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Azimuthal DPD Distribution Analysis with Prototype Shielding Configurations

This analysis explores azimuthal distributions of deposited energy in shielding configurations comprising tungsten and helium. Simulations were conducted for various material combinations (80% tungsten + 20% helium, 60% tungsten + 40% helium, etc.) with a focus on neutron energy cutoffs and proton beam interactions at 8 GeV energy levels. The study encompasses detailed statistical distributions and energy counting across 100,000 and 500,000 event samples, utilizing advanced computational methods and results from the MCNP code.

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Azimuthal DPD Distribution Analysis with Prototype Shielding Configurations

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  1. IDS120j WITH/WITHOUT GAPS SH#4 AZIMUTHAL DPD DISTRIBUTION ANALYSIS Nicholas Souchlas, PBL (3/14/2012) 1

  2. IDS120j WITHOUT ( LEFT ) AND WITH GAPS ( TWO SHIELDING CONFIGURATIONS RIGHT ) YZ CROSS SECTION PLOTS. 2

  3. IDS120j: DP DISTRIBUTION WITHOUT GAPS ( LEFT ) AND WITH GAPS ( RIGHT ) 3 IDS120h with shielding vessels. # Different cases of shielding material. # N=100,000 AND N=500,000 events simulation for 80%W+20%He SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h with shielding vessels. # Different cases of shielding material. # N=500,000 events simulation for 60%W+40%He AND 60%W+40%H2 60%W+40%H2 SHIELDING SHIELDING # Energy counting for N=500,000 events simulation for 80%W+20%He SHIELDING >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING:60%W+40%He , 80%W+20%He, 88%W+12%He ( WITH W VESSELS) >4 MW proton beam, Np=100,000/500,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h: introducing shielding vessels (STST OR W) Different cases of shielding material. >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING: 60%WC+40%H2O/60%WC+40%H2O/ >4 MW proton beam, Np=100,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h: introducing shielding vessels (STST OR W) Different cases of shielding material. >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING: 60%WC+40%H2O/60%WC+40%H2O/ >4 MW proton beam, Np=100,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm. IDS120h: introducing shielding vessels (STST OR W) Different cases of shielding material. >mars1510/MCNP >10-11 MeV NEUTRON ENERGY CUTOFF >SHIELDING: 60%WC+40%H2O/60%WC+40%H2O/ >4 MW proton beam, Np=100,000 >PROTONS ENERGY E=8 GeV. >GAUSSIAN PROFILE: σx=σy=0.12 cm.

  4. IDS120j: GAP BETWEEN CRYO 1-2 AND SC#4 SEGMENTATION DETAILS. 90 < r < 147.61 cm dr = 14.40 cm Nr = 4 bins 459.0 < z < 480.31 cm dz = 21.31 cm Nz = 1 bin 0.0 < φ < 360.0 deg. dφ = 30 deg. Nφ= 12 bins Ntot = 48 ''pieces'' 4 90 < r < 147.61 cm dr=14.40 cm Nr= 4 bins 459.0 < z < 480.31 cm dz=21.31 cm Nr= 1 bin

  5. SH#4 DPD AZIMUTHAL DISTRIBUTION WITHOUT GAPS: 15.8 g/cc ( LEFT ) AND 18.2 g/cc ( RIGHT ) W DENSITY. DPD ≲ 0.008 mW/g DPD ≲ 0.011 mW/g PEAKS APPEAR TO BE IN THE UPPER HALF OF SC#4, TOWARD – x AXIS 5

  6. SH#4 DPD AZIMUTHAL DISTRIBUTION WITH GAPS: 15.8 g/cc W DENSITY ( LEFT ). AZIMUTHALLY AVERAGE DPD PLOT BY USING ROOT SOFTWARE ( RIGHT ). SH#4 DPD AZIMUTHAL DISTRIBUTION WITH GAPS: 15.8 g/cc W DENSITY ( LEFT ). AZIMUTHALLY AVERAGE DPD PLOT BY USING ROOT SOFTWARE. z r SH#4: DPD ≲ 2.4 mW/g DPD ≲ 0.7 mW/g FROM RIGHT PLOT: DOES THAT MEAN THE STUDY II GEOMETRY SC#1 PEAK IS IN REALITY > 19 mW/g ?!! 6

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