


Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
A chemistry homework assignment from a university-level course, focusing on topics such as time-dependent wave functions for a free particle, probability concepts, operator practice, and the commutator identity. The assignment also includes problems related to simple harmonic motion, molecular conjugated systems, and non-stationary states for a particle in a box. Students are expected to solve problems using the provided textbook and may need to use tools like maple to animate plots.
Typology: Assignments
1 / 4
This page cannot be seen from the preview
Don't miss anything!



Homework 2. Due Monday Oct 10 at 5pm in Prof. Ginger’s mailbox. Page 1/ CIRCLE YOUR ANSWERS AND KEY RESULTS STAPLE YOUR PAPERS TOGETHER
Levine 2.17 – time dependent wave function for a free particle 2.29 – probability concept review 3.5 – basic operator practice 3.15 – commutator identity 3.42 – operator concept review – provide counter-examples for false cases!
Additional Problems: 1) Why is simple harmonic motion so common in classical mechanics? We solved the ODE for the simple harmonic oscillator (mass on a spring) in class last week, we will solve the quantum version next week. In the meantime, why do you think so many classical systems exhibit simple harmonic motion? We derived the equation of motion based on a Hooke’s law restoring force (i.e. F=-k*x), however, we can also see this results from any harmonic potential.
a) Since F = −∇⋅ V for any conservative force, what kind of potential function leads to a Hooke’s law like restoring force and resulting simple harmonic motion? b) Take any arbitrary potential that we will call U(x). Write out the Taylor expansion for U(x) about a local minimum x 0. c) Thus, from b) what kind of motion can be expected for sufficiently small displacements from the local potential minimum? What do we mean by “sufficiently small displacements”?
2) Do Levine problem 2.15 for a longer molecule and compare with the butadiene result from Levine 2.15 (you don’t need to work the butadiene problem if you are familiar with it):
a) γ-Carotene, one of the precursors of vitamin A, is a conjugated system containing 11- double bonds (you will need to calculate the total bond length). Calculate the wavelength of light needed to excite the HOMO-LUMO transition of the pi electrons for carotene using the simple free electron model. Compare the calculated value with the observed transition at 460 nm.
b) Explain why the ‘free electron model’ gives an error for butadiene? Hint: do electrons attract or repel one another?
3) Nonstationary states for a particle in a box Consider a particle in an infinite square well of width L. Initially, (at t =0) the system is described by a wavefunction that is equal parts a superposition of the ground and first excited states. In other words, the time zero wavefunction is: Ψ( x , 0 )= C [ ψ (^) 1 ( x )+ ψ 2 ( x )]
a) Find C so that the wavefunction is normalized.
b) Write the time-dependent wave function Ψ ( x , t )for any later time t
c) Show that this superposition is not a stationary state (i.e. show that |ψ |^2 evolves in time). Then use Maple to animate a plot of |ψ |^2 as a function of t
d) If many systems are prepared in this state and their energies are measured, what will the result be? Discuss both the average of these measurements, and discuss the statistics of the specific results of a series of individual measurements.
e) Find as a function of t for this superposition state 4) Particle in the FINITE box: (read the handout first) As promised, move from the idealized INFINITE walled box, to the FINITE walled box. Consider a box of width a , centered at the origin. Instead of rising to infinity outside the box, the potential is now V 0. a) Given a=1.0 nm, and V 0 =1.2x10-18^ J Determine the lowest 5 energy levels for an electron placed into this box. What is the wavelength of the electron in each of these 5 states. Compare this electron wavelength with the wavelengths of an electron placed in the lowest 5 energy levels of an infinite box of the same width. b) Repeat the calculation for a box of width 0.9 nm and depth 5x10-19^ J. For these parameters will there be fewer or more bound states than for those in part a? How many allowed energy levels are there and what are their energies? 5) Free-particle wave packets: The wave-functions for the free particle with well-defined momentum (momentum operator eigenfunctions) tell us nothing about the position of the particle. We would like to construct wave-functions for a free particle which also contain some position information. We know we can create new wavefunctions from a linear superposition of any set eigenfunctions, we use momentum eigenfunctions as our basis below. We consider a “free” electron that has kinetic energy of roughly ~ 100 eV traveling in towards the right. a) Write down the wave function, and Plot Re(ψ ) and |ψ |^2 over the range x=-5 to + Angstroms for an electron with KE=100 eV traveling to the right. e) Use the Fourier Transform relationships given in part c to compute the distribution of wavevectors k needed to create this wavefunction. Plot G(k) for k=-10E10 to 10E reciprocal meters (1/10 angstroms to 1/10 Angstroms). f) Repeat d and e for a width sigma of 0.25 Angstroms. Compare the result with that in d and e. Interpret this result in the context of your understanding of the postulates and of Heisenberg’s uncertainty principle. g) Though they exist, we haven’t yet introduced a position eigenfunction. What do you think are the properties of a “position eigenfunction”? Do you know of any functions with such properties?