Hydrogen atom (finding electron probability)

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Homework Help Overview

The discussion revolves around finding the electron probability in a hydrogen atom, specifically focusing on the eigenstate and the probability of locating the electron within certain angular and radial limits. The context includes expectation values related to the hydrogen atom's wavefunctions.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to determine the eigenstate of the hydrogen atom based on given expectation values and seeks to calculate the probability of finding the electron in a specified region. Participants discuss methods for integrating the probability expression and explore simplifications based on the relationship between the first minimum of the radial wavefunction and the Bohr radius.

Discussion Status

Participants are actively engaging with the problem, offering various approaches to the integration required for calculating the probability. There is a focus on approximations and the relationship between parameters, with some participants suggesting different methods for handling the integral.

Contextual Notes

There is a question regarding the determination of the first minimum of the radial wavefunction, denoted as rm, and its relationship to the Bohr radius. Some participants express uncertainty about the assumptions related to the size of rm compared to the Bohr radius.

natugnaro
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[SOLVED] Hydrogen atom (finding electron probability)

Homework Statement


For electron in eigensate of Hydrogen we have these expectation values

<r>= 6a , <r^-1>= 1/4a

(a is Bohr radius)

a) find that eigenstate.
b) find the probability of finding electron in region 0 < phi < Pi/6 , 0 < theta < Pi/8
and 0 < r < rm
where rm is the first minimum of radial wavefunction in which electron is.



Homework Equations





The Attempt at a Solution



a) Using <nl|r^-1|nl>=1/((n^2)*a) it follows that n=2

then using <nl|r|nl>=1/2*[3*n^2-l(l+1)]a I got l=0 ,
so the eigenstate must be Psi(200).

b) To find the probability, I have to integrate

[tex]P=\int|\psi_{200}|^{2}r^{2}Sin\theta drd\phi d\theta = \frac{1-Cos(\frac{\pi}{8})}{(2a)^{3}6}\int^{r_{m}}_{0}(1-\frac{r}{2a})^{2}e^{\frac{-r}{a}}r^{2}dr[/tex]

I can do the integral using tables, but can this integral be simplified. I only have to integrate from 0 to rm so if rm is much less than Bohr radius a, I can make an approximation (series expansion of e^x).
I'm not shure is rm<<a ? , also how are rm and a (Bohr radius) related ?
 
Last edited:
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How do you determine "r_{m}" ? From what equation ?
 
[tex]\frac{\partial}{\partial r}(R_{20}(r))=0 \Rightarrow \frac{e^{-r/2a}(-4a+r)}{4\sqrt{2}a^{7/2}}=0 \Rightarrow r_{m}=4a[/tex]

So, rm is four times smaller than a.
Well, I think this is ok, since I'm just trynig to avoid some integral, not build something that suppose to work :smile: .
 
You can also expand the [tex](1-\frac{r}{2a})^{2}[/tex] term, multiply with [tex]r^2[/tex] and integrate by parts. Quite painful, but exact!
 
PhysiSmo said:
You can also expand the [tex](1-\frac{r}{2a})^{2}[/tex] term, multiply with [tex]r^2[/tex] and integrate by parts. Quite painful, but exact!

and multiply by e^(-r/a), then I have integral of r^4*e^(-r/a)
 
I'll just use [tex]e^{\frac{-r}{a}} \approx 1-\frac{r}{a}[/tex]. [tex]r_{m}[/tex] is small enough for me.
thanks.
 
I meant that you could integrate by parts the integral

[tex]\int_0^{r_m} r^4e^{-r/a}dr=r^4\frac{e^{-r/a}}{-1/a}\left|_0^{r_m}-\int_0^{r_m} 4r^3e^{-r/a}\left(-\frac{1}{a}\right)dr=\cdots[/tex]

and so on...
 
Last edited by a moderator:
ah, yes , tahnks again.
 

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