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1. magnetic confinement - ENEA - Fusione

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5. INERTIAL CONFINEMENT 125<br />

5.3 Theory<br />

density and laser rays are displayed. About 10 ps later the light is transmitted.<br />

In the picture at left in figure 5.4 the density r is represented as function of the space<br />

coordinates. The map in the center is the density as function of the calculation grid<br />

indexes. At right is shown a detail of rays propagation, with different colors for<br />

different incidence angle.<br />

The situation near t s<br />

is represented in figure 5.5. Rays are refracted in a sort of ring<br />

as seen in the map at top of figure 5.5. In the same figure are also represented the<br />

quantities Z k T e<br />

(where Z is the average ion charge and T e<br />

the electronic<br />

temperature) and the average ion kinetic energy in the flow (that is 1/2 m i<br />

n 2 , where<br />

n is the flow velocity and m i<br />

the ionic mass). Both are measured in °K. Kinetic energy<br />

prevails only in a thin, dense layer destined to splash on the next one in a multi foil<br />

target. From this follows that the flow energy is partially dissipated in a shock wave<br />

driven in the next layer.<br />

The last map shows the distribution of the flow velocity (U z is the component along<br />

z, the positive axis pointing towards the laser).<br />

The process of layer collision was produced in simulations for the interaction of a<br />

three layer target with a light beam focused in such a way to initially reproduce, at the<br />

first exposed surface, the conditions at surface of case 3.<br />

Fig. 5.3 - Fraction of<br />

absorbed light as function<br />

of time for a single foil. A<br />

fast drop in absorption<br />

occurs when the target<br />

becomes transparent.<br />

At the time 0.65 ns the irradiated foil<br />

impinges on the second foil. In figure<br />

5.6 is shown the map of the velocity<br />

along z at this time. Typical negative<br />

velocity is about 2 (in units of 10 7<br />

cm/s). In figure 5.7 is shown the<br />

density map at the same time. The<br />

propagation of the shock wave in the<br />

second foil is clearly seen by the<br />

representation of density in terms of<br />

grid indexes.<br />

-6 -5 -4 -3 -2 -1 0<br />

Logr(g/cc)<br />

Fig. 5.4 – Left: density (r) map 10 ps before light starts to be transmitted<br />

through the target. Center: the figure is a representation of the density as<br />

function of the grid coordinates. Details of ray propagation are shown in the<br />

figure at right.

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