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Lecture 11b Polyatomic ideal gas

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Presentation on theme: "Lecture 11b Polyatomic ideal gas"— Presentation transcript:

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

2 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

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

4 Rotation Rotation energies: Degeneracy
r is the rotational temperature

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

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

7 Vibrations - continuation
Partition function Vibrational temperature

8 Ideal Gases Molecular Energies
The schematic below gives an indication of the relative spacing between energy levels for the various energies electronic vibrational rotational translational

9 Characteristic Temperatures
Characteristic temperature of vibration of diatomic molecules Substance θvib(K) H O N HCl CO NO Cl Characteristic temperature of rotation of diatomic molecules Substance θrot(K) H O N HCl CO NO Cl

10 Partition function Q and free energy F
translation rotation vibrations electronic

11 Energy translation rotation vibrations electronic

12 For a diatomic molecule system
Discussing the relationship of T and Cv

13 Heat capacity Translation rotation vibrations

14 Heat capacity for diatomic molecules

15 Chemical potential


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