Viability of particle in a box modeling

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SUMMARY

The particle in a box model is widely applicable in various physical scenarios, including calculating degeneracy pressure in neutron stars through Fermi energy derived from a 3D particle in a box. This model's relevance stems from the Pauli exclusion principle, which constrains particle position and momentum, allowing for the interpretation of potential energy curves as "boxes." The model serves as an ideal theoretical framework for illustrating complex quantum mechanics concepts that are often overlooked in educational materials.

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  • Potential energy curves in quantum systems
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I've noticed that the example of a particle in a box is heavily used even for physical situations where there is no obvious box: for example when finding the degeneracy pressure in a neutron star one calculates the fermi-energy from a 3D-particle in a box.

So I wondered: is there any good reason why the particle in a box-model holds for a large variety of situations?

Does this has to do with the pauli-exclusion principle? I.e. that the position is constrained by ##\delta x \delta_p = \hbar /2## and we can think of these boxes as ##\delta x## wide?
 
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The "box" in the particle-in-a-box calculation is not necessarily a literal one with solid barriers. The "box" is the shape of the potential energy curve that confines the particle. It's a reasonable approximation for any potential that is small over some finite range before sharply increasing.
 
The particle in a (rigid wall) box is a perfect theoretical example for the mathematical subleties of quantum mechanics, usually swept under the carpet when textbooks are written and students are taught.
 

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