CFS consideration on the Main Dump and around

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Presentation transcript:

CFS consideration on the Main Dump and around Nobuhiro Terunuma and Yu Morikawa, KEK 29th May, 2018, ALCW2018, Fukuoka, Japan

Design of Main Dump and around Shielding for rock and groundwater Dump hall design Decommissioning issues Around Muon Wall Positron Tune-up Dump Photon Dump (undulator positron source) CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Main beam dump Peak temp. by beam: 155℃ P. Satyamurthy, et. al., NIM A 679 (2012) p67-81. Water dump (10 atom; boiling temp. 180℃) Peak temp. by beam: 155℃ Water flow: 2.17m/s Inlet temp.: 50℃ Diam. 1.8m、length 11m(30X0) SUS 316LN, thickness 2 inch End plate: SUS t7.5cm 11 m CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka. Temp. profile at Z=290cm

Radiation shield for groundwater should be strengthen. Main Dump Cavern (TDR) Radiation shield for groundwater should be strengthen. CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Beam dump materials in FLUKA simulation Water vessel SUS: diam. 1.8m, thick. 5cm Dummy room for window exchange in simulation Boron Concrete: 50cm+150cm = 2m Iron shield: 50cm CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Radioactivity Estimation for Decommissioning Decommissioning is one of the questions by MEXT and the TDR validation committee. Main beam dump will be the most activated device and concerns the level in the case of underground disposal. The estimation had been done by FLUKA Monte Carlo simulation. assume a maximum intense beam accumulation and decay in 20 years operation No beam beam 5000 h No beam beam 5000 h Decay/ Cool down De-commissioning No beam beam 5000 h 1 year 20 years CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Radioactive Disposal Category-1 Law in Japan: Act on the Regulation of Nuclear Source Material, Nuclear Fuel Material and Reactors Regulations Concerning the Activities of Radioactive Waste Disposal and Storage Radioactive Disposal Category-1 Category limit Deep underground more than 300m Radioactive Disposal Category-2 Underground more than 50m Dose limit Shallow underground pit Shallow underground trench

Radioactive nucleus generated by main dump A lot of radioactive nucleus are generated in the material of dump and its shields. 60Co is a target to evaluate because of the effectiveness (energy, lifetime). Most of 60Co is generated from the contamination of 59Co (stable) in the materials. SUS: 10~100ppm  use 100ppm for FLUKA Others: 10~50ppm Results of simulation All activated material of dump will be ranked to the easier disposal such as in a shallow trench. It is not like a show stopper. CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Build up of the activated Co-60 in the water vessel Water vessel is the highest activated material. Assume a range of the initial contamination of Co-59(stable) in SUS as from 10 to 100ppm. Beam operation period (Calendar year) CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Decay of the activated Co-60 in the water vessel Assume a range of the initial contamination of Co-59(stable) in SUS as from 10 to 100ppm. In the case of Japanese law for the radioactive waste by a nuclear L2:Disposal in shallow Pit L3:Disposal in shallow Trench 60Co: 10 GBq/ton After the beam operation (Calendar year) CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Radiation control for the underground environment Activation of Rock and Groundwater should be lower than the authorized level. A guideline have been established for J-PARC. 5 mSv/h (neutron) when Beam ON Neutron is dominant component especially for the transverse radiation from a high power absorber even for electron machine. The guideline for ILC have to be established as soon as possible, anyway. Local Shielding is required for the higher radiation sources. It is not only for workers but also for the outside of 30 cm concrete of the tunnel wall as a public environment. CFS consideration on the positron source; target and dumps, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Radiation dose from Main Dump Beam for simulation  1 TeV, 14 MW Dump design with 20% margin  17 MW Iron Shield 0.5 m and (Boronized) Concrete 4 m Geometry used for FLUKA Study Iron 0.5m Normal Concrete 3m Boronized Concrete 2m 5 mSv/h 4m CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Main Dump Cavern Shield blocks For the decommissioning in future Avoid 2m-thick selling shield Crane (40t) for dump and blocks Utility cavern for activated water and air CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

2nd Main Dump For the serious failure of the highly activated main dump, 2nd dump has been suggested. avoid too-long years shutdown due to a heavy activation. Put on the same beamline because of the MW beamstrahlung will come from IP. Installation will be done when required. Concrete shields for groundwater have to be constructed with tunnel, especially for bottom and side. Utilities can be switched from 1st dump. 2nd 1st CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Muon Wall Starting by 5m-thick muon wall then extend up to 19m in future. Location was 350m from IP, just behind the main dump shield. Some discussions on the muon background for ILC250 seems suggesting no need of the muon wall. No installation first, but need a space for future? CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Photon Dump from Undulator TDR photon dump will not work then alternative ideas have been proposed. One of them is a Graphite dump with 2km photon line. It will be near the main dump room and in the same accelerator tunnel (on the line 1.6m from BDS). It needs a space to exchange an activated graphite dump. The dump with shield will be 2m(W) X 1m(H) X 7m(L). Working space should be proposed by positron group. Beamline layout should be re-optimized. CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

e- dump for 5+5Hz option Beam power for this dump will be 8 MW at maximum, then it will be a copy of 17 MW Main Dump. Same scenario of the measure for failure will bring the 2nd dump. Cooling water system can be shared with the main dump. It will be located somewhere in BDS region. Then it will be better to joint a cavern following main dump and muon wall. No installation at first, but need radiation-shield walls both for bottom and side. CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Summary: Main Beam Dump and Around Time for the CFS engineering design is limited. Fix beamlines, location and size of systems! Photon Dump (120kW) Positron Linac Tune-up Dump (60kW) DR Positron Source IP Reserved for 8MW e- dump (5+5Hz) Reserved for 2nd Dump Reserved for Muon wall 1st Main Dump Utility Cavern for main dump Where the 2nd-loop water come from? CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Backup slides

Beam Power at Main Dump TDR ILC250 Power (MW) with 20% margin 17.0 3.1 Lum. upgrade Energy upgrade Beam Energy (GeV) 250 500 125 Rep. rate (Hz) 5 4 bunch per pulse 1312 2625 2450 bunch spacing (nsec) 554 366 pulse length (msec) 0.727 0.961 0.897 particles per bunch 2x1010 (3.2nC) 1.74x1010 (2.79nC) bunch charge (μC) 4.20 8.41 6.83 bunch current (mA) 5.78 8.75 7.61 pulse energy (MJ) 1.05 2.10 3.41 0.53 Power (MW) 5.25 10.5 13.7 2.6 5.3 with 20% margin 17.0 3.1 6.3 CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Activation after 20-years operation (1TeV) ”Rigid” water in simulation i.e.; generated H3 and Be7. 1 month 5 years

Dose rate by residual activation: 1 TeV, 20 years BDS tunnel Dose rate will be OK for the radiation workers. Water dump Iron Shield Boron Concrete Center of the beam dump CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.

Radioactivity Estimation for Decommissioning Shield blocks will be categorized in a group of a disposal in trench (L3) It can be reused and minimized the amount of disposal. Total weight 615t Iron Shield Total weight 292t Total weight 2025t Boron Concrete (Inner layer) Boron Concrete (Outer layer) After the beam operation (Calendar year) CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka. After the beam operation (Calendar year)

Shallow underground trench Shallow underground pit Underground more than 50m Deep underground more than 300m CFS consideration on the main dump and around, Nobuhiro Terunuma (KEK), 29 May 2018, ALCW2018, Fukuoka.