Conceptual Design of a Plasma Exhaust and Fuel Recovery System for an Inertial Fusion Energy (IFE) Power Reactor

Author(s):  
C.A. Gentile ◽  
S.W. Langish ◽  
T. Kozub ◽  
C. Priniski ◽  
T. Dodson ◽  
...  
2008 ◽  
Vol 54 (2) ◽  
pp. 371-374
Author(s):  
C. A. Gentile ◽  
T. Kozub ◽  
S. W. Langish ◽  
L. P. Ciebiera ◽  
A. Nobile ◽  
...  

1999 ◽  
Vol 44 (1-4) ◽  
pp. 401-405 ◽  
Author(s):  
H. Matsui ◽  
T. Eguchi ◽  
T. Kanabe ◽  
M. Yamanaka ◽  
M. Nakatsuka ◽  
...  

2000 ◽  
Vol 28 (3) ◽  
pp. 176-181 ◽  
Author(s):  
Hiroki MATSUI ◽  
Takeyoshi EGUCHI ◽  
Tadashi KANABE ◽  
Masanobu YAMANAKA ◽  
Masahiro NAKATSUKA ◽  
...  

2008 ◽  
Vol 26 (4) ◽  
pp. 517-523 ◽  
Author(s):  
D. Chatain ◽  
J.P. Périn ◽  
P. Bonnay ◽  
E. Bouleau ◽  
M. Chichoux ◽  
...  

AbstractThe Low Temperatures Laboratory of CEA/Grenoble (France) is involved in the development of cryogenic systems for inertial fusion since a ten of years. A conceptual design for the cryogenic infrastructure of the Laser MegaJoule (LMJ) facility has been proposed. Several prototypes have been designed, built and tested like for example the 1500 bars cryo compressor for the targets filling, the target positioner and the thermal shroud remover.The HIPER project will necessitate the development of such equipments. The main difference is that this time, the cryogenic targets are direct drive targets. The first phase of HIPER experiments is a single shot period. Based on the experience gained the last years, not only by our laboratory but also by Omega and G.A teams, we could design the new HIPER equipments for this phase.Some experimental results obtained with the prototypes of the LMJ cryogenic system are given and a first conceptual design for the HIPER single shot cryogenic system is shown.


2003 ◽  
Vol 43 (2) ◽  
pp. 230-249 ◽  
Author(s):  
Sebahattin Ünalan ◽  
S. Orhan Akansu ◽  
Hanifi Saraç

2004 ◽  
Vol 22 (4) ◽  
pp. 469-477 ◽  
Author(s):  
XING ZHONG LI ◽  
BIN LIU ◽  
SI CHEN ◽  
QING MING WEI ◽  
HEINRICH HORA

The application of selective resonant tunneling model is extended from d + t fusion to other light nucleus fusion reactions, such as d + d fusion and d + 3He. In contrast to traditional formulas, the new formula for the cross-section needs only a few parameters to fit the experimental data in the energy range of interest. The features of the astrophysical S-function are derived in terms of this model. The physics of resonant tunneling is discussed.


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