Particle of mass m in a box of length L Quantum Mechanics

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SUMMARY

The discussion focuses on a particle of mass m confined in a one-dimensional box of length L, applying quantum mechanics principles, specifically the Schrödinger equation. It is established that outside the box, the potential is zero, leading to the conclusion that the energy eigenstates are solutions to the Schrödinger equation. The expectation value is calculated using the normalized wave function, confirming that the denominator is 1. The key takeaway is that measuring the energy collapses the particle's state into an eigenstate of the Hamiltonian.

PREREQUISITES
  • Understanding of the Schrödinger equation in quantum mechanics
  • Familiarity with quantum states and eigenstates
  • Knowledge of normalization of wave functions
  • Basic concepts of potential energy in quantum systems
NEXT STEPS
  • Study the solutions to the one-dimensional infinite potential well problem
  • Learn about the implications of wave function normalization in quantum mechanics
  • Explore the concept of energy eigenstates and their physical significance
  • Investigate the role of measurements in quantum mechanics and state collapse
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Students and professionals in physics, particularly those studying quantum mechanics, as well as educators looking for insights into teaching concepts related to quantum states and the Schrödinger equation.

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1. http://img10.imageshack.us/img10/8602/232cw.jpg /b][/URL]

Homework Equations


http://img199.imageshack.us/img199/484/232ag.jpg

sorry about the insert pictures, i don't know how to type up the eqns easily

The Attempt at a Solution


Now I know that outside the box the Schrödinger equation should give 0 right. I'm just not sure how to go about (a) and (b). (c) The expectation value is pretty straightforward in that you just evalutate <psi|omega|psi>/<psi|psi> with the boundaries from 0 to L and we know the denominator here is 1 since it's normalized.
 
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I think for part(a) .. you have to solve the schroedinger`s equation to obtain the energy and you know that the potential inside the box is zero , so go from there ..
 
One fundamental postulate of QM is that if you make an observation, then you collapse the state of the particle into an eigenstate of the observable. Eigenstates of the Hamiltonian (the energy observable) are exactly the solutions to the Schroedinger equation. From this information, can you see what are the possibilities when you measure the energy of the system?
 

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