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9) (7) and ( 6 ) , 46 with small 3// (Κ, ^ Κ ^ ) , we 1// 2// where we have taken: get: (11) For a linear scussed p r o f i l e , CJp'Cx-) = ^ 5 ^ 4 - ^ y ^ ) , density in / 3 / . A suitable solution Eq. oo) E^^ away from the region is now g i v e n gTTvnc^ is the / electric ^ cJ^ field . B (¿Coj f cJ/ (o,) (Í3) V k i ^ O J of m a g n i t u d e of of the radiated energy flux we a£ sume : L = 10cm, η = 4 χ o f ^= ^ ± = G H z , CJ^ = 60 1 0 ^ ^ cm"'^, Κ. = 2// and we o b t a i n |sx| 10 estimated experimental We remark that in the o r d i n a r y momentum mode; Jn ( C J ^ ) \ = I n(cj¿)|'^l0 -3 η lO^cm"^ watts/cm value in this model conservation.

Fus. Molvig, 1404 /3/. Komm, Int. C o n f . Costley, M . S . Tekula and A . B e r s , P h y s . Rev. L e t t . 38_, (1977) M . N . Rosembluth (1972) and C . S . Liu, P h y s . Rev. 2_9, 701 48 DISCUSSION on paper presented by 8 . RAMPONI et al. BORNATICI Should there n o t be another non-linear the background density city? I mean t h a t , another non-linear and I think, that n^ times source term that t h e second order in the r o t Β equation, term. ^7)· POZZOLI To what e x t e n t does t h i s city distribution?

Brossier, Sixth /2/. Tamor, P h y s i c s and C o n t r . N u c l . Fus. Molvig, 1404 /3/. Komm, Int. C o n f . Costley, M . S . Tekula and A . B e r s , P h y s . Rev. L e t t . 38_, (1977) M . N . Rosembluth (1972) and C . S . Liu, P h y s . Rev. 2_9, 701 48 DISCUSSION on paper presented by 8 . RAMPONI et al. BORNATICI Should there n o t be another non-linear the background density city? I mean t h a t , another non-linear and I think, that n^ times source term that t h e second order in the r o t Β equation, term.

### 301 circuits Practical electronic circuits for the home constructor

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