Particle in 1D Box: What Happens When Wall Removed?

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Discussion Overview

The discussion revolves around the behavior of a particle in a one-dimensional box with infinitely high walls when one of the walls is suddenly removed. It explores the implications for the wavefunction and energy measurements in this altered potential configuration.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant describes the initial conditions of a particle in a 1D box and questions the outcome of removing a wall.
  • Another participant suggests that there may be insufficient information to address the question adequately.
  • A third participant reiterates the initial scenario and outlines the procedure for determining the new energy eigenfunctions and eigenvalues after the wall removal, emphasizing the need to solve the eigenvalue equation in the new configuration.
  • This participant also mentions the calculation of probabilities for measurement outcomes based on the new wavefunction.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as there are differing views on the sufficiency of the information provided and the implications of the wall removal on the wavefunction and energy measurements.

Contextual Notes

Some assumptions regarding the initial state of the particle and the nature of the measurement process may be missing or not fully articulated, which could affect the discussion.

jayanth
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A particle is moving in a 1D box with infinitely high walls. The potential is zero inside and infinite outside. What will happen if one of the walls is suddenly removed??
 
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Is this coursework?
 
Seems like insufficient information.
 
jayanth said:
A particle is moving in a 1D box with infinitely high walls. The potential is zero inside and infinite outside. What will happen if one of the walls is suddenly removed??

First you must know the wavefunction for the infinite well. At the instant the wall is removed you still have the same wavefunction. Assuming you intend to measure the energy in the new configuration, you follow the usual procedure: determine the new energy eigenfunctions and new energy eigenvalues, i.e. solve the eigenvalue equation in the new configuration, and then write the wavefunction in terms of the new eigenfunctions. You now know the possible results of a measurement (the eigenvalues) and the probability of obtaining each result is \left| {\left\langle {{E_k }}<br /> \mathrel{\left | {\vphantom {{E_k } \psi }}<br /> \right. \kern-\nulldelimiterspace}<br /> {\psi } \right\rangle } \right|^2, where \varphi (x) = \left\langle {x}<br /> \mathrel{\left | {\vphantom {x {E_k }}}<br /> \right. \kern-\nulldelimiterspace}<br /> {{E_k }} \right\rangle are the energy eigenfunctions.

Best wishes
 

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