Microcanonical ensemble: Difference between revisions

From SklogWiki
Jump to navigation Jump to search
mNo edit summary
mNo edit summary
Line 21: Line 21:
*<math> \left( p \right)^{3n} </math> represents the 3N momenta.
*<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> 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]]
*<math> \delta \left( x \right) </math> is the [[Dirac delta distribution]]
Line 31: Line 31:
where:
where:


*<math> \left. S \right. </math> is the [[Entropy|entropy]]·
*<math> \left. S \right. </math> is the [[Entropy|entropy]].


*<math> \left. k_B \right. </math> is the [[Boltzmann constant]]
*<math> \left. k_B \right. </math> is the [[Boltzmann constant]]

Revision as of 10:52, 27 February 2007

Ensemble variables

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

  • N: Number of Particles
  • V: Volume
  • E: Internal energy (kinetic + potential)

Partition function

QNVE=1h3NN!∫∫d(p)3Nd(q)3Nδ(H(p,q)−E).

where:

  • (q)3n represents the 3N Cartesian position coordinates.
  • (p)3n represents the 3N momenta.
  • H(p,q) represent the Hamiltonian, i.e. the total energy of the system as a function of coordinates and momenta.

Thermodynamics

S=kBlogQNVE

where:

References

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