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High-temperature plumbing and advanced reactors
The use of nuclear fission power and its role in impacting climate change is hotly debated. Fission advocates argue that short-term solutions would involve the rapid deployment of Gen III+ nuclear reactors, like Vogtle-3 and -4, while long-term climate change impact would rely on the creation and implementation of Gen IV reactors, “inherently safe” reactors that use passive laws of physics and chemistry rather than active controls such as valves and pumps to operate safely. While Gen IV reactors vary in many ways, one thing unites nearly all of them: the use of exotic, high-temperature coolants. These fluids, like molten salts and liquid metals, can enable reactor engineers to design much safer nuclear reactors—ultimately because the boiling point of each fluid is extremely high. Fluids that remain liquid over large temperature ranges can provide good heat transfer through many demanding conditions, all with minimal pressurization. Although the most apparent use for these fluids is advanced fission power, they have the potential to be applied to other power generation sources such as fusion, thermal storage, solar, or high-temperature process heat.1–3
M. Glugla, R.D. Penzhorn, J.L. Anderson, J.R. Bartlit
Fusion Science and Technology | Volume 14 | Number 2 | September 1988 | Pages 683-688
Tritium Properties and Interactions with Material | Proceedings of the Third Topical Meeting on Tritium Technology in Fission, Fusion and Isotopic Applications (Toronto, Ontario, Canada, May 1-6, 1988) | doi.org/10.13182/FST88-A25213
Articles are hosted by Taylor and Francis Online.
Based on experimental results on the catalytic decomposition of ammonia and methane into the elements a process for DT - recycling of molecular and chemically bonded deuterium / tritium from the fusion reactor exhaust gas is under development at KfK. In this context typical plasma contaminants like methane and ammonia tritiated to nearly 50% were synthesized on a 1 to 2·1012 Bq (30 to 50 Ci) scale. The radiolytic reactions were followed from the rate of disappearance of ammonia and the formation of nitrogen / hydrogen in case of tritiated ammonia and from the disappearance of methane and the formation of hydrogen in case of tritiated methane. The apparent half-lifes of tritiated methane and tritiated ammonia were determined to be approx. 250 hours and 550 hours respectively. The catalytic cracking reactions of tritiated ammonia and tritiated methane followed the behaviour anticipated from corresponding cold experiments.