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{{Expert-subject|Physics|date=February 2008}}
 
The '''excess chemical potential''' is defined as the difference between the [[chemical potential]] of a given species and that of an [[ideal gas]] under the same conditions (in particular, at the same [[pressure]], [[temperature]], and [[wikt:composition|composition]]).<ref>{{cite book | last = Frenkel | first = Daan | authorlink = Daan Frenkel | coauthors = Smit, Berend | title = Understanding Molecular Simulation : from algorithms to applications | publisher = [[Academic Press]] | year = 2001 | location = [[San Diego, California]] | pages = | url = | doi = | id = | isbn = 0-12-267351-4 }}</ref>
 
Chemical potential of pure fluid can be estimated by the [[Widom insertion method]].
 
For a system of diameter <math>L</math> and volume <math>V</math>, at constant temperature :<math>T</math>, the classical [[partition function (statistical mechanics)|partition function]]  <math>Q(N,V,T)=\frac{V^{N}}{\Lambda^{dN}N!}\int_{0}^{1}\ldots\int_{0}^{1}ds^{N}\exp[-\beta U(s^{N};L)]</math>
s is a scaled coordinate.
 
:<math>F(N,V,T)= -k_{B}T\ln Q=-k_{B}T\ln\left(\frac{V^{N}}{\Lambda^{dN}N!}\right)-k_{B}T \ln{\int ds^{N}\exp[-\beta U(s^{N};L)]}=</math>
::<math>\;=F_{id}(N,V,T)+F_{ex}(N,V,T)</math>
 
combining the above equation with the definition of chemical potential:  <math>\mu_{a}= \left(\frac{\partial G}{\partial N_{a}}\right)_{PTN}</math>
 
we get the chemical potential of a sufficient large system is :
 
:<math>\mu= -k_{B}T\ln(Q_{N+1}/Q_{N})=-k_{B}T\ln\left(\frac{V/\Lambda^{d}}{N+1}\right) - k_{B}T \ln{\frac{\int ds^{N+1}\exp[-\beta U(s^{N+1})]}{\int ds^{N}\exp[-\beta U(s^{N})]}}=\mu_{id}(\rho) + \mu_{ex}</math>
 
wherein the chemical potential of ideal gas can be evaluated analytically.  
Now let's focus on <math>\mu_{ex}</math>, since the potential energy of an N+1 particle system can be separated into the potential energy of an N [[particle system]] and the potential of the excess particle interacts with the N particle system, there is
 
:<math>\Delta U\equiv U(s^{N+1}) - U(s^{N})</math>
 
and  
 
:<math>\mu_{ex}= -k_{B}T \ln \int ds_{N+1} \langle \exp(-\beta\Delta U)\rangle_{N}</math>
 
thus far we converted the excess chemical potential into an ensemble average, and the integral in the above equation can be sampled by brute force [[Monte Carlo method]].
 
The calculating of excess chemical potential is not only limited to homogeneous system, it has also been extended to inhomogeneous system by [[Widom insertion method]], or other [[Statistical ensemble (mathematical physics)|ensembles]] such as NPT, [[Microcanonical ensemble|NVE]].
 
==See also==
[[Apparent molar property]]
 
==References==
* Note: the equations and presentation in this article are drawn from [http://www.pages.drexel.edu/~cfa22/msim/node39.html Excess Chemical Potential via the Widom Method]<!-- not a copyright violation--see talk page and [[Wikipedia talk:Copyright problems#Copyright violations in Excess chemical potential]] -->
{{Reflist}}
 
{{DEFAULTSORT:Excess Chemical Potential}}
[[Category:Potentials]]
[[Category:Thermodynamics]]
[[Category:Chemical thermodynamics]]
 
[[ro:Mărimi molare de exces]]

Revision as of 09:06, 15 December 2013

Template:Expert-subject

The excess chemical potential is defined as the difference between the chemical potential of a given species and that of an ideal gas under the same conditions (in particular, at the same pressure, temperature, and composition).[1]

Chemical potential of pure fluid can be estimated by the Widom insertion method.

For a system of diameter L and volume V, at constant temperature :T, the classical partition function Q(N,V,T)=VNΛdNN!0101dsNexp[βU(sN;L)] s is a scaled coordinate.

F(N,V,T)=kBTlnQ=kBTln(VNΛdNN!)kBTlndsNexp[βU(sN;L)]=
=Fid(N,V,T)+Fex(N,V,T)

combining the above equation with the definition of chemical potential: μa=(GNa)PTN

we get the chemical potential of a sufficient large system is :

μ=kBTln(QN+1/QN)=kBTln(V/ΛdN+1)kBTlndsN+1exp[βU(sN+1)]dsNexp[βU(sN)]=μid(ρ)+μex

wherein the chemical potential of ideal gas can be evaluated analytically. Now let's focus on μex, since the potential energy of an N+1 particle system can be separated into the potential energy of an N particle system and the potential of the excess particle interacts with the N particle system, there is

ΔUU(sN+1)U(sN)

and

μex=kBTlndsN+1exp(βΔU)N

thus far we converted the excess chemical potential into an ensemble average, and the integral in the above equation can be sampled by brute force Monte Carlo method.

The calculating of excess chemical potential is not only limited to homogeneous system, it has also been extended to inhomogeneous system by Widom insertion method, or other ensembles such as NPT, NVE.

See also

Apparent molar property

References

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