Generation of net electric power with a tokamak reactor under foreseeable physical and engineering conditions

被引:8
作者
Hiwatari, R [1 ]
Asaoka, Y [1 ]
Okano, K [1 ]
Yoshida, T [1 ]
Tomabechi, K [1 ]
机构
[1] Cent Res Inst Elect Power Ind, Komae Res Lab, Komae, Tokyo 2018511, Japan
关键词
D O I
10.1088/0029-5515/44/1/013
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
This study reveals for the first time the plasma performance required for a tokamak reactor to generate net electric power under foreseeable engineering conditions. It was found that the reference plasma performance of the ITER inductive operation mode with beta(N) = 1.8, HH = 1.0, and fn(GW) = 0.85 had sufficient potential to achieve the electric break-even condition (net electric power P-e(net) = 0 MW) under the following engineering conditions: machine major radius 6.5 m less than or equal to R-p less than or equal to 8.5 m, the maximum magnetic field on TF coils B-tmax = 16 T, thermal efficiency eta(e) = 30%, and NBI system efficiency eta(NBI) = 50%. The key parameters used in demonstrating net electric power generation in tokamak reactors are beta(N) and fn(GW). beta(N) greater than or equal to 3.0 is required for P-e(net) similar to 600 MW with fusion power P-f similar to 3000 MW. On the other hand, fn(GW) greater than or equal to 1.0 is inevitable to demonstrate net electric power generation, if high temperatures, such as average temperatures of T-ave > 16 keV, cannot be selected for the reactor design. To apply these results to the design of a tokamak reactor for demonstrating net electric power generation, the plasma performance diagrams on the Q vs P-f (energy multiplication factor vs fusion power) space for several major radii (i.e. 6.5, 7.5, and 8.5 m) were depicted. From these figures, we see that a design with a major radius R-p similar to 7.5 m seems preferable for demonstrating net electric power generation when one aims at early realization of fusion energy.
引用
收藏
页码:106 / 116
页数:11
相关论文
共 28 条
[21]  
Takase Y., 2002, J PLASMA FUSION RES, V78, P719, DOI [10.1585/jspf.78.719, DOI 10.1585/JSPF.78.719]
[22]   Studies of breakeven prices and electricity supply potentials of nuclear fusion by a long-term world energy and environment model [J].
Tokimatsu, K ;
Asaoka, Y ;
Konishi, S ;
Fujino, J ;
Ogawa, Y ;
Okano, K ;
Nishio, S ;
Yoshida, T ;
Hiwatari, R ;
Yamaji, K .
NUCLEAR FUSION, 2002, 42 (11) :1289-1298
[23]  
TOKIMATSU K, 2000, P 18 IAEA FUS EN C S
[24]   MHD-LIMITS TO PLASMA-CONFINEMENT [J].
TROYON, F ;
GRUBER, R ;
SAURENMANN, H ;
SEMENZATO, S ;
SUCCI, S .
PLASMA PHYSICS AND CONTROLLED FUSION, 1984, 26 (01) :209-215
[25]  
UCKAN N, 1989, ITER DOCUMENTATION S, V10
[26]  
Wakatani M, 1999, NUCL FUSION, V39, P2175, DOI 10.1088/0029-5515/39/12/302
[27]  
*WORK GROUP 3, 2001, CLIM CHANG 2001 MIT, P25
[28]  
YOSHIDA T, 1994, T94001 CRIEPI