SUMMARY
The average value of \( x^2 \) in a one-dimensional quantum well is calculated using the formula \( (x^2)_{av} = L^2 \left( \frac{1}{3} - \frac{1}{2n^2 \pi^2} \right) \). The wave function for the one-dimensional well is given by \( \psi_n(x) = \sqrt{\frac{2}{L}} \sin\left(\frac{n \pi x}{L}\right) \). To evaluate the integral \( x^2_{av} = \frac{2}{L} \int_0^L \sin^2\left(\frac{n \pi x}{L}\right) x^2 dx \), integration by parts is recommended, and utilizing double angle identities simplifies the process.
PREREQUISITES
- Understanding of quantum mechanics principles, specifically one-dimensional potential wells.
- Familiarity with wave functions and their properties.
- Knowledge of integration techniques, particularly integration by parts.
- Ability to apply trigonometric identities, such as double angle formulas.
NEXT STEPS
- Study integration by parts in the context of quantum mechanics problems.
- Learn about the application of double angle identities in integrals.
- Explore tables of integrals relevant to quantum mechanics.
- Investigate the implications of average values in quantum systems.
USEFUL FOR
Students of quantum mechanics, particularly those studying one-dimensional potential wells, as well as educators seeking to enhance their teaching of integration techniques in physics.