Bohr Model: Energy Jump in Hydrogen Atom

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SUMMARY

The forum discussion centers on the energy transitions of electrons in a hydrogen atom, specifically the transition from the second orbit (n=2) to the first orbit (n=1). It is established that this transition results in the largest energy change compared to other transitions, as confirmed by the Rydberg formula. The calculations demonstrate that the energy change for the transition from n=∞ to n=2 is less than that from n=2 to n=1, highlighting the clustering of energy levels near the continuum. Misconceptions regarding energy levels and orbit radii were clarified, emphasizing the importance of understanding effective nuclear charge.

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  • Understanding of quantum mechanics and atomic structure
  • Familiarity with the Rydberg formula for hydrogen
  • Knowledge of energy levels and transitions in atomic physics
  • Concept of effective nuclear charge and electron shielding
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  • Study the Rydberg formula in detail to understand its application in energy transitions
  • Explore quantum mechanics principles related to atomic orbitals and energy levels
  • Investigate the concept of effective nuclear charge and its impact on electron behavior
  • Examine the differences between classical and quantum mechanical models of the atom
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Students of physics, educators teaching atomic theory, and researchers interested in quantum mechanics and atomic energy transitions will benefit from this discussion.

hav0c
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Am I right in saying that in a Hydrogen atom when an electron jumps from the second orbit to the first one the energy change is more than any other possible jump (when the jump is not to the first orbit). The calculations seem to support me but it doesn't feel right.
 
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hav0c said:
Am I right in saying that in a Hydrogen atom when an electron jumps from the second orbit to the first one the energy change is more than any other possible jump (when the jump is not to the first orbit). The calculations seem to support me but it doesn't feel right.
Why does it not feel right?
What calculations seem to support you and how?

The transition from continuum to the n=1 shell (the "first one") releases the most potential energy, but for a transition of the type n+1 to n, the transition 2->1 has the largest energy change.
You should be able to verify this from the Rydberg formula.
 
Simon Bridge said:
Why does it not feel right?
What calculations seem to support you and how?

The transition from continuum to the n=1 shell (the "first one") releases the most potential energy, but for a transition of the type n+1 to n, the transition 2->1 has the largest energy change.
You should be able to verify this from the Rydberg formula.
this is exactly what i am getting, but thinking logically shouldn't the transition from n=∞ to n=2 produce a greater energy change?(than n=2 to n=1)
Also wouldn't this imply that to ionize an atom from the second shell the energy required is atleast less than half than that to ionize it from the first shell?
 
hav0c said:
but thinking logically shouldn't the transition from n=∞ to n=2 produce a greater energy change?(than n=2 to n=1)

Can you describe the logic?
 
well since energy increases as distance from nucleus increases and the energy gap b/w consecutive orbits decreases, it seems to me that if what i am saying is true, then distance b/w n=1 and n=2 should be greater than n=2 to n=∞, which is wrong.
Edit: thanks a lot i got my mistake
Edit 2: this is true right?Also wouldn't this imply that to ionize an atom from the second shell the energy required is atleast less than half than that to ionize it from the first shell?
 
The transition inf->2 is not a transition of form n+1 -> n; but never mind.

The energy changes are proportional to the difference in the reciprocal of the squares of the start and finish quantum numbers.

transition from inf->2 would be proportional to |0-1/4|=1/4
transition from 2->1 would be proportional to |1-1/4|=3/4
(notice how taking 1/4 from 0 gets a smaller number than taking 1/4 from 1?)

simiarly:
transition from inf->3 would be proportional to 1/9
transition from 3->1 would be proportional to 8/9

i.e. the energy levels tend to cluster close to the continuum level. re:

hyd_levels.gif


I think you are confusing energy levels with orbit radii.
You should not be picturing radii at all in connection with atomic shells: it is a completely false picture.
 
Last edited:
hav0c said:
this is exactly what i am getting, but thinking logically shouldn't the transition from n=∞ to n=2 produce a greater energy change?(than n=2 to n=1)

Imagine an enormous flat plain at 100 meters above sea level. In the middle of this plain there's a shallow depression; the bottom of the depression is 90 meters above sea level. And then right at the low point of this depression someone has drilled a well 500 meters into the ground.

Send a 1kg ball rolling from infinity to the bottom of the depression and it will drop 10 meters with energy change ##mgh## equal to 100 Joules; that's the transition from n=∞ to n=2. But when it falls to the bottom of the well (n=2 to n=1) it will pick up another 5000 Joules.
 
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Simon Bridge said:
The transition inf->2 is not a transition of form n+1 -> n; but never mind.

The energy changes are proportional to the difference in the reciprocal of the squares of the start and finish quantum numbers.

transition from inf->2 would be proportional to |0-1/4|=1/4
transition from 2->1 would be proportional to |1-1/4|=3/4
(notice how taking 1/4 from 0 gets a smaller number than taking 1/4 from 1?)

simiarly:
transition from inf->3 would be proportional to 1/9
transition from 3->1 would be proportional to 8/9

i.e. the energy levels tend to cluster close to the continuum level. re:

hyd_levels.gif


I think you are confusing energy levels with orbit radii.
You should not be picturing radii at all in connection with atomic shells: it is a completely false picture.
Thanks a lot i was not considering the decrease in effective charge. that's why i wasn't able to understand the numbers
 
hav0c said:
Thanks a lot i was not considering the decrease in effective charge. that's why i wasn't able to understand the numbers
The "effective charge" of a nucleus is usually due to inner-shell electrons screening the nuclear charge from the outer shell electrons. That is different from what you are talking about: the electron still sees the entire +e charge from the nucleus no matter what it's energy level.

[BTW: thanks for spotting the typo - edited in original]
 
  • #10
When the theory conflicts with your intuition, it's time to fix the intuition! (well, actually, intuition is a very useful guiding force, but in this case it's wrong)
 

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