Microcanonical ensemble: Difference between revisions

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*<math> \delta \left( x \right) </math> is the [[Dirac delta distribution|Dirac delta function]]
*<math> \delta \left( x \right) </math> is the [[Dirac delta distribution|Dirac delta function]]
== Thermodynamics ==
: <math> \left. S = k_B \log Q_{NVE} \right. </math>
where:
*<math> \left. S \right. </math> is the [[entropy]]


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

Revision as of 10:30, 27 February 2007

Microcanonical Ensemble (Clasical statistics):

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