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The d r i f t tube body is made of a copper tube, with the end a t t h e beam e x i t made from a copper p l a t e hard soldered i n t o the tube, and with B threaded ring $ 8 i n the opposite end. Into t h i s threaded r i n g i s screwed a cap, which i n t u r n receives a grid holder, The e x i t end of the d r i f t tube has a re-entrant opening, formed by a brass t a i l tube about 3 inches in length, and varying i m i d e diameter t o 1-1/2 sizes, inches inside diameter, f o r t h e range of a A l l external edges a r e uniformly rounded with a radius of 3 threaded cap was o r i g i n a l l y designe e screwed i n t o t h e d r i f t a f t e r the grid holder had been inse rom the inside.

30 d i f f e r s from a simple l i n e of i d e n t i c a l sections esign of i t s leading section. 4 ,*,I ion) the voltage on discharge would r i s e t o 2V, r e s u l t t. j portion of the appro of the charging interval. wave. As T+ soid, symmetrica . - _ e 1 e charging cycle approa The principal a d v k t a g e 0 f . a large value of J - c is fluctuation reflected i n t h e power line. d the large magnetic energy storage reactor. the l i n e i n case * - L overload protection is thus needed Table 11 presents the r e l e formation of int system design.

Ate that the accelerator a -L The pulse length (600 p set% maximum) is a compromise between cavity build-up time and available energy stor As h2gh 1.. duty as i s permissibl I - considerations is d point of view o f minimizing accidental coincidences in coincide - experiments For the parameters involved here,energy storage in rotating machinery is not practical. Accordingly, the system adopted is a pulse f o transmission line continuously f the power supply 6481 . 4 0 -L total Revised 42 = To f u l f i l l these s p e c i f i c a t i o standard three-phase mercury vapor r e c t through a reactor.

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Berkeley Proton Linear Accelerator


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