Atomistic modeling of diffusion coefficient in fusion reactor first wall material tungsten

2014 ◽  
Vol 73 (1) ◽  
pp. 111-115 ◽  
Author(s):  
Zenghui Wang ◽  
Kaixuan Zhao ◽  
Weiming Chen ◽  
Xiaodi Chen ◽  
Longyan Zhang
TANSO ◽  
1991 ◽  
Vol 1991 (150) ◽  
pp. 354-364 ◽  
Author(s):  
Toshiro Yamashina ◽  
Tomoaki Hino

2013 ◽  
Vol 59 (1-2) ◽  
pp. 498-503 ◽  
Author(s):  
Zenghui Wang ◽  
Kaixuan Zhao ◽  
Weiming Chen ◽  
Xiaodi Chen ◽  
Longyan Zhang

2013 ◽  
Vol 364 ◽  
pp. 547-552
Author(s):  
Fan Liu ◽  
Ling Zhang

The first wall material in a nuclear fusion reactor endures a series of complex processes, resulting in irradiation damage of its structural materials and eventually questioning its operative safety. Experimental and computer simulation are currently applied to search for irradiation damage. We used, the Material Studio software to model and calculate the crystal structure and mechanical properties, and the CASTEP module, primitive cell of iron, Fe-Cr alloy and Fe-Cr alloy with defects to calculate, analyze, and obtain the values of elastic constants and Young’s modulus. Our results showed that addition of Cr atom to conventional first wall metal materials of nuclear reactor, enhanced endurance by increasing the values of elastic constant and Young’s modulus, but distorted the symmetry of the crystal structure. We preliminarily prove and predict the possibility of the changes of mechanical properties of Low-activation martensite/ferrite under irradiation effects.


Author(s):  
J. V. Vas ◽  
J. Q. Pan ◽  
N. L. Wang ◽  
J. H. Xu ◽  
R. Medwal ◽  
...  

Author(s):  
E. Ruedl ◽  
P. Schiller

The low Z metal aluminium is a potential matrix material for the first wall in fusion reactors. A drawback in the application of A1 is the rel= atively high amount of He produced in it under fusion reactor conditions. Knowledge about the behaviour of He during irradiation and deformation in Al, especially near the surface, is therefore important.Using the TEM we have studied Al disks of 3 mm diameter and 0.2 mm thickness, which were perforated at the centre by double jet polishing. These disks were bombarded at∽200°C to various doses with α-particles, impinging at any angle and energy up to 1.5 MeV at both surfaces. The details of the irradiations are described in Ref.1. Subsequent observation indicated that in such specimens uniformly distributed He-bubbles are formed near the surface in a layer several μm thick (Fig.1).After bombardment the disks were deformed at 20°C during observation by means of a tensile device in a Philips EM 300 microscope.


1987 ◽  
Vol 12 (1) ◽  
pp. 104-113 ◽  
Author(s):  
K. Taghavi ◽  
M. S. Tillack ◽  
H. Madarame

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