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Chem 322: Physical Chemistry II
This text is an introduction to quantum chemistry, atomic and molecular structure, and spectroscopy. The detailed consequences of quantum theory are examined in the light of the molecular model.
- Author
- Mary Crawford
- Publisher
- Knox College
- Source
- LibreTexts
- Language
- EN
- Category
- Basic Sciences
Contents· 162 sections
- 01: Chemical Kinetics
- 1.01: Reaction Rates
- 1.02: Reaction Order
- 1.03: Molecularity of a Reaction
- 1.04: More Complex Reactions
- 1.05: The Effect of Temperature on Reaction Rates
- 1.06: Potential Energy Surfaces
- 1.07: Theories of Reaction Rates
- 1.08: Isotope Effects in Chemical Reactions
- 1.09: Reactions in Solution
- 1.10: Fast Reactions in Solution
- 1.11: Oscillating Reactions
- 1.12: Chemical Kinetics (Exercises)
- 02: Chemical Kinetics II
- 2.01: The Rates of Chemical Reactions
- 2.02: Integrated Rate Laws
- 2.03: Reactions Approaching Equilibrium
- 2.04: The Arrhenius Equation
- 2.05: Reaction Mechanisms
- 2.06: Examples of Reaction Mechanisms
- 2.07: Photochemistry
- 2.08: Enzymes
- 03: Reaction Dynamics
- 3.01: Collision Theory
- 3.02: Diffusion-controlled Reactions
- 3.03: Transition-state Theory
- 3.04: The Dynamics of Molecular Collisions
- 3.05: Electron Transfer in Homogeneous Systems
- 3.06: Processes at Electrodes
- 04: Enzyme Kinetics
- 4.01: General Principles of Catalysis
- 4.02: The Equations of Enzyme Kinetics
- 4.03: Chymotrypsin- A Case Study
- 4.04: Multisubstrate Systems
- 4.05: Enzyme Inhibition
- 4.06: Allosteric Interactions
- 4.07: The Effect of pH on Enzyme Kinetics
- 4.08: The Effect of Temperature on Enzyme Kinetics
- 4.09: Exercises
- 05: Lasers Laser Spectroscopy and Photochemistry
- 5.01: Electronically Excited Molecules
- 5.02: Transitions Modeled as Kinetics
- 5.03: Two-Level Systems Cannot Form Population Inversions
- 5.04: Population Inversion via Three-Level Systems
- 5.05: Laser Fundamentals
- 5.06: The Helium-Neon Laser
- 5.07: High-Resolution Laser Spectroscopy
- 5.08: Photochemical Dynamics
- 06: Nuclear Magnetic Resonance Spectroscopy
- 6.01: Nuclei Have Intrinsic Spin Angular Momenta
- 6.02: Magnetic Moments Interact with Magnetic Fields
- 6.03: Proton NMR Spectrometers Operate at Frequencies Between 60 MHz and 750 MHz
- 6.04: The Magnetic Field Acting upon Nuclei in Molecules Is Shielded
- 6.05: Chemical Shifts is Sensitive to Chemical Environment of the Nucleus
- 6.06: Spin-Spin Coupling Results in Multiplets in NMR Spectra
- 6.07: Spin-Spin Coupling Between Chemically Equivalent Protons Is Not Observed
- 6.08: The n1 Rule Applies Only to First-Order Spectra
- 6.09: Second-Order Spectra Can Be Calculated Exactly Using the Variational Method
- 07: Molecular Spectroscopy
- 7.01: The Electromagnetic Spectrum
- 7.02: Rotational Transitions Accompany Vibrational Transitions
- 7.03: The Vibration-Rotation Spectrum
- 7.04: The Pure Rotational Spectrum has Unequal Spacings
- 7.05: Vibrational Overtones
- 7.06: Electronic Spectra Contain Electronic Vibrational and Rotational Information
- 7.07: The Franck-Condon Principle
- 7.08: Rotational Spectra of Polyatomic Molecules
- 7.09: Normal Modes in Polyatomic Molecules
- 7.10: Irreducible Representation of Point Groups
- 7.11: Time-Dependent Perturbation Theory
- 7.12: The Selection Rule for the Rigid Rotator
- 7.13: The Harmonic Oscillator Selection Rule
- 7.14: Group Theory Determines Infrared Activity
- 7.15: Molecular Spectroscopy (Exercises)
- 08: The Schrodinger Equation and a Particle in a Box
- 8.01: The Schrodinger Equation
- 8.02: Linear Operators in Quantum Mechanics
- 8.03: The Schrodinger Equation is an Eigenvalue Problem
- 8.04: The Quantum Mechanical Free Particle
- 8.05: Wavefunctions Have a Probabilistic Interpretation
- 8.06: The Energy of a Particle in a Box is Quantized
- 8.07: Wavefunctions Must Be Normalized
- 8.08: The Average Momentum of a Particle in a Box is Zero
- 8.09: Particle in a Finite Box and Tunneling (optional)
- 8.10: The Uncertainty Principle Redux - Estimating Uncertainties from Wavefunctions
- 8.11: A Particle in a Two-Dimensional Box
- 8.12: A Particle in a Three-Dimensional Box
- 8.13: The Schrodinger Equation and a Particle in a Box (Exercises)
- 09: Postulates and Principles of Quantum Mechanics
- 9.01: The Wavefunction Specifies the State of a System
- 9.02: Quantum Operators Represent Classical Variables
- 9.03: Observable Quantities Must Be Eigenvalues of Quantum Mechanical Operators
- 9.04: The Time-Dependent Schrodinger Equation
- 9.05: The Eigenfunctions of Operators are Orthogonal
- 9.06: Heisenburg Uncertainy Principle III - Commuting Operators
- 9.07: Postulates and Principles of Quantum Mechanics (Exercises)
- 10: The Harmonic Oscillator and the Rigid Rotor
- 10.01: A Harmonic Oscillator Obeys Hooke's Law
- 10.02: The Equation for a Harmonic-Oscillator Model of a Diatomic Molecule Contains the Reduced Mass of the Molecule
- 10.03: The Harmonic Oscillator is an Approximation
- 10.04: The Harmonic Oscillator Energy Levels
- 10.05: The Harmonic Oscillator and Infrared Spectra
- 10.06: The Harmonic-Oscillator Wavefunctions Involve Hermite Polynomials
- 10.07: Hermite Polynomials are either Even or Odd Functions
- 10.08: The Energy Levels of a Rigid Rotor
- 10.09: The Rigid Rotator is a Model for a Rotating Diatomic Molecule
- 10.10: The Harmonic Oscillator and the Rigid Rotor (Exercises)
- 11: The Hydrogen Atom
- 11.01: The Schrodinger Equation for the Hydrogen Atom Can Be Solved Exactly
- 11.02: The Wavefunctions of a Rigid Rotator are Called Spherical Harmonics
- 11.03: The Three Components of Angular Momentum Cannot be Measured Simultaneously with Arbitrary Precision
- 11.04: Hydrogen Atomic Orbitals Depend upon Three Quantum Numbers
- 11.05: s Orbitals are Spherically Symmetric
- 11.06: Orbital Angular Momentum and the p-orbitals
- 11.07: The Helium Atom Cannot Be Solved Exactly
- 11.08: The Hydrogen Atom (Exercises)
- 12: Approximation Methods
- 12.01: Slater's Rules for Shielding
- 12.02: The Variational Method
- 12.03: Linear Variational Method and the Secular Determinant
- 12.04: Trial Functions Can Be Linear Combinations of Functions with Variational Parameters
- 12.05: Perturbation Theory Expresses the Solutions in Terms of Solved Problems
- 12.06: Approximation Methods (Exercises)
- 13: Multielectron Atoms
- 13.01: Atomic and Molecular Calculations are Expressed in Atomic Units
- 13.02: Perturbation Theory and the Variational Method for Helium
- 13.03: Hartree-Fock Equations are Solved by the Self-Consistent Field Method
- 13.04: An Electron Has An Intrinsic Spin Angular Momentum
- 13.05: Wavefunctions must be Antisymmetric to Interchange of any Two Electrons
- 13.06: Antisymmetric Wave Functions can be Represented by Slater Determinants
- 13.07: Hartree-Fock Calculations Give Good Agreement with Experimental Data
- 13.08: Term Symbols Gives Detailed Descriptions of an Electron Configuration
- 13.09: Multi-electron Considerations - A Closer Look at Helium
- 13.10: The Allowed Values of J - the Total Angular Momentum Quantum Number
- 13.11: Hund's Rules Determine the Term Symbols of the Ground Electronic States
- 13.12: Using Atomic Term Symbols to Describe Atomic Spectra
- 13.13: Multielectron Atoms (Exercises)
- 14: Bonding in Polyatomic Molecules
- 14.01: Hybrid Orbitals Account for Molecular Shape
- 14.02: Different Hybrid Orbitals Used for Bonding in Water
- 14.03: Why is BeH Linear and HO Bent
- 14.04: Photoelectron Spectroscopy
- 14.05: The (pi)-Electron Approximation of Conjugation
- 14.06: Butadiene is Stabilized by a Delocalization Energy
- 15: Computational Quantum Chemistry
- 15.01: Overview of Quantum Calculations
- 15.02: Gaussian Basis Sets
- 15.03: Extended Basis Sets
- 15.04: Orbital Polarization Terms
- 15.05: The Ground-State Energy of H
- 15.06: Quantum Calculations
- 16: MathChapters
- 16.01: Complex Numbers
- 16.02: Probability and Statistics
- 16.03: Vectors
- 16.04: Spherical Coordinates
- 16.05: Determinants
- 16.06: Matrices
- 16.07: Numerical Methods
- 16.08: Partial Differentiation
- 16.09: Series and Limits
- 16.10: The Binomial Distribution and Stirling's Appromixation