2-D MHD Simulation of a Magnetized Target Fusion Configuration with a Z-Pinch Target Plasma

2005 ◽  
Author(s):  
P.V. Subhash ◽  
V.R. Ikkurthi ◽  
A. Majalee ◽  
S. Chaturvedi
Keyword(s):  
Magnetized Target Fusion ◽  
Mhd Simulation ◽  
Target Plasma ◽  
Z Pinch

3D MHD simulation of wire-array Z-pinch implosion under the action of high current pulse

2014 ◽  
Author(s):  
Vladimir A. Gasilov ◽  
Olga G. Olkhovskaya ◽  
Alexey S. Boldarev ◽  
Gennadiy A. Bagdasarov ◽  
Elizaveta Yu. Dorofeeva ◽  
...  
Keyword(s):  
Current Pulse ◽  
Wire Array ◽  
High Current ◽  
Mhd Simulation ◽  
Z Pinch ◽  
3D Mhd Simulation

MHD simulation of gas embedded Z-pinch

2001 ◽  
Author(s):  
Andrey Esaulov ◽  
Pavel Sasorov ◽  
Leopoldo Soto
Keyword(s):  
Mhd Simulation ◽  
Z Pinch

Target Plasma Formation for Magnetic Compression/Magnetized Target Fusion

1995 ◽  
Vol 75 (10) ◽  
pp. 1953-1956 ◽  
Author(s):  
I. R. Lindemuth ◽  
R. E. Reinovsky ◽  
R. E. Chrien ◽  
J. M. Christian ◽  
C. A. Ekdahl ◽  
...  
Keyword(s):  
Plasma Formation ◽  
Magnetized Target Fusion ◽  
Magnetic Compression ◽  
Target Plasma

scholarly journals Stopping Power and Partial Stopping Power Effective Charge in The Plasma

2020 ◽  
Vol 31 (2) ◽  
pp. 45
Author(s):  
Maryam Yahya Al-Abdallah ◽  
Baida M. Ahmed ◽  
Khalid A. Ahmed
Keyword(s):  
Effective Charge ◽  
Random Phase Approximation ◽  
Random Phase ◽  
Stopping Power ◽  
Target Interaction ◽  
Target Plasma ◽  
Different Temperatures ◽  
Fortran 90 ◽  
Z Pinch ◽  
Projectile Charge

The energy losses of ions moving in an electron gas can be studied through the stopping power of the medium. A large number of calculations of the stopping power of ions and electrons in plasmas have been carried out using the random phase approximation (RPA) in the dielectric formalism, for low and high energies. Then we calculated the partial stopping power effective charge (PSPEC) from the energy loss of an incident proton, Ar-ion, and He-ion in target plasma. The Brandt-Kitagawa (BK) model is used to describe the projectile charge fraction (q) and calculate the stopping power and PSPEC, which depends on temperature and electron density ρ(k) of the plasma. This is a topic of relevance to understanding the beam-target interaction in the contexts of particle driven fusion. The presented study is formulated in terms of classical dielectric functions. The programming language Fortran - 90 was used for a required calculation. In the present work, three systems of plasma (Z-pinch, Tokamak, ICF) for different temperatures and densities were covered. Additionally, a comparison has been done with the previous work of plasma.

MHD simulation of wire ablation and implosion in wire-array Z-pinch

2010 ◽  
Author(s):  
Deok-Kyu Kim ◽  
Jeremy P. Chittenden ◽  
Sergey V. Lebedev ◽  
Alberto Marocchino ◽  
Francisco Suzuki-Vidal
Keyword(s):  
Wire Array ◽  
Mhd Simulation ◽  
Z Pinch
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