Understanding Electron Motion in the Thomson Model of the Atom: Where to Begin?

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SUMMARY

The discussion focuses on the Thomson model of the atom, specifically analyzing the motion of an electron within a uniformly charged sphere. The electric field intensity is defined as Qr/4πεR^3 for r < R, leading to the conclusion that the electron undergoes simple harmonic motion about the center. The derived formula for the frequency of oscillation is essential for comparing the electron's oscillation frequency in the hydrogen atom with the spectral lines of hydrogen. The initial approach involves using Newton's second law, F = ma, and solving the resulting differential equation.

PREREQUISITES
  • Understanding of electric fields and forces in electrostatics
  • Familiarity with differential equations and their solutions
  • Knowledge of simple harmonic motion principles
  • Basic concepts of atomic structure and the Thomson model
NEXT STEPS
  • Study the derivation of simple harmonic motion equations in physics
  • Learn about the implications of the Thomson model in atomic theory
  • Explore the mathematical techniques for solving differential equations
  • Investigate the relationship between electron frequencies and spectral lines in hydrogen
USEFUL FOR

Students of physics, educators teaching atomic theory, and researchers interested in the foundational models of atomic structure will benefit from this discussion.

CollectiveRocker
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Can someone please give me a nudge in the right direction on how to solve this problem? The electric field intensity at a distance r from the center of a uniformly charged sphere of radius R and total charge Q is Qr/4πεR^3, when r < R. Such a sphere corresponds to the Thomson model of the atom. Show that an electron in this sphere executes simple harmonic motion about its center and derive a formula for the frequency of motion. Evaluate the frequency of the electron oscillations for the case of the hydrogen atom and compare it with the frequencies of the spectral lines of hydrogen. How do i even start?
 
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You start with "F= ma". F, the force on an electron with charge e, is -Qer/(4πεR^3) so ma= m (d2r/dt2= -(Qe/(4πεR3)) Can you solve that differential equation? (Note that Qe/(4πεR3[/sup) is a constant.)
 
HallsofIvy said:
You start with "F= ma". F, the force on an electron with charge e, is -Qer/(4πεR^3) so ma= m (d2r/dt2= -(Qe/(4πεR3)) Can you solve that differential equation? (Note that Qe/(4πεR3[/sup) is a constant.)


I think you may have missed a factor of "r" in your differential equation. This is the crucial piece that makes it have a sinusoidal solution.

Zz.
 

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