Understanding Hydrogen Fine Structure Validity and Field Discrepancies

In summary, the site provides an approximation for the value of B, which is in units of Tesla. B is not a single value, but comes from the shift of 2p in both cases.
  • #1
bobie
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Homework Statement


This is not homework, I am trying learn fine structure.
This site is reliable : http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html, can you tell me if the content of "hydrogen fine structure" is still valid or dated?.
Even if it were classical oudated model, I'd like to understand it. Just a few preliminary questions:

- the wavelength of transition 3s => 2p is given as 656.11 or (with reduced mass) 656.47 in the text, but in the picture it becomes 656.3, why that?
- the real values of fine structure are then 656.316 and 656.284?
- B field is indicated (at 2p) 0.4 T while in the third frame it becomes 0.3 T, which is right?

Homework Equations


- the right formula to find B is: μ0* qv /4πr2 ?, does it work both in mks and cgs?

I'll post an attempt at a solution, after your answers

Thanks for your help
 
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  • #2
For the absolute values and at this level of precision, you have to account for relativistic effects and the refractive index of air, the difference could come from a different treatment of those.
Spectral line database

can you tell me if the content of "hydrogen fine structure" is still valid or dated?.
The fine-structure is known for several decades now and nothing changed.The magnetic field is not a constant value everywhere, those calculated numbers are a rough estimate and cannot agree perfectly.
Formulas work independent of the unit system.
 
  • #3
mfb said:
The fine-structure is known for several decades now and nothing changed..
Thanks for the link.
I was referring to the article "Hydrogen fine structure" in this site http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html.
I would like to know if the data in there are a good approximation of what are considered today the real values.

-In particular if the formula they give in the 3rd and 4th frame to calculate the value of B
[itex]B = \frac{\mu0*qv}{4πr^2}[/itex]
which gives 12.5 T for 1s level and 0.39 for 2p.

- Also I do not understand why (in the first frame) the value of the spin-orbit split is the same (i.e. 0.000045 eV) for the 2p => 1s transition ( at the top of the frame) and the 3s => 2p (at the bottom). Since B is 32 times greater and only the value of the spin magnetic moment is always the same (1/2*h/2π) I expected the delta value of the splits of the fine structure to be different.

I'd appreciate any help on these issues. Thanks
 
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  • #4
All those Tesla values are not "real" field strengths. They are a classical approach to a quantum mechanical effect. They can lead to some interesting insights, but don't think something could be replaced by a magnetic field of that strength.

- Also I do not understand why (in the first frame) the value of the spin-orbit split is the same (i.e. 0.000045 eV) for the 2p => 1s transition ( at the top of the frame) and the 3s => 2p (at the bottom).
The split comes from the shift of 2p in both cases.

Direct link
 
  • #5
mfb said:
All those Tesla values are not "real" field strengths.
..They can lead to some interesting insights, but don't think something could be replaced by a magnetic field of that strength.
Thanks for the direct link, :smile: mfb, I was going mad trying to post it properly. How did you do it ?
Sorry, but I do not understand the bolded bit, to what is something referring?

Can I get a good approximation of B dividing the energy of the split E (0.000045 eV) by [itex]\mu[/itex] since [itex]\mu*B = E[/itex] ?
B = 0.000045*4pi T ?
 
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  • #6
bobie said:
How did you do it ?
Check where the site is linked at, copy this link.

Sorry, but I do not understand the bolded bit, to what is something referring?
Looking for a single value for a magnetic field strength is as meaningful as looking for a single value for the speed of cars (yes, as general as that). So, how fast are cars?
It just does not make sense to reduce this to a simple number. You can still say "a typical speed is 50 to 100km/h", this is equivalent to the values you see for B at those pages.
 
  • #7
mfb said:
Looking for a single value for a magnetic field strength is as meaningful as looking for a single value for the speed of cars (yes, as general as that).

My question was more modest, I probably should have quoted the article in my first post.
"the splitting of each of them is about 0.016 nm, corresponding to an energy difference of about 0.000045 eV. This corresponds to an internal magnetic field on the electron of about 0.4 Tesla.

0.000045 eV = 7.2 *10-24 J
in another thread, here, I just learned that [itex]\mu[/itex] = ≈3.2*10-23 J/T

E =7.2*10-24 J, now E= mu*B, but E/ itex]\mu[/itex] it is not near 0.4
Where is my mistake?
Thanks for your help.
 
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  • #8
E=µB is valid if B is constant everywhere, but that is not the case.
 
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  • #9
mfb said:
E=µB is valid if B is constant everywhere, but that is not the case.
Thanks, mfb, what baffled me (and that's why I went on posting) is that maybe in QM things are different , but they state that it works all the same in Bohr's model, so they must have worked it out some way
.
Thanks you for your help
 
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  • #10
Bohr's model is wrong, even if it gives some right values for hydrogen-like atoms.
 
  • #11
bobie said:
[itex]\mu[/itex] = ≈3.2*10-23 J/T
The magnetic moment of the electron is ##\mu_\mathrm{e} = -9.284764 \times 10^{-24}\ \mathrm{J/T}##. If you add the additional g-factor, ##g \approx 2##, you will get the right answer for the energy splitting.
 
  • #12
DrClaude said:
The magnetic moment of the electron is ##\mu_\mathrm{e} = -9.284764 \times 10^{-24}\ \mathrm{J/T}##. If you add the additional g-factor, ##g \approx 2##, you will get the right answer for the energy splitting.
That value is Bohr magneton 9.274 multiplied by g/2: 1.00116
I have been told that :
dauto said:
...The electron's magnetic dipole moment is given by [tex]\boldsymbol{\mu} = g \frac{-e}{2m_e} \mathbf{L}[/tex]
where L is √3/2 [itex]\hbar[/itex]
 
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  • #13
bobie said:
That value is Bohr magneton 9.274 multiplied by g/2: 1.00116
Yes, I made a small mistake there with the g-factor. The magnetic moment to use to calculate the splitting is ##\mu = g \mu_\mathrm{B} = -2 \mu_\mathrm{e}##.


bobie said:
I have been told that :

where L is √3/2 [itex]\hbar[/itex]
If there is an L, it means you are considering orbital angular momentum, which is not what you are supposed to do here.

The idea is to find the equivalent uniform B field such that the two spin orientations of a free electron differ in energy exactly the same as the fine structure. Take the field to be aligned along +z. The energy of the electron is given by
##
\hat{H} = - \mu \cdot \mathbf{B} = 2 \mu_\mathrm{e} B M_\mathrm{s}
##
such that
##
\Delta E = -2 \mu_\mathrm{e} B
##
 
  • #14
DrClaude said:
The idea is to find the equivalent uniform B field such that the two spin orientations of a free electron differ in energy exactly the same as the fine structure.
In the other thread, dauto (in the post I quoted) corrected me when I considered the value of Le on the z-axis, which I supposed the direction perpendicular to the plane of the orbit,
the point here, is to find a justification, if not a derivation of B in the classical model, the way yhey did at hyperphysics. Do you know if it is possible to ask them?
If B = 0.4 then [itex]\mu[/itex] must be 1.8

I hope you could help understand the role of the spin angular momentum Le:
- how do we establish that it exists? is there an experiment in which it is possible to separate it from the magnetic moment of the spin [itex]\mu[/itex], isn't it possible that all shifts are caused by magnetic momentum?
- the angular momentum of the orbit is greater in upper levels Lo (n*[itex]\hbar[/itex]) ,can you tell me if the angular or magnetic momenta have always the same value [itex]1.0016*\hbar[/itex]? Also the magnetic moment is intrinsic?
 
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  • #15
bobie said:
- the wavelength of transition 3s => 2p is given as 656.11 or (with reduced mass) 656.47 in the text, but in the picture it becomes 656.3, why that?
It took me a while to figure this one out! The value of 656.3 nm is what you get when you take the spectrum of hydrogen in air. The value of 656.47 nm is the wavelength in vacuum, and hence the one you get when starting from the energy levels of H and the Rydberg formula.

bobie said:
- the real values of fine structure are then 656.316 and 656.284?
When taking the spectrum in air.

bobie said:
- B field is indicated (at 2p) 0.4 T while in the third frame it becomes 0.3 T, which is right?
Neither! As I explained previously, the value of 0.4 T is what you obtain when you take the actual value of the fine structure splitting and try to figure out what field you you need such that a free electron would have such an energy difference between its parallel and anti-parallel states. The value of 0.3 T is what you get with the simple classical model to explain the origin of the fine structure. As mfb said, the actual magnetic field is not uniform.
 

1. What is the fine structure of hydrogen?

The fine structure of hydrogen refers to the splitting of the spectral lines in the hydrogen atom due to the interaction between the electron's spin and orbital angular momentum. This results in a more complex energy level structure and finer lines in the atomic spectrum.

2. Why is the fine structure of hydrogen important?

The fine structure of hydrogen provides important information about the fundamental properties of the atom, such as the electron's spin and angular momentum. It also plays a crucial role in understanding the behavior of other atoms and molecules.

3. How is the fine structure of hydrogen calculated?

The fine structure of hydrogen is calculated using the relativistic Dirac equation, which takes into account the effects of relativity on the electron's motion. This equation predicts the energy levels and spectral lines of hydrogen with great accuracy.

4. What is the significance of the fine structure constant?

The fine structure constant, also known as the Sommerfeld constant, is a dimensionless number that describes the strength of the interaction between the electron's spin and orbital angular momentum. It has a value of approximately 1/137 and is a fundamental constant of nature.

5. How does the fine structure of hydrogen relate to quantum mechanics?

The fine structure of hydrogen is a consequence of quantum mechanics, which describes the behavior of particles at the atomic and subatomic level. The theory of quantum mechanics is essential for understanding the fine structure of atoms and the nature of matter in general.

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