Semi-grand ensembles: Difference between revisions

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(New page: == General Features == Semi-grand ensembles are used in Monte Carlo simulation of mixtures. In this ensembles the total number of molecules is fixed, but the composition can change. == F...)
 
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In this ensembles the total number of molecules is fixed, but the composition can change.
In this ensembles the total number of molecules is fixed, but the composition can change.


== Fixed Volume and Temperature ==
== Canonical Ensemble: fixed volume, temperature and number(s) of molecules ==


We will consider a binary system; The [[Helmhotz energy function]]
We will consider a binary system;.
In the Canonical Ensemble, the differential
equation energy for the [[Helmholtz energy function]] can be written as:
 
: <math> d \left( \beta A \right) = E d \beta - (\beta p) d V + \sum_{i=1}^2 (\beta \mu_i) d N_i </math>,
where:
 
*<math> A </math> is the [[Helmholtz energy function]]
*<math> \beta \equiv 1/k_B T </math>
*<math> k_B</math> is the [[Boltzmann constant]]
*<math> T </math> is the absolute temperature
*<math> E </math> is the internal energy
*<math>  p </math> is the pressure
*<math> \mu_i </math> is the chemical potential of the species "i"
*<math> N_i </math> is the number of molecules of the species "i"
 
== Semi-grand ensemble at fixed volume and temperature ==

Revision as of 14:00, 5 March 2007

General Features

Semi-grand ensembles are used in Monte Carlo simulation of mixtures.

In this ensembles the total number of molecules is fixed, but the composition can change.

Canonical Ensemble: fixed volume, temperature and number(s) of molecules

We will consider a binary system;. In the Canonical Ensemble, the differential equation energy for the Helmholtz energy function can be written as:

,

where:

  • is the Helmholtz energy function
  • is the Boltzmann constant
  • is the absolute temperature
  • is the internal energy
  • is the pressure
  • is the chemical potential of the species "i"
  • is the number of molecules of the species "i"

Semi-grand ensemble at fixed volume and temperature