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On the Lagrangian of the linearized MHD equations

Technical Report:

Abstract

Lagrangian for the linearized, ideal and resistive, MHD equations is discussed, by introducing the perturbation of the total pressure. In the resistive MHD equations, the Lagrangian is expressed in terms of the electric displacement vector (time integral of the electric current) as well as the plasma displacement. The NOVA and NOVA-R formulation can be derived by using the obtained Lagrangian. (author).
Authors:
Publication Date:
Jun 01, 1992
Product Type:
Technical Report
Report Number:
NIFS-154
Reference Number:
SCA: 700370; PA: JPN-92:011236; SN: 93000918641
Resource Relation:
Other Information: PBD: Jun 1992
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY; CLOSED PLASMA DEVICES; MHD EQUILIBRIUM; MAGNETIC CONFINEMENT; MAGNETOHYDRODYNAMICS; ANALYTICAL SOLUTION; LAGRANGE EQUATIONS; LAGRANGIAN FUNCTION; 700370; PLASMA FLUID AND MHD PROPERTIES
OSTI ID:
10111306
Research Organizations:
National Inst. for Fusion Science, Nagoya (Japan)
Country of Origin:
Japan
Language:
English
Other Identifying Numbers:
Other: ON: DE93753315; TRN: JP9211236
Availability:
OSTI; NTIS; INIS
Submitting Site:
JPN
Size:
12 p.
Announcement Date:
Jun 30, 2005

Technical Report:

Citation Formats

Todoroki, Jiro. On the Lagrangian of the linearized MHD equations. Japan: N. p., 1992. Web.
Todoroki, Jiro. On the Lagrangian of the linearized MHD equations. Japan.
Todoroki, Jiro. 1992. "On the Lagrangian of the linearized MHD equations." Japan.
@misc{etde_10111306,
title = {On the Lagrangian of the linearized MHD equations}
author = {Todoroki, Jiro}
abstractNote = {Lagrangian for the linearized, ideal and resistive, MHD equations is discussed, by introducing the perturbation of the total pressure. In the resistive MHD equations, the Lagrangian is expressed in terms of the electric displacement vector (time integral of the electric current) as well as the plasma displacement. The NOVA and NOVA-R formulation can be derived by using the obtained Lagrangian. (author).}
place = {Japan}
year = {1992}
month = {Jun}
}