Lecture 11b Polyatomic ideal gas

Slides:



Advertisements
Similar presentations
Lecture 27 Electron Gas The model, the partition function and the Fermi function Thermodynamic functions at T = 0 Thermodynamic functions at T > 0.
Advertisements

15.5 Electronic Excitation
The Heat Capacity of a Diatomic Gas
Q18.1 A quantity of an ideal gas is contained in a balloon. Initially the gas temperature is 27°C. You double the pressure on the balloon and change the.
Knight: Chapter 18 The Micro/Macro Connection
Molecular Modeling: Molecular Vibrations C372 Introduction to Cheminformatics II Kelsey Forsythe.
Thermo & Stat Mech - Spring 2006 Class 20 1 Thermodynamics and Statistical Mechanics Heat Capacities.
MSEG 803 Equilibria in Material Systems 10: Heat Capacity of Materials Prof. Juejun (JJ) Hu
Lecture 5 Vibrational Spectra of Simple Molecules.
Thermo & Stat Mech - Spring 2006 Class 19 1 Thermodynamics and Statistical Mechanics Partition Function.
Thermochemistry in Gaussian. The Internal Thermal Energy The internal thermal energy can be obtaine from the partition function, q. The contributions.
Motion near an equilibrium position can be approximated by SHM
Vibrational Transitions
Rotational Spectroscopy Born-Oppenheimer Approximation; Nuclei move on potential defined by solving for electron energy at each set of nuclear coordinates.
Intro/Review of Quantum
15.4 Rotational modes of diatomic molecules The moment of inertia, where μ is the reduced mass r 0 is the equilibrium value of the distance between the.
Partition Functions for Independent Particles
Molecular Information Content
The Helmholtz free energyplays an important role for systems where T, U and V are fixed - F is minimum in equilibrium, when U,V and T are fixed! by using:
Lecture 9 Energy Levels Translations, rotations, harmonic oscillator
Applications of diatomic and polyatomic ideal gases 1.
Diatomic and Polyatomic Gases
The Ideal Monatomic Gas. Canonical ensemble: N, V, T 2.
Lecture 12b Debye Model of Solid  Debye model - phonon density of states  The partition function  Thermodynamic functions  Low and high temperature.
Molecular Partition Function
Chapter 6--Potential Energy of a Spring System Surroundings.
Partition functions of ideal gases. We showed that if the # of available quantum states is >> N The condition is valid when Examples gases at low densities.
IR Spectroscopy Wave length ~ 100 mm to 1 mm
Which of the following refer to the basic categories associated with the energy of a single molecule in a gaseous phase?
Review Of Statistical Mechanics Continued
The Heat Capacity of a Diatomic Gas Chapter Introduction Statistical thermodynamics provides deep insight into the classical description of a.
Quantum Chemistry: Our Agenda Postulates in quantum mechanics (Ch. 3) Schrödinger equation (Ch. 2) Simple examples of V(r) Particle in a box (Ch. 4-5)
The Advanced Chemical Engineering Thermodynamics The first law of thermodynamics Q&A_-4- 10/06/2005(4) Ji-Sheng Chang.
The Ideal Diatomic and Polyatomic Gases. Canonical partition function for ideal diatomic gas Consider a system of N non-interacting identical molecules:
Energy Basics. Part 1: The Relationship Between Matter and Energy 1.Define matter and energy Matter is anything that occupies space and has mass. Energy.
Lecture 26 — Review for Exam II Chapters 5-7, Monday March 17th
Lecture 23: Heat l Internal Energy l Heat l Specific Heat l Latent Heat l Phase Diagrams.
The Kinetic Theory of Gases
What would you predict for the molar heat capacity of N2, based on
MIT Microstructural Evolution in Materials 4: Heat capacity
15.4 Rotational modes of diatomic molecules
Chapter 6 Applications of
Atomic/molecular collisions and pressure
Classical Thermodynamics of Multicomponent Systems
Lecture 25 Goals: Chapter 18
Physical Chemistry IV The Use of Statistical Thermodynamics
- + Thermodynamics Thermo = heat or energy dynamics = movement System
Q18.1 A quantity of an ideal gas is contained in a balloon. Initially the gas temperature is 27°C. You double the pressure on the balloon and change the.
The Kinetic Theory of Gases
Recall the Equipartition
Reminder: Chemical Equilibrium
Einstein Model for the Vibrational Heat Capacity of Solids
Polyatomic Ideal Gases “Borrowed” from various sources on the web!
Lecture 11b Polyatomic ideal gas
Einstein Model of Solid
Recall the Equipartition Theorem: In Ch 6,
Lecture 11b Polyatomic ideal gas
Kinetic Theory of Gases & the Equipartition Theorem
Probability of Finding
Recall the Equipartition
MIT Microstructural Evolution in Materials 4: Heat capacity
Lecture 27 Electron Gas The model, the partition function and the Fermi function Thermodynamic functions at T = 0 Thermodynamic functions at T > 0.
Statistical Thermodynamics
Classical Statistical Mechanics (ONLY!)
Ideal gas: Statistical mechanics
1.3. Equipartition Of Energy Per Molecule And Its Constituent Parts
The Micro/Macro Connection
Lecture 11a Ideal gas Number of states and density of states
Rotational Energy Levels for rigid rotor: Where Rotational Spectra of Rigid Diatomic molecule. BY G JANAKIRAMAN EGS A&S COLLAGE
Vibrational Energy Levels
Presentation transcript:

Lecture 11b Polyatomic ideal gas Model - translation, rotation, vibration Rotational partition function Vibrational partition function - harmonic oscillator Thermodynamic functions Problems

Single polyatomic molecule Translational, rotational, vibrational and electronic energies additive qt - evaluated last lecture qr and qv - will evaluated today Typically with De - binding energy

Translation Consider a single diatomic molecule is the box M =m1+m2

Rotation Rotation energies: Degeneracy r is the rotational temperature

Rotation - continuation Unless temperature is very low: If two atoms are the same we overcounted states by  - symmetry number

Vibrations Vibrations - harmonic oscillator - frequency Near potential minimum With reduced mass

Vibrations - continuation Partition function Vibrational temperature

Partition function Q and free energy F translation rotation vibrations electronic

Energy translation rotation vibrations electronic

Heat capacity Translation rotation vibrations

Chemical potential