Grand canonical ensemble: Difference between revisions
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* Temperature, <math> \left. T \right. </math> | * Temperature, <math> \left. T \right. </math> | ||
== | == 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: | ||
| Line 16: | Line 16: | ||
where: | where: | ||
* | * ''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.}