Journal of Microwave Power
and Electromagnetic Energy (JMPEE) |
|
TITLE |
The Canadian Intense
Neutron Generator [PDF] |
AUTHORS |
P.R. Tunnicliffe 1967 2 3 67-74 |
YEAR |
|
VOLUME |
|
ISSUE |
|
PAGES |
|
Abstract Atomic Energy of Canada Ltd.
has proposed construction of an Intense Neutron-Generator. The generator
would produce uniquely-intense beams of thermal neutrons for solid-state and
low-energy nuclear studies and would yield significant quantities of
radioisotopes of both research and commercial value; it would also produce
copious sources of mesons and energetic nucleons for use in
intermediate-energy nuclear physics and in nuclear- structure studies. The
primary neutron source of 1019/sec would be generated by
bombarding a heavy-element target with a continuous beam of 65 mA of I GeV
protons. The target of circulating and cooled Pb-Bi eutectic would be
surrounded by a tank of heavy water moderator yielding a maximum useful flux
of 1016 thermal neutrons/cm2/sec in the region where neutron
beams can be extracted. This high-energy
spallation process for producing neutrons is nearly four times more efficient
in producing neutrons per unit of thermal energy released in the neutron
source compared with a fission reactor. Nevertheless, if energy costs for
producing the 65 MW proton beam are to be within reason, the machine
producing the beam must be efficient. A O.X, machine is in
principle ideal but practical achievement of I GV is not likely within the
time desired. An accelerator where the protons gain energy from
radio-frequency fields is the most likely prospect. We have selected a linear
accelerator as our reference design and detailed theoretical and experimental
studies are in progress. The machine is based on the Los Alamos Meson Physics
Facility design reoptimized for continuous rather than pulsed operation. It
is approximately one mile long and is expected to achieve nearly 50 percent
overall efficiency. There are two major
portions, an 'Alvarez' section operating at 200 MHz accelerating the beam to
about 150 MeV, followed by a 'Waveguide' section operating at 800 MHz.
Protons are initially injected by an 0.75 MV D.C. accelerator. The Alvarez section
consists of thirteen resonant high-Q tanks each requiring a 1.5 MW R.F. power
supply; the 308 waveguide resonators are fed in pairs through a power divider
from 0.5 MW R,F, units. The total R.F. power required is in excess of 90 MW
C.W. Each R.F. unit is an amplifier fed from a common drive line; outputs
have to be controlled to keep relative phase and absolute amplitude of the
accelerator R.F. fields to within -1° and 1 percent respectively over a
loading range of -5:1. Efficiency of R.F. generation is primarily determined
by the final power-amplifier stage. While efficiency is a dominant
requirement (80 percent A.C. to R.F. conversion is our objective), the
amplifier must be capable of operating into a very narrowband load over a
wide range of output with satisfactory control characteristics. It must
moreover be reliable as indeed the whole amplifier chain must be. A crossed-field reentrant
electron-beam device seems most suitable for the purpose and we have begun an
experimental study of a possible 800 MHz tube. Pending review of the design
frequencies we have chosen to study a superpower triode for the 200 MHz
generator; it will enable us to gain experience with gridded tubes and give
power for testing experimental accelerator structures. |