Schaum's Outline of Quantum Mechanics 8.11

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SUMMARY

The discussion centers on calculating the probability of an electron in a hydrogen atom being within the Bohr radius when in the state n = 2, l = 0. The user applied the wave function equation (8.8) and the radial function (8.33) to derive a probability of 0.0343, contrasting with the book's answer of 0.176. The user expressed skepticism regarding the average radius of 6 Bohr radii, given the calculated probability. The integral was also solved numerically, confirming the 0.0343 result, leading to a discussion on potential errors in approach rather than calculation.

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  • Understanding of quantum mechanics, specifically hydrogen atom wave functions
  • Familiarity with spherical coordinates and integration techniques
  • Knowledge of the Bohr model and its parameters, including the Bohr radius
  • Experience with numerical integration methods
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Students and professionals in physics, particularly those focusing on quantum mechanics and atomic structure, as well as educators seeking to clarify concepts related to electron probability distributions in hydrogen atoms.

Jimmy Snyder
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Homework Statement


If a hydrogen atom is in the state n = 2, l = 0, what is the probability that an electron has a value of r that is smaller than the Bohr radius.

Homework Equations


eqn (8.8)
\psi_{200}(r, \theta, \phi) = R_{20}Y_0^0(\theta, \phi)

Page 305
Y_0^0(\theta, \phi) = \frac{1}{\sqrt{4\pi}}

eqn (8.33)
R_{20} = 2(2a_0)^{-3/2}(1 - \frac{r}{2a_0})e^{-r/2a_0}

The Attempt at a Solution


P = \int_0^{2\pi}d\phi \int_0^{\pi}d\theta\int_0^{a_0}dr r^2|\psi(r, \theta, \phi)|^2sin(\theta)
= \int_0^{2\pi}d\phi \int_0^{\pi}d\theta sin(\theta) (Y_0^0(\theta, \phi))^2 \int_0^{a_0}dr r^2 4(2a_0)^{-3}(1 - \frac{r}{2a_0})^2e^{-r/a_0}
Now let z = r/a_0; dr = a_0dz then
P = \frac{4\pi}{4\pi}\frac{4}{(2a_0)^3}\int_0^1 a_0dz a_0^2z^2(1 - \frac{z}{2})^2e^{-z}
= \frac{1}{2}\int_0^1 dz (z^2 - z^3 + \frac{z^4}{4})e^{-z}
= (-1 -z -\frac{z^2}{2} - \frac{z^4}{8})e^{-z}|_0^1
= 1 - \frac{21}{8e} = 0.0343

The book gives the answer .176

I calculated that the probability of r being less than 4 times the Bohr radius is .176

Placing n = 2, l = 0 in equation 8.42 gives that the mean value for r is 6 times the Bohr radius. I find it hard to believe that the electron could spend nearly 18% of the time at less than 1 Bohr radius and yet average out to 6 Bohr radii.
 
Last edited:
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It's + z^4/4 inside the bracket under the integral sign. And are you sure about the integrations ?
 
dextercioby said:
It's + z^4/4 inside the bracket under the integral sign. And are you sure about the integrations ?
Thank you. I fixed that. I am as sure about them as I can be, but if I were 100% sure, I wouldn't have posted. By the way, I also solved the integral numerically using a calculator and got the same 0.0343 result. I believe that if I am wrong, it is because I am using the wrong approach, not because of an error in calculation.
 

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