
External
Physical Chemistry for Biological Sciences
- Author
- Carey Southern
- Publisher
- DePaul University
- Source
- LibreTexts
- Language
- EN
- Category
- Basic Sciences
Contents· 165 sections
- 01: The Dawn of the Quantum Theory
- 1.01: Blackbody Radiation Cannot Be Explained Classically
- 1.02: Quantum Hypothesis Used for Blackbody Radiation Law
- 1.03: Photoelectric Effect Explained with Quantum Hypothesis
- 1.04: The Hydrogen Atomic Spectrum
- 1.05: The Rydberg Formula and the Hydrogen Atomic Spectrum
- 1.06: Matter Has Wavelike Properties
- 1.07: de Broglie Waves can be Experimentally Observed
- 1.08: The Bohr Theory of the Hydrogen Atom
- 1.09: The Heisenberg Uncertainty Principle
- 1.E: The Dawn of the Quantum Theory (Exercises)
- 02: Waves and the Schrodinger Equation
- 2.01: The One-Dimensional Wave Equation
- 2.02: The Schrodinger Equation
- 2.03: Linear Operators in Quantum Mechanics
- 2.04: The Schrodinger Equation is an Eigenvalue Problem
- 03: Postulates and Principles of Quantum Mechanics
- 3.01: The Wavefunction Specifies the State of a System
- 3.02: Wavefunctions Have a Probabilistic Interpretation
- 3.03: Wavefunctions Must Be Normalized
- 3.04: Quantum Operators Represent Classical Variables
- 3.05: Observable Quantities Must Be Eigenvalues of Quantum Mechanical Operators
- 3.06: The Time-Dependent Schrodinger Equation
- 3.E: Postulates and Principles of Quantum Mechanics (Exercises)
- 04: The Particle in a Box
- 4.01: The Energy of a Particle in a Box is Quantized
- 4.02: The Average Momentum of a Particle in a Box is Zero
- 4.03: The Uncertainty Principle - Estimating Uncertainties from Wavefunctions
- 4.04: A Particle in a Three-Dimensional Box
- 4.E: The Schrodinger Equation and a Particle in a Box (Exercises)
- 05: The Harmonic Oscillator and the Rigid Rotor
- 5.01: A Harmonic Oscillator Obeys Hooke's Law
- 5.02: The Equation for a Harmonic-Oscillator Model of a Diatomic Molecule Contains the Reduced Mass of the Molecule
- 5.03: The Harmonic Oscillator Approximates Molecular Vibrations
- 5.04: The Harmonic Oscillator Energy Levels
- 5.05: The Harmonic Oscillator Wavefunctions involve Hermite Polynomials
- 5.06: Hermite Polynomials are either Even or Odd Functions
- 5.07: The Harmonic Oscillator and Infrared Spectra
- 5.08: The Rigid Rotator is a Model for a Rotating Diatomic Molecule
- 5.09: The Energy Levels of a Rigid Rotor
- 5.E: The Harmonic Oscillator and the Rigid Rotor (Exercises)
- 06: The Hydrogen Atom
- 6.01: The Schrodinger Equation for the Hydrogen Atom Can Be Solved Exactly
- 6.02: The Wavefunctions of a Rigid Rotator are Called Spherical Harmonics
- 6.03: Hydrogen Atomic Orbitals Depend upon Three Quantum Numbers
- 6.04: s-orbitals are Spherically Symmetric
- 6.05: Orbital Angular Momentum and the p-Orbitals
- 6.06: The Helium Atom Cannot Be Solved Exactly
- 6.E: The Hydrogen Atom (Exercises)
- 07: Multielectron Atoms
- 7.01: Perturbation Theory and the Variational Method for Helium
- 7.02: Hartree-Fock Equations are Solved by the Self-Consistent Field Method
- 7.03: An Electron has an Intrinsic Spin Angular Momentum
- 7.04: Wavefunctions must be Antisymmetric to Interchange of any Two Electrons
- 7.05: Hartree-Fock Calculations Give Good Agreement with Experimental Data
- 7.E: Multielectron Atoms (Exercises)
- 08: Chemical Bonding in Diatomic Molecules
- 8.01: The Born-Oppenheimer Approximation Simplifies the Schrodinger Equation for Molecules
- 8.02: The H Prototypical Species
- 8.03: The Overlap Integral
- 8.04: Chemical Bond Stability
- 8.05: Bonding and Antibonding Orbitals
- 8.06: A Simple Molecular-Orbital Treatment of H Places Both Electrons in a Bonding Orbital
- 8.07: Molecular Orbitals Can Be Ordered According to Their Energies
- 8.08: Molecular-Orbital Theory Does not Predict a Stable Diatomic Helium Molecule
- 8.09: Electrons Populate Molecular Orbitals According to the Pauli Exclusion Principle
- 8.10: SCF-LCAO-MO Wavefunctions are Molecular Orbitals formed from a Linear Combination of Atomic Orbitals and Whose Coefficients Are Determined Self-Consistently
- 8.11: Most Molecules Have Excited Electronic States
- 8.E: Chemical Bond in Diatomic Molecules (Exercises)
- 09: Molecular Spectroscopy
- 9.01: The Electromagnetic Spectrum
- 9.02: Electronic Spectra Contain Electronic Vibrational and Rotational Information
- 9.03: The Franck-Condon Principle
- 9.04: What Causes Molecules to Absorb UV and Visible Light
- 9.05: Fluorescence and Phosphorescence
- 9.06: Jablonski diagram
- 9.E: Molecular Spectroscopy (Exercises)
- 10: The First Law of Thermodynamics
- 10.01: Overview of Classical Thermodynamics
- 10.02: All Dilute Gases Behave Ideally
- 10.03: van der Waals and Redlich-Kwong Equations of State
- 10.04: Pressure-Volume Work
- 10.05: Work and Heat are not State Functions
- 10.06: Work and Heat Have a Simple Molecular Interpretation
- 10.07: Energy is a State Function
- 10.08: Heat Capacity is a Path Function
- 10.09: An Adiabatic Process is a Process in which No Energy as Heat is Transferred
- 10.10: The Temperature of a Gas Decreases in a Reversible Adiabatic Expansion
- 10.11: Enthalpy is a State Function
- 10.12: Relative Enthalpies Can Be Determined from Heat Capacity Data and Heats of Transition
- 10.13: Enthalpy Changes for Chemical Equations are Additive
- 10.14: Heats of Reactions Can Be Calculated from Tabulated Heats of Formation
- 10.15: The Temperature Dependence of H
- 10.E: The First Law of Thermodynamics (Exercises)
- 11: Entropy and The Second Law of Thermodynamics
- 11.01: Energy Does not Determine Spontaneity
- 11.02: Nonequilibrium Isolated Systems Evolve in a Direction That Increases Their Energy Dispersal
- 11.03: Unlike heat Entropy is a State Function
- 11.04: The Second Law of Thermodynamics
- 11.05: The Famous Equation of Statistical Thermodynamics is Sk ln W
- 11.06: We Must Always Devise a Reversible Process to Calculate Entropy Changes
- 11.07: Thermodynamics Provides Insight into the Conversion of Heat into Work
- 11.E: Entropy and The Second Law of Thermodynamics (Exercises)
- 12: Helmholtz and Gibbs Energies
- 12.01: Helmholtz Energy
- 12.02: Gibbs Energy Determines the Direction of Spontaneity at Constant Pressure and Temperature
- 12.03: The Maxwell Relations
- 12.04: The Enthalpy of an Ideal Gas is Independent of Pressure
- 12.05: Thermodynamic Functions have Natural Variables
- 12.06: The Standard State for a Gas is an Ideal Gas at 1 Bar
- 12.07: The Gibbs-Helmholtz Equation
- 12.E: Helmholtz and Gibbs Energies (Exercises)
- 13: Chemical Equilibrium
- 13.01: Equilibrium Results when Gibbs Energy is Minimized
- 13.02: An Equilibrium Constant is a Function of Temperature Only
- 13.03: Standard Gibbs Energies of Formation Can Be Used to Calculate Equilibrium Constants
- 13.04: Gibbs Energy of a Reaction vs. Extent of Reaction is a Minimum at Equilibrium
- 13.05: Reaction Quotient and Equilibrium Constant Ratio Determines Reaction Direction
- 13.06: The Sign of G and not G Determines the Direction of Reaction Spontaneity
- 13.07: The van 't Hoff Equation
- 13.08: Thermodynamic Equilibrium Constants Are Expressed in Terms of Activities
- 13.09: Activities are Important for Ionic Species
- 13.10: Homework Problems
- 14: Solutions I - Volatile Solutes
- 14.01: A Mixture is a Combination of Two or More Substances
- 14.02: The Gibbs-Duhem Equation Relates Chemical Potential and Composition at Equilibrium
- 14.03: Chemical Potential of Each Component Has the Same Value in Each Phase in Which the Component Appears
- 14.04: Ideal Solutions obey Raoult's Law
- 14.05: Most Solutions are Not Ideal
- 14.06: Vapor Pressures of Volatile Binary Solutions
- 14.07: Activities of Nonideal Solutions
- 14.08: Activities are Calculated with Respect to Standard States
- 14.09: Gibbs Energy of Mixing of Binary Solutions in Terms of the Activity Coefficient
- 14.E: Solutions I- Liquid-Liquid Solutions (Exercises)
- 15: Solutions II - Nonvolatile Solutes
- 15.01: Standard State of Nonvolatile Solutions
- 15.02: The Activities of Nonvolatile Solutes
- 15.03: Colligative Properties Depend only on Number Density
- 15.04: Osmotic Pressure can Determine Molecular Masses
- 15.05: Electrolytes Solutions are Nonideal at Low Concentrations
- 15.06: The Debye-Huckel Theory
- 15.07: Extending Debye-Huckel Theory to Higher Concentrations
- 15.08: Homework Problems
- 16: Chemical Kinetics I - Rate Laws
- 16.01: The Time Dependence of a Chemical Reaction is Described by a Rate Law
- 16.02: Rate Laws Must Be Determined Experimentally
- 16.03: First-Order Reactions Show an Exponential Decay of Reactant Concentration with Time
- 16.04: Different Rate Laws Predict Different Kinetics
- 16.05: Reactions can also be Reversible
- 16.E: Chemical Kinetics I - Rate Laws (Exercises)
- 17: Chemical Kinetics II- Reaction Mechanisms
- 17.01: A Mechanism is a Sequence of Elementary Reactions
- 17.02: The Principle of Detailed Balance
- 17.03: Multiple Mechanisms are often Indistinguishable
- 17.04: The Steady-State Approximation
- 17.05: Rate Laws Do Not Imply Unique Mechanism
- 17.06: The Lindemann Mechanism
- 17.07: Some Reaction Mechanisms Involve Chain Reactions
- 17.08: A Catalyst Affects the Mechanism and Activation Energy
- 17.09: The Michaelis-Menten Mechanism for Enzyme Catalysis
- 17.E: Chemical Kinetics II- Reaction Mechanisms (Exercises)
- 18: Kinetics- Temperature Dependence and Relaxation Methods
- 18.01: Rate Constants Are Usually Strongly Temperature Dependent
- 18.02: The Rate Constants of a Reversible Reaction Can Be Determined Using Relaxation Techniques
- 18.03: Transition-State Theory Can Be Used to Estimate Reaction Rate Constants