Solving Bohr Atom Problem (Qs a-e)

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SUMMARY

The discussion focuses on solving the Bohr atom problem, specifically addressing questions (c) and (e). Participants clarify that the energy levels scale linearly, with the equation En = E1n indicating that energy levels are equidistant and positive. The ionization energy is defined as the difference between the last bound state and the ground state, with the limit of energy approaching infinity as n approaches infinity. This model parallels the quantum harmonic oscillator, which lacks a defined energy limit for bound states.

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StillAnotherDave
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Homework Statement
Help with parts (c) and (e)
Relevant Equations
Given in the screenshot
1583324443717.png


Hello folks,

I've managed questions (a) and (b) but don't get what to do with part (c). Normally you would equate the velocity equations v2=e2/4πεmr=(n2h2)/(m2r2 ). This let's you isolate the radius and use it to calculate En. But I can't see how you could do this for v given in (a) and (b).

Also, part (e). If En = E1n then the energy levels simply scale linearly ... that can't be right?
 
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Okay. I managed to solve part (c) by isolating r2.

But part (e) is still unclear ...
 
StillAnotherDave said:
Okay. I managed to solve part (c) by isolating r2.

But part (e) is still unclear ...
Remember, this is not a "real"atom where electric force acts between the proton and electron. You derived that En = Ein .Are those energy levels equidistant?
 
They would be linear (equidistant) and positive - i.e. n=1 is 1eV; n=2 is 2eV; n=3 is 3eV ... is that correct?

But wouldn't n = ∞ need to be 0eV?

It makes the remaining parts of the question (f) and (g) very confusing:

1583331082927.png
 
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Clearly this is ludicrous ... help!
 
StillAnotherDave said:
They would be linear (equidistant) and positive - i.e. n=1 is 1eV; n=2 is 2eV; n=3 is 3eV ... is that correct?
Yes.

StillAnotherDave said:
But wouldn't n = ∞ need to be 0eV?
The choice of zero of energy is arbitrary. For the hydrogen atom, the ionization limit (separated particles) is often chosen as the 0, but this is arbitrary. One could also take the ground state to be 0.
 
Okay ... so for question (f), could photons not be emitted for any energy multiple of E1? And how would the ionisation energy be determined?
 
StillAnotherDave said:
Okay ... so for question (f), could photons not be emitted for any energy multiple of E1?
Yes.

StillAnotherDave said:
And how would the ionisation energy be determined?
How is it determined for the hydrogen atom?
 
The lowest energy level, n=1 at E1 is given as 1.0 eV ... so that would be the ionisation energy?
 
  • #10
Okay ... so for question (f), could photons not be emitted for any energy multiple of E1?

DrClaude said:
Yes.

But this doesn't seem to make sense for a 3 mark question ...
 
  • #11
StillAnotherDave said:
The lowest energy level, n=1 at E1 is given as 1.0 eV ... so that would be the ionisation energy?
No. Again, how is the ionization energy calculated in hydrogen?

StillAnotherDave said:
But this doesn't seem to make sense for a 3 mark question ...
I'm not responsible the grading scheme :smile:. I guess some explanation is expected.
 
  • #12
Ionisation works by removing an electron from it's most outer bound shell ... but if the energy is increasing as En=E1n then essentially you're saying you can't remove the electron ... ?
 
  • #13
As far as I understand ionization energy, it depends on which state the electron is in.
 
  • #14
You're almost there, so I'll give you the answer. The ionization energy is the difference in energy between the last bound state and the ground state. Here, you have
$$
\lim_{n\rightarrow \infty} E_n = \infty
$$
so it is impossible to remove the electron.

By the way, you are basically creating a model for the harmonic oscillator, which indeed has no limit in energy for bound states.
https://en.wikipedia.org/wiki/Quantum_harmonic_oscillator
 

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