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

Size: px
Start display at page:

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

Transcription

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 in spectroscopic notation(b) Using the selection rules of equation 88 draw all the allowed transitions of B + Such diagrams are called Grotian diagrams The ground state B + has three electrons, electronic configuration is 1s s 1 As shown in class, only the electron in the unfilled subshell s 1 contributes to the angular momentum of the atom We show in class that S = s 1 = 1/,L = l 1 = 0, J = L+ S = S = 1/, with term symbol S 1/ The first excited states electronic configuration is 1s p 1 There is a single electron in the unfilledp 1 ( l 1 = 1) subshell So S = 1/ and L = 1 The possible values of J = L+1/,L 1/ gives two states J = 3/,1/ The states are: 1) S = 1/,L = 1, J = 1/giving P 1/ ; ) S = 1/,L = 1, J = 3/giving P 3/ The next excited state electronic configuration is 1s 3s 1 It should be clear that that S = s 1 = 1/,L = l 1 = 0, J = L+ S = S = 1/, with term symbol 3 S 1/ The next excited states electronic configuration is 1s 3p 1 The 3p 1 electron gives S = 1/and L = 1 The possible values of J = L+1/,L 1/ gives two states J = 3/,1/ The states are: 1) S = 1/,L = 1, J = 1/giving3 P 1/ ; ) S = 1/,L = 1, J = 3/giving3 P 3/ The final excited states for the n = 3 shell has electronic configuration is 1s 3d 1 The ( ) electron gives S = 1/ and L = l 1 = The possible values of 3d 1 l 1 = J = L+1/,L 1/ gives J = 5/,3/ The states are: 1) S =1/, L =, J = 3/ giving 3 D 3/ ; ) S = 1/,L =, J = 5/giving3 D 5/ The schematic energy diagram is below: Just like the p states, Hund s rule 3 suggests has lower energy than Using Hund s rule 3, since the p (3p) subshell is less than half filled P 1/ ( 3 P 1/ ) has lower energy than P 3/ ( 3 P 1/ ) s 1 S 1/ In the diagram, a thick line indicates a state of B +, with the term symbol, n L J, on the right of the line The electronic configurations are on the left of the lines The

2 double-arrow lines that connect two states indicate allowed transitions that obey the transition rules of equation 88 Question Atomic Physics (Fine Structure and Zeeman Effects) Excited states of atoms, fine-structure, and Zeeman effects The ground-state configuration of SODIUM (Z = 11) is1s s p 6 3s 1, in term symbol is 3 S 1/ A) Write is the first excited state electronic configuration of Sodium Find the spectroscopic notation (term symbol) of the two states associated with this excited state Hint: find all the total orbital Angular Momentum (L) and total spin (S), and all the possible total angular momentum (J) Also see equation sheet for energy order!! The electronic configuration of the first excited state is1s s p 6 3p 1 For this configuration, only the 3p 1 electron contribute to the angular momentum, and hence S = 1 /, L = 1 The total angular momentum is J = L + S, L S There are two states: i) J = L + S = 3 / with S = 1 / and L = 1 The term symbol is 3 P 3/ ii) J = L S = 1 / with S = 1 / and L = 1 The term symbol is 3 P 1/ B) Write the second excited state electronic configuration of SODIUM Find the spectroscopic notation (term symbol) of the one state associated with this excited state Briefly explain why there is only one state Look at the energy order list in back! The electronic configuration of the second excited state is1s s p 6 4s 1 For this configuration, only the 4s 1 electron contribute to the angular momentum, and hence S = 1 /, L = 0 There is only value of total angular momentum is J = S = 1 / For J = 1 /, S = 1 / and L = 0 The term symbol is 4 S 1/ C) The first excited state of LITHIUM (Z = 3) has electronic configuration 1s p 1, and is split into two states (doublet) P 1/ and P 3/ It is estimated that the internal magnetic field for this state is B int = 036T Find the fine-structure energy difference between the P 1/ and P 3/ states Fine-structure splitting is ΔV fs B int = ev / T ( ) 036T ( ) = ev D) Suppose the LITHIUM atom is placed in an external magnetic field of magnitude B = 05T How many energy levels do the P 3/ have? Draw a schematic diagram to illustrate these energy levels Find the energy spacing between adjacent energy levels HINT: This is the Zeeman Effects! Lande factor is relevant! The Zeeman energy of these levels are given by V z B ext g For P 3/, J = 3 / and = 3, 1, 1, 3 giving four distinct energy levels

3 E P 3/ = 1 / The energy separation between adjacent levels (for example m j = 3 / and m j = 1 /, or m j = 0 and m j = 1 / ) is simply, ΔV z B ext gδm j B ext g, where Δm j = 1 for adjacent levels For P 3/ state J = 3, L = 1, and S = ½ ( ) + 05( 05 +1) 1 ( 1+1 ) ( )( 15 +1) g = = 133 For B ext = 050T, we use µ B = ev / T and g = 133 to obtain for the energy difference between adjacent Zeeman P 3/ levels, ΔV z gb ext = ev / T 05T = 3 / ( )( 133) = ev = 1 / = 3 / Question 3 Molecular Spectroscopy: It is known that the hydrogen molecule H has a vibration absorption (emission) frequency of ν 0 = Hz A) Model the H molecule as two H atoms connected by a spring Based on the data given calculate the spring constant k Use mh = 1u Reduced mass µ = m m H H = 1 m H + m H m = H kg ω = k µ ν = 1 π k µ k = 4π ν µ = 4π ( s 1 ) ( kg) = 573 N m B) Now consider a deuterium molecule D, where D is a heavy hydrogen with nucleus of one proton and one neutron with a mass md = amu Use the data of part A to calculate the vibration frequency of this molecule µ = m Dm D m D + m D = 1 m D = kg ν = 1 π k µ = 1 π 573N / m kg = Hz C) Are H and D infrared active? Briefly explain your answer No Only vibration modes that induce a change in the dipole moment of the molecule are infrared active Since homonuclear diatomic molecules such as H and D do not even have dipole moments, they cannot be infrared active

4 Question 4 Vibrational Energy Level of oxygen molecule O A) Assume that the O molecule behaves like a harmonic oscillator with a force constant of 10 N/m Find the energy (in ev) of its ground (n = 0) and first excited (n = 1) vibrational states For 16 O, m O = 16 u, where 1 u = kg For 16 O, m O = 1 6u, where 1 u = kg First m O = 1 6u kg / u Reduced mass µ = ( ) = kg ( ) m m O O = m O m O + m O kg = = kg The fundamental vibrational frequency is ω = k, where k = 10 N/m µ ω = 10N / m kg = Hz, E vibr = n +1/ ( )!ω, n = 0,1, ( )( Hz) Ground state v = 0, E 0 =!ω = J s = J 1 ev In ev, ΔE 0 = J J = 00415eV (05 point) First excited state v = 1, ( )( Hz) E 1 = 3hν 0 = J s = J (05 point) In ev, ΔE 1 = ev J J = 014eV (05 point) B) Find the vibration quantum number that approximately corresponds to its 15-eV dissociation energy Hint: see dissociation equation on the equation sheet E vibr = ( n +1/ )!ω U 0, where U0 is the dissociation energy The dissociation energy is found when E vibr = 0, which gives 0 = ( n +1/ )!ω U 0 n = U 0!ω 1 Using U 0 = 15eV, ω = Hz, and h = ev s The vibrational quantum number that approximately corresponds to its 15-eV dissociation energy is v = U 0!ω 1 = 15eV ev s After rounding off v = 18 ( )( Hz) 1 = 176 C) Is O infrared active? Briefly explain your answer For a vibrational mode to be active, the vibration must change the dipole moment Since O is a homonulcear diatomic molecule, it possesses no dipole moment, and its one stretch vibration mode does not change the dipole Hence it is infrared inactive

5 Question 5 Microwave Spectroscopy: The rotational transition from the l = to the l = 1 state in CO is accompanied by the emission of a ev photon A) Use this information to find the rotational inertia of the CO molecule Use E l = l( l +1) " I, and the transition For the l l 1transition, the change of energy is ΔE = E l E l 1 = " l I, which equals the photon energy is ΔE = ev J i ev 1 = J ==! l I h = J i s or! = h π = Jis, and l =, I =! l ΔE = kg i m I =! l ΔE Use B) What is the bond length between the C and O atoms Data: Mass of carbon m C = 1u ; Mass of oxygen m O = 16u ; 1 u = kg Mass of carbon m C = 1 u kg / u Mass of oxygen m O = 1 6u kg / u Reduced Mass µ = m C m O m C + m O = ( ) = kg ( ) = kg ( kg) ( kg) kg kg = kg I = µr R = I / µ = kg m / kg = m

6

Please read the following instructions:

Please read the following instructions: MIDTERM #1 PHYS 33 (MODERN PHYSICS II) DATE/TIME: February 11, 016 (8:30 a.m. - 9:45 a.m.) PLACE: RB 306 Only non-programmable calculators are allowed. Name: ID: Please read the following instructions:

More information

Please read the following instructions:

Please read the following instructions: MIDTERM #1 PHYS 33 (MODERN PHYSICS II) DATE/TIME: February 16, 17 (8:3 a.m. - 9:45 a.m.) PLACE: RB 11 Only non-programmable calculators are allowed. Name: ID: Please read the following instructions: This

More information

Please read the following instructions:

Please read the following instructions: MIDTERM #1 PHYS 33 (MODERN PHYSICS II) DATE/TIME: February 16, 17 (8:3 a.m. - 9:45 a.m.) PLACE: RB 11 Only non-programmable calculators are allowed. Name: ID: Please read the following instructions: This

More information

Chapter 8 Problem Solutions

Chapter 8 Problem Solutions Chapter 8 Problem Solutions 1. The energy needed to detach the electron from a hydrogen atom is 13.6 ev, but the energy needed to detach an electron from a hydrogen molecule is 15.7 ev. Why do you think

More information

Atomic Term Symbols and Energy Splitting. λ=5890 Å

Atomic Term Symbols and Energy Splitting. λ=5890 Å Chemistry 362 Spring 2018 Dr. Jean M. Standard April 18, 2018 Atomic Term Symbols and Energy Splitting 1. Atomic Term Symbols and the Sodium D-Line The sodium D-line is responsible for the familiar orange

More information

Physics 43 Exam 2 Spring 2018

Physics 43 Exam 2 Spring 2018 Physics 43 Exam 2 Spring 2018 Print Name: Conceptual Circle the best answer. (2 points each) 1. Quantum physics agrees with the classical physics limit when a. the total angular momentum is a small multiple

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

A more comprehensive theory was needed. 1925, Schrödinger and Heisenberg separately worked out a new theory Quantum Mechanics.

A more comprehensive theory was needed. 1925, Schrödinger and Heisenberg separately worked out a new theory Quantum Mechanics. Ch28 Quantum Mechanics of Atoms Bohr s model was very successful to explain line spectra and the ionization energy for hydrogen. However, it also had many limitations: It was not able to predict the line

More information

64-311/5: Atomic and Molecular Spectra

64-311/5: Atomic and Molecular Spectra 64-311-Questions.doc 64-311/5: Atomic and Molecular Spectra Dr T Reddish (Room 89-1 Essex Hall) SECTION 1: REVISION QUESTIONS FROM 64-310/14 ε ο = 8.854187817 x 10-1 Fm -1, h = 1.0545766 x 10-34 Js, e

More information

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

Final Exam Tuesday, May 8, 2012 Starting at 8:30 a.m., Hoyt Hall Duration: 2h 30m Final Exam Tuesday, May 8, 2012 Starting at 8:30 a.m., Hoyt Hall. ------------------- Duration: 2h 30m Chapter 39 Quantum Mechanics of Atoms Units of Chapter 39 39-1 Quantum-Mechanical View of Atoms 39-2

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

Many-Electron Atoms. Thornton and Rex, Ch. 8

Many-Electron Atoms. Thornton and Rex, Ch. 8 Many-Electron Atoms Thornton and Rex, Ch. 8 In principle, can now solve Sch. Eqn for any atom. In practice, -> Complicated! Goal-- To explain properties of elements from principles of quantum theory (without

More information

Many-Electron Atoms. Thornton and Rex, Ch. 8

Many-Electron Atoms. Thornton and Rex, Ch. 8 Many-Electron Atoms Thornton and Rex, Ch. 8 In principle, can now solve Sch. Eqn for any atom. In practice, -> Complicated! Goal-- To explain properties of elements from principles of quantum theory (without

More information

PAPER No. : 8 (PHYSICAL SPECTROSCOPY) MODULE No. : 5 (TRANSITION PROBABILITIES AND TRANSITION DIPOLE MOMENT. OVERVIEW OF SELECTION RULES)

PAPER No. : 8 (PHYSICAL SPECTROSCOPY) MODULE No. : 5 (TRANSITION PROBABILITIES AND TRANSITION DIPOLE MOMENT. OVERVIEW OF SELECTION RULES) Subject Chemistry Paper No and Title Module No and Title Module Tag 8 and Physical Spectroscopy 5 and Transition probabilities and transition dipole moment, Overview of selection rules CHE_P8_M5 TABLE

More information

Chapter 10: Multi- Electron Atoms Optical Excitations

Chapter 10: Multi- Electron Atoms Optical Excitations Chapter 10: Multi- Electron Atoms Optical Excitations To describe the energy levels in multi-electron atoms, we need to include all forces. The strongest forces are the forces we already discussed in Chapter

More information

Physical Chemistry II Exam 2 Solutions

Physical Chemistry II Exam 2 Solutions Chemistry 362 Spring 208 Dr Jean M Standard March 9, 208 Name KEY Physical Chemistry II Exam 2 Solutions ) (4 points) The harmonic vibrational frequency (in wavenumbers) of LiH is 4057 cm Based upon this

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

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

Introduction to Molecular Vibrations and Infrared Spectroscopy

Introduction to Molecular Vibrations and Infrared Spectroscopy hemistry 362 Spring 2017 Dr. Jean M. Standard February 15, 2017 Introduction to Molecular Vibrations and Infrared Spectroscopy Vibrational Modes For a molecule with N atoms, the number of vibrational modes

More information

16.1 Molecular Vibrations

16.1 Molecular Vibrations 16.1 Molecular Vibrations molecular degrees of freedom are used to predict the number of vibrational modes vibrations occur as coordinated movement among many nuclei the harmonic oscillator approximation

More information

Physical Chemistry Lab II CHEM 4644 Spring 2011 Final Exam 5 questions at 3 points each equals 15 total points possible.

Physical Chemistry Lab II CHEM 4644 Spring 2011 Final Exam 5 questions at 3 points each equals 15 total points possible. Physical Chemistry Lab II Name: KEY CHEM 4644 Spring 2011 Final Exam 5 questions at 3 points each equals 15 total points possible. Constants: c = 3.00 10 8 m/s h = 6.63 10-34 J s 1 Hartree = 4.36 10-18

More information

Atomic spectra of one and two-electron systems

Atomic spectra of one and two-electron systems Atomic spectra of one and two-electron systems Key Words Term symbol, Selection rule, Fine structure, Atomic spectra, Sodium D-line, Hund s rules, Russell-Saunders coupling, j-j coupling, Spin-orbit coupling,

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

wbt Λ = 0, 1, 2, 3, Eq. (7.63)

wbt Λ = 0, 1, 2, 3, Eq. (7.63) 7.2.2 Classification of Electronic States For all diatomic molecules the coupling approximation which best describes electronic states is analogous to the Russell- Saunders approximation in atoms The orbital

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

Electronic Spectra of Complexes

Electronic Spectra of Complexes Electronic Spectra of Complexes Interpret electronic spectra of coordination compounds Correlate with bonding Orbital filling and electronic transitions Electron-electron repulsion Application of MO theory

More information

Name Class Date. Chapter: Arrangement of Electrons in Atoms

Name Class Date. Chapter: Arrangement of Electrons in Atoms Assessment Chapter Test A Chapter: Arrangement of Electrons in Atoms In the space provided, write the letter of the term that best completes each sentence or best answers each question. 1. Which of the

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

eigenvalues eigenfunctions

eigenvalues eigenfunctions Born-Oppenheimer Approximation Atoms and molecules consist of heavy nuclei and light electrons. Consider (for simplicity) a diatomic molecule (e.g. HCl). Clamp/freeze the nuclei in space, a distance r

More information

Sample Exercise 6.1 Concepts of Wavelength and Frequency

Sample Exercise 6.1 Concepts of Wavelength and Frequency Sample Exercise 6.1 Concepts of Wavelength and Frequency Two electromagnetic waves are represented in the margin. (a) Which wave has the higher frequency? (b) If one wave represents visible light and the

More information

MOLECULAR ENERGY LEVELS DR IMRANA ASHRAF

MOLECULAR ENERGY LEVELS DR IMRANA ASHRAF MOLECULAR ENERGY LEVELS DR IMRANA ASHRAF OUTLINE q q q q MOLECULE MOLECULAR ORBITAL THEORY MOLECULAR TRANSITIONS INTERACTION OF RADIATION WITH MATTER q TYPES OF MOLECULAR ENERGY LEVELS q MOLECULE q In

More information

Energy Level Energy Level Diagrams for Diagrams for Simple Hydrogen Model

Energy Level Energy Level Diagrams for Diagrams for Simple Hydrogen Model Quantum Mechanics and Atomic Physics Lecture 20: Real Hydrogen Atom /Identical particles http://www.physics.rutgers.edu/ugrad/361 physics edu/ugrad/361 Prof. Sean Oh Last time Hydrogen atom: electron in

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

DETECTION OF UNPAIRED ELECTRONS

DETECTION OF UNPAIRED ELECTRONS DETECTION OF UNPAIRED ELECTRONS There are experimental methods for the detection of unpaired electrons. One of the hallmarks of unpaired electrons in materials is interaction with a magnetic field. That

More information

PAPER No. : 8 (PHYSICAL SPECTROSCOPY) MODULE NO. : 23 (NORMAL MODES AND IRREDUCIBLE REPRESENTATIONS FOR POLYATOMIC MOLECULES)

PAPER No. : 8 (PHYSICAL SPECTROSCOPY) MODULE NO. : 23 (NORMAL MODES AND IRREDUCIBLE REPRESENTATIONS FOR POLYATOMIC MOLECULES) Subject Chemistry Paper No and Title Module No and Title Module Tag 8/ Physical Spectroscopy 23/ Normal modes and irreducible representations for polyatomic molecules CHE_P8_M23 TABLE OF CONTENTS 1. Learning

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

Atoms, Molecules and Solids (selected topics)

Atoms, Molecules and Solids (selected topics) Atoms, Molecules and Solids (selected topics) Part I: Electronic configurations and transitions Transitions between atomic states (Hydrogen atom) Transition probabilities are different depending on the

More information

Problem Set 8 Solutions

Problem Set 8 Solutions University of Alabama Department of Physics and Astronomy PH 253 / LeClair Spring 21 Problem Set 8 Solutions 1. Multiplicity of atomic magnetic moments. Calculate the magnetic moments that are possible

More information

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

An Aside: Application of Rotational Motion. Vibrational-Rotational Spectroscopy An Aside: Application of Rotational Motion Vibrational-Rotational Spectroscopy Rotational Excited States of a Diatomic Molecule are Significantly Populated at Room Temperature We can estimate the relative

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

Chapter 4. Table of Contents. Section 1 The Development of a New Atomic Model. Section 2 The Quantum Model of the Atom

Chapter 4. Table of Contents. Section 1 The Development of a New Atomic Model. Section 2 The Quantum Model of the Atom Arrangement of Electrons in Atoms Table of Contents Section 1 The Development of a New Atomic Model Section 2 The Quantum Model of the Atom Section 3 Electron Configurations Section 1 The Development of

More information

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

Rotational spectroscopy., 2017 Uwe Burghaus, Fargo, ND, USA Rotational spectroscopy, 2017 Uwe Burghaus, Fargo, ND, USA Atomic spectroscopy (part I) Absorption spectroscopy Bohr model QM of H atom (review) Atomic spectroscopy (part II) Visualization of wave functions

More information

CDO CP Chemistry Unit 5

CDO CP Chemistry Unit 5 1. Of the three particles; protons, neutrons, and electrons, which one(s) are responsible for most of the mass of an atom? a) the protons only b) the electrons only c) the neutrons only d) the protons

More information

CHAPTER 8 Atomic Physics

CHAPTER 8 Atomic Physics CHAPTER 8 Atomic Physics 8.1 Atomic Structure and the Periodic Table 8.2 Total Angular Momentum 8.3 Anomalous Zeeman Effect What distinguished Mendeleev was not only genius, but a passion for the elements.

More information

Atomic Structure, Periodic Table, and Other Effects: Chapter 8 of Rex and T. Modern Physics

Atomic Structure, Periodic Table, and Other Effects: Chapter 8 of Rex and T. Modern Physics Atomic Structure, Periodic Table, and Other Effects: Chapter 8 of Rex and T Modern Physics 11/16 and 11/19/2018 1 Introduction In Chapter 7, we studied the hydrogen atom. What about other elements, e.g.,

More information

NPTEL/IITM. Molecular Spectroscopy Lectures 1 & 2. Prof.K. Mangala Sunder Page 1 of 15. Topics. Part I : Introductory concepts Topics

NPTEL/IITM. Molecular Spectroscopy Lectures 1 & 2. Prof.K. Mangala Sunder Page 1 of 15. Topics. Part I : Introductory concepts Topics Molecular Spectroscopy Lectures 1 & 2 Part I : Introductory concepts Topics Why spectroscopy? Introduction to electromagnetic radiation Interaction of radiation with matter What are spectra? Beer-Lambert

More information

Atomic Quantum number summary. From last time. Na Optical spectrum. Another possibility: Stimulated emission. How do atomic transitions occur?

Atomic Quantum number summary. From last time. Na Optical spectrum. Another possibility: Stimulated emission. How do atomic transitions occur? From last time Hydrogen atom Multi-electron atoms This week s honors lecture: Prof. Brad Christian, Positron Emission Tomography Course evaluations next week Tues. Prof Montaruli Thurs. Prof. Rzchowski

More information

Atomic Structure Ch , 9.6, 9.7

Atomic Structure Ch , 9.6, 9.7 Ch. 9.2-4, 9.6, 9.7 Magnetic moment of an orbiting electron: An electron orbiting a nucleus creates a current loop. A current loop behaves like a magnet with a magnetic moment µ:! µ =! µ B " L Bohr magneton:

More information

Vibrational Spectroscopy

Vibrational Spectroscopy Vibrational Spectroscopy In this part of the course we will look at the kind of spectroscopy which uses light to excite the motion of atoms. The forces required to move atoms are smaller than those required

More information

MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY

MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY 20 CHAPTER MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY 20.1 Introduction to Molecular Spectroscopy 20.2 Experimental Methods in Molecular Spectroscopy 20.3 Rotational and Vibrational Spectroscopy 20.4 Nuclear

More information

where, c is the speed of light, ν is the frequency in wave numbers (cm -1 ) and µ is the reduced mass (in amu) of A and B given by the equation: ma

where, c is the speed of light, ν is the frequency in wave numbers (cm -1 ) and µ is the reduced mass (in amu) of A and B given by the equation: ma Vibrational Spectroscopy A rough definition of spectroscopy is the study of the interaction of matter with energy (radiation in the electromagnetic spectrum). A molecular vibration is a periodic distortion

More information

24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability ellipsoid. Selection rules.

24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability ellipsoid. Selection rules. Subject Chemistry Paper No and Title Module No and Title Module Tag 8/ Physical Spectroscopy 24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability

More information

Lecture 19: Building Atoms and Molecules

Lecture 19: Building Atoms and Molecules Lecture 19: Building Atoms and Molecules +e r n = 3 n = 2 n = 1 +e +e r y even Lecture 19, p 1 Today Nuclear Magnetic Resonance Using RF photons to drive transitions between nuclear spin orientations in

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

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

Potential energy, from Coulomb's law. Potential is spherically symmetric. Therefore, solutions must have form

Potential energy, from Coulomb's law. Potential is spherically symmetric. Therefore, solutions must have form Lecture 6 Page 1 Atoms L6.P1 Review of hydrogen atom Heavy proton (put at the origin), charge e and much lighter electron, charge -e. Potential energy, from Coulomb's law Potential is spherically symmetric.

More information

The atomic number is equal to the number of protons in the nucleus.

The atomic number is equal to the number of protons in the nucleus. Atomic Number The atomic number is equal to the number of protons in the nucleus. Sometimes given the symbol Z. On the periodic chart Z is the uppermost number in each element s box. In 1913 H.G.J. Moseley

More information

2m 2 Ze2. , where δ. ) 2 l,n is the quantum defect (of order one but larger

2m 2 Ze2. , where δ. ) 2 l,n is the quantum defect (of order one but larger PHYS 402, Atomic and Molecular Physics Spring 2017, final exam, solutions 1. Hydrogenic atom energies: Consider a hydrogenic atom or ion with nuclear charge Z and the usual quantum states φ nlm. (a) (2

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

Saturation Absorption Spectroscopy of Rubidium Atom

Saturation Absorption Spectroscopy of Rubidium Atom Saturation Absorption Spectroscopy of Rubidium Atom Jayash Panigrahi August 17, 2013 Abstract Saturated absorption spectroscopy has various application in laser cooling which have many relevant uses in

More information

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

Molecular Physics. Attraction between the ions causes the chemical bond. Molecular Physics A molecule is a stable configuration of electron(s) and more than one nucleus. Two types of bonds: covalent and ionic (two extremes of same process) Covalent Bond Electron is in a molecular

More information

V( x) = V( 0) + dv. V( x) = 1 2

V( x) = V( 0) + dv. V( x) = 1 2 Spectroscopy 1: rotational and vibrational spectra The vibrations of diatomic molecules Molecular vibrations Consider a typical potential energy curve for a diatomic molecule. In regions close to R e (at

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

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

2.4. Quantum Mechanical description of hydrogen atom

2.4. Quantum Mechanical description of hydrogen atom 2.4. Quantum Mechanical description of hydrogen atom Atomic units Quantity Atomic unit SI Conversion Ang. mom. h [J s] h = 1, 05459 10 34 Js Mass m e [kg] m e = 9, 1094 10 31 kg Charge e [C] e = 1, 6022

More information

Chapter 4: The Electron

Chapter 4: The Electron Chapter 4: The Electron C. Goodman Doral Academy Preparatory High School, 2012-2013 Based on a PowerPoint presentation by Sarah Temple By PresenterMedia.com Section 4-1 Electromagnetic Spectrum Essential

More information

Chem 3502/4502 Physical Chemistry II (Quantum Mechanics) 3 Credits Spring Semester 2006 Christopher J. Cramer. Lecture 10, February 10, / 4

Chem 3502/4502 Physical Chemistry II (Quantum Mechanics) 3 Credits Spring Semester 2006 Christopher J. Cramer. Lecture 10, February 10, / 4 Chem 350/450 Physical Chemistry II (Quantum Mechanics 3 Credits Spring Semester 006 Christopher J. Cramer Lecture 10, February 10, 006 Solved Homework We are asked to find and for the first two

More information

Explain the mathematical relationship among the speed, wavelength, and frequency of electromagnetic radiation.

Explain the mathematical relationship among the speed, wavelength, and frequency of electromagnetic radiation. Preview Objectives Properties of Light Wavelength and Frequency The Photoelectric Effect The Hydrogen-Atom Line-Emission Spectrum Bohr Model of the Hydrogen Atom Photon Emission and Absorption Section

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

Atomic Structure. Chapter 8

Atomic Structure. Chapter 8 Atomic Structure Chapter 8 Overview To understand atomic structure requires understanding a special aspect of the electron - spin and its related magnetism - and properties of a collection of identical

More information

Chapter 6. Electronic. Electronic Structure of Atoms Pearson Education

Chapter 6. Electronic. Electronic Structure of Atoms Pearson Education Chapter 6 Laser: step-like energy transition 6.1 The Wave Nature of Light 6.2 Quantized Energy and Photons 6.3 Line Spectra and the Bohr Model 6.4 The Wave Behavior of Matter 6.5 Quantum Mechanics and

More information

Chemistry 11. Unit 8 Atoms and the Periodic Table Part II Electronic Structure of Atoms

Chemistry 11. Unit 8 Atoms and the Periodic Table Part II Electronic Structure of Atoms Chemistry 11 Unit 8 Atoms and the Periodic Table Part II Electronic Structure of Atoms 2 1. Atomic number and atomic mass In the previous section, we have seen that from 50 to 100 years after Dalton proposed

More information

PHYS3113, 3d year Statistical Mechanics Tutorial problems. Tutorial 1, Microcanonical, Canonical and Grand Canonical Distributions

PHYS3113, 3d year Statistical Mechanics Tutorial problems. Tutorial 1, Microcanonical, Canonical and Grand Canonical Distributions 1 PHYS3113, 3d year Statistical Mechanics Tutorial problems Tutorial 1, Microcanonical, Canonical and Grand Canonical Distributions Problem 1 The macrostate probability in an ensemble of N spins 1/2 is

More information

I. Multiple Choice Questions (Type-I)

I. Multiple Choice Questions (Type-I) I. Multiple Choice Questions (Type-I) 1. Which of the following conclusions could not be derived from Rutherford s α -particle scattering experiement? (i) Most of the space in the atom is empty. (ii) The

More information

Lecture 19: Building Atoms and Molecules

Lecture 19: Building Atoms and Molecules Lecture 19: Building Atoms and Molecules +e r n = 3 n = 2 n = 1 +e +e r ψ even Lecture 19, p 1 Today Nuclear Magnetic Resonance Using RF photons to drive transitions between nuclear spin orientations in

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

Materials Science. Atomic Structures and Bonding

Materials Science. Atomic Structures and Bonding Materials Science Atomic Structures and Bonding 1 Atomic Structure Fundamental concepts Each atom consists of a nucleus composed of protons and neutrons which are encircled by electrons. Protons and electrons

More information

Key Equations. Determining the smallest change in an atom's energy.

Key Equations. Determining the smallest change in an atom's energy. ATOMIC STRUCTURE AND PERIODICITY Matter and Energy Key Equations λν = c ΔE = hν Relating speed of a wave to its wavelength and frequency. Determining the smallest change in an atom's energy. H( λ =R n

More information

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

Molecular spectroscopy Multispectral imaging (FAFF 020, FYST29) fall 2017 Molecular spectroscopy Multispectral imaging (FAFF 00, FYST9) fall 017 Lecture prepared by Joakim Bood joakim.bood@forbrf.lth.se Molecular structure Electronic structure Rotational structure Vibrational

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

Numerical Solution of a Potential Final Project

Numerical Solution of a Potential Final Project Numerical Solution of a Potential Final Project 1 Introduction The purpose is to determine the lowest order wave functions of and energies a potential which describes the vibrations of molecules fairly

More information

Chapter 6 Electronic Structure of Atoms. 許富銀 ( Hsu Fu-Yin)

Chapter 6 Electronic Structure of Atoms. 許富銀 ( Hsu Fu-Yin) Chapter 6 Electronic Structure of Atoms 許富銀 ( Hsu Fu-Yin) 1 The Wave Nature of Light The light we see with our eyes, visible light, is one type of electromagnetic radiation. electromagnetic radiation carries

More information

ATMO 551a Fall Resonant Electromagnetic (EM) Interactions in Planetary atmospheres. Electron transition between different electron orbits

ATMO 551a Fall Resonant Electromagnetic (EM) Interactions in Planetary atmospheres. Electron transition between different electron orbits Resonant Electromagnetic (EM) Interactions in Planetary atmospheres There are three classes of energy states that interact with EM radiation that we are interested in to understand how light (EM radiation)

More information

Atomic Structure & Radiative Transitions

Atomic Structure & Radiative Transitions Atomic Structure & Radiative Transitions electron kinetic energy nucleus-electron interaction electron-electron interaction Remember the meaning of spherical harmonics Y l, m (θ, ϕ) n specifies the

More information

Atomic Spectroscopy II

Atomic Spectroscopy II Applied Spectroscopy Atomic Spectroscopy II Multielectron Atoms Recommended Reading: Banwell And McCash Chapter 5 The Building-Up (aufbau) Principle How do the electrons in multi-electron atoms get distributed

More information

CHEM J-5 June 2014

CHEM J-5 June 2014 CHEM1101 2014-J-5 June 2014 The molecular orbital energy level diagrams for H 2, H 2 +, H 2 and O 2 are shown below. Fill in the valence electrons for each species in its ground state and label the types

More information

Problem Set 5 Solutions

Problem Set 5 Solutions Chemistry 362 Dr Jean M Standard Problem Set 5 Solutions ow many vibrational modes do the following molecules or ions possess? [int: Drawing Lewis structures may be useful in some cases] In all of the

More information

Atoms and Their Isotopes

Atoms and Their Isotopes Atoms and Their Isotopes Why? Atoms and isotopes are identified by the number of protons, neutrons, and electrons that they contain. Before you can understand the properties of atoms, how atoms combine

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

Light. October 16, Chapter 5: Electrons in Atoms Honors Chemistry. Bohr Model

Light. October 16, Chapter 5: Electrons in Atoms Honors Chemistry. Bohr Model Chapter 5: Electrons in Atoms Honors Chemistry Bohr Model Niels Bohr, a young Danish physicist and a student of Rutherford improved Rutherford's model. Bohr proposed that an electron is found only in specific

More information

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions I. General Features of Electronic spectroscopy. A. Visible and ultraviolet photons excite electronic state transitions. ε photon = 120 to 1200

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

Molecular Structure & Spectroscopy Friday, February 4, 2010

Molecular Structure & Spectroscopy Friday, February 4, 2010 Molecular Structure & Spectroscopy Friday, February 4, 2010 CONTENTS: 1. Introduction 2. Diatomic Molecules A. Electronic structure B. Rotation C. Vibration D. Nuclear spin 3. Radiation from Diatomic Molecules

More information

Chapter IV: Electronic Spectroscopy of diatomic molecules

Chapter IV: Electronic Spectroscopy of diatomic molecules Chapter IV: Electronic Spectroscopy of diatomic molecules IV.2.1 Molecular orbitals IV.2.1.1. Homonuclear diatomic molecules The molecular orbital (MO) approach to the electronic structure of diatomic

More information

Atoms, Molecules and Solids (selected topics)

Atoms, Molecules and Solids (selected topics) Atoms, Molecules and Solids (selected topics) Part I: Electronic configurations and transitions Transitions between atomic states (Hydrogen atom) Transition probabilities are different depending on the

More information

Atomic Structure. Standing Waves x10 8 m/s. (or Hz or 1/s) λ Node

Atomic Structure. Standing Waves x10 8 m/s. (or Hz or 1/s) λ Node Atomic Structure Topics: 7.1 Electromagnetic Radiation 7.2 Planck, Einstein, Energy, and Photons 7.3 Atomic Line Spectra and Niels Bohr 7.4 The Wave Properties of the Electron 7.5 Quantum Mechanical View

More information

The importance of constants

The importance of constants The importance of constants Sourendu Gupta TIFR Graduate School Quantum Mechanics 1 September 22, 2008 Sourendu Gupta (TIFR Graduate School) The importance of constants QM I 1 / 13 Outline 1 Universal

More information

ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY

ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY All matter is made of atoms. There are a limited number of types of atoms; these are the elements. (EU 1.A) Development of Atomic Theory Atoms are so small

More information

Georgia Institute of Technology CHEM 1310 revised 10/8/09 Spring The Development of Quantum Mechanics. ν (nu) = frequency (in s -1 or hertz)

Georgia Institute of Technology CHEM 1310 revised 10/8/09 Spring The Development of Quantum Mechanics. ν (nu) = frequency (in s -1 or hertz) The Development of Quantum Mechanics Early physicists used the properties of electromagnetic radiation to develop fundamental ideas about the structure of the atom. A fundamental assumption for their work

More information

The early periodic table based on atomic weight. (Section 5.1) Lets review: What is a hydrogen atom? 1 electron * nucleus H 1 proton

The early periodic table based on atomic weight. (Section 5.1) Lets review: What is a hydrogen atom? 1 electron * nucleus H 1 proton PERIODICITY AND ATOMIC STRUCTURE CHAPTER 5 How can we relate the structure of the atom to the way that it behaves chemically? The process of understanding began with a realization that many of the properties

More information