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THORIUM AS AN ENERGY SOURCE - Opportunities for Norway ...

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Thorium as an Energy Source - <strong>Opportunities</strong> <strong>for</strong> <strong>Norway</strong><br />

products that produces the heat required to melt the reactor. The Energy Amplifier as shown in<br />

figure 5.9 will probably not melt if the heat removal from the lead-bismuth coolant stops, because<br />

it contains around 8000 metric tonnes of passively cooled metal that will absorb the heat. But, if<br />

the coolant leaks from the tank the core will certainly melt.<br />

5.4.4.3 Sub-criticality and the Accelerator<br />

In an ADS, the sustainability of the nuclear fission reactions is made possible because of the<br />

presence of an external source of neutrons provided by the proton beam; the working point of the<br />

core itself is far below criticality. Two alternatives, based on well established technologies, can be<br />

envisaged in order to fulfil the indicated requirements <strong>for</strong> the accelerator:<br />

1. Super-conducting cavity LINACs, <strong>for</strong> which a vast experience exists in Europe, including on<br />

the industrial production of the cavities and of the associated RF sources, especially as a<br />

consequence of the realisation, now dismantled, of LEP200 8 at CERN and of the work at<br />

DESY (Germany) and elsewhere (Italy, France) in association with the TESLA 9 program. The<br />

most powerful LINAC is now being commissioned at the Spallation Neutron Source facility at<br />

ORNL.<br />

2. Isochronous cyclotrons, <strong>for</strong> which the world reference with respect to the ADS question is PSI<br />

(Switzerland). There is also a strong experience accumulated at G<strong>AN</strong>IL (France), CAL<br />

(France) and LNS (Italy) facilities. The guiding magnetic field can be produced either by<br />

ordinary magnets (PSI, G<strong>AN</strong>IL, CAL) or super-conducting coils (LNS).<br />

The system needed to drive an ADS represents only a reasonable extrapolation of what has<br />

already been achieved in current accelerator technology [108], [109], [110], [111], [112] and [113].<br />

An important element <strong>for</strong> the accelerator is a high reliability in continuous operation and in<br />

particular the absence of “beam glitches”, namely of short interruptions of the beam current. A<br />

beam interruption will induce very strong stresses in the window between the accelerator vacuum<br />

and the target and produce a fatigue of the reactor elements, reducing the lifetime of the system.<br />

So this topic is of first importance. The LEP200 super-conducting LINAC has demonstrated a<br />

remarkable level of continuity of operation, since a single short glitch would imply the immediate<br />

loss of the colliding beams. At PSI, however, some beam instabilities due to discharges in the RFfeed<br />

through to the cavities have been observed. It is believed that this problem can be overcome<br />

with a more advanced design of such components 10 , which are known to operate without such<br />

inconveniences in other installations (CERN).<br />

It is expected that both accelerator schemes (LINAC and cyclotron) will offer highly reliable and<br />

redundant methods to control the beam current and to switch it off extremely quickly (a few<br />

microseconds) and reliably if and when required by the sub-critical unit. However, it seems that<br />

the LINAC option is favoured by the international accelerator community [114].<br />

5.4.4.4 Technology Issues of Medium-to-High Power Spallation Targets <strong>for</strong> ADS<br />

The spallation target has to provide the highest possible neutron yield, be transparent to<br />

neutrons, and at the same time sustain a large beam power of 10 to 20 MW. In this respect,<br />

molten lead is almost an ideal candidate since it has also excellent thermodynamic properties and<br />

can contribute to cooling. The use of liquid targets is a tendency which is presently developing in<br />

8 The LEP200 programme ultimately consists of about 3.6 GeV gradient <strong>for</strong> the continuous acceleration of<br />

relativistic electrons and positrons with a current of up to 7 mA.<br />

9 The TESLA programme aims at the realisation of advanced super conducting cavities, of high gradient and lower<br />

cost in order to open the way to the realisation of a Linear Collider in the 1/2 TeV range and eventually beyond.<br />

10 New cavities are under development also at PSI.<br />

60

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