COMPLETE DOCUMENT (1862 kb) - OECD Nuclear Energy Agency
COMPLETE DOCUMENT (1862 kb) - OECD Nuclear Energy Agency
COMPLETE DOCUMENT (1862 kb) - OECD Nuclear Energy Agency
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Spallation target<br />
Reliable nuclear data and codes for the intermediate energy region are required for the design<br />
of an ADS. At present, most of the data and codes are available for an approximate evaluation of<br />
conceptual designs and for feasibility studies. Detailed designs will need much higher accuracy. If a<br />
±2% accuracy on the system’s energy balance is required, the spallation neutron yield should be<br />
calculated with an accuracy of ±2%. Uncertainties still seem large in predicting the spallation product<br />
yields and the high energy component of the neutron spectrum to evaluate activation and damage in<br />
materials.<br />
Injection of the intense proton beam into the target causes high fluxes of protons and fast<br />
neutrons in the beam window, target, and wall material surrounding the target. These, particularly for<br />
the beam window, suffer irradiation damage and are degraded in mechanical properties and dimensional<br />
stability. The exposure of the materials to high fluxes and energies would be more severe than in normal<br />
reactors. Research on the interaction between high-energy proton and neutron beam and window as well<br />
as structural materials is required.<br />
An intense proton beam deposits heat in the target. Heat removal requirements for the target<br />
are essentially identical to those for the fuel.<br />
Subcritical core<br />
A subcritical core can be very similar in principle to a critical core except that the effective<br />
neutron multiplication factor is less than unity. A subcritical core cooled by liquid metal can fully utilise<br />
existing LMFR technologies.<br />
Subcritical operation provides great freedom in design and operation. Criticality in a<br />
conventional reactor imposes tight constraints on the fuel specifications and cycle length.<br />
Accelerator-driven systems can accept fuels that would be impossible or difficult to use in critical<br />
reactors, and can extend their cycle length if necessary.<br />
Trips and fluctuations of the incident proton beam are inevitable, causing thermal shocks in<br />
the core components. The design must take this into consideration; power distribution, effective neutron<br />
multiplication factor, the neutron flux shape transient response and the size of the system.<br />
Safety features [98]<br />
The subcriticality of an ADS has clear safety advantages for severe reactivity accidents. It can<br />
cope with fast ramp rate accidents which could occur too rapidly for scram systems in critical reactors.<br />
A margin to accommodate fast reactivity insertions is important to avoid super-criticality accidents.<br />
The consequences of cooling failure for ADSs are similar to critical reactors. A reliable beam<br />
shut-off system is, therefore, required for an ADS, just as a reliable scram system is required for a<br />
critical reactor. A reliable emergency decay heat removal system is required for both.<br />
Performance assessment of accelerator-driven systems<br />
Over the past few years a number of different ADS concepts have been developed. For the<br />
purpose of illustration, the performance of an ADS described in References 102 and 103 is discussed<br />
here. The objective is to incinerate Np, Am and Cm and transmute 99 Tc and 129 I in spent LWR fuel.<br />
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