Electron Inside the Nucleus on Helium Atoms Problem

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SUMMARY

The discussion centers on the theoretical analysis of an electron confined within a helium nucleus, specifically addressing the kinetic energy of the electron compared to the attractive potential energy at the nucleus's surface. The calculations utilize the kinetic energy formula K=p²/2m and the momentum derived from the wavelength λ, which is determined to be 4R. The potential energy is calculated using Coulomb's law, leading to the conclusion that the kinetic energy (K) exceeds the potential energy (U), confirming the impossibility of an electron residing within the nucleus due to the uncertainty principle.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave-particle duality.
  • Familiarity with the kinetic energy formula K=p²/2m and momentum calculations.
  • Knowledge of Coulomb's law for calculating potential energy in electrostatic interactions.
  • Basic grasp of the uncertainty principle in quantum mechanics.
NEXT STEPS
  • Explore the implications of the uncertainty principle on particle confinement in quantum mechanics.
  • Study the relativistic energy-momentum relationship E²=(pc)²+(mc²)² for high-energy particles.
  • Investigate the role of standing waves in quantum systems and their applications in atomic models.
  • Learn about the properties of helium atoms and their electron configurations in quantum chemistry.
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Students and researchers in quantum mechanics, physicists analyzing atomic structures, and educators teaching advanced concepts in atomic theory and wave mechanics.

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Homework Statement



Quantum mechanics makes the electrons-in-the-nucleus theory untenable (for example on helium nucleus where before they know that a neutron exist, they thought that it was composed of four protons and 2 electrons). A confined electron is a standing wave, whose wavelength in the nucleus could be no longer than approx. 4R (R=radius of nucleus).

By analogy, the "fundamental" standing wave on a string has a wavelength satisfying L=1/2(lambda). In the case of the nucleus the "length of the string" is 2R.

Assuming a nuclear charge of 2e and a typical nuclear radius of R=5E-15. Show that the kinetic energy of an electron standing wave confined in the nucleus would be much greater then the magnitude of the attractive potential energy when the electron is at the surface of the nucleus?

And also I am confused about this, why at the surface of the nucleus? can the electron be found somewhere inside? and Is the electron moving fast or slow so I'm not sure if i have to consider relativistic effects.

Homework Equations



well here are the formulas I used (I don't know if they are correct)

For the kinetic energy of the electron
K=p^2/2m (p=momentum, m=mass)

to find the momentum I used

p=h/(lambda) (h=plank's, lamda=wavelength)

and to find lamda I used the given

1/2 lamda = 2 R thus, lamda=4R


To find the potential) i used (coulumb's law?)

U= 1/[4(pi)Eo] * (q1q2)/R

where q1=+2e (charge of the nucleus), q2=-e(charge of electron) and R=Radius of nucleus
(should i consider the contribution by the other electron, Helium has two electron right?)

The Attempt at a Solution



Well, I did the math and I indeed got K>U, kinetic energy is higher. But I'm not sure if my approach is correct ^^;

thanks ^^
 
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I think that the electron cannot be found in the nucleus, because the uncertainty principle will require a momentum uncertainty so high, so inside the nucleus it's worse. So i think you have to calculate the uncertainty in momentum of electron in nucleus surface, and use the relativistic energy E^2=(pc)^2+(mc^2)^2, to show aproximatelly that uncertainty in energy is so high compared with potencial energy.
 

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