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Homework Problems in Quantum Mechanics and Vibrations, Assignments of Physics

A set of homework problems for a university-level course in physics. The problems cover topics in quantum mechanics, including the schrödinger equation and boundary conditions, as well as vibrations and differential equations. Students are asked to use separation of variables, find solutions to ordinary differential equations, and determine allowed energies. They are also asked to analyze a damped, driven simple harmonic oscillator and find the condition for resonance. Additionally, they are asked to write down finite difference approximations for various derivatives.

Typology: Assignments

2009/2010

Uploaded on 02/25/2010

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Download Homework Problems in Quantum Mechanics and Vibrations and more Assignments Physics in PDF only on Docsity! Homework 1 PHZ 5156 Due Thursday, August 31 1. Consider a particle of mass m trapped in a two-dimensional box with infinitely high walls at x = 0, x = a, y = 0, and y = b. Inside the box, the potential is zero and the Hamiltonian is given by Ĥ = −~ 2∇2 2m = − ~ 2 2m ( ∂2 ∂x2 + ∂2 ∂y2 ) (1) The infinitely high potential walls that trap the particle result in the boundary conditions for the wave function ψ(x = 0, y) = 0, ψ(x = a, y) = 0, ψ(x, y = 0) = 0, and ψ(x, y = b) = 0. a) Use the method of separation of variables to write the time-independent Schrodinger equation Ĥψ(x, y) = Eψ(x, y) (2) as two ordinary differential equations. b) Determine the solutions to the two equations obtained in part a). c) What are the allowed energies E? 2. The torsion of a bar is described by the fourth-order equation, d4θ dx4 + τθ = 0 (3) Show how this can be expressed as a system of coupled first-order differential equa- tions. 3. Consider the equation of a damped, driven simple harmonic oscillator, m d2y dt2 + γ dy dt + ky = Fcos(ωt) (4) a) Find the particular solution y(t) to this equation. Write your answer in the form y(t) = |A|cos(ωt + δ), and determine expressions for |A| and the phase angle δ. To keep your work simple, use the definition for the natural frequency of the oscillator ω0 = √ k m . 1
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