Homework Week 1. electronic excited state. electronic ground state

Size: px
Start display at page:

Download "Homework Week 1. electronic excited state. electronic ground state"

Transcription

1 Statistical Molecular Thermodynamics University of Minnesota Homework Week. The diagram below shows the energy of a diatomic molecule as a function of the separation between the atoms, R. A electronic excited state energy,v(r) B C electronic ground state D E R Which dashed line marks the defined zero, V (R) = 0, for the electronic energy of the diatomic? (a) A (b) B (c) C (d) D (e) E The zero of electronic energy for a diatomic molecule is taken to be that of the separated constituent atoms at infinite distance from one another. Thus, the correct answer is (C). t is not (E); this represents the minimum (not zero) value of the electronic energy. 2. f a hydrogen atom in the first excited state (n = 2) relaxes to the ground state (n = ) it will emit a photon to conserve energy. Which of the following is closest to the wavelength (λ) of the emitted photon?

2 (a) 75 nm (b) 22 nm (c) 225 nm (d) 500 nm (e) 667 nm (f) 000 nm ε = ε n=2 ε n= = ( cm ) ( 2 ) 2 2 ε = ( cm ) ( ) = ( cm ) ( ) 3 = cm Convert to wavelength: λ = ν = cm = cm ( ) 0 λ = nm cm = 22 nm cm 3. You have a diatomic molecule. You measure the bond dissociation energy and find that it is D 0 = 400 kj mol. You measure the vibrational frequency using R absorption and find that there is an absorption line at ν = 2000 cm. What is the electronic energy, D e, of the bond in this molecule? (a) kj mol (b) kj mol (c) kj mol (d) 42.0 kj mol (e) kj mol (f) kj mol Start with D e = D 0 + hν. Remember to convert the second term to kj/mol, 2 hν = N A hc ν: ( D e = J mol mol ) ( J s) ( cm s ) (2000 cm ) + 2 D e = J mol J mol D e = J mol = 42.0 kj mol 4. Convert ν = 000 cm to kj mol using the following values for standard constants: h = J s, c = m s, N A = mol.

3 (a) kj mol (b) kj mol (c) kj mol (d).96 kj mol (e).96 kj mol (f) 08.4 kj mol (g) 080 kj mol f Planck s constant is taken as h = J s, then E = hν (per molecule) and E = N A hν (per mole, where N A is Avogadro s number) and, ν = c ν, so E = N A hc ν = ( mol ) ( J s) ( cm s ) (0 3 cm ) = J mol =.96 kj mol 5. A ground-state hydrogen atom absorbs a photon of light that has a wavelength of 97.2 nm. t then gives off a photon that has a wavelength of 486 nm. What is the final state of the hydrogen atom (n =?). (a) (b) 2 (c) 3 (d) 4 (e) 2.3 (f) 8 (g) 5 For this problem start by making a diagram of the relevant energy levels, see figure. First we realize from the diagram that the energy difference between the initial (ground state) and the final state of our hydrogen atom is equal to the energy difference between the absorbed photon and the emitted photon, E final E ground = E photon absorbed E photon emitted To calculate the energy difference we will need to convert wavelength to an energy unit, and we can do this combining E = hν and c = νλ to give us E = h c λ, c E final E ground = h h λ ( absorbed = hc λ absorbed c λ emitted λ emitted ) = ( J s ) ( cm s ) ( cm cm = J

4 E intermediate Energy photon absorbed λ = 97.2 nm Eabsorbed Eemitted λ = 486 nm photon emitted Efinal Eground E final E ground n final =? n = Figure : Hydrogen atom energy levels for problem 3. Now that we know the energy difference between the ground state and the unknown final state, we can use the equation from question 2 to express the energy difference in terms of n. We know that n ground = for the ground state, which only leaves us to solve for n final, J n 2 final ( J ) ( E final E ground = J J = J n 2 final J n final = n 2 ground J J n 2 ground ) ( ) n 2 final = n 2 final n final = 2 = J = J = J J = 0.25 = 4 6. Given that ν = 2330 cm and D 0 = 7875 cm for N 2 (g), calculate the value of D e. Note that the value of ν is the position of an absorption peak in the R/Raman spectrum of N 2. This means that it is equal to the gap between quantized vibrational levels. (Hint: See the lecture slide titled Dissociation Energy) (a) cm (b) 8045 cm (c) cm (d) 7875 cm

5 (e) cm (f) cm The electronic energy, D e, is the sum of the bond dissociation energy, D 0, and the zero point vibrational energy, hν, 2 D e = D hν The only tricky issue is keeping the units all the same in energy. Since they were given in the same units it is trivial to calculate D e in wavenumbers. The only other thing to note is that we were given the position of the R/Raman absorption ( ν = 2330 cm ). Since this is the gap between two adjacent quantized vibrational levels, we know that it is equal to hν in energy. As a result, we need to multiply this energy by in the 2 last term, ( ) D e = 7875 cm cm = cm 2 This can, of course, be converted into other units, for example to get kj/mol, E = N A hν = N A hc ν D e = 956 kj mol 7. The energy difference between the J = 0 and J = rotational levels of carbon monoxide ( 2 C 6 O(g)) is ν = MHz. Calculate the energy difference between J = 0 and J = 2 and give the answer in cm. (a) cm (b) cm (c).54 cm (d) cm (e) cm (f) cm Here we start with the energy levels of the rigid rotor, E J = 2 J (J + ) 2 and consider the energy difference between two adjacent levels, J + and J, E J+ E J = 2 2 E J,J+ = 2 2 (J + ) ((J + ) + ) J (J + ) 2 = 2 [(J + ) (J + 2) J (J + )] 2 = 2 [ J 2 + 3J + 2 J 2 J ] 2 = 2 [2 (J + )] 2 (J + )

6 Now write the energy difference between J = 2 and J = 0 as the sum of the difference between J = 0 and J =, and J = and J = 2, E J=0,J=2 = E J=0,J= + E J=,J=2 = 2 = 3 2 (0 + ) + 2 ( + ) Compare this with just E J=0,J= (which was given in the problem), and you find that, E J=0,J= = 2 (0 + ) = 2 E J=0,J=2 = 3 E J=0,J= Using the given value for E J=0,J=, E J=0,J=2 = 3 ( MHz ) ( ) 0 6 Hz MHz Convert this to wavenumbers, = Hz ν = ν c = s cm s =.54 cm 8. Calculate the degeneracy of the first 4 rotational levels of carbon monoxide: (a) 0,,3,5 (b) 0,2,4,6 (c) (,),(3,3) (d),3,6,9 (e) 2,3,5,8 (f),3,5,7 (g) Cannot be determined, there are only three rotational levels possible. (h),2,3,4 The degeneracy is g J = 2J +, J g J = 2J + 0 g 0 = 2 (0) + = g = 2 () + = 3 2 g 2 = 2 (2) + = 5 3 g 3 = 2 (3) + = 7

7 9. Determine the number of various (translational, rotational, vibrational) degrees of freedom of N 2 : (a) 3,2, (b) 6,2, (c) 3,3,0 (d) 3,,2 (e) 5,3, (f) 6,, (g) 6,2,2 The total number of degrees of freedom must be 3 times the total number of atoms (3N), since each atom can move in 3D space. There are always 3 translational degrees of freedom (the whole molecule moving in 3D space). For rotations, the only question is whether the molecule is linear or nonlinear. For a linear molecule there are 2 rotations, and for a nonlinear molecule there are 3 rotations. The vibrations are whatever is left from the total (total minus translations minus rotations). Thus, for a linear molecule there are 3N 5 vibrations, and for a nonlinear molecule there are 3N 6 vibrations. Nitrogen, being diatomic, is perforce linear. molecule N total (3N) translations rotations vibrations N Determine the number of various (translation, rotation, vibration) degrees of freedom of C 2 H 6 : (a) 3,3,5 (b) 3,3,8 (c) 8,3,3 (d) 5,3,8 (e) 3,3,24 (f) 24,3,3 (g) 3,2,9 (h) 3,2,7 The total number of degrees of freedom must be 3 times the total number of atoms (3N), since each atom can move in 3D space. There are always 3 translational degrees of freedom (the whole molecule moving in 3D space). For rotations, the only question is whether the molecule is linear or nonlinear. For a linear molecule there are 2 rotations, and for a nonlinear molecule there are 3 rotations. The vibrations are whatever is left from the total (total minus translations minus rotations). Thus, for a linear molecule there are 3N 5 vibrations, and for a nonlinear molecule there are 3N 6 vibrations. Ethane (C 2 H 6 ) is non-linear.

8 molecule N total (3N) translations rotations vibrations C 2 H

Intro/Review of Quantum

Intro/Review of Quantum Intro/Review of Quantum QM-1 So you might be thinking I thought I could avoid Quantum Mechanics?!? Well we will focus on thermodynamics and kinetics, but we will consider this topic with reference to the

More information

Intro/Review of Quantum

Intro/Review of Quantum Intro/Review of Quantum QM-1 So you might be thinking I thought I could avoid Quantum Mechanics?!? Well we will focus on thermodynamics and kinetics, but we will consider this topic with reference to the

More information

Chemistry 213 Practical Spectroscopy

Chemistry 213 Practical Spectroscopy Chemistry 213 Practical Spectroscopy Dave Berg djberg@uvic.ca Elliott 314 A course in determining structure by spectroscopic methods Different types of spectroscopy afford different information about molecules

More information

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

THEORY OF MOLECULE. A molecule consists of two or more atoms with certain distances between them THEORY OF MOLECULE A molecule consists of two or more atoms with certain distances between them through interaction of outer electrons. Distances are determined by sum of all forces between the atoms.

More information

THE ATOMIC SPECTRUM OF HYDROGEN

THE ATOMIC SPECTRUM OF HYDROGEN THE ATOMIC SPECTRUM OF HYDROGEN When atoms are excited, either in an electric discharge or with heat, they tend to give off light. The light is emitted only at certain wavelengths that are characteristic

More information

AH Chemistry Unit 1. Electromagnetic Radiation and Atomic Spectra

AH Chemistry Unit 1. Electromagnetic Radiation and Atomic Spectra AH Chemistry Unit 1 Electromagnetic Radiation and Atomic Spectra Introduction This topic describes the Electromagnetic Spectrum and how it can interact with atoms, Spectroscopy. Much information about

More information

Lecture 10 Diatomic Vibration Spectra Harmonic Model

Lecture 10 Diatomic Vibration Spectra Harmonic Model Chemistry II: Introduction to Molecular Spectroscopy Prof. Mangala Sunder Department of Chemistry and Biochemistry Indian Institute of Technology, Madras Lecture 10 Diatomic Vibration Spectra Harmonic

More information

CHAPTER 13 LECTURE NOTES

CHAPTER 13 LECTURE NOTES CHAPTER 13 LECTURE NOTES Spectroscopy is concerned with the measurement of (a) the wavelengths (or frequencies) at which molecules absorb/emit energy, and (b) the amount of radiation absorbed at these

More information

Homework Due by 5PM September 20 (next class) Does everyone have a topic that has been approved by the faculty?

Homework Due by 5PM September 20 (next class) Does everyone have a topic that has been approved by the faculty? Howdy Folks. Homework Due by 5PM September 20 (next class) 5-Problems Every Week due 1 week later. Does everyone have a topic that has been approved by the faculty? Practice your presentation as I will

More information

( )( s 1

( )( s 1 Chemistry 362 Dr Jean M Standard Homework Problem Set 6 Solutions l Calculate the reduced mass in kg for the OH radical The reduced mass for OH is m O m H m O + m H To properly calculate the reduced mass

More information

Lesmahagow High School AHChemistry Inorganic and Physical Chemistry Lesmahagow High School CfE Advanced Higher Chemistry

Lesmahagow High School AHChemistry Inorganic and Physical Chemistry Lesmahagow High School CfE Advanced Higher Chemistry Lesmahagow High School CfE Advanced Higher Chemistry Unit 1 Inorganic and Physical Chemistry Electromagnetic Radiation and Atomic Spectra 1 Electromagnetic Radiation Radiation such as light, microwaves,

More information

SIMPLE QUANTUM SYSTEMS

SIMPLE QUANTUM SYSTEMS SIMPLE QUANTUM SYSTEMS Chapters 14, 18 "ceiiinosssttuu" (anagram in Latin which Hooke published in 1676 in his "Description of Helioscopes") and deciphered as "ut tensio sic vis" (elongation of any spring

More information

2. Infrared spectroscopy

2. Infrared spectroscopy 2. Infrared spectroscopy 2-1Theoretical principles An important tool of the organic chemist is Infrared Spectroscopy, or IR. IR spectra are acquired on a special instrument, called an IR spectrometer.

More information

Hint: unit of energy transferred is equal to: hν = hc

Hint: unit of energy transferred is equal to: hν = hc CH 0 Fall 08 Discussion # Chapter 8 Your name: TF s name Discussion Day/Time: Things you should know when you leave Discussion today: Atomic (matter) Emission and absorption of light. Energy Conservation

More information

WEEK 2: 4 SEP THRU 10 SEP; LECTURES 4-6

WEEK 2: 4 SEP THRU 10 SEP; LECTURES 4-6 Learning Objectives Energy: Light as energy Describe the wave nature of light, wavelength, and frequency using the equation c = λν What is meant by the particle nature of light? Calculate the energy of

More information

4 Diatomic molecules

4 Diatomic molecules s manual for Burrows et.al. Chemistry 3 Third edition 4 Diatomic molecules Answers to worked examples WE 4.1 The Lewis model (on p. 174 in Chemistry 3 ) Use the Lewis model to describe the bonding in (a)

More information

Infrared Spectroscopy

Infrared Spectroscopy Infrared Spectroscopy The Interaction of Light with Matter Electric fields apply forces to charges, according to F = qe In an electric field, a positive charge will experience a force, but a negative charge

More information

5.111 Lecture Summary #5 Friday, September 12, 2014

5.111 Lecture Summary #5 Friday, September 12, 2014 5.111 Lecture Summary #5 Friday, September 12, 2014 Readings for today: Section 1.3 Atomic Spectra, Section 1.7 up to equation 9b Wavefunctions and Energy Levels, Section 1.8 The Principle Quantum Number.

More information

CHEM 301: Homework assignment #12

CHEM 301: Homework assignment #12 CHEM 301: Homework assignment #12 Solutions 1. Let s practice converting between wavelengths, frequencies, and wavenumbers. (10%) Express a wavelength of 442 nm as a frequency and as a wavenumber. What

More information

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

Physical Chemistry I Fall 2016 Second Hour Exam (100 points) Name: Physical Chemistry I Fall 2016 Second Hour Exam (100 points) Name: (20 points) 1. Quantum calculations suggest that the molecule U 2 H 2 is planar and has symmetry D 2h. D 2h E C 2 (z) C 2 (y) C 2 (x)

More information

CHM Physical Chemistry II Chapter 12 - Supplementary Material. 1. Einstein A and B coefficients

CHM Physical Chemistry II Chapter 12 - Supplementary Material. 1. Einstein A and B coefficients CHM 3411 - Physical Chemistry II Chapter 12 - Supplementary Material 1. Einstein A and B coefficients Consider two singly degenerate states in an atom, molecule, or ion, with wavefunctions 1 (for the lower

More information

Homework 04 - Electromagnetic Radiation

Homework 04 - Electromagnetic Radiation HW04 - Electromagnetic Radiation This is a preview of the published version of the quiz Started: Jul 7 at 9:43am Quiz Instructions Homework 04 - Electromagnetic Radiation Question 1-7 What is the frequency

More information

where n = (an integer) =

where n = (an integer) = 5.111 Lecture Summary #5 Readings for today: Section 1.3 (1.6 in 3 rd ed) Atomic Spectra, Section 1.7 up to equation 9b (1.5 up to eq. 8b in 3 rd ed) Wavefunctions and Energy Levels, Section 1.8 (1.7 in

More information

Principles of Molecular Spectroscopy

Principles of Molecular Spectroscopy Principles of Molecular Spectroscopy What variables do we need to characterize a molecule? Nuclear and electronic configurations: What is the structure of the molecule? What are the bond lengths? How strong

More information

Chapter 7. Part I Dr. Stone Stan State

Chapter 7. Part I Dr. Stone Stan State Chapter 7 Part I Dr. Stone Stan State 1 2 Electromagnetic Radiation Perpendicular oscillating fields: Electric: PET scan: gamma rays X-rays Visible light Infrared (heat) Microwaves Magnetic MRI = magnetic

More information

Physical Chemistry - Problem Drill 15: Vibrational and Rotational Spectroscopy

Physical Chemistry - Problem Drill 15: Vibrational and Rotational Spectroscopy Physical Chemistry - Problem Drill 15: Vibrational and Rotational Spectroscopy No. 1 of 10 1. Internal vibration modes of a molecule containing N atoms is made up of the superposition of 3N-(5 or 6) simple

More information

10.40 Lectures 23 and 24 Computation of the properties of ideal gases

10.40 Lectures 23 and 24 Computation of the properties of ideal gases 1040 Lectures 3 and 4 Computation of the properties of ideal gases Bernhardt L rout October 16 003 (In preparation for Lectures 3 and 4 also read &M 1015-1017) Degrees of freedom Outline Computation of

More information

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

CHEM6416 Theory of Molecular Spectroscopy 2013Jan Spectroscopy frequency dependence of the interaction of light with matter CHEM6416 Theory of Molecular Spectroscopy 2013Jan22 1 1. Spectroscopy frequency dependence of the interaction of light with matter 1.1. Absorption (excitation), emission, diffraction, scattering, refraction

More information

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p Introduction to Spectroscopy (Chapter 6) Electromagnetic radiation (wave) description: Wavelength λ Velocity v Electric Field Strength 0 Amplitude A Time t or Distance x Period p Frequency ν time for 1

More information

Chemistry 795T. Lecture 7. Electromagnetic Spectrum Black body Radiation. NC State University

Chemistry 795T. Lecture 7. Electromagnetic Spectrum Black body Radiation. NC State University Chemistry 795T Lecture 7 Electromagnetic Spectrum Black body Radiation NC State University Black body Radiation An ideal emitter of radiation is called a black body. Observation: that peak of the energy

More information

Chemistry 795T. Black body Radiation. The wavelength and the frequency. The electromagnetic spectrum. Lecture 7

Chemistry 795T. Black body Radiation. The wavelength and the frequency. The electromagnetic spectrum. Lecture 7 Chemistry 795T Lecture 7 Electromagnetic Spectrum Black body Radiation NC State University Black body Radiation An ideal emitter of radiation is called a black body. Observation: that peak of the energy

More information

Chemistry 2. Assumed knowledge

Chemistry 2. Assumed knowledge Chemistry 2 Lecture 8 IR Spectroscopy of Polyatomic Molecles Assumed knowledge There are 3N 6 vibrations in a non linear molecule and 3N 5 vibrations in a linear molecule. Only modes that lead to a change

More information

Lecture 2: The basics: atoms, moles, energy & light

Lecture 2: The basics: atoms, moles, energy & light Lecture 2: The basics: atoms, moles, energy & light Read: BLB Chap. 2.3 2.4; 5.1 5.3; 6.1 HW: BLB 2:4,23,25,31; 5:3,25,28 Sup 2:1 3; 6:1,3,4,5 do NOT do Sup 6.2! Know: the mole atomic structure protons,

More information

CHEM N-3 November Explain why the electron on an H atom does not crash into the nucleus.

CHEM N-3 November Explain why the electron on an H atom does not crash into the nucleus. CHM0 03-N-3 November 03 xplain why the electron on an H atom does not crash into the nucleus. 3 The negatively charged electron is attracted to the positively charged nucleus. The electron behaves like

More information

Assignment: Read Atkins, Chapter 27 sections 7 and 8 or McQuarrie and Simon, Chapter 30 sections 7 and 10, before coming to lab on Monday

Assignment: Read Atkins, Chapter 27 sections 7 and 8 or McQuarrie and Simon, Chapter 30 sections 7 and 10, before coming to lab on Monday Classical Trajectory 1 Classical Trajectory Calculations H + H-F H-H + F Assignment: Read Atkins, Chapter 27 sections 7 and 8 or McQuarrie and Simon, Chapter 30 sections 7 and 10, before coming to lab

More information

Radiant energy is proportional to its frequency (cycles/s = Hz) as a wave (Amplitude is its height) Different types are classified by frequency or

Radiant energy is proportional to its frequency (cycles/s = Hz) as a wave (Amplitude is its height) Different types are classified by frequency or CHEM 241 UNIT 5: PART B INFRA-RED RED SPECTROSCOPY 1 Spectroscopy of the Electromagnetic Spectrum Radiant energy is proportional to its frequency (cycles/s = Hz) as a wave (Amplitude is its height) Different

More information

Lecture 6 - spectroscopy

Lecture 6 - spectroscopy Lecture 6 - spectroscopy 1 Light Electromagnetic radiation can be thought of as either a wave or as a particle (particle/wave duality). For scattering of light by particles, air, and surfaces, wave theory

More information

What is spectroscopy?

What is spectroscopy? Absorption Spectrum What is spectroscopy? Studying the properties of matter through its interaction with different frequency components of the electromagnetic spectrum. With light, you aren t looking directly

More information

- Why are phase labels required? Because phase changes either absorb or release energy. ... what does this mean?

- Why are phase labels required? Because phase changes either absorb or release energy. ... what does this mean? 155 SINCE the enthalpy change does NOT depend on path, this means that we can use standard values for enthalpy to predict the heat change in reactions that we have not tested in a calorimeter. THERMOCHEMICAL

More information

6.05 Computational Raman Spectroscopy

6.05 Computational Raman Spectroscopy 2nd/3rd year Physical Chemistry Practical Course, Oxford University 6.05 Computational Raman Spectroscopy (5 points) Raman spectra are obtained by irradiating a sample with very intense monochromatic radiation,

More information

Chapter 6. Quantum Theory and the Electronic Structure of Atoms Part 1

Chapter 6. Quantum Theory and the Electronic Structure of Atoms Part 1 Chapter 6 Quantum Theory and the Electronic Structure of Atoms Part 1 The nature of light Quantum theory Topics Bohr s theory of the hydrogen atom Wave properties of matter Quantum mechanics Quantum numbers

More information

CHEM1901/ J-5 June 2013

CHEM1901/ J-5 June 2013 CHEM1901/3 2013-J-5 June 2013 Oxygen exists in the troposphere as a diatomic molecule. 4 (a) Using arrows to indicate relative electron spin, fill the left-most valence orbital energy diagram for O 2,

More information

Lecture 2 nmr Spectroscopy

Lecture 2 nmr Spectroscopy Lecture 2 nmr Spectroscopy Pages 427 430 and Chapter 13 Molecular Spectroscopy Molecular spectroscopy: the study of the frequencies of electromagnetic radiation that are absorbed or emitted by substances

More information

Microscopic Treatment of the Equilibrium Constant. Lecture

Microscopic Treatment of the Equilibrium Constant. Lecture Microscopic Treatment of the Equilibrium Constant Lecture The chemical potential The chemical potential can be expressed in terms of the partition function: μ = RT ln Q j j N j To see this we first expand

More information

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

Exercises 16.3a, 16.5a, 16.13a, 16.14a, 16.21a, 16.25a. SPECTROSCOPY Readings in Atkins: Justification 13.1, Figure 16.1, Chapter 16: Sections 16.4 (diatomics only), 16.5 (omit a, b, d, e), 16.6, 16.9, 16.10, 16.11 (omit b), 16.14 (omit c). Exercises 16.3a,

More information

Lecture 8. Assumed knowledge

Lecture 8. Assumed knowledge Chemistry 2 Lecture 8 IR Spectroscopy of Polyatomic Molecles Assumed knowledge There are 3N 6 vibrations in a non linear molecule and 3N 5 vibrations in a linear molecule. Only modes that lead to a change

More information

Structure Determination. How to determine what compound that you have? One way to determine compound is to get an elemental analysis

Structure Determination. How to determine what compound that you have? One way to determine compound is to get an elemental analysis Structure Determination How to determine what compound that you have? ne way to determine compound is to get an elemental analysis -basically burn the compound to determine %C, %H, %, etc. from these percentages

More information

Properties of Light and Atomic Structure. Chapter 7. So Where are the Electrons? Electronic Structure of Atoms. The Wave Nature of Light!

Properties of Light and Atomic Structure. Chapter 7. So Where are the Electrons? Electronic Structure of Atoms. The Wave Nature of Light! Properties of Light and Atomic Structure Chapter 7 So Where are the Electrons? We know where the protons and neutrons are Nuclear structure of atoms (Chapter 2) The interaction of light and matter helps

More information

ChemWiki BioWiki GeoWiki StatWiki PhysWiki MathWiki SolarWiki

ChemWiki BioWiki GeoWiki StatWiki PhysWiki MathWiki SolarWiki Ashley Robison My Preferences Site Tools FAQ Sign Out If you like us, please share us on social media. The latest UCD Hyperlibrary newsletter is now complete, check it out. ChemWiki BioWiki GeoWiki StatWiki

More information

Lecture 4: Polyatomic Spectra

Lecture 4: Polyatomic Spectra Lecture 4: Polyatomic Spectra 1. From diatomic to polyatomic Ammonia molecule A-axis. Classification of polyatomic molecules 3. Rotational spectra of polyatomic molecules N 4. Vibrational bands, vibrational

More information

The relationship between these aspects is described by the following equation: E = hν =

The relationship between these aspects is described by the following equation: E = hν = 1 Learning Outcomes EXPERIMENT A10: LINE SPECTRUM Upon completion of this lab, the student will be able to: 1) Examine the line spectrum of the hydrogen atom. 2) Calculate the frequency and energy of the

More information

Physical Chemistry II Exam 2 Solutions

Physical Chemistry II Exam 2 Solutions Chemistry 362 Spring 2017 Dr Jean M Standard March 10, 2017 Name KEY Physical Chemistry II Exam 2 Solutions 1) (14 points) Use the potential energy and momentum operators for the harmonic oscillator to

More information

CHEM Atomic and Molecular Spectroscopy

CHEM Atomic and Molecular Spectroscopy CHEM 21112 Atomic and Molecular Spectroscopy References: 1. Fundamentals of Molecular Spectroscopy by C.N. Banwell 2. Physical Chemistry by P.W. Atkins Dr. Sujeewa De Silva Sub topics Light and matter

More information

Molecular energy levels and spectroscopy

Molecular energy levels and spectroscopy Molecular energy levels and spectroscopy 1. Translational energy levels The translational energy levels of a molecule are usually taken to be those of a particle in a three-dimensional box: n x E(n x,n

More information

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

Indicate if the statement is True (T) or False (F) by circling the letter (1 pt each): Indicate if the statement is (T) or False (F) by circling the letter (1 pt each): False 1. In order to ensure that all observables are real valued, the eigenfunctions for an operator must also be real

More information

Exam 2. Remember to refer to the Periodic Table handout that is separate from this exam copy.

Exam 2. Remember to refer to the Periodic Table handout that is separate from this exam copy. 001 version last name first name signature McCord CH301 unique: 49885 TTh 9:30 am - 11 am Exam 2 Oct 15, 2018 Monday 7:30-9:00 PM A - Mi in BUR 106 Mo - Z in JES A121A Remember to refer to the Periodic

More information

R BC. reaction coordinate or reaction progress R. 5) 8pts) (a) Which of the following molecules would give an infrared spectrum? HCl O 2 H 2 O CO 2

R BC. reaction coordinate or reaction progress R. 5) 8pts) (a) Which of the following molecules would give an infrared spectrum? HCl O 2 H 2 O CO 2 Physical Chemistry Spring 2006, Prof. Shattuck Final Name Part Ia. Answer 4 (four) of the first 5 (five) questions. If you answer more than 4, cross out the one you wish not to be graded. 1) 8pts) Of absorption

More information

ATMO/OPTI 656b Spring 2009

ATMO/OPTI 656b Spring 2009 Nomenclature and Definition of Radiation Quantities The various Radiation Quantities are defined in Table 2-1. Keeping them straight is difficult and the meanings may vary from textbook to textbook. I

More information

Workshop 4: Diatomic molecule vibrational and rotational spectra CH351 Physical Chemistry, Fall 2004

Workshop 4: Diatomic molecule vibrational and rotational spectra CH351 Physical Chemistry, Fall 2004 Workshop 4: Diatomic molecule vibrational and rotational spectra CH35 Physical Chemistry, Fall 004 http://quantum.bu.edu/courses/ch35/pltl/4.pdf Last updated Monday, November 9, 004 6:59:3-05:00 Copyright

More information

There are 6 parts to this exam. Parts 1-3 deal with material covered since the midterm exam. Part 4-6 cover all course material.

There are 6 parts to this exam. Parts 1-3 deal with material covered since the midterm exam. Part 4-6 cover all course material. Chemistry 453 March 9, 03 Enter answers in a lue ook Final Examination Key There are 6 parts to this exam. Parts -3 deal with material covered since the midterm exam. Part 4-6 cover all course material.

More information

QuickCheck. Collisions between molecules. Collisions between molecules

QuickCheck. Collisions between molecules. Collisions between molecules Collisions between molecules We model molecules as rigid spheres of radius r as shown at the right. The mean free path of a molecule is the average distance it travels between collisions. The average time

More information

I 2 Vapor Absorption Experiment and Determination of Bond Dissociation Energy.

I 2 Vapor Absorption Experiment and Determination of Bond Dissociation Energy. I 2 Vapor Absorption Experiment and Determination of Bond Dissociation Energy. What determines the UV-Vis (i.e., electronic transitions) band appearance? Usually described by HOMO LUMO electron jump LUMO

More information

Ch 7 Quantum Theory of the Atom (light and atomic structure)

Ch 7 Quantum Theory of the Atom (light and atomic structure) Ch 7 Quantum Theory of the Atom (light and atomic structure) Electromagnetic Radiation - Electromagnetic radiation consists of oscillations in electric and magnetic fields. The oscillations can be described

More information

Molecular spectroscopy

Molecular spectroscopy 10 Molecular spectroscopy Answers to worked examples W.E. 10.1 Using the Beer-Lambert law (on p. 462 in Chemistry 3 ) What concentration of the solution is required to absorb 35% of the light at the same

More information

Unit 1. Electronic Structure page 1

Unit 1. Electronic Structure page 1 Unit 1 Electronic Structure Section 1. Learning Outcomes Practice Questions Answers Electronic Structure Electromagnetic spectrum / calculations Electron configuration / Periodic Table Electronic Structure

More information

Organic Chemistry: CHEM2322

Organic Chemistry: CHEM2322 Etiquette & Course Overview Organic Chemistry: Structure Determination MS & IR Dr. Christopher J. O Brien 203 CRB, cobrien@uta.edu Classroom etiquette Arrive on time if you are late you must quietly take

More information

Introduction. The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants

Introduction. The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants Introduction The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants Spectroscopy and the Electromagnetic Spectrum Unlike mass spectrometry,

More information

I understand the relationship between energy and a quanta I understand the difference between an electron s ground state and an electron s excited

I understand the relationship between energy and a quanta I understand the difference between an electron s ground state and an electron s excited NCCS 1.1.2 & 1.1.3 I understand the relationship between energy and a quanta I understand the difference between an electron s ground state and an electron s excited state I will describe how an electron

More information

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

Quantum mechanics (QM) deals with systems on atomic scale level, whose behaviours cannot be described by classical mechanics. A 10-MINUTE RATHER QUICK INTRODUCTION TO QUANTUM MECHANICS 1. What is quantum mechanics (as opposed to classical mechanics)? Quantum mechanics (QM) deals with systems on atomic scale level, whose behaviours

More information

Collisions between molecules

Collisions between molecules Collisions between molecules We model molecules as rigid spheres of radius r as shown at the right. The mean free path of a molecule is the average distance it travels between collisions. The average time

More information

Chemistry Instrumental Analysis Lecture 2. Chem 4631

Chemistry Instrumental Analysis Lecture 2. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 2 Electromagnetic Radiation Can be described by means of a classical sinusoidal wave model. Oscillating electric and magnetic field. (Wave model) wavelength,

More information

(3 pts) 2. In which gas sample do the molecules have a lower average kinetic energy? (A) Gas A (B) Gas B (C) Neither

(3 pts) 2. In which gas sample do the molecules have a lower average kinetic energy? (A) Gas A (B) Gas B (C) Neither Consider two samples of gas, A and B, as shown in the figure below. Both containers are at the same temperature and pressure. Gas A 1.0 L 0.32 g Gas B 1.0 L 0.48 g (3 pts) 1. Which gas sample contains

More information

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency. Light We can use different terms to describe light: Color Wavelength Frequency Light is composed of electromagnetic waves that travel through some medium. The properties of the medium determine how light

More information

Atmospheric Sciences 321. Science of Climate. Lecture 6: Radiation Transfer

Atmospheric Sciences 321. Science of Climate. Lecture 6: Radiation Transfer Atmospheric Sciences 321 Science of Climate Lecture 6: Radiation Transfer Community Business Check the assignments Moving on to Chapter 3 of book HW #2 due next Wednesday Brief quiz at the end of class

More information

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

( ) electron gives S = 1/2 and L = l 1 Practice Modern Physics II, W018, Set 1 Question 1 Energy Level Diagram of Boron ion B + For neutral B, Z = 5 (A) Draw the fine-structure diagram of B + that includes all n = 3 states Label the states

More information

Chem 3502/4502 Physical Chemistry II (Quantum Mechanics) 3 Credits Spring Semester 2006 Christopher J. Cramer. Lecture 9, February 8, 2006

Chem 3502/4502 Physical Chemistry II (Quantum Mechanics) 3 Credits Spring Semester 2006 Christopher J. Cramer. Lecture 9, February 8, 2006 Chem 3502/4502 Physical Chemistry II (Quantum Mechanics) 3 Credits Spring Semester 2006 Christopher J. Cramer Lecture 9, February 8, 2006 The Harmonic Oscillator Consider a diatomic molecule. Such a molecule

More information

Chapter 6. Electronic Structure. Electronic Structure and the Periodic Table ( 전자구조와주기율표 ) 강의개요. 2) The Particle Nature of Light: Photon Energies

Chapter 6. Electronic Structure. Electronic Structure and the Periodic Table ( 전자구조와주기율표 ) 강의개요. 2) The Particle Nature of Light: Photon Energies Chapter 6 Electronic Structure and the Periodic Table ( 전자구조와주기율표 ) 강의개요 Electronic Structure Electron arrangement in atoms energy levels orbitals electron configurations orbital diagram Periodic Table

More information

Light and Matter: Reading Messages from the Cosmos Pearson Education, Inc.

Light and Matter: Reading Messages from the Cosmos Pearson Education, Inc. Light and Matter: Reading Messages from the Cosmos Light and Color Light is a form of energy (think of the warmth of sunlight or a lightbulb) White light is actually made up of many different colors. How

More information

A few principles of classical and quantum mechanics

A few principles of classical and quantum mechanics A few principles of classical and quantum mechanics The classical approach: In classical mechanics, we usually (but not exclusively) solve Newton s nd law of motion relating the acceleration a of the system

More information

Chem120a : Exam 3 (Chem Bio) Solutions

Chem120a : Exam 3 (Chem Bio) Solutions Chem10a : Exam 3 (Chem Bio) Solutions November 7, 006 Problem 1 This problem will basically involve us doing two Hückel calculations: one for the linear geometry, and one for the triangular geometry. We

More information

3. RATE LAW AND STOICHIOMETRY

3. RATE LAW AND STOICHIOMETRY Page 1 of 39 3. RATE LAW AND STOICHIOMETRY Professional Reference Shelf R3.2 Abbreviated Lecture Notes Full Lecture Notes I. Overview II. Introduction A. The Transition State B. Procedure to Calculate

More information

The Bohr Model of the Atom

The Bohr Model of the Atom Unit 4: The Bohr Model of the Atom Properties of light Before the 1900 s, light was thought to behave only as a wave. Light is a type of electromagnetic radiation - a form of energy that exhibits wave

More information

PHYS 172: Modern Mechanics Fall 2009

PHYS 172: Modern Mechanics Fall 2009 PHYS 172: Modern Mechanics Fall 2009 Lecture 14 Energy Quantization Read 7.1 7.9 Reading Question: Ch. 7, Secs 1-5 A simple model for the hydrogen atom treats the electron as a particle in circular orbit

More information

Vibrational and Rotational Analysis of Hydrogen Halides

Vibrational and Rotational Analysis of Hydrogen Halides Vibrational and Rotational Analysis of Hydrogen Halides Goals Quantitative assessments of HBr molecular characteristics such as bond length, bond energy, etc CHEM 164A Huma n eyes Near-Infrared Infrared

More information

KEY Chem 1A First Midterm Examination February 7, 2005 Professor David Chandler

KEY Chem 1A First Midterm Examination February 7, 2005 Professor David Chandler KEY Chem 1A First Midterm Examination February 7, 2005 Professor David Chandler 1 2 3 4 5 6 7 8 9 10 Extra Name: Signature: Section: GSI: Instructions As indicated, either fill in blank space with appropriate

More information

Probing Bonding Using Infrared Spectroscopy Chem

Probing Bonding Using Infrared Spectroscopy Chem Probing Bonding Using Infrared Spectroscopy Chem 112-2011 INTRODUCTION First, watch the short video on how to record an infrared spectrum using an infrared spectrometer, linked at: http://employees.oneonta.edu/viningwj/chem112/labs/ir_video/ir_video_controller.swf

More information

24 Introduction to Spectrochemical Methods

24 Introduction to Spectrochemical Methods 24 Introduction to Spectrochemical Methods Spectroscopic method: based on measurement of the electromagnetic radiation produced or absorbed by analytes. electromagnetic radiation: include γ-ray, X-ray,

More information

Chem 115 POGIL Worksheet - Week 8 - Answers Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra. ΔH o = 285.

Chem 115 POGIL Worksheet - Week 8 - Answers Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra. ΔH o = 285. Chem 115 POGIL Worksheet - Week 8 - Answers Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra Key Questions & Exercises 1. Calculate ΔH o for the reaction, Given: C 2 H 2 (g) + H

More information

So far in talking about thermodynamics, we ve mostly limited ourselves to

So far in talking about thermodynamics, we ve mostly limited ourselves to 251 Lecture 33 So far in talking about thermodynamics, we ve mostly limited ourselves to discussions of thermochemistry, a quantification of the heat absorbed or given off as the result of a chemical reaction.

More information

Today: general condition for threshold operation physics of atomic, vibrational, rotational gain media intro to the Lorentz model

Today: general condition for threshold operation physics of atomic, vibrational, rotational gain media intro to the Lorentz model Today: general condition for threshold operation physics of atomic, vibrational, rotational gain media intro to the Lorentz model Laser operation Simplified energy conversion processes in a laser medium:

More information

Chapter 7 QUANTUM THEORY & ATOMIC STRUCTURE Brooks/Cole - Thomson

Chapter 7 QUANTUM THEORY & ATOMIC STRUCTURE Brooks/Cole - Thomson Chapter 7 QUANTUM THEORY & ATOMIC STRUCTURE 1 7.1 The Nature of Light 2 Most subatomic particles behave as PARTICLES and obey the physics of waves. Light is a type of electromagnetic radiation Light consists

More information

Phys 172 Modern Mechanics Summer 2010

Phys 172 Modern Mechanics Summer 2010 Phys 172 Modern Mechanics Summer 2010 r r Δ p = F Δt sys net Δ E = W + Q sys sys net surr r r Δ L = τ Δt Lecture 14 Energy Quantization Read:Ch 8 Reading Quiz 1 An electron volt (ev) is a measure of: A)

More information

CHAPTER 5. The Structure of Atoms

CHAPTER 5. The Structure of Atoms CHAPTER 5 The Structure of Atoms Chapter Outline Subatomic Particles Fundamental Particles The Discovery of Electrons Canal Rays and Protons Rutherford and the Nuclear Atom Atomic Number Neutrons Mass

More information

ATMOS 5140 Lecture 11 Chapter 9

ATMOS 5140 Lecture 11 Chapter 9 ATMS 5140 Lecture 11 hapter 9 Absorption by Atmospheric Gases Rotational Vibrational Applications Basis for Molecular Absorption/Emission hanges in the translational kinetic energy of molecules (i.e. temperature)

More information

Chemistry 1411 Practice Exam 2, Chapters 5-8 Brown

Chemistry 1411 Practice Exam 2, Chapters 5-8 Brown Chemistry 1411 Practice Exam 2, Chapters 5-8 Brown Some constants and equations: E = q + w q = C p T Heat = m T Cs h = 6.626 X 10 34 J. s c = 2.998 X 10 8 m/s R H = 2.18 X 10 18 J E = (2.18 X 10 18 J)(1/n

More information

General Considerations 1

General Considerations 1 General Considerations 1 Absorption or emission of electromagnetic radiation results in a permanent energy transfer from the emitting object or to the absorbing medium. This permanent energy transfer can

More information

Physics 4C Chapter 19: The Kinetic Theory of Gases

Physics 4C Chapter 19: The Kinetic Theory of Gases Physics 4C Chapter 19: The Kinetic Theory of Gases Whether you think you can or think you can t, you re usually right. Henry Ford The only thing in life that is achieved without effort is failure. Source

More information

Goals for Today. Clarify some Rydberg Concepts Absorption vs. emission

Goals for Today. Clarify some Rydberg Concepts Absorption vs. emission Note: Due to recent changes the exam 2 material for these slides ends at Ionization Energy Exceptions. You can omit Lewis Structures through General Formal Charge Rules. CH301 Unit 2 QUANTUM NUMBERS AND

More information

Symmetric Stretch: allows molecule to move through space

Symmetric Stretch: allows molecule to move through space BACKGROUND INFORMATION Infrared Spectroscopy Before introducing the subject of IR spectroscopy, we must first review some aspects of the electromagnetic spectrum. The electromagnetic spectrum is composed

More information

Magnetic Resonance Spectroscopy EPR and NMR

Magnetic Resonance Spectroscopy EPR and NMR Magnetic Resonance Spectroscopy EPR and NMR A brief review of the relevant bits of quantum mechanics 1. Electrons have spin, - rotation of the charge about its axis generates a magnetic field at each electron.

More information