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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

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