Phu Xuan University Library
Physical Chemistry for Biological Sciences

External

Physical Chemistry for Biological Sciences

Author
Carey Southern
Publisher
DePaul University
Source
LibreTexts
Language
EN
Category
Basic Sciences
Contents· 165 sections
  1. 01: The Dawn of the Quantum Theory
  2. 1.01: Blackbody Radiation Cannot Be Explained Classically
  3. 1.02: Quantum Hypothesis Used for Blackbody Radiation Law
  4. 1.03: Photoelectric Effect Explained with Quantum Hypothesis
  5. 1.04: The Hydrogen Atomic Spectrum
  6. 1.05: The Rydberg Formula and the Hydrogen Atomic Spectrum
  7. 1.06: Matter Has Wavelike Properties
  8. 1.07: de Broglie Waves can be Experimentally Observed
  9. 1.08: The Bohr Theory of the Hydrogen Atom
  10. 1.09: The Heisenberg Uncertainty Principle
  11. 1.E: The Dawn of the Quantum Theory (Exercises)
  12. 02: Waves and the Schrodinger Equation
  13. 2.01: The One-Dimensional Wave Equation
  14. 2.02: The Schrodinger Equation
  15. 2.03: Linear Operators in Quantum Mechanics
  16. 2.04: The Schrodinger Equation is an Eigenvalue Problem
  17. 03: Postulates and Principles of Quantum Mechanics
  18. 3.01: The Wavefunction Specifies the State of a System
  19. 3.02: Wavefunctions Have a Probabilistic Interpretation
  20. 3.03: Wavefunctions Must Be Normalized
  21. 3.04: Quantum Operators Represent Classical Variables
  22. 3.05: Observable Quantities Must Be Eigenvalues of Quantum Mechanical Operators
  23. 3.06: The Time-Dependent Schrodinger Equation
  24. 3.E: Postulates and Principles of Quantum Mechanics (Exercises)
  25. 04: The Particle in a Box
  26. 4.01: The Energy of a Particle in a Box is Quantized
  27. 4.02: The Average Momentum of a Particle in a Box is Zero
  28. 4.03: The Uncertainty Principle - Estimating Uncertainties from Wavefunctions
  29. 4.04: A Particle in a Three-Dimensional Box
  30. 4.E: The Schrodinger Equation and a Particle in a Box (Exercises)
  31. 05: The Harmonic Oscillator and the Rigid Rotor
  32. 5.01: A Harmonic Oscillator Obeys Hooke's Law
  33. 5.02: The Equation for a Harmonic-Oscillator Model of a Diatomic Molecule Contains the Reduced Mass of the Molecule
  34. 5.03: The Harmonic Oscillator Approximates Molecular Vibrations
  35. 5.04: The Harmonic Oscillator Energy Levels
  36. 5.05: The Harmonic Oscillator Wavefunctions involve Hermite Polynomials
  37. 5.06: Hermite Polynomials are either Even or Odd Functions
  38. 5.07: The Harmonic Oscillator and Infrared Spectra
  39. 5.08: The Rigid Rotator is a Model for a Rotating Diatomic Molecule
  40. 5.09: The Energy Levels of a Rigid Rotor
  41. 5.E: The Harmonic Oscillator and the Rigid Rotor (Exercises)
  42. 06: The Hydrogen Atom
  43. 6.01: The Schrodinger Equation for the Hydrogen Atom Can Be Solved Exactly
  44. 6.02: The Wavefunctions of a Rigid Rotator are Called Spherical Harmonics
  45. 6.03: Hydrogen Atomic Orbitals Depend upon Three Quantum Numbers
  46. 6.04: s-orbitals are Spherically Symmetric
  47. 6.05: Orbital Angular Momentum and the p-Orbitals
  48. 6.06: The Helium Atom Cannot Be Solved Exactly
  49. 6.E: The Hydrogen Atom (Exercises)
  50. 07: Multielectron Atoms
  51. 7.01: Perturbation Theory and the Variational Method for Helium
  52. 7.02: Hartree-Fock Equations are Solved by the Self-Consistent Field Method
  53. 7.03: An Electron has an Intrinsic Spin Angular Momentum
  54. 7.04: Wavefunctions must be Antisymmetric to Interchange of any Two Electrons
  55. 7.05: Hartree-Fock Calculations Give Good Agreement with Experimental Data
  56. 7.E: Multielectron Atoms (Exercises)
  57. 08: Chemical Bonding in Diatomic Molecules
  58. 8.01: The Born-Oppenheimer Approximation Simplifies the Schrodinger Equation for Molecules
  59. 8.02: The H Prototypical Species
  60. 8.03: The Overlap Integral
  61. 8.04: Chemical Bond Stability
  62. 8.05: Bonding and Antibonding Orbitals
  63. 8.06: A Simple Molecular-Orbital Treatment of H Places Both Electrons in a Bonding Orbital
  64. 8.07: Molecular Orbitals Can Be Ordered According to Their Energies
  65. 8.08: Molecular-Orbital Theory Does not Predict a Stable Diatomic Helium Molecule
  66. 8.09: Electrons Populate Molecular Orbitals According to the Pauli Exclusion Principle
  67. 8.10: SCF-LCAO-MO Wavefunctions are Molecular Orbitals formed from a Linear Combination of Atomic Orbitals and Whose Coefficients Are Determined Self-Consistently
  68. 8.11: Most Molecules Have Excited Electronic States
  69. 8.E: Chemical Bond in Diatomic Molecules (Exercises)
  70. 09: Molecular Spectroscopy
  71. 9.01: The Electromagnetic Spectrum
  72. 9.02: Electronic Spectra Contain Electronic Vibrational and Rotational Information
  73. 9.03: The Franck-Condon Principle
  74. 9.04: What Causes Molecules to Absorb UV and Visible Light
  75. 9.05: Fluorescence and Phosphorescence
  76. 9.06: Jablonski diagram
  77. 9.E: Molecular Spectroscopy (Exercises)
  78. 10: The First Law of Thermodynamics
  79. 10.01: Overview of Classical Thermodynamics
  80. 10.02: All Dilute Gases Behave Ideally
  81. 10.03: van der Waals and Redlich-Kwong Equations of State
  82. 10.04: Pressure-Volume Work
  83. 10.05: Work and Heat are not State Functions
  84. 10.06: Work and Heat Have a Simple Molecular Interpretation
  85. 10.07: Energy is a State Function
  86. 10.08: Heat Capacity is a Path Function
  87. 10.09: An Adiabatic Process is a Process in which No Energy as Heat is Transferred
  88. 10.10: The Temperature of a Gas Decreases in a Reversible Adiabatic Expansion
  89. 10.11: Enthalpy is a State Function
  90. 10.12: Relative Enthalpies Can Be Determined from Heat Capacity Data and Heats of Transition
  91. 10.13: Enthalpy Changes for Chemical Equations are Additive
  92. 10.14: Heats of Reactions Can Be Calculated from Tabulated Heats of Formation
  93. 10.15: The Temperature Dependence of H
  94. 10.E: The First Law of Thermodynamics (Exercises)
  95. 11: Entropy and The Second Law of Thermodynamics
  96. 11.01: Energy Does not Determine Spontaneity
  97. 11.02: Nonequilibrium Isolated Systems Evolve in a Direction That Increases Their Energy Dispersal
  98. 11.03: Unlike heat Entropy is a State Function
  99. 11.04: The Second Law of Thermodynamics
  100. 11.05: The Famous Equation of Statistical Thermodynamics is Sk ln W
  101. 11.06: We Must Always Devise a Reversible Process to Calculate Entropy Changes
  102. 11.07: Thermodynamics Provides Insight into the Conversion of Heat into Work
  103. 11.E: Entropy and The Second Law of Thermodynamics (Exercises)
  104. 12: Helmholtz and Gibbs Energies
  105. 12.01: Helmholtz Energy
  106. 12.02: Gibbs Energy Determines the Direction of Spontaneity at Constant Pressure and Temperature
  107. 12.03: The Maxwell Relations
  108. 12.04: The Enthalpy of an Ideal Gas is Independent of Pressure
  109. 12.05: Thermodynamic Functions have Natural Variables
  110. 12.06: The Standard State for a Gas is an Ideal Gas at 1 Bar
  111. 12.07: The Gibbs-Helmholtz Equation
  112. 12.E: Helmholtz and Gibbs Energies (Exercises)
  113. 13: Chemical Equilibrium
  114. 13.01: Equilibrium Results when Gibbs Energy is Minimized
  115. 13.02: An Equilibrium Constant is a Function of Temperature Only
  116. 13.03: Standard Gibbs Energies of Formation Can Be Used to Calculate Equilibrium Constants
  117. 13.04: Gibbs Energy of a Reaction vs. Extent of Reaction is a Minimum at Equilibrium
  118. 13.05: Reaction Quotient and Equilibrium Constant Ratio Determines Reaction Direction
  119. 13.06: The Sign of G and not G Determines the Direction of Reaction Spontaneity
  120. 13.07: The van 't Hoff Equation
  121. 13.08: Thermodynamic Equilibrium Constants Are Expressed in Terms of Activities
  122. 13.09: Activities are Important for Ionic Species
  123. 13.10: Homework Problems
  124. 14: Solutions I - Volatile Solutes
  125. 14.01: A Mixture is a Combination of Two or More Substances
  126. 14.02: The Gibbs-Duhem Equation Relates Chemical Potential and Composition at Equilibrium
  127. 14.03: Chemical Potential of Each Component Has the Same Value in Each Phase in Which the Component Appears
  128. 14.04: Ideal Solutions obey Raoult's Law
  129. 14.05: Most Solutions are Not Ideal
  130. 14.06: Vapor Pressures of Volatile Binary Solutions
  131. 14.07: Activities of Nonideal Solutions
  132. 14.08: Activities are Calculated with Respect to Standard States
  133. 14.09: Gibbs Energy of Mixing of Binary Solutions in Terms of the Activity Coefficient
  134. 14.E: Solutions I- Liquid-Liquid Solutions (Exercises)
  135. 15: Solutions II - Nonvolatile Solutes
  136. 15.01: Standard State of Nonvolatile Solutions
  137. 15.02: The Activities of Nonvolatile Solutes
  138. 15.03: Colligative Properties Depend only on Number Density
  139. 15.04: Osmotic Pressure can Determine Molecular Masses
  140. 15.05: Electrolytes Solutions are Nonideal at Low Concentrations
  141. 15.06: The Debye-Huckel Theory
  142. 15.07: Extending Debye-Huckel Theory to Higher Concentrations
  143. 15.08: Homework Problems
  144. 16: Chemical Kinetics I - Rate Laws
  145. 16.01: The Time Dependence of a Chemical Reaction is Described by a Rate Law
  146. 16.02: Rate Laws Must Be Determined Experimentally
  147. 16.03: First-Order Reactions Show an Exponential Decay of Reactant Concentration with Time
  148. 16.04: Different Rate Laws Predict Different Kinetics
  149. 16.05: Reactions can also be Reversible
  150. 16.E: Chemical Kinetics I - Rate Laws (Exercises)
  151. 17: Chemical Kinetics II- Reaction Mechanisms
  152. 17.01: A Mechanism is a Sequence of Elementary Reactions
  153. 17.02: The Principle of Detailed Balance
  154. 17.03: Multiple Mechanisms are often Indistinguishable
  155. 17.04: The Steady-State Approximation
  156. 17.05: Rate Laws Do Not Imply Unique Mechanism
  157. 17.06: The Lindemann Mechanism
  158. 17.07: Some Reaction Mechanisms Involve Chain Reactions
  159. 17.08: A Catalyst Affects the Mechanism and Activation Energy
  160. 17.09: The Michaelis-Menten Mechanism for Enzyme Catalysis
  161. 17.E: Chemical Kinetics II- Reaction Mechanisms (Exercises)
  162. 18: Kinetics- Temperature Dependence and Relaxation Methods
  163. 18.01: Rate Constants Are Usually Strongly Temperature Dependent
  164. 18.02: The Rate Constants of a Reversible Reaction Can Be Determined Using Relaxation Techniques
  165. 18.03: Transition-State Theory Can Be Used to Estimate Reaction Rate Constants