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

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SUMMARY

When one wall of a 1D box with infinitely high walls is suddenly removed, the wavefunction of the particle remains unchanged at the instant of removal. To analyze the new configuration, one must determine the new energy eigenfunctions and eigenvalues by solving the eigenvalue equation specific to the altered system. The probability of measuring each energy result is calculated using the formula \(\left| {\left\langle {{E_k }} \mathrel{\left | {\vphantom {{E_k } \psi }} \right. \kern-\nulldelimiterspace} {\psi } \right\rangle } \right|^2\), where \(\varphi (x) = \left\langle {x} \mathrel{\left | {\vphantom {x {E_k }}} \right. \kern-\nulldelimiterspace} {{E_k }} \right\rangle\) represents the energy eigenfunctions.

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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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