How to Estimate the Energy of a Delocalized π Electron in Benzene?

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Discussion Overview

The discussion revolves around estimating the energy of a delocalized π electron in benzene (C6H6) by modeling it as a "particle on a ring." Participants explore the implications of quantum numbers, energy states, and the structure of nodes in relation to the problem, which is framed as a homework question involving theoretical and mathematical reasoning.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants express uncertainty about how to approach the problem and the meaning of quantum numbers in this context.
  • There is a discussion about how each energy state n can hold multiple electrons, with n=0 holding 2 electrons and n>0 holding 4 electrons, though the reasoning behind determining n is questioned.
  • One participant suggests that the quantum number n is related to the angular momentum of the electron, noting that n can be both positive and negative, but clarifies that all energies are non-negative.
  • Another participant emphasizes the importance of understanding the relationship between quantum numbers and nodes, suggesting that the number of nodes relates to the de Broglie wavelength of the electrons.
  • There is mention of the need to calculate energies for degenerate pairs of states and how to fill these states with the six π electrons, drawing parallels to atomic filling rules.
  • Participants question what important interactions might be neglected in this model, hinting at deeper complexities in the system.

Areas of Agreement / Disagreement

Participants generally agree on the framework of the problem and the basic principles involved, but there is no consensus on how to determine the quantum number n or the implications of the model. The discussion remains unresolved regarding the specifics of calculating energy and the assumptions made in the model.

Contextual Notes

Limitations include the potential neglect of interactions between electrons and the assumptions made about the model's applicability to benzene's electronic structure. The discussion also highlights the complexity of determining quantum states and their corresponding energies.

spaghettibretty
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Homework Statement



Six of the electrons from benzene C6H6 form a delocalized conjugated π-bond. We will model it as a "particle on a ring" with ring radius a, particle (electron) mass m, and "moment of inertia" I = ma2. After obtaining the energy diagram, we will fill in these 6 electrons. Please estimate the energy (in Joules) of a single delocalized π electron in the specific state shown above. Assume the radius a = 0.15 nanometers. (Hint: Just like the "quantum square" or particle in a 1-D box" problem, one can estimate the quantum number or which state from the number and structure of the nodes)

d0fz4Iw.png


Homework Equations



E = n2 * (h-bar)2 / (2 * I)
h-bar = reduced Planck's constant = h / (2 * pi)
I = ma2

The Attempt at a Solution



I'm not sure where to go with this problem, I don't really understand this problem since this is one of those "extended knowledge" problems not generally covered. I know, after solving the energy formula, that each energy state n after 0 can hold 4 electrons since there is a positive and negative energy state n, and each n holds 2 electrons. Therefore on the energy level diagram, n=0 holds 2 electrons and n>0 holds four electrons. I'm pretty sure you just plug in numbers to the energy equation, but I have no idea how to determine the n's.
 
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spaghettibretty said:
I know, after solving the energy formula, that each energy state n after 0 can hold 4 electrons since there is a positive and negative energy state n, and each n holds 2 electrons. Therefore on the energy level diagram, n=0 holds 2 electrons and n>0 holds four electrons. I'm pretty sure you just plug in numbers to the energy equation, but I have no idea how to determine the n's.
There is just one n to determine to answer the question:
spaghettibretty said:
Please estimate the energy (in Joules) of a single delocalized π electron in the specific state shown above.
To do that, you need to use the hint
spaghettibretty said:
(Hint: Just like the "quantum square" or particle in a 1-D box" problem, one can estimate the quantum number or which state from the number and structure of the nodes)
So, in the particle in a box, what is the relation between n and the nodes?
 
spaghettibretty said:

Homework Statement



Six of the electrons from benzene C6H6 form a delocalized conjugated π-bond. We will model it as a "particle on a ring" with ring radius a, particle (electron) mass m, and "moment of inertia" I = ma2. After obtaining the energy diagram, we will fill in these 6 electrons. Please estimate the energy (in Joules) of a single delocalized π electron in the specific state shown above. Assume the radius a = 0.15 nanometers. (Hint: Just like the "quantum square" or particle in a 1-D box" problem, one can estimate the quantum number or which state from the number and structure of the nodes)

d0fz4Iw.png


Homework Equations



E = n2 * (h-bar)2 / (2 * I)
h-bar = reduced Planck's constant = h / (2 * pi)
I = ma2

The Attempt at a Solution



I'm not sure where to go with this problem, I don't really understand this problem since this is one of those "extended knowledge" problems not generally covered. I know, after solving the energy formula, that each energy state n after 0 can hold 4 electrons since there is a positive and negative energy state n, and each n holds 2 electrons. Therefore on the energy level diagram, n=0 holds 2 electrons and n>0 holds four electrons. I'm pretty sure you just plug in numbers to the energy equation, but I have no idea how to determine the n's.

Remember, the n's are quantum numbers. These are integers.

The first relevant equation uses unfortunate choices for quantum numbers. The particle on a ring is an interesting example to show the quantization of angular momentum. In the first equation, the quantum number "n" is actually a measure of the electron-bead's angular momentum. If you imagine an electron-bead living/spinning around on the ring, what might its angular momentum be? You could have a ground-state (non-moving) electron, delocalized over the entire ring (n=0). With a moving electron/bead (n<>0) how might it be moving? As you note, n can be positive or negative, and n=-1 and n=1 states have the same energy (you alluded to "positive and negative energy states" which is not quite right -- all of the energies in this >= 0.

You will have an "energy level" with n=0, whose energy is E0 = 0; a degenerate pair of |n| = 1 levels, whose energy you can calculate; a degenerate pair of |n| = 2 levels, whose energy you can caclulate; etc. You have six pi electrons to fill these levels -- you do this just like you did in atoms (Aufbau + Pauli) in general chemistry. The total energy is the sum of the energies of the individual electrons.

What important interaction is this problem neglecting?
 
Quantum Defect said:
Remember, the n's are quantum numbers. These are integers.

The first relevant equation uses unfortunate choices for quantum numbers. The particle on a ring is an interesting example to show the quantization of angular momentum. In the first equation, the quantum number "n" is actually a measure of the electron-bead's angular momentum. If you imagine an electron-bead living/spinning around on the ring, what might its angular momentum be? You could have a ground-state (non-moving) electron, delocalized over the entire ring (n=0). With a moving electron/bead (n<>0) how might it be moving? As you note, n can be positive or negative, and n=-1 and n=1 states have the same energy (you alluded to "positive and negative energy states" which is not quite right -- all of the energies in this >= 0.

You will have an "energy level" with n=0, whose energy is E0 = 0; a degenerate pair of |n| = 1 levels, whose energy you can calculate; a degenerate pair of |n| = 2 levels, whose energy you can caclulate; etc. You have six pi electrons to fill these levels -- you do this just like you did in atoms (Aufbau + Pauli) in general chemistry. The total energy is the sum of the energies of the individual electrons.

What important interaction is this problem neglecting?

Doh! Forgot the point of the problem. The n=0 electron is delocalized over the whole ring (no nodes). The |n|=1 electrons are moving, they have a de Broglie wavelenth. How could you fit something with a wavelength into the ring (this is like the Bohr model of the hydrogen atom)? If you draw the picture of the wave, are there any nodal planes? How many? A higher |n| will be for an electron with a shorter de Broglie wavelength. What do these waves look like? How do the number of nodal planes change as the de Broglie wavelength decreases?
 

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