CHEM2912 Lecture Notes - Lecture 4: Ideal Gas

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CHEM2912
Chemical structure & Stability
Monica Zanuttini !
460381099
Lecture 4 Translational energy levels - Monoatomic gas
These equations assume that many transitional states are occupied (little are in the ground state).
Energy levels: !
As translation is the only possible degree of freedom for an atomic (i.e. monatomic) gas, the
allowed energies are all specified.
To build the ideal gas equation, it is possible to derive it from the particle in a box equation. !
Particle in a 1-Dimensional box: !
Particle in a 3-Dimensional box: !
Total energy of ideal gas system: !
Partition function: !
The molecular partition function is similarly given by a sum over all energy states: !
!
Equilibrium occupation number: !
For mathematical convenience (to make the equation solvable), we replace the sums over discrete
states with a continuous function. However this is only physically reasonable if the number of
occupied states is very large:
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These equations assume that many transitional states are occupied (little are in the ground state). As translation is the only possible degree of freedom for an atomic (i. e. monatomic) gas, the allowed energies are all speci ed. To build the ideal gas equation, it is possible to derive it from the particle in a box equation. The molecular partition function is similarly given by a sum over all energy states: For mathematical convenience (to make the equation solvable), we replace the sums over discrete states with a continuous function. However this is only physically reasonable if the number of occupied states is very large: This is equivalent to saying that the temperature must be much greater than the characteristic temperature for translation, t > trans. This gives an analytical expression for the molecular partition function (energy of gas): Thus, from this we understand that our expression for qtrans is a high temperature approximation.

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