scholarly journals IEFIT-an interactive approach to high temperature fusion plasma magnetic equilibrium fitting

Author(s):  
Q. Peng ◽  
J. Schachter ◽  
D.P. Schissel ◽  
L.L. Lao
2005 ◽  
Vol 94 (13) ◽  
Author(s):  
R. Nazikian ◽  
K. Shinohara ◽  
G. J. Kramer ◽  
E. Valeo ◽  
K. Hill ◽  
...  

1998 ◽  
Vol 3 (1) ◽  
pp. 74-80 ◽  
Author(s):  
Olgerts Dumbrajs

Gyrotron is a special tube generating powerful radiowaves in the millimeter wave range. Gyrotrons are mainly used to heat nuclear fusion plasma, in order to induce controlled thermonuclear reactions on earth. In addition, they have found a wide utility in radars and the high‐temperature processing of materials. Differential equations describing gyrotron operation are analyzed from the mathematical point of view. Phase portraits of electron trajectories in realistic resonators are determined.


2006 ◽  
Vol 96 (10) ◽  
Author(s):  
R. Nazikian ◽  
H. L. Berk ◽  
R. V. Budny ◽  
K. H. Burrell ◽  
E. J. Doyle ◽  
...  

2013 ◽  
Vol 64 (2) ◽  
pp. 298-302
Author(s):  
B. Berlinger ◽  
A. Brooks ◽  
H. Feder ◽  
J. Gumbas ◽  
T. Franckowiak ◽  
...  

1979 ◽  
Vol 18 (6) ◽  
pp. 1127-1133 ◽  
Author(s):  
Tohru Matoba ◽  
Tokiyoshi Itagaki ◽  
Toshihiko Yamauchi ◽  
Akimasa Funahashi

1994 ◽  
Vol 2 (3) ◽  
pp. 148-159 ◽  
Author(s):  
Chris M. Bishop ◽  
Paul S. Haynes ◽  
Mike E. U. Smith ◽  
Tom N. Todd ◽  
David L. Trotman

2020 ◽  
Vol 86 (5) ◽  
Author(s):  
A. J. Creely ◽  
M. J. Greenwald ◽  
S. B. Ballinger ◽  
D. Brunner ◽  
J. Canik ◽  
...  

The SPARC tokamak is a critical next step towards commercial fusion energy. SPARC is designed as a high-field ( $B_0 = 12.2$ T), compact ( $R_0 = 1.85$ m, $a = 0.57$ m), superconducting, D-T tokamak with the goal of producing fusion gain $Q>2$ from a magnetically confined fusion plasma for the first time. Currently under design, SPARC will continue the high-field path of the Alcator series of tokamaks, utilizing new magnets based on rare earth barium copper oxide high-temperature superconductors to achieve high performance in a compact device. The goal of $Q>2$ is achievable with conservative physics assumptions ( $H_{98,y2} = 0.7$ ) and, with the nominal assumption of $H_{98,y2} = 1$ , SPARC is projected to attain $Q \approx 11$ and $P_{\textrm {fusion}} \approx 140$ MW. SPARC will therefore constitute a unique platform for burning plasma physics research with high density ( $\langle n_{e} \rangle \approx 3 \times 10^{20}\ \textrm {m}^{-3}$ ), high temperature ( $\langle T_e \rangle \approx 7$ keV) and high power density ( $P_{\textrm {fusion}}/V_{\textrm {plasma}} \approx 7\ \textrm {MW}\,\textrm {m}^{-3}$ ) relevant to fusion power plants. SPARC's place in the path to commercial fusion energy, its parameters and the current status of SPARC design work are presented. This work also describes the basis for global performance projections and summarizes some of the physics analysis that is presented in greater detail in the companion articles of this collection.


Sign in / Sign up

Export Citation Format

Share Document