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EUTERPE: Difference between revisions
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<ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref> | <ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref> | ||
<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref>. Afterwards, the code has been heavily optimized and improved and non-linear dynamics have been included. | <ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref>. Afterwards, the code has been heavily optimized and improved and non-linear dynamics have been included. | ||
The EUTERPE code solves the gyroaveraged Vlasov equa- | |||
tion for the distribution function of ions | |||
<math> | |||
\begin{equation} | |||
\frac{\partial f}{\partial t} + \frac{\rm{d}v_{||}}{\rm{d}t} \frac{\partial f}{\partial v_{||}} + \frac{\rm{d}\vec{R}}{\rm{d}t} \frac{\partial f}{\partial \vec{R}} = 0 | |||
\end{equation} | |||
</math> | |||
==References== | ==References== | ||
<references /> | <references /> | ||