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Bradner, Rev. Sci. Instr. 19, 662 (1948). R. Serber, Phys. Rev. (A), 9. ' 10. Panofsky, C. Richman, F. Oppenheimer, B u l l . Am, Phys. 12. L. C. Slater, Microwave Electronics, Rev. 13. E. M. &Millan, Phys. Rev. 80, 493 (1950). 14. J. P. Blewett, phys. Rev. j 1 150 M. L o - 88, 1197 (1952). - . I -s - * GP/b-l47 (1953). z - 170 Baker, Edwards, Farly, and Kerns, Rev. Sci. I n s t r . 19, 899 (1948). j 18. (1948). Mod. Phys. 18, 441 (1946); Sec. 7. Good, Bull. Am. Phy~. SOC. 27, NO. 6 (1952). 160 L.

90 megavolts per foot,or a t o t a l end t o end voltage of 36 mega... 1 v o l t s (peak value), This d i f f e r s from t h e energy gain (28 Mev) of the p a r t i c l e s due t o the operating phase angle and t r a n s i t time loss. , i f J 9I i kilowatts. 4 t h e s per a duty cycle of 111, t h e average power i s approximately 20 -r operation in Oct 434 tubes, wh talled in Feb er oscillators the correct lectron will e electrons uc such as t o accelerate them back a more electrons. ap again where This proces amount of energy.

Pulses p r drift or 4 sm/cm2 . on t h e * This pulsed force i s sufficient 5 t o loosen the g r i d holders, so s tubes. ( 7 ) Radiation Shielding. The radiation around t h e 1 has been investigated t o determine i ces and energies. almost e n t i r e l y from x-rays produced by electron bodxrdment of ends. These sources were detennined t h e x-rays near the exit end of t r a t o r were found by absorpt F. - measureqents t o be up t o 2 Xev, corresponding t o electrons passing through one i -_ - o r two gaps between Bo.

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