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[en] We may identify two main areas where auxiliary heating may be used in breakeven Tokamak reactors. (1) In the start up phase of a Tokamak reactor, having a thermal energy distribution, auxiliary heating is required to bridge the gap between the ohmic state where the temperature will probably be approximately 1 keV, and the ignited condition where T>5 keV. (2) In two component and three component systems, auxiliary power is required to maintain a non-thermal ion distribution. I will follow a similar line to that taken in the above papers and will assess the auxiliary heating requirements of a 'Breakeven Tokamak' producing approximately 500 MW of thermal power, using the D-T cycle. I will consider two and three component systems insofar as they may be used during the start up phase, but not as reactor systems in their own right. In the first lecture I will not discuss details of the heating methods. Symbols and units are given in the Appendix
Source
Knoepfel, H. (ed.); Commission of the European Communities, Luxembourg; p. 511-528; ISBN 0-08-022034-7; 
; 1978; p. 511-528; International school of fusion reactor technology; Erice-Trapani, Italy; 21 Sep - 1 Oct 1976; Published for the CEC by Pergamon Press, Oxford
; 1978; p. 511-528; International school of fusion reactor technology; Erice-Trapani, Italy; 21 Sep - 1 Oct 1976; Published for the CEC by Pergamon Press, Oxford
No abstract available
Source
Stringer, T.; Pozzoli, R.; Sindoni, E.; Carnihan, J.P.; Leotta, G.G. (eds.); Commission of the European Communities, Brussels (Belgium); p. 281; ISBN 0-08-023426-7; ; 1978; p. 281; Workshop on plasma transport, heating and MHD theory; Varenna, Italy; 12 - 16 Sep 1977; Published for the CEC by Pergamon Press; Published in summary form only.
; 1978; p. 281; Workshop on plasma transport, heating and MHD theory; Varenna, Italy; 12 - 16 Sep 1977; Published for the CEC by Pergamon Press; Published in summary form only.
[en] Recent experiments, and scalings deduced from them, have indicated that relatively high density plasmas can be produced and well confined in toroidal configurations capable of sustaining high current densities without inducing macroscopic instabilities. Here we propose to develop a line of compact devices sustaining sufficiently high plasma currents to confine the 3.5 MeV α-particles that are produced in D-T reactions. This line is proposed as a parallel program to the development of large volume Tokamaks which is being undertaken on a worldwide basis
Source
Knoepfel, H. (ed.); Commission of the European Communities, Luxembourg; p. 303-326; ISBN 0-08-022034-7; ; 1978; p. 303-326; International school of fusion reactor technology; Erice-Trapani, Italy; 21 Sep - 1 Oct 1976; Published for the CEC by Pergamon Press, Oxford
; 1978; p. 303-326; International school of fusion reactor technology; Erice-Trapani, Italy; 21 Sep - 1 Oct 1976; Published for the CEC by Pergamon Press, Oxford
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