By George L. Ph.D., D.Sc. Clark

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Harrison T (eV) Fig. 5. Power density functions for a pure D-T fusion plasma plotted against plasma temperature T. {Tdl 2 2 n and Pa(Ti)/n are given2 by Eqs. (13) and (14), respectively. Phr(Te)/n is given by Eq. 2 (15) and Pcy(Te)/n is determined from Eq. 9. the p l a s m a t e m p e r a t u r e must be in excess of about 5 keV before energy deposited by ex-particles e x c e e d s that lost by bremsstrahlung radiation. This t e m p e r a t u r e is indicative of ignition conditions for a p u r e D - T p l a s m a but in practice the losses due to p l a s m a transport of energy must also be taken into account.

T h e ablating cloud e x p a n d s with a velocity comparable to the sound speed, and if nondegeneracy is a s s u m e d , cs - {2kTJmy'\ w h e n Te = Tx. T h e transit time of an acoustic w a v e across this pellet is r F / c s 2. Basic Concepts of Fusion Research 47 and so m a y be regarded as equivalent to the fuel confinement time. , Ribe, 1975), r d - r E - rF/4cs. 2 x 1 0 " g for D - T fuel. T h e reactor must be pulsed and the repetition rate is limited by technological constraints of the driving s y s t e m ; —10 H z is typical.

T h e D - T reaction time is a b o u t 1 0 ~ s. 7 M J . S o m e appreciation of the p r o b l e m s of constructing a suitable r e a c t o r vessel can b e gained from the fact that the preceding value of E F is equivalent to the explosion of a b o u t 1 kg of T N T . T w o o t h e r properties of the pellet are w o r t h y of consideration. 5-MeV a-particles should b e less than r F and this is well satisfied 3 3 w h e n p = 10 g c m " . S e c o n d , t h e time feq required for electrons to transfer energy to the ions m u s t be appreciably less than r d .