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(2cosθ1cosθ2sinθ1sinθ2cosϕ)

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(2cosθ1cosθ2sinθ1sinθ2cosϕ)(σr)3}

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

Critical properties

In the range 0μ*2.45 (Ref. 1)

Tc*=1.313+0.2999μ*20.2837ln(μ*2+1)
ρc*=0.30090.00785μ*20.00198μ*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