Response to “Comment on ‘One-dimensional model of the plasma flow in a Hall thruster’ ” [Phys. Plasmas 10, 1172 (2003)]

2003 ◽  
Vol 10 (4) ◽  
pp. 1174-1174
Author(s):  
E. Ahedo ◽  
M. Martı́nez-Sánchez
Keyword(s):  
Plasma Flow ◽  
Hall Thruster ◽  
Dimensional Model ◽  
One Dimensional

One-dimensional model of the plasma flow in a Hall thruster

2001 ◽  
Vol 8 (6) ◽  
pp. 3058-3068 ◽  
Author(s):  
E. Ahedo ◽  
P. Martı́nez-Cerezo ◽  
M. Martı́nez-Sánchez
Keyword(s):  
Plasma Flow ◽  
Hall Thruster ◽  
Dimensional Model ◽  
One Dimensional

Comment on “One-dimensional model of the plasma flow in a Hall thruster” [Phys. Plasmas 8, 3058 (2001)]

2003 ◽  
Vol 10 (4) ◽  
pp. 1172-1173
Author(s):  
Mrityunjay Kundu ◽  
R. Srinivasan ◽  
S. P. Deshpande
Keyword(s):  
Plasma Flow ◽  
Hall Thruster ◽  
Dimensional Model ◽  
One Dimensional

Modelling Techniques in Applied Glaciology: Numerical Modelling of Avalanches

1983 ◽  
Vol 4 ◽  
pp. 297-297
Author(s):  
G. Brugnot
Keyword(s):  
Finite Difference Method ◽  
Transverse Velocity ◽  
Longitudinal Velocity ◽  
Momentum Conservation ◽  
Dimensional Model ◽  
One Dimensional ◽  
Modelling Techniques ◽  
Reference Grid ◽  
The One ◽  
Near Future

We consider the paper by Brugnot and Pochat (1981), which describes a one-dimensional model applied to a snow avalanche. The main advance made here is the introduction of the second dimension in the runout zone. Indeed, in the channelled course, we still use the one-dimensional model, but, when the avalanche spreads before stopping, we apply a (x, y) grid on the ground and six equations have to be solved: (1) for the avalanche body, one equation for continuity and two equations for momentum conservation, and (2) at the front, one equation for continuity and two equations for momentum conservation. We suppose the front to be a mobile jump, with longitudinal velocity varying more rapidly than transverse velocity.We solve these equations by a finite difference method. This involves many topological problems, due to the actual position of the front, which is defined by its intersection with the reference grid (SI, YJ). In the near future our two directions of research will be testing the code on actual avalanches and improving it by trying to make it cheaper without impairing its accuracy.

Tilting transitions in a one-dimensional model lipid monolayer

1992 ◽  
Vol 25 (10) ◽  
pp. 2889-2896 ◽  
Author(s):  
R D Gianotti ◽  
M J Grimson ◽  
M Silbert
Keyword(s):  
Lipid Monolayer ◽  
Dimensional Model ◽  
One Dimensional

A time-dependent model for high-pressure discharges in narrow ablative capillaries

1993 ◽  
Vol 50 (1) ◽  
pp. 51-70 ◽  
Author(s):  
D. Zoler ◽  
S. Cuperman ◽  
J. Ashkenazy ◽  
M. Caner ◽  
Z. Kaplan
Keyword(s):  
High Pressure ◽  
Equation Of State ◽  
Time Dependent ◽  
Dimensional Model ◽  
Plasma Sources ◽  
One Dimensional ◽  
Space And Time ◽  
Dependent Model ◽  
Energy Equations ◽  
Time Dependent Model

A time-dependent quasi-one-dimensional model is developed for studying high- pressure discharges in ablative capillaries used, for example, as plasma sources in electrothermal launchers. The main features of the model are (i) consideration of ablation effects in each of the continuity, momentum and energy equations; (ii) use of a non-ideal equation of state; and (iii) consideration of space- and time-dependent ionization.

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