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/10.1016/0010-4655(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. Hirschmann et al, ''Three-dimensional free boundary calculations using a spectral Green's function method'', Computer Physics Communications '''43''', 1 (1986) 143-155]</ref> | ||
Revision as of 10:08, 17 August 2009
The three-dimensional Variational Moments Equilibrium Code (VMEC) minimizes the energy functional
over the toroidal domain ωp. The solution is obtained in flux co-ordinates (s, θ, ζ), related to the cylindrical co-ordinates (R, φ, Z) by
The code assumes nested flux surfaces. [1] [2]
Implementations of the code
The code is being used at:
- IPP-Garching, Germany
- NIFS, Japan
- LNF, Spain
Enhancements / extensions of the code
References
- ↑ S.P. Hirschmann et al, Steepest-descent moment method for three-dimensional magnetohydrodynamic equilibria, Phys. Fluids 26 (1983) 3553
- ↑ 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
- ↑ H.J. Gardner, Nucl. Fusion 30 (1990) 1417
- ↑ E. Strumberger, Finite-β magnetic field line tracing for Helias configurations, Nucl. Fusion 37 (1997) 19
- ↑ D.A. Spong et al., Physics issues of compact drift optimized stellarators, Nucl. Fusion 41 (2001) 711