3. 8  Certain Prospects in the Achievement of Steady, High-Speed, Liquid Lithium Flow
- Development of a Lithium Target for a High Power Neutron Source
 


Fig. 3-17 Set-up of International Fusion Materials Irradiation Facility (IFMIF)

An accelerator System generates a continuous deuteron beam of maximum 40 MeV, 250 mA. The target system consists of a liquid Li target and Li loop apparatus, and a deuteron beam collides with Li and generates neutrons by a stripping reaction. The test cell system performs neutron irradiation of the various materials of a nuclear fusion reactor.


Fig. 3-18 Plastic model of the liquid Li target

From a target nozzle, a liquid Li column of 26 cm in width, 2.5 cm in thickness, and 20 m/s at the maximum flow velocity flows down along with the concave back-wall of 25 cm curvature radius. The test assembly which holds irradiation test materials is set up behind the target.


Fig. 3-19 Results of the two-dimensional thermal-hydraulic analysis

The maximum temperature in the Li flow is 400 degrees cent. at the point about 2 cm from the free surface. The peak temperature has enough margin to the boiling point in consideration of the centrifugal force, and the restriction effect of boiling by the curved flow is confirmed by this analysis.



For the development of a D-T fusion reactor, it is indispensable to develop the materials which will be proof against radiation damage by 14 MeV neutrons. So the elemental technology of the International Fusion Materials Irradiation Facility (IFMIF) is under development now. In IFMIF, the liquid lithium (Li) target irradiated with a deuteron beam (max. 40 MeV, 250 mA) generates 14 MeV neutrons (Fig. 3-17).
A heat load at the Li target by the deuteron beam irradiation reaches 1 GW/m2 so that the flow velocity of the Li target should be a maximum 20 m/s for heat removal. The Li flow thickness to the beam direction is about 25 mm. Measures for the stabilization of the Li free surface and for the prevention of boiling in the Li flow are indispensable.
In order to solve these problems, we developed a Li target system that has a double reducer nozzle and a concave back-wall to produce a pressure by centrifugal force in the Li flow and to stabilize its free surface (Fig. 3-18).
Under the condition of a centrifugal force field associated with an acceleration 1,600 m/s2 that is generated at the maximum velocity of the concave flow, the boiling point is about 1,100 degrees cent. at 0.2 atm. It was confirmed by the thermal-hydraulic analysis code that the maximum temperature in liquid Li was 400 degrees cent. and that boiling could be prevented even at the peak temperature point (Fig. 3-19). The stability of the high-speed liquid Li was corroborated by water flow simulation experiments and now, we are planning demonstration experiments by a liquid Li loop.



Reference
H. Nakamura et al., Status of Lithium Target System for International Fusion Materials Irradiation Facility (IFMIF), Fusion Eng. Des., 58-59, 919 (2001).

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Persistent Quest - Research Activities 2001
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