Microcanonical ensemble: Difference between revisions

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m (New page: Microcanonical Ensemble (Clasical statistics): Ensemble variables (One component system, 3-dimensional system, ... ): * <math> \left. N \right. </math>: Number of Particles * <math> \le...)
 
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Microcanonical Ensemble (Clasical statistics):
Microcanonical Ensemble (Clasical statistics):


Ensemble variables (One component system, 3-dimensional system, ... ):
== Ensemble variables ==
(One component system, 3-dimensional system, ... ):


* <math> \left. N \right. </math>: Number of Particles
* <math> \left. N \right. </math>: Number of Particles
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* <math> \left. E \right. </math>: Internal enerrgy (kinetic + potential)
* <math> \left. E \right. </math>: Internal enerrgy (kinetic + potential)


Partition function
== Partition function ==


<math> Q_{NVE} = \frac{1}{h^{3N} N!} \int \int d  (p)^{3N} d(q)^{3N} \delta ( H(p,q) - E).
<math> Q_{NVE} = \frac{1}{h^{3N} N!} \int \int d  (p)^{3N} d(q)^{3N} \delta ( H(p,q) - E).
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where:
where:


*<math>  \left. h \right. </math> is   
*<math>  \left. h \right. </math> is  the [[Planck constant]]


*<math> \left( q \right)^{3n} </math> represents the 3N Cartesian position coordinates.


... in construction ---
*<math> \left( p \right)^{3n} </math> represents the 3N momenta.
 
* <math> H \left(p,q\right) </math> represent the Hamiltonian, i.e. the total energy of the system as a function of coordinates and momenta.
 
*<math> \delta \left( x \right) </math> is the [[Dirac delta distribution|Dirac delta function]]
 
== References ==
# D. Frenkel and B. Smit, "Understanding Molecular Simulation: From Alogrithms to Applications", Academic Press

Revision as of 12:25, 27 February 2007

Microcanonical Ensemble (Clasical statistics):

Ensemble variables

(One component system, 3-dimensional system, ... ):

  • : Number of Particles
  • : Volumne
  • : Internal enerrgy (kinetic + potential)

Partition function

where:

  • represents the 3N Cartesian position coordinates.
  • represents the 3N momenta.
  • represent the Hamiltonian, i.e. the total energy of the system as a function of coordinates and momenta.

References

  1. D. Frenkel and B. Smit, "Understanding Molecular Simulation: From Alogrithms to Applications", Academic Press