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3) - Magnetic confinement (p 1 - 2 - 3 - 4 )
c) Particles and heat transport Once a stable magnetic equilibrium has been established, we have seen that the particles, when they are considered individually, follow the magnetic field lines, if the Larmor radius and drift movements are neglected. However, they undergo other phenomena, which will change this simple image and result in rather more complex transport mechanisms, which may be divided into two major categories:
Heat transport is a phenomenon quite comparable to particle transport. First of all, diffusing particles carry their own energy : this is the phenomenon of convection. Then collisions allow particles to exchange energy: this is thermal conduction. This diffusion phenomenon from inside plasma towards the outside tends to " empty " the plasma of its content in particles and energy, and determines the confinement machine performance. The diffusion of particles is characterised by a coefficient of proportionality, called diffusion coefficient, between the particles flow and the density gradient. Similarly, for heat, the diffusion coefficient is defined by the ratio between the heat flow and the temperature gradient. The larger this coefficient, the greater the diffusion, and the worse the confinement. Experimentally, we observe much greater losses of energy (and therefore a much shorter time of confinement) than those predicted by neoclassical transport alone. Anoumalous transport would seem to be the dominant term. Many studies are underway to refine the comprehension of phenomena likely to explain this transport. In particular, we are trying to establish the dependence of the diffusion coefficient on the machine and plasma parameters . Two types of behaviour have been identified:
The trends arising from the latest studies are that behaviour is different according to the specie under consideration (electrons or ions) and confinement mode :
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