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Reimagining nuclear materials for the future of medicine
Nuclear medicine has come a long way since Henri Becquerel first observed the penetrating energy of radioactive materials in 1896. Today, technetium-99m alone is used in more than 40 million diagnostic procedures every year—from cardiovascular imaging and bone scans to cancer detection—making it the undisputed workhorse of nuclear medicine. That single statistic tells you something important: An enormous portion of modern diagnostic medicine rests on a surprisingly narrow foundation, one built around a small number of aging research reactors that were never originally designed for continuous isotope production.
Keiji Tani, Ryuji Yoshino, Takashi Tuda, Tomonori Takizuka, Masafumi Azumi
Fusion Science and Technology | Volume 21 | Number 2 | March 1992 | Pages 103-113
Technical Paper | Plasma Engineering | doi.org/10.13182/FST92-A29730
Articles are hosted by Taylor and Francis Online.
The technique of ripple injection has been proposed for refueling in tokamak reactors. The usefulness of ripple-assisted fueling has been investigated by using an orbit-following Monte Carlo code. The penetration depth strongly depends on the beam energy. The ripple-enhanced outward flow of ripple-detrapped fast ions is not a serious problem. If Eb/Te0 ≤ 4 is chosen, the fuel efficiency becomes >80%. There is an optimum toroidal angle of the injection beamline to enhance the penetration depth of fast ions, and the range of angles that are effective for fueling is rather wide. The loss of alpha particles incident to the fueling has also been investigated by using the same code. By regulating the shape of the ripple-well region, the total alpha-particle loss can be reduced to <5%. Ripple-assisted fueling in the International Thermonuclear Experimental Reactor (ITER) has also been investigated. Because of the small aspect ratio, the field ripple is strongly decayed in the plasma. Consequently, central fueling presents some difficulties in ITER. However, fueling near one-half of the plasma minor radius is possible with an ∼6% alpha-particle power loss.