Selection of a toroidal fusion reactor concept for a magnetic fusion production reactor

1987 ◽  
Vol 6 (1) ◽  
pp. 65-88 ◽  
Author(s):  
D. L. Jassby
1977 ◽  
Vol 55 (12) ◽  
pp. 1047-1054 ◽  
Author(s):  
Boye Ahlborn

The particle end losses from a linear magnetic fusion reactor can be suppressed by establishing an ablation front in a cold gas blanket. The power density W(W/cm2) to drive the thermal front may be drawn from inside (energy end losses) or outside (auxiliary heating). With W below 109 W/cm2 and a D–T blanket the particle outflow is retarded. With higher W values the flow is completely stopped and the fusion plasma is recompressed by a shock wave traveling inwards from the ends.


1985 ◽  
Vol 4 (2-3) ◽  
pp. 187-197 ◽  
Author(s):  
John Sheffield

Sign in / Sign up

Export Citation Format

Share Document