VMEC: Difference between revisions

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The code assumes nested flux surfaces.
The code assumes nested flux surfaces.
<ref>[http://dx.doi.org/10.1063/1.864116 S.P. Hirschmann et al, ''Steepest-descent moment method for three-dimensional magnetohydrodynamic equilibria'',  Phys. Fluids '''26''' (1983) 3553]</ref>
<ref>[http://dx.doi.org/10.1063/1.864116 S.P. Hirschman et al, ''Steepest-descent moment method for three-dimensional magnetohydrodynamic equilibria'',  Phys. Fluids '''26''' (1983) 3553]</ref>
<ref>[http://dx.doi.org/10.1016/0010-4655(86)90058-5 S.P. Hirschmann et al, ''Three-dimensional free boundary calculations using a spectral Green's function method'', Computer Physics Communications '''43''', 1 (1986) 143-155]</ref>
<ref>[http://dx.doi.org/10.1016/0010-4655(86)90058-5 S.P. Hirschman et al, ''Three-dimensional free boundary calculations using a spectral Green's function method'', Computer Physics Communications '''43''', 1 (1986) 143-155]</ref>


== Implementations of the code ==
== Implementations of the code ==

Revision as of 13:16, 3 November 2010

The three-dimensional Variational Moments Equilibrium Code (VMEC) minimizes the energy functional

over the toroidal domain ωp. The solution is obtained in flux coordinates (s, θ, ζ), related to the cylindrical coordinates (R, φ, Z) by

The code assumes nested flux surfaces. [1] [2]

Implementations of the code

The code is being used at:

  • ORNL, Oak Ridge, TN, USA (code origin)
  • PPPL, Princeton, NJ, USA
  • IPP, Garching, Germany
  • CRPP, Lausanne, Switzerland
  • NIFS, Japan
  • LNF, Spain

Enhancements / extensions of the code

  • DIAGNO, [3] to calculate the response of magnetic diagnostics
  • MFBE [4]
  • STELLOPT [5]

References