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1. magnetic confinement - ENEA - Fusione

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5. INERTIAL CONFINEMENT 127<br />

Time=0.65 ns<br />

5.3 Theory<br />

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

Log[r(g/cc)]<br />

Time=0.9 ns<br />

Fig. 5.7 - Density maps at<br />

different times and ray<br />

tracing at 0.9 ns when the<br />

second layer impinges on<br />

the third.<br />

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

Log[r(g/cc)]<br />

At 0.9 ns the second foil, and a part of the first, start to impinge on the third. To be<br />

noted that the impinging time of the first foil on the second foil was 0.65 ns, whereas<br />

the collision with the third follows after 0.25 additional nanoseconds. At 0.9 ns a<br />

substantial transverse flow can be seen. Part of the first foil material flows<br />

transversally between the unperturbed remnants of the first and second foil. Due to<br />

this expansion the light succeeds in penetrating near the second foil surface. The ray<br />

trajectories become quite complex and a remarkable transverse light excursion is<br />

noted. In the same figure 5.7 it is represented the detail of the propagation for 10 rays<br />

and, separately, the path of two most external rays.<br />

The computation has been advanced up to t=0.97781ns. At this time the<br />

computational grid becomes severely distort. At any rate many of the most

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