Prime pagine RA2010FUS:Copia di Layout 1 - ENEA - Fusione
Prime pagine RA2010FUS:Copia di Layout 1 - ENEA - Fusione
Prime pagine RA2010FUS:Copia di Layout 1 - ENEA - Fusione
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070<br />
progress report<br />
2010<br />
15 cm ra<strong>di</strong>us); b) neutron and gamma spectra at the<br />
detector location; c) analysis of the components of the<br />
collided neutron spectrum.<br />
The estimation of neutron spectra and<br />
collided–to–uncollided ratio(C/U) is useful to evaluate<br />
the neutronic performance of the HRNS collimator in<br />
both configurations (i.e. variation of the background with<br />
the <strong>di</strong>stance inside the cavity) and to characterize the<br />
ra<strong>di</strong>ation field inside it. Figure 3.29 shows the C/U values<br />
for 15 cm and 5 cm ra<strong>di</strong>us: the latter option is more<br />
effective in the collimation, especially in the front regions.<br />
Neutron spectra for 15 cm and 5 cm ra<strong>di</strong>i at the detector<br />
position are shown in figure 3.30.<br />
Figure 3.28 – The HRNS inside the port plug: in pale<br />
blue the concrete collar<br />
Collided/uncollided<br />
1.6<br />
1.2<br />
0.8<br />
0.4<br />
0.0<br />
800<br />
5 cm ra<strong>di</strong>us<br />
15 cm ra<strong>di</strong>us<br />
1200<br />
1600<br />
Distance from the torus axis (cm)<br />
Figure 3.29 – Collided to uncollided ratio at <strong>di</strong>fferent<br />
positions along the HRNS collimator: 15 cm (red) and<br />
5 cm (black) ra<strong>di</strong>us<br />
Neutron flux (n cm2/MeV/source n)<br />
10 -10<br />
10 -12<br />
10 -14<br />
0 10 20<br />
Energy (MeV)<br />
Figure 3.30 – Neutron spectra at the detector position<br />
D for 15 cm (dotted blue) and 5 cm (straight black)<br />
ra<strong>di</strong>us<br />
In order to fully characterize the ra<strong>di</strong>ation field at the<br />
detector position D, photon flux and spectra have been<br />
evaluated as well. The absolute values of the gamma flux<br />
are: 5.32×10 8 γ/cm 2 /s and 3.29×10 9 γ/cm 2 /s for 5 cm<br />
and 15 cm ra<strong>di</strong>us respectively .<br />
The collided spectrum at the detector position has been<br />
analyzed in order to isolate the contribution due to<br />
<strong>di</strong>fferent zones of the torus (inboard and outboard zones).<br />
The results obtained show that a large contribution to the<br />
collided neutron spectrum is due to the particles scattered<br />
only by the inboard side, which penetrate into the<br />
collimator, thus reaching the detector position. These<br />
results confirm the effectiveness of the port plug shiel<strong>di</strong>ng<br />
capability [3.11].<br />
Three–<strong>di</strong>mensional neutronic analysis of the ITER<br />
in–vessel coils<br />
In the frame of the contract ITER/CT/09/4100001120<br />
a complete neutronic analysis has been performed for the<br />
design of the in–vessel coil systems by using the MCNP5<br />
code in a full 3–D geometry. A detailed geometry of edge<br />
localised mode (ELM) and vertical stabilizing (VS) coils<br />
based on the last design specifications has been integrated<br />
into the last version of 40° ITER Alite MCNP model<br />
(fig. 3.31).<br />
cm<br />
800<br />
400<br />
0<br />
VS upper<br />
Upper ELM<br />
Central<br />
ELM<br />
Lower<br />
ELM<br />
-400<br />
VS lower<br />
Figure 3.31 – Vertical section of Alite–4<br />
MCNP model with In–vessel coils<br />
-800<br />
-800<br />
-400<br />
0<br />
cm<br />
400 800