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Abstract

A variational principle for two-fluid plasmas is obtained by using Clebsch variables. A Hamiltonian formalism is derived and canonical Poisson brackets are defined.

Additional information

Authors: CALDAS I L, MAX-PLANCK-INSTITUTE FUER PLASMAPHYSIK, GARCHING BEI MUENCHEN (GERMANY);TASSO H MAX-PLANCK-INSTITUTE FUER PLASMAPHYSIK, GARCHING BEI MUENCHEN (GERMANY), MAX-PLANCK-INSTITUTE FUER PLASMAPHYSIK, GARCHING BEI MUENCHEN (GERMANY)
Bibliographic Reference: WRITE TO MAX-PLANCK-INSTITUT FUER PLASMAPHYSIK, 8046 GARCHING BEI MUENCHEN (GERMANY), MENTIONING REPORT IPP 6/227, 1983
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