5.4 What Happens If Coolant Water Spills in a Fusion Reactor Vacuum Vessel?
- Experimental Study of the Thermal-Hydraulic Safety of a Fusion Reactor-

Fig. 5-7

Concept of ICE and LOVA in a fusion reactor

Fig. 5-8

Pressure rise in the vacuum vessel under simulated ICE

The maximum pressure reaches about 0.7 MPa (0.1 MPa is about 1 atm.). Heat transfer to the injected water from the vacuum vessel, boiling and evaporation processes of water and other phenomena are investigated experimentally.

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Fig. 5-9

Behavior of buoyancy-driven exchange flow at the breach under LOVA

At the breach in the vacuum vessel, air flowing into the vacuum vessel is heated by the high temperature vessel. After the pressure is balanced between the inside and the outside of the vessel, a flow out of the vessel is induced due to the difference of gas densities at the two sides caused by the temperature difference at the breach (exchange flow).

As a part of the ITER engineering design activities we have carried out experimental studies of various aspects of the engineering safety of a vacuum vessel which is a major component of a fusion reactor.
Inside the vacuum vessel there will be various structures such as the first wall and the divertor exposed directly to the high temperature plasma, and many complicated pipings for their heat removal. If a local heat concentration exceeding the design value occurs in a short time on these structures due to plasma instabilities, for example, it may lead to a break of cooling pipes and a jet of cooling water into the vacuum vessel, technically called as ingress of coolant event (ICE). This may further lead to a break of the vacuum vessel by a rapid increase in pressure due to the evaporation of high-temperature and high-pressure water emerging from the breakage in the cooling pipes (loss of vacuum event, LOVA). As a result, a serious leak of the fuel tritium gas and gaseous radioactive micro-dust from the vacuum vessel as exchange flows should be postulated.
We have started a preliminary study of ICE and LOVA by a simulation experiment; boiling evaporation phenomena, pressure rise processes, and thermal-hydraulic charac-teristics of exchange flows through breaches in a vacuum vessel are quantitatively investigated. Parts of the experimental data obtained from this study are immediately used as validation data for the safety analysis codes used in the ITER design activities. Figure 5-8 is the result of an ICE experiment showing the time evolution of the pressure rise in a vacuum vessel. We have also found different behaviors of exchange flows arising at the breach depending on the part of the vacuum vessel where the breach occurs as shown in Fig. 5-9. This finding also contributed to the ITER design; they have changed a postulated breach region in the vacuum vessel from an upper part to a side part of the vessel to secure safety against a possible severe accident of the vacuum vessel.

Reference
K. Takase et al., Present Status of Fusion Safety Experiments for Thermal-Hydration, Purazuma Kaku Yugo Gakkai-Shi, 73 (8), 781 (1997).

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