A Quantum Mechanical Model for the Vibration and Rotation of Molecules. Rigid Rotor

Similar documents
Lecture 5: Harmonic oscillator, Morse Oscillator, 1D Rigid Rotor

Chemistry 795T. NC State University. Lecture 4. Vibrational and Rotational Spectroscopy

Indicate if the statement is True (T) or False (F) by circling the letter (1 pt each):

Physical Chemistry I Fall 2016 Second Hour Exam (100 points) Name:

Rotational spectroscopy., 2017 Uwe Burghaus, Fargo, ND, USA

A few principles of classical and quantum mechanics

THE RIGID ROTOR. mrmr= + m K = I. r 2 2. I = m 1. m + m K = Diatomic molecule. m 1 r 1. r 2 m 2. I moment of inertia. (center of mass) COM K.E.

The one and three-dimensional particle in a box are prototypes of bound systems. As we

Angular Momentum. Classically the orbital angular momentum with respect to a fixed origin is. L = r p. = yp z. L x. zp y L y. = zp x. xpz L z.

An Aside: Application of Rotational Motion. Vibrational-Rotational Spectroscopy

Quantum Mechanics: The Hydrogen Atom

Intro/Review of Quantum

Intro/Review of Quantum

Fun With Carbon Monoxide. p. 1/2

ONE AND MANY ELECTRON ATOMS Chapter 15

Angular momentum. Quantum mechanics. Orbital angular momentum

Physics 228 Today: Ch 41: 1-3: 3D quantum mechanics, hydrogen atom

Sample Quantum Chemistry Exam 2 Solutions

CHAPTER 8 The Quantum Theory of Motion

Introduction to Vibrational Spectroscopy

eigenvalues eigenfunctions

Atkins & de Paula: Atkins Physical Chemistry 9e Checklist of key ideas. Chapter 8: Quantum Theory: Techniques and Applications

Principles of Molecular Spectroscopy

Diatomic Molecules. 7th May Hydrogen Molecule: Born-Oppenheimer Approximation

Atoms 2012 update -- start with single electron: H-atom

Quantum mechanics (QM) deals with systems on atomic scale level, whose behaviours cannot be described by classical mechanics.

obtained in Chapter 14 to this case requires that the E1 approximation

Modern Physics. Unit 6: Hydrogen Atom - Radiation Lecture 6.3: Vector Model of Angular Momentum

Lecture 4 Quantum mechanics in more than one-dimension

IV. Electronic Spectroscopy, Angular Momentum, and Magnetic Resonance

5.61 Lecture #17 Rigid Rotor I

More On Carbon Monoxide

We now turn to our first quantum mechanical problems that represent real, as

CHEM 301: Homework assignment #5

Molecular spectroscopy Multispectral imaging (FAFF 020, FYST29) fall 2017

Section 5 Time Dependent Processes

Lecture 10. Central potential

PHYS 3313 Section 001 Lecture # 22

CHAPTER 13 LECTURE NOTES

Chemistry 431. NC State University. Lecture 17. Vibrational Spectroscopy

Exercises 16.3a, 16.5a, 16.13a, 16.14a, 16.21a, 16.25a.

Vibrational spectroscopy., 2017 Uwe Burghaus, Fargo, ND, USA

Lecture 4 Quantum mechanics in more than one-dimension

(2 pts) a. What is the time-dependent Schrödinger Equation for a one-dimensional particle in the potential, V (x)?

Rotations and vibrations of polyatomic molecules

Welcome back to PHY 3305

Determining the Normal Modes of Vibration

Lecture 4: Polyatomic Spectra

Advanced Spectroscopy. Dr. P. Hunt Rm 167 (Chemistry) web-site:

Vibrational states of molecules. Diatomic molecules Polyatomic molecules

Final Exam Tuesday, May 8, 2012 Starting at 8:30 a.m., Hoyt Hall Duration: 2h 30m

One-electron Atom. (in spherical coordinates), where Y lm. are spherical harmonics, we arrive at the following Schrödinger equation:

Molecular energy levels and spectroscopy

Lecture #21: Hydrogen Atom II

CHEM-UA 127: Advanced General Chemistry I

The Hydrogen Atom. Dr. Sabry El-Taher 1. e 4. U U r

From quantum to classical statistical mechanics. Polyatomic ideal gas.

Math 3435 Homework Set 11 Solutions 10 Points. x= 1,, is in the disk of radius 1 centered at origin

CHM 671. Homework set # 6. 2) Do problems 3.4, 3.7, 3.10, 3.14, 3.15 and 3.16 in the book.

Reading: Mathchapters F and G, MQ - Ch. 7-8, Lecture notes on hydrogen atom.

CHEM6416 Theory of Molecular Spectroscopy 2013Jan Spectroscopy frequency dependence of the interaction of light with matter

Physical Chemistry - Problem Drill 15: Vibrational and Rotational Spectroscopy

H atom solution. 1 Introduction 2. 2 Coordinate system 2. 3 Variable separation 4

Chem 442 Review of Spectroscopy

Molecular orbitals, potential energy surfaces and symmetry

Chem 442 Review for Exam 2. Exact separation of the Hamiltonian of a hydrogenic atom into center-of-mass (3D) and relative (3D) components.

Model for vibrational motion of a diatomic molecule. To solve the Schrödinger Eq. for molecules, make the Born- Oppenheimer Approximation:

13, Applications of molecular symmetry and group theory

Vibrational and Rotational Analysis of Hydrogen Halides

Nuclear models: Collective Nuclear Models (part 2)

Atoms 2010 update -- start with single electron: H-atom

1.6. Quantum mechanical description of the hydrogen atom

Time part of the equation can be separated by substituting independent equation

Advanced Physical Chemistry Chemistry 5350 ROTATIONAL AND VIBRATIONAL SPECTROSCOPY

Chimica Inorganica 3

Harmonic Oscillator Eigenvalues and Eigenfunctions

Summary: angular momentum derivation

Vibrational Spectra (IR and Raman) update Tinoco has very little, p.576, Engel Ch. 18, House Ch. 6

Total Angular Momentum for Hydrogen

Quantum Theory of Angular Momentum and Atomic Structure

Molecular Physics. Attraction between the ions causes the chemical bond.

Chemistry 532 Practice Final Exam Fall 2012 Solutions

( ) electron gives S = 1/2 and L = l 1

Non-stationary States and Electric Dipole Transitions

Spin Dynamics Basic Theory Operators. Richard Green SBD Research Group Department of Chemistry

Physical Chemistry II Exam 2 Solutions

Legendre Polynomials and Angular Momentum

Physical Chemistry II (Chapter 4 1) Rigid Rotor Models and Angular Momentum Eigenstates

Chapter 5.3: Series solution near an ordinary point

(3.1) Module 1 : Atomic Structure Lecture 3 : Angular Momentum. Objectives In this Lecture you will learn the following

CHEM 301: Homework assignment #12

THEORY OF MOLECULE. A molecule consists of two or more atoms with certain distances between them

Vibrations and Rotations of Diatomic Molecules

Quantum Mechanics & Atomic Structure (Chapter 11)

The Hydrogen Atom. Chapter 18. P. J. Grandinetti. Nov 6, Chem P. J. Grandinetti (Chem. 4300) The Hydrogen Atom Nov 6, / 41

Quantum Theory. Thornton and Rex, Ch. 6

Collection of formulae Quantum mechanics. Basic Formulas Division of Material Science Hans Weber. Operators

20 The Hydrogen Atom. Ze2 r R (20.1) H( r, R) = h2 2m 2 r h2 2M 2 R

/2Mα 2 α + V n (R)] χ (R) = E υ χ υ (R)

Transcription:

A Quantum Mechanical Model for the Vibration and Rotation of Molecules Harmonic Oscillator Rigid Rotor

Degrees of Freedom Translation: quantum mechanical model is particle in box or free particle. A molecule has 3 translational degrees of freedom. Vibration: quantum mechanical model is harmonic oscillator. A molecule has 3n 6 (3n 5 for linear) vibrational modes. Rotation: quantum mechanical model is rigid id rotor. A molecule has 3 ( for linear) principal axes of rotation.

Degrees of Freedom vibration, rotation, and translation Ignoring coupling: basic motions are independent of each other Hˆ = Hˆ + Hˆ + Hˆ trans vib rot ψ = ψ ψ ψ trans vib rot E = E + E + E trans vib rot

Classical Vibration Classical harmonic oscillator Center of mass and reduced mass defined by x CM mx 1 1 + mx mm 1 =, μ = m + m m + m 1 1

QM Harmonic Oscillator Harmonic potential not bad approximation for low energies

QM Harmonic Oscillator Schrödinger equation ( ) d ψ n x kx + ψ = μ dx Solutions: ψ ( x ) E ψ ( x ) n n n 14 1 α 1 α x n( x) = Hn( α x) e, n = 0,1,,3... n n! π ( ) 1 where α = kμ/ and Hn α x is the Hermite polynomial 1 E n = hν n+ 1 k where ν = π μ

QM Harmonic Oscillator f i f i f Wave functions are even functions for n = 0,, 4 ; odd functions for n = 1, 3, 5

QM Harmonic Oscillator Oscillations similar to particle in a box Equally spaced energy levels Δ E = hν Zero point energy E 0 = 1 hν Finite valued wave function in forbidden regions

Example The infrared absorption spectrum of 1 H 35 Cl has its strongest band at 8.65 10 13 Hz. (1) calculate the force constant () calculate the zero-point vibrational energy (3) what happens to the force constant if we deuterate the molecule? (4) What happens to the strongest absorption band in IR spectrum if we deuterate the molecule?

Vibrational Modes Vibrational modes of CO and H O

Degrees of Freedom vibration, rotation, and translation Ignoring coupling: basic motions are independent of each other Hˆ = Hˆ + Hˆ + Hˆ trans vib rot ψ = ψ ψ ψ trans vib rot E = E + E + E trans vib rot

Rigid Rotor Rigid rotor model: A system of two atoms (m 1 and m ) and a fixed bond length r 0 rotating around their center of mass is reduced d to a single reduced d mass rotating on the surface of a sphere of radius r 0 μ = mm 1 m + m 1 ( H p ) x py pz r= r0 V( x, y, z ) = 0 ˆ 1 = ˆ + ˆ + ˆ = + + μ μ x y z y r = r 0

Rigid Rotor Spherical coordinates r = x + y + z x = rsinθcos φ y = rsinθ sinφ z = rcosθ SPHERICAL COORDINATES Hˆ 1 1 = sinθ r μr + + sinθ θ θ sin θ φ r r

Rigid Rotor Schrödinger equation in spherical coordinates 1 Y ( θφ, ) 1 Y ( θφ, ) sin θ + EY, = μr0 sinθ θ θ sin θ φ ( θ φ )

Rigid Rotor ( θ ) ( Φ ( φ )) 1 d dθ 1 d sinθ sinθ + βsin ( θ) = Θ( θ) dθ dθ Φ( φ) dφ ( Φ ( φ )) ( θ ) 1 d dθ sinθ sinθ + βsin ( θ) = ml Θ( θ) dθ dθ 1 Φ ( φ) d dφ = m l

Rigid Rotor Solution spherical harmonic function l + 1 ( l m l )!)! i Yl ( θ, φ) = Pl ( cosθ) e 4 π ( l+ m )! m m im φ l l l l m l P l is a Legendre polynomial ( 1 ) ( ) 0 ( ) ( 1 ) m = l, l 1, l,...,0,..., l, l 1, l l

Rigid Rotor Solution spherical harmonic function ml ( θφ ) = EY ( θφ ) ˆ ml HY,, l l E = l( l+ 1, ) for l = 0,1,,3... I I = μ r 0 is the moment of inertia

Rigid Rotor l determines frequency (energy) of rotation m l determines orientation of rotational axis Energy is quantized and is given by El = l ( l + 1 ), for l = 01 0,1,,3... I The degeneracy of each energy level is l + 1 m l = -l.+l

Rigid Rotor Angular momentum operators lˆ lˆ lˆ x y z l=r p i x y z x y z lˆ x = i y z = i sinφ cotθcosφ z θ y φ lˆ y = i z x = i cosφ cotθsinφ x z θ φ lˆz = i x y = i y x φ l ˆ = l ˆ + l ˆ + l ˆ x y z

Rigid Rotor Spherical harmonic functions are eigenfunctions i of ˆ l and lˆ z ˆ ml l, 1 l, ml ( θφ) = ( + ) ( θφ) ly l l Y ˆ ˆ l, H = 0 and E = l I ˆ ml ly,, ml ( θφ) = m Y ( θφ) z l l l lˆ, 0 and ˆ, ˆ z H l l = = 0 ˆ 0 and z 0

Rigid Rotor Spherical harmonic functions complex except for m l = 0 Chemistry conventions

Rigid Rotor Chemistry conventions l = 0,1,,3, 4 s, p, d, f, g orbital quantum number m l is the angular momentum quantum number s p, p, p x y z d, d, d, d, d z xz yz xy x y f 3, f 3, f 3, f, f, f, f x y z xz ( y ) yz ( x ) zx ( y ) g, g, g, g, g,,,, z ( x y ) g g g xy( x y ) g + 4 3 3 3 3 4 4 z z x z y z xy zx zy x y xyz

Rigid Rotor p functions

Rigid Rotor d functions

Example 0 At what values of θ does Y ( θφ, ) = π ( cos θ 1 ) have 16 maxima? 5 1

Example The rotational energy levels l of molecules l are studied d by microwave spectroscopy. If the frequency of the absorption peak that corresponds to transition of l = 0 1is 3.65 10 1 Hz for HCl molecule. () (1) What is the bond length? () If we deuterate H without affecting the bond length, what will happen to the position of the absorption peak?