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5) Plasma-wall interaction and particles and heat extraction (p 1 - 2 - 3 - 4 - 5 - 6 - 7 )
c) The different edge plasma configurations After optimisation of materials, a second idea was to push away the zone where plasma-wall interaction takes place, so as to avoid that impurities emitted in this zone reach the discharge core: this is the axisymetric divertor configuration, where the LCMF is no longer defined by the point of contact with a solid, as in the case of the limiter configuration, but by a "magnetic" frontier created by adding a coil around the tokamak. We can see the advantage of the system on the figure below. The flow of particles leaving the plasma by radial diffusion is represented by the large white arrow with a red outline. In the first configuration, on the left, particles follow the field lines and meet the limiter (red arrow 1). These then neutralise, and may, on impact, tear impurities away from the wall, also in the form of neutrals. These neutral particles are not forced to follow the field lines (green arrow 2) and freely flow until they are again ionised by the plasma. Given the proximity of the central plasma, they are very likely to ionise again in the central plasma (red arrow 3). On the other hand, in the divertor configuration, on the right, the flow leaving the plasma is guided by following the field lines towards neutralisation plates far from the central plasma. The impurities are thus more likely to be ionised again in the edge zone, where they follow the field lines, to be once again intercepted by the neutralisation plates. They then remain in closed circuit without interfering with the central plasma: we then talk in terms of impurities screening. It is while testing this new configuration that the improved confinement H mode was discovered on the German machine Asdex during the eighties, which definitively ensured the success of this system. The largest present machines, like JET and JT60-U, are fitted with this type of device.
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