
Nguồn ngoài
General Physical Chemistry I
CHEM 351 is an-unit upper-division course titled Physical Chemistry I: Thermodynamics and Kinetics. It focuses on the quantitative interpretation of macroscopic matter, covering chemical thermodynamics, kinetics, and the laws governing energy, enthalpy, entropy, and reaction rates.
- Tác giả
- Nancy Gerber
- Nhà xuất bản
- San Francisco State University
- Nguồn
- LibreTexts
- Ngôn ngữ
- EN
- Danh mục
- Khoa học cơ bản
Mục lục· 148 mục
- 01: The Properties of Gases
- 1.01: Properties of Gas
- 1.02: All Dilute Gases Behave Ideally
- 1.03: van der Waals and Redlich-Kwong Equations of State
- 1.04: A Cubic Equation of State
- 1.05: The Law of Corresponding States
- 1.06: The Second Virial Coefficient
- 1.07: The Repulsive Term in the Lennard-Jones Potential
- 1.08: Van der Waals Constants in Terms of Molecular Parameters
- 1.E: The Properties of Gases (Exercises)
- 02: The Kinetic Theory of Gases
- 2.01: Basics of Kinetic Molecular Theory
- 2.02: Common Ideal Gas Difficulties
- 2.03: Connecting Gas Properties to Kinetic Theory of Gases
- 2.04: Kinetic Molecular Theory of Gases
- 2.05: Real Gases
- 2.06: The Average Translational Kinetic Energy of a Gas
- 2.07: The Gaussian Distribution of One Component of the Molecular Velocity
- 2.08: The Distribution of Molecular Speeds is Given by the Maxwell-Boltzmann Distribution
- 2.09: The Frequency of Collisions with a Wall
- 2.10: The Maxwell-Boltzmann Distribution Has Been Verified Experimentally
- 2.11: Mean Free Path
- 2.12: Rates of Gas-Phase Chemical Reactions
- 2.E: The Kinetic Theory of Gases (Exercises)
- 03: Properties of Liquids
- 3.01: Capillary Action
- 3.02: Cohesive and Adhesive Forces
- 3.03: Contact Angles
- 3.04: Surface Tension
- 3.05: Unusual Properties of Water
- 3.06: Vapor Pressure
- 3.07: Viscosity
- 3.08: Wetting Agents
- 04: The First Law of Thermodynamics
- 4.01: Overview of Classical Thermodynamics
- 4.02: Pressure-Volume Work
- 4.03: Work and Heat are not State Functions
- 4.04: Energy is a State Function
- 4.05: An Adiabatic Process is a Process in which No Energy as Heat is Transferred
- 4.06: The Temperature of a Gas Decreases in a Reversible Adiabatic Expansion
- 4.07: Work and Heat Have a Simple Molecular Interpretation
- 4.08: Pressure-Volume Work
- 4.09: Heat Capacity is a Path Function
- 4.10: Relative Enthalpies Can Be Determined from Heat Capacity Data and Heats of Transition
- 4.11: Enthalpy Changes for Chemical Equations are Additive
- 4.12: Heats of Reactions Can Be Calculated from Tabulated Heats of Formation
- 4.13: The Temperature Dependence of H
- 4.14: Enthalpy is a State Function
- 4.E: The First Law of Thermodynamics (Exercises)
- 05: Entropy and The Second Law of Thermodynamics
- 5.01: Energy Does not Determine Spontaneity
- 5.02: Nonequilibrium Isolated Systems Evolve in a Direction That Increases Their Energy Dispersal
- 5.03: Unlike heat Entropy is a State Function
- 5.04: The Second Law of Thermodynamics
- 5.05: The Famous Equation of Statistical Thermodynamics is Sk ln W
- 5.06: We Must Always Devise a Reversible Process to Calculate Entropy Changes
- 5.07: Thermodynamics Provides Insight into the Conversion of Heat into Work
- 5.08: Entropy Can Be Expressed in Terms of a Partition Function
- 5.09: The Statistical Definition of Entropy is Analogous to the Thermodynamic Definition
- 5.E: Entropy and The Second Law of Thermodynamics (Exercises)
- 06: Entropy and the Third Law of Thermodynamics
- 6.01: Entropy Increases With Increasing Temperature
- 6.02: The 3rd Law of Thermodynamics Puts Entropy on an Absolute Scale
- 6.03: The Entropy of a Phase Transition can be Calculated from the Enthalpy of the Phase Transition
- 6.04: The Debye Function is Used to Calculate the Heat Capacity at Low Temperatures
- 6.05: Practical Absolute Entropies Can Be Determined Calorimetrically
- 6.06: Practical Absolute Entropies of Gases Can Be Calculated from Partition Functions
- 6.07: Standard Entropies Depend Upon Molecular Mass and Structure
- 6.08: Spectroscopic Entropies sometimes disgree with Calorimetric Entropies
- 6.09: Standard Entropies Can Be Used to Calculate Entropy Changes of Chemical Reactions
- 6.E: Entropy and the Third Law of Thermodynamics (Exercises)
- 07: Helmholtz and Gibbs Energies
- 7.01: Helmholtz Energy
- 7.02: Gibbs Energy Determines the Direction of Spontaneity at Constant Pressure and Temperature
- 7.03: The Maxwell Relations
- 7.04: The Enthalpy of an Ideal Gas is Independent of Pressure
- 7.05: Thermodynamic Functions have Natural Variables
- 7.06: The Standard State for a Gas is an Ideal Gas at 1 Bar
- 7.07: The Gibbs-Helmholtz Equation
- 7.08: Fugacity Measures Nonideality of a Gas
- 7.E: Helmholtz and Gibbs Energies (Exercises)
- 08: Phase Equilibria
- 8.01: A Phase Diagram Summarizes the Solid-Liquid-Gas Behavior of a Substance
- 8.02: Gibbs Energies and Phase Diagrams
- 8.03: The Chemical Potentials of a Pure Substance in Two Phases in Equilibrium
- 8.04: The Clausius-Clapeyron Equation
- 8.05: Chemical Potential Can be Evaluated From a Partition Function
- 8.E: Phase Equilibria (Exercises)
- 09: Solutions
- 9.01: Partial Molar Quantities in Solutions
- 9.02: The Gibbs-Duhem Equation
- 9.03: Chemical Potential of Each Component Has the Same Value in Each Phase in Which the Component Appears
- 9.04: Ideal Solutions obey Raoult's Law
- 9.05: Most Solutions are Not Ideal
- 9.06: Vapor Pressures of Volatile Binary Solutions
- 9.07: Activities of Nonideal Solutions
- 9.08: Activities are Calculated with Respect to Standard States
- 9.09: Gibbs Energy of Mixing of Binary Solutions in Terms of the Activity Coefficient
- 9.E: Solutions I- Liquid-Liquid Solutions (Exercises)
- 10: Chemical Equilibrium
- 10.01: Equilibrium Results when Gibbs Energy is Minimized
- 10.02: An Equilibrium Constant is a Function of Temperature Only
- 10.03: Standard Gibbs Energies of Formation Can Be Used to Calculate Equilibrium Constants
- 10.04: Gibbs Energy of a Reaction vs. Extent of Reaction is a Minimum at Equilibrium
- 10.05: Reaction Quotient and Equilibrium Constant Ratio Determines Reaction Direction
- 10.06: The Sign of G and not G Determines the Direction of Reaction Spontaneity
- 10.07: The van 't Hoff Equation
- 10.08: Equilibrium Constants in Terms of Partition Functions
- 10.09: Molecular Partition Functions and Related Thermodynamic Data Are Extensively Tabulated
- 10.10: Real Gases Are Expressed in Terms of Partial Fugacities
- 10.11: Thermodynamic Equilibrium Constants Are Expressed in Terms of Activities
- 10.12: Activities are Important for Ionic Species
- 10.13: Homework Problems
- 11: Chemical Kinetics I - Rate Laws
- 11.01: The Time Dependence of a Chemical Reaction is Described by a Rate Law
- 11.02: Rate Laws Must Be Determined Experimentally
- 11.03: First-Order Reactions Show an Exponential Decay of Reactant Concentration with Time
- 11.04: Different Rate Laws Predict Different Kinetics
- 11.05: Reactions can also be Reversible
- 11.06: The Rate Constants of a Reversible Reaction Can Be Determined Using Relaxation Techniques
- 11.07: Rate Constants Are Usually Strongly Temperature Dependent
- 11.08: Transition-State Theory Can Be Used to Estimate Reaction Rate Constants
- 11.E: Chemical Kinetics I - Rate Laws (Exercises)
- 12: Chemical Kinetics II- Reaction Mechanisms
- 12.01: A Mechanism is a Sequence of Elementary Reactions
- 12.02: The Principle of Detailed Balance
- 12.03: Multiple Mechanisms are often Indistinguishable
- 12.04: The Steady-State Approximation
- 12.05: Rate Laws Do Not Imply Unique Mechanism
- 12.06: The Lindemann Mechanism
- 12.07: Some Reaction Mechanisms Involve Chain Reactions
- 12.08: A Catalyst Affects the Mechanism and Activation Energy
- 12.09: The Michaelis-Menten Mechanism for Enzyme Catalysis
- 12.E: Chemical Kinetics II- Reaction Mechanisms (Exercises)
- 13: Math Chapters
- 13.01: Complex Numbers
- 13.02: Probability and Statistics
- 13.03: Vectors
- 13.04: Spherical Coordinates
- 13.05: Determinants
- 13.06: Matrices
- 13.07: Numerical Methods
- 13.08: Partial Differentiation
- 13.09: Series and Limits
- 13.10: Fourier Analysis
- 13.10.01: Fourier Analysis in Matlab
- 13.10.02: Fourier Synthesis of Periodic Waveforms
- 13.11: The Binomial Distribution and Stirling's Appromixation