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Hydrogen atom two-body problem

July 5, 2017
by
MIT OpenCourseWare
YouTube video player
Hydrogen atom two-body problem

TL;DR

The Schrodinger equation and canonical variables are used to analyze the behavior of particles in a hydrogen atom, allowing for the separation of center of mass and relative motion.

Transcript

BARTON ZWIEBACH: Hydrogen atom is the beginning of our analysis. It still won't solve differential equations, but we will now two particles, a proton, whose coordinates are going to be coordinate of the proton, subbing Xp for the proton, and momentum of the proton. And there's an electron. And there's the coordinates, the three coordinates of the e... Read More

Key Insights

  • 🫀 Canonical variables, such as coordinates and momenta, are essential in studying quantum systems like the hydrogen atom.
  • 💆 The Schrodinger equation can be separated into terms representing center of mass and relative motion, simplifying the analysis.
  • 👋 The wave function for the system depends on the coordinates of both particles, but can be normalized by integrating over the proton coordinates.

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Questions & Answers

Q: What are the canonical variables used to analyze the hydrogen atom?

The canonical variables used are the coordinates and momenta of the electron and proton, denoted by Xp, Xe, Pp, and Pe.

Q: How is the wave function for the system normalized?

The wave function is normalized by integrating it squared over the proton coordinates, ensuring that the total probability is equal to 1.

Q: How is the Schrodinger equation for the hydrogen atom simplified?

The Schrodinger equation is separated into a term representing the center of mass motion and a term representing the relative motion, making the analysis more manageable.

Q: Why are canonical variables important in analyzing the hydrogen atom?

Canonical variables allow for the proper commutation relations and help in separating the system into distinct parts, making the analysis easier to handle.

Summary & Key Takeaways

  • The hydrogen atom is analyzed using the Schrodinger equation and canonical variables, which represent the coordinates and momenta of the electron and proton.

  • The wave function for the system depends on the coordinates of both particles, but can be normalized by integrating over the proton coordinates.

  • The Schrodinger equation for the system can be separated into a center of mass motion term and a relative motion term, simplifying the analysis.


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