scholarly journals A polar direct drive liquid deuterium–tritium wetted foam target concept for inertial confinement fusion

2021 ◽  
Vol 28 (12) ◽  
pp. 122704
Author(s):  
R. E. Olson ◽  
M. J. Schmitt ◽  
B. M. Haines ◽  
G. E. Kemp ◽  
C. B. Yeamans ◽  
...  
2003 ◽  
Vol 10 (5) ◽  
pp. 1906-1918 ◽  
Author(s):  
V. N. Goncharov ◽  
J. P. Knauer ◽  
P. W. McKenty ◽  
P. B. Radha ◽  
T. C. Sangster ◽  
...  

2001 ◽  
Vol 8 (5) ◽  
pp. 2257-2267 ◽  
Author(s):  
Michael E. Cuneo ◽  
Roger A. Vesey ◽  
John L. Porter ◽  
Gordon A. Chandler ◽  
David L. Fehl ◽  
...  

2008 ◽  
Vol 100 (18) ◽  
Author(s):  
S. X. Hu ◽  
V. A. Smalyuk ◽  
V. N. Goncharov ◽  
J. P. Knauer ◽  
P. B. Radha ◽  
...  

1990 ◽  
Vol 8 (1-2) ◽  
pp. 3-17 ◽  
Author(s):  
C. Yamanaka

Inertial confinement fusion (ICF) has made great progress. In fact several significant scientific firsts have been achieved in the last year. These developments have presented the ICF community with an opportunity to embark on a new phase in ICF research. The key issues of laser fusion are to attain a high absorption of laser light in a plasma, to prevent preheating of fuel during the compression, and to achieve highly efficient implosion by uniform compression of fuel due to the homogeneous deposition of laser energy on the pellet surface. Direct drive and indirect drive have been investigated. The progress in both schemes is remarkable. The neutron yield by the stagnation free compression of the LHART target has attained 1013 which corresponds to a pellet gain of 1/500. The plastic shell target has reached a fuel density as large as 600 times the liquid density which is measured by the Si activation method as well as the D knockon method. A cryogenic foam target is now under investigation.


2016 ◽  
Vol 34 (3) ◽  
pp. 539-544 ◽  
Author(s):  
V. Brandon ◽  
B. Canaud ◽  
M. Temporal ◽  
R. Ramis

AbstractHot-spot path in the thermodynamic space $({\rm \rho} R,T_{\rm i} )_{{\rm hs}} $ is investigated for direct-drive scaled-target family covering a huge interval of kinetic energy on both sides of kinetic threshold for ignition. Different peak implosion velocities and two initial aspect ratios have been considered. It is shown that hot spot follows almost the same path during deceleration up to stagnation whatever the target is. As attended, after stagnation, a clear distinction is done between non-, marginally-, or fully igniting targets. For the last, ionic temperature can reach very high values when the thermonuclear energy becomes very high.


2005 ◽  
Vol 901 ◽  
Author(s):  
Reny Richard Paguio ◽  
Abbas Nikroo ◽  
Jared F Hund ◽  
Christopher A. Frederick ◽  
Javier Jaquez ◽  
...  

AbstractHollow foam spheres are needed for laser fusion experiments on the OMEGA laser facility at the University of Rochester as part of the demonstration of the feasibility of inertial confinement fusion. Previously polymer based foam and aerogel shells have been produced using resorcinol-formaldehyde (R/F) and divinylbenzene (DVB). In this paper we discuss the development of silica aerogel (SAG) shells. SAG may have the increased robustness, which is important in processing these laser targets. SAG shells were fabricated by the microencapsulation method using a triple orifice droplet generator. This technique allows for precise control of the shell diameter and wall thickness. Reduction of the aerogel gelation time is crucial to fabrication of intact shells with high yield. In addition, the proper choice of the components of the different phases of the microencapsulation process is essential for fabrication of intact SAG shells with proper sphericity and wall uniformity. The density of shells fabricated is approximately 100 mg/cc and the diameter ranges from 700–2000 μm, with a wall thickness of 50–200 μm. Development of a full density permeation barrier for retention of the fusion fuel will also be discussed.


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