Grand canonical ensemble: Difference between revisions

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* Temperature, <math> \left. T \right. </math>
* Temperature, <math> \left. T \right. </math>


== Partition Function ==
== Grand canonical partition function ==
The classical grand canonical partition function for a one-component system in a three-dimensional space is given by:  
The classical grand canonical partition function for a one-component system in a three-dimensional space is given by:  


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where:
where:


*<math> \left. N \right. </math> is the number of particles
* ''N'' is the number of particles


* <math> \left. \Lambda \right. </math> is the [[de Broglie thermal wavelength]] (which depends on the temperature)
* <math> \left. \Lambda \right. </math> is the [[de Broglie thermal wavelength]] (which depends on the temperature)

Revision as of 16:33, 26 June 2007

The grand-canonical ensemble is particularly well suited to simulation studies of adsorption.

Ensemble variables

  • Volume,
  • Temperature, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \left.T\right.}

Grand canonical partition function

The classical grand canonical partition function for a one-component system in a three-dimensional space is given by:

where:

  • N is the number of particles
  • Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \left.\Lambda \right.} is the de Broglie thermal wavelength (which depends on the temperature)
  • , with being the Boltzmann constant
  • U is the potential energy, which depends on the coordinates of the particles (and on the interaction model)
  • Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \left(R^{*}\right)^{3N}} represent the Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle 3N} position coordinates of the particles (reduced with the system size): i.e. Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int d(R^{*})^{3N}=1}

Helmholtz energy and partition function

The corresponding thermodynamic potential, the grand potential, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \Omega } , for the aforementioned grand canonical partition function is:

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \Omega =\left.A-\mu N\right.} ,

where A is the Helmholtz energy function. Using the relation

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \left.U\right.=TS-PV+\mu N}

one arrives at

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \left.\Omega \right.=-PV}

i.e.:

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \left.pV=k_{B}T\log Q_{\mu VT}\right.}