in the probability wave and correlates with higher energy states due to increased frequency.
  • Others argue that the relationship between n and energy is more complex, noting that n indexes discrete energy eigenstates and can correspond to the number of radial peaks, but this is context-dependent.
  • There is a discussion about the azimuthal quantum number (l) and its effect on the shape of orbitals, with some participants questioning how different values of l affect the number of peaks and energy levels.
  • One participant emphasizes that peaks in the probability wave indicate points of high electron probability, forming the electronic cloud boundary, while questioning the quantization of orbits in the Bohr model.
  • Participants discuss the concept of screening effects and how they influence the energy levels of electrons in different orbitals, particularly comparing 2s and 2p states.
  • There are inquiries about the relationship between the peaks of the probability density function and the energy of electrons, with some suggesting that as l increases, the number of peaks decreases due to zero probability regions.

Areas of Agreement / Disagreement

Participants express various viewpoints on the relationship between quantum numbers, energy, and probability waves, indicating that multiple competing views remain. There is no consensus on the implications of quantum numbers for energy levels or the interpretation of probability peaks.

Contextual Notes

Participants note limitations in understanding the relationship between quantum numbers and energy, as well as the effects of screening on electron states. Some statements rely on specific interpretations of atomic wavefunctions and may not universally apply across different contexts.

Who May Find This Useful

This discussion may be of interest to students and enthusiasts of quantum mechanics, atomic theory, and those exploring the foundational concepts of quantum numbers and their implications for electron behavior in atoms.

Chemer
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Hi,
Just wanted to ask, the principal quantum number represent the number of peaks of the probability wave and I think more the value of n, more the energy of the electron as the wave has more peaks so higher frequency,am I right? Then in azimuthal quantum number, the orbitals with same energy have different number of peaks, means different energy? But why? I'm referring to the point in this site:

http://www.chem1.com/acad/webtext/atoms/atpt-4.html

Maybe I've misunderstood the point because I'm really a beginner, please guide.
 
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Depends... principle quantum number of what?
Usually, "n", in textbooks, indexes the discrete energy eigenstate.
This can correspond to the number of antinodes in the associated energy eigenfunction.
But it does not have to... check the context.

I did not find a reference to "azimuthal quantum number" in your link.
The context is "atomic wavefunctions in chemistry" and the site encourages you to think of n as indexing the average distance from the nucleus.
Since an atom is a 3d object, there are several ways to get peaks in the probability density function. You will have seen that n is the number of radial peaks.
 
Last edited:
s-orb_shells.png
I was referring to this point on the site:

"Each wave pattern is identified by an integer number n, which in the case of the atom is known as the principal quantum number. The value of n tells how many peaks of amplitude (antinodes) exist in that particular standing wave pattern; the more peaks there are, the higher the energy of the state."

And that:

"When l = 0, the orbital is spherical in shape. If l = 1, the orbital is elongated into something resembling a figure-8 shape, and higher values of l correspond to still more complicated shapes— but note that the number of peaks in the radial probability distributions (below) decreases with increasing l."

Can you explain it in easy words? Aren't the peaks representing the frequency and energy of the probability wave?
 

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Put simply, l and n states are different and have different rules.
The peaks do not represent frequency or energy of the wave.
The wavey shapes on the graph are not waves in the sense of water or sound waves.
 
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The peaks of probability wave are the points where the electron is mostly likely to be found, and these peaks form the electronic cloud boundary with a radius in agreement to that predicted by Bohr's model. And each cloud has a specific wave pattern represented by specific number of peaks, the principal quantum number. So, didn't the orbits were quantized in Bohr model, and greater n greater number of peaks, so greater energy? Am I right? Please guide.
and then what the peaks represents in case of the sub shells?
 
Chemer said:
The peaks of probability wave are the points where the electron is mostly likely to be found, and these peaks form the electronic cloud boundary with a radius in agreement to that predicted by Bohr's model
What is the radius for the n=1 peak?
What is the Bohr model radius for n=1?
Do these agree?
 
I realized now, from the Ist image the average radius of n= 3 agrees with Bohr's radius of n=1 that's 53 pm I think. But I don't understand why?
And what does these peaks represent?
Also when we say electron in 2s has lower energy than 2p, because of screening effect,I couldn't understand what is meant by p orbital being higher than s? They've same n, so same energy but the energy lowers because of the screening effect?
 
The peaks represent the maxima of the probability density function.

The 2s and 2p electrons would have the same energy if the electrons did not have any effect on each other.

If you have a 5 proton nucleus (B) with two electrons in 1s, can you see that this looks from farther away like a Li nucleus?
That effect is called "screening".
Add two more electrons, what is the lowest state they can go to?
 
"The peaks represent the maxima of the probability density function."

So, as the increase in l, means increase in zero probability region thus the number of peaks decrease, am I right? And in case of n, the energy is nothing to do with probability density but with the electron's distance from the nucleus?

"The 2s and 2p electrons would have the same energy if the electrons did not have any effect on each other.

"If you have a 5 proton nucleus (B) with two electrons in 1s, can you see that this looks from farther away like a Li nucleus? That effect is called "screening".
Add two more electrons, what is the lowest state they can go to?"

Do you mean as Li has 3 protons, 2 are shielded by its 1s electrons and the outermost electron feels the effect of only one proton? So, in boron 2 protons are shielded by 1s electrons, then the 2s state has now lower energy and electrons will go to 2s? What about the remaining nuclear charge? How will it effect the electrons preference? And the n has changed as well, so does it have any effect on this phenomena?
 

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