eurisol-ds - WP5

12343567589 3 5. Page 45. EURISOL-DS: Task#4. Meeting - Saclay 27-28 October 2005. RFQ - cooler. LT14. Page 46. Diapositive 24. LT14. 12343567589 3 5 ...
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EURISOL-DS Task#4 – Fission Target

Preliminary design of fission target R&D on UC2 target

First result from IRENA ion source (C. Lau)

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Baseline parameters of the MMW Hg target

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Sketch of the target/ion source system Ion source Insulator

Extraction

Drift tube

RIB out

Heater & thermal shielding

UC2 target Water cooled vacuum chamber

BeO reflector

Hg proton EURISOL-DS: Task#4

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General assumption:

Target length

50 cm

Target dia.

42 cm (in.) – 60 cm (out.)

UC2 material

density 11,4 gcm-3 (238U, natU, reactU)

Layer thickness

1 mm

Target thickness

6 cm

Reflector BeO

thickness 10 cm

FLUKA calculation

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238U

without reflector

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Fission density/incident proton

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natU

with reflector Fission density/incident proton

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natU

without reflector

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Fission density/incident proton

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reactU

with reflector

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Fission density/incident proton

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reactU

without reflector

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Fission density/incident proton

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Fission rate without reflector Fission rate with reflector

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Power deposit in the target

450

Without reflector

400

350

HD (11,4)

HD (11,4)

350

LD (3)

300 without refl 3

]

with refl

250

Power density [W/cm

Total power [kW]

300

200 150 100

250

200

150

100

50 50 0 238

nat

react

0 238

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Total weight (ion source & extraction excluded):

UC2 (11,4 g/cm3)

248

kg

Vacuum chamber & flangies

440

kg

Container & heater

68,5 kg

Graphite

71,6 kg

BeO

183

kg

TOTAL > 1010 kg

Plutonium (ORIGEN)

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290 g (60 days)

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Uranium Target weight

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Effusion calculation (by M. Barbui)

The simulation is performed using the GEANT4 toolkit (NIM A 506(2003),250-303). The isotopes of different mass (A) are simulated by alpha particles with the proper thermal energy. Eth=3/2(8.615*10-5) T 4/A The temperature is T = 2273 K. EURISOL-DS: Task#4

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Geometry 18 lamellas

3 cm 7 cm 50cm

1.6 cm EURISOL-DS: Task#4

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Preliminary results Exit, back open Isotopes considered: 81Ga, 90Kr, 131In 132Sn. Average number of bounces before exit: 54000 A lot of times the nuclei bounce on the lamella surfaces. In a first approssimation we assume for the lamellas the same sticking time of the walls. EURISOL-DS: Task#4

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Preliminary results/low statistics

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Preliminary results/low statistics

Ion

Effusion efficiency

Diffusion efficiency

Ionization efficiency

Total efficiency

132Sn (39,7 s)

0.89

0.19

0.1

0.017

90Kr (32.3 s)

0.99

0.16

0.95

0.15

81Ga (1,22 s)

0.6

0.018

0.4

0.0043

1321In (0.35 s)

0.8

0.056

0.1

0.0045

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Disks UCx 1 15 mm

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Alternative solution

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RFQ - cooler

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Comparison between PARRNe and Gatchina Uranium Carbide

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Preliminary results PARRNe Uranium Carbide: Faster than Gatchina UC2 Follow diffusion law Yields about a factor 2 more efficient for short-lived nuclei EURISOL-DS: Task#4

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Preliminary conclusions

Barrel target seems in part satisfing the requirements Need more detailed estimations on the total release efficiency Because of its weight vertical geometry is suggested Both versions, LD and HD uranium carbide, are suitable Target thickness of 3 cm seems sufficient (both with/without reflector) Low voltage extraction will semplify the target/source assembly Construction of a sector as a prototype R&D on Uranium Carbide targets is in progress at Gatchina 1 PhD position at LNL (3 years) EURISOL-DS: Task#4

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