1. magnetic confinement - ENEA - Fusione
1. magnetic confinement - ENEA - Fusione
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.