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Jules Horowitz Reactor

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The reactor is designed to have a good neutron economy that results in large numbers of thermal neutrons being available around the outside of the reactor core. The neutrons from this source can be used in many materials testing and other experimental roles. The system also allows samples to be inserted directly into the core, where they are exposed to high-energy neutrons, which is useful for isotope preparation. Similar reactors were common in the 1950s and 60s, but most have reached the end of their practical lifespans, and few new ones have been commissioned. This has led to a crisis in the worldwide supply of medical isotopes, one of the major roles of the JHR.

Site preparation began in 2007, followed by the first concrete in the summer of 2009. The central containment structure was completed with the addition of a 105-tonne (103-long-ton; 116-short-ton) dome in December 2013. At the time it was predicted the system would be operational in 2014. Since then the site has suffered from significant delays, leading to a complete re-organization of the management. Current estimates suggest first criticality sometime after 2030.

Design

The Jules Horowitz Reactor is a materials testing reactor, with a power output of approximately 100 megawatts. It has roughly twice the neutron flux of the OSIRIS design. It has a planned service lifespan of around 50 years, and is designed to be adaptable for a variety of research uses by nuclear utilities, nuclear steam system suppliers, nuclear fuel manufacturers, research organisations and safety authorities. The reactor's versatile modular design allows it to accommodate up to 20 simultaneous experiments. Its instrumentation allows previously unavailable real-time analysis to be performed.

Its primary uses will be research into the performance of nuclear fuel at existing reactors, testing of materials used in reactors, testing designs for fuel for future reactors and the production of radioisotopes for use in medicine. The reactor is intended to produce radioisotopes in coordination with existing production facilities at Petten in the Netherlands. The reactor's coolant flow is ascending, in the order of nearly 2.36 m3/s (83 cu ft/s), with maximum pressure in the order of 1.0–1.5 megapascals (150–220 psi), depending on the required flow and the core head loss.

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