Estimating Diameter of Hydrogen Atom from Lyman Alpha Radiation

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The discussion revolves around estimating the diameter of a hydrogen atom using Lyman alpha radiation, specifically focusing on the transition from n=2 to n=1 with a wavelength of 1216 angstroms. Participants explore the relationship between the energy levels of an infinite potential well and the emitted radiation, ultimately concluding that the length of the well can approximate the atom's diameter. The correct approach involves using the electron mass rather than the proton mass in calculations, leading to a final estimate of the atom's diameter around 3.325x10^-10 meters. The conversation highlights the importance of proper unit handling and understanding the physics behind the potential well model. This method provides a valuable approximation for the hydrogen atom's size in relation to established constants like the Bohr radius.
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Homework Statement


The Lyman alpha radiation for hydrogen (nf=2, ni=1) has a wavelength of 1216 angstroms. Using the simplified model of an infinite 1D potential well, derive an estimate of the diameter of the hydrogen atom. How does this value compare with twice the Bohr radius 2r=1.06anstroms?


Homework Equations


I imagine maybe De Broglie's relation, or the energy of a potential well.


The Attempt at a Solution


I have no idea how I can relate a potential well to the radiation given off by hydrogen. I realize that I'm supposed to work this out myself, but my exam is tomorrow morning and would appreciate if I could get the solution, or at least a hefty hint.
 
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Hi ultimateguy, you know the energy levels of an infinite well, right? What frequency of light would be emitted if an electron made a transition from n=2 to n=1 in an infinite well of size L?
 
The energy levels for an infinite well are E_{n}=\frac{n^2h^2}{8mL^2} and the frequency is \omega=\frac{E}{\hbar}.

EDIT: Is the length of the potential well the same as the diameter of the atom?
 
Last edited:
ultimateguy said:
The energy levels for an infinite well are E_{n}=\frac{n^2h^2}{8mL^2} and the frequency is \omega=\frac{E}{\hbar}.

EDIT: Is the length of the potential well the same as the diameter of the atom?

First, the frequency for n=2 to n=1 is \omega = (E_2 - E_1)/\hbar, not just E.

Second, they clearly want you to approximate the atom with the potential well, so what do you think will correspond to the atom diameter?
 
I think that the length of the well approximates the atom. For E_1 the wavelength \lambda=2L and for E_2 that \lambda=L. Although this is the wavelength of the wavefunction and not the photon.
 
Last edited:
If the length of the well approximates the diameter of the atom then you should figure out what the length of the well is.
 
I tried doing that already. I had E_2-E_1=\frac{3h^2}{8mL^2}. I then substituted into \omega=\frac{E_2-E_1}{\hbar} to get \omega=\frac{3h\pi}{4mL^2} and solving for L I get L=\sqrt{\frac{3h\lambda}{4m}}. I got 7.77x10^-21m using this.
 
You did your algebra wrong. For one thing you forget a factor of c, the speed of light.
 
Don't know where c comes in.
 
  • #10
What are the units of frequency? How did you relate angular frequency to wavelength? What are the units of wavelength? Notice anything? Your current expression does not have the right units, so there is no way you could get some number of meters from it.
 
  • #11
\omega=\frac{2c\pi}{\lambda}. Damn it I'm an idiot.
 
  • #12
My equation for length is L=\sqrt{\frac{3h\lambda}{8mc}}. If I use the proton mass for m I get 7.76x10^-12m. This isn't right, is it?
 
  • #13
Nope. Why are you using the proton mass?
 
  • #14
I figured it was a hydrogen atom, has one proton. Now I see that it is an electron mass I need to use, and I get 3.325x10^-10m. I guess the electron mass is used because that is what's in a potential well. That must be right :P.
 

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