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The '''rotational partition function''' relates the rotational degrees of freedom to the rotational part of the energy.
 
== Definition ==
 
The [[Partition function (statistical mechanics)#Partition functions of subsystems|total partition function]] <math>Z</math> of a system of identical particles can be divided into molecular partition functions <math>\zeta</math>. Under the assumption that that all energy levels <math>E_i</math> can be partitioned into its contributions from different degrees of freedom (weakly coupled degrees of freedom)
 
: <math>E_j = \sum_i E_j^i=E_j^{trans}+E_j^{rot}+E_j^{vib}+E_j^{e}</math>
 
and the number of [[Degenerate energy level|degenerate states]] are given as products of the single contributions
 
: <math>g_j =\prod_i g_j^i =g_j^{trans}g_j^{rot}g_j^{vib}g_j^{e},</math>
 
where "trans", "rot", "vib" and "e" denotes translational, rotational and vibrational contributions as well as electron excitation, the molecular partition functions
 
: <math>\zeta=\sum_j g_j e^{-E_j/k_B T}</math>
 
can be written as a product itself
 
: <math>\zeta =\prod_i \zeta^i =\zeta^{trans}\zeta^{rot}\zeta^{vib}\zeta^{e}.</math>
 
[[Rotational energy|Rotational energies]] are quantized. For a [[diatomic molecule]] like CO or HCl, the allowed rotational energies are
 
: <math>E_j^{rot}=\frac{\bold{J}^2}{2I}=\frac{j(j+1)\hbar^2}{2I}=j(j+1)\epsilon.</math>
 
Now <math>g_j</math> for each level <math>j</math> is <math>2j+1</math>, so the rotational partition function is therefore
 
: <math>\zeta^{rot}=\sum_{j=0}^{\infty}g_je^{-E_j/kT}=\sum_{j=0}^{\infty}(2j+1)e^{-j(j+1)\epsilon/kT}.</math>
 
If the difference between energy levels <math>E_j^{rot}</math> is very small compared to <math>k_B T</math>, then the sum can be approximated by an integral and is found to be proportional to the temperature. For more complex polyatomic molecules, the situation is more difficult.
 
For the CO molecule at <math>T=300K</math>, the (unit less) contribution <math>\zeta^{rot}</math> to <math>\zeta</math> turns out to be in the range of <math>10^2</math>.
 
The rotational energy can now be computed by taking the derivative of <math>\zeta^{rot}</math> with respect to temperature <math>T</math>. This can of course also be done by using the [[equipartition theorem]], which says that in an equilibrium the energies of all degrees of freedom are proportional to the temperature.
 
==See also==
* [[Translational partition function]]
* [[Vibrational partition function]]
* [[Partition function (mathematics)]]
 
{{Statistical mechanics topics}}
 
[[Category:Concepts in physics]]
[[Category:Partition functions]]
 
 
{{Physics-stub}}

Latest revision as of 09:59, 29 April 2013

The rotational partition function relates the rotational degrees of freedom to the rotational part of the energy.

Definition

The total partition function Z of a system of identical particles can be divided into molecular partition functions ζ. Under the assumption that that all energy levels Ei can be partitioned into its contributions from different degrees of freedom (weakly coupled degrees of freedom)

Ej=iEji=Ejtrans+Ejrot+Ejvib+Eje

and the number of degenerate states are given as products of the single contributions

gj=igji=gjtransgjrotgjvibgje,

where "trans", "rot", "vib" and "e" denotes translational, rotational and vibrational contributions as well as electron excitation, the molecular partition functions

ζ=jgjeEj/kBT

can be written as a product itself

ζ=iζi=ζtransζrotζvibζe.

Rotational energies are quantized. For a diatomic molecule like CO or HCl, the allowed rotational energies are

Ejrot=𝐉22I=j(j+1)22I=j(j+1)ϵ.

Now gj for each level j is 2j+1, so the rotational partition function is therefore

ζrot=j=0gjeEj/kT=j=0(2j+1)ej(j+1)ϵ/kT.

If the difference between energy levels Ejrot is very small compared to kBT, then the sum can be approximated by an integral and is found to be proportional to the temperature. For more complex polyatomic molecules, the situation is more difficult.

For the CO molecule at T=300K, the (unit less) contribution ζrot to ζ turns out to be in the range of 102.

The rotational energy can now be computed by taking the derivative of ζrot with respect to temperature T. This can of course also be done by using the equipartition theorem, which says that in an equilibrium the energies of all degrees of freedom are proportional to the temperature.

See also

Template:Statistical mechanics topics


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