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).
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}
}
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}
}