Coronal radiative losses

From formulasearchengine
Revision as of 02:15, 19 October 2013 by en>Myasuda (→Optically-thin plasma emission: sp)
Jump to navigation Jump to search

The Stockmayer potential is a mathematical model for representing the interactions between pairs of atoms or molecules. It consists of the Lennard-Jones potential with an embedded point dipole. Thus the Stockmayer potential becomes:

Φ12(r,θ1,θ2,ϕ)=4ϵ[(σr)12−(σr)6]−μ1μ24πϵ0r3(2cos⁡θ1cos⁡θ2−sin⁡θ1sin⁡θ2cos⁡ϕ)

where:

If one defines the reduced dipole moment, μ∗

μ∗:=μ24πϵ0ϵσ3

one can rewrite the expression as

Φ(r,θ1,θ2,ϕ)=ϵ{4[(σr)12−(σr)6]−μ∗2(2cos⁡θ1cos⁡θ2−sin⁡θ1sin⁡θ2cos⁡ϕ)(σr)3}

For this reason the potential is sometimes known as the Stockmayer 12-6-3 potential.

Critical properties

In the range 0≤μ∗≤2.45 (Ref. 1)

Tc∗=1.313+0.2999μ∗2−0.2837ln⁡(μ∗2+1)
ρc∗=0.3009−0.00785μ∗2−0.00198μ∗4
Pc∗=0.127+0.0023μ∗2

References

  1. M. E. Van Leeuwe "Deviation from corresponding-states behaviour for polar fluids", Molecular Physics 82 pp. 383-392 (1994)
  2. Reinhard Hentschke, Jörg Bartke, and Florian Pesth "Equilibrium polymerization and gas-liquid critical behavior in the Stockmayer fluid", Physical Review E 75 011506 (2007)
Attribution

Template:CCBYSASource