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R&D Status of NFM and Neutron Source in China. YANG Jin-wei YANG Qingwei SONG Xian-ying. S outh W estern I nstitute of P hysics. Development status of NFM MCNP calculations HL-2A Neutron monitor Calibration neutron source Primary neutron detectors for comparison calibration
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R&D Status of NFM and Neutron Source in China YANG Jin-wei YANG Qingwei SONG Xian-ying SouthWestern Institute of Physics
Development status of NFM MCNP calculations HL-2A Neutron monitor Calibration neutron source Primary neutron detectors for comparison calibration Micro-fission chamber development for Neutronics and trillium production-test blanket module Plan and summary Outline of talk
pulse width is 1µs, the plateau length from 300—800V, the plateau width is 500V,and the slope of plateau is 0.9%, sensitivity:1±0.15cps/nν,insulation resistance≥1×109 ohm. Anti γ-rayradiation 2.8×10-2Gy/s This assembly has being used for photo-neutron measurement in the HL-2A tokamak Conclusion and discussion
MCNP calculations • Profile of DD neutron flux • DD neutron spectrum • Profile of DT neutron flux • DT neutron spectrum • Profile of fusion power density • Deposition of fusion energy
Tandem:Beam current 10A; Working voltage:215MV;Energy range :7~30MeV;Pulse width:1ns;repeat rates:4MHz。 Cascade generator(1): Beam current 15A; Energy range of output neutron:0.144, 1.2, 2.5, 5.0 14.8MeV;Neutron yields:108-109n/s。 Cascade generator(2): Working voltage:600kV; Neutron yields:1011n/s Neutron Source and Calibration for Efficiencies
Energy:14MeV Neutron yield:2×109n/s(available),5×1010n/s (reform) Pulse width:10μs—1ms Continued acceleration voltage:140kV Current≤400mA Life time7000h ( working home temperature) Size:76 ×1500mm(available), 100 ×800mm (reform) Portable neutron source
Neutron flux measurement for neutron source Here, N1/2 is the counts of the half area of the measured recoil proton spectrum in high energy part. The counts have been normalized to monitor counts corrected for dead time and scattering, and removed background; R is the radius of cathode of the proportional counter; σn,p is (n,p) cross section; n is the number of hydrogen atoms per cm3 in the counter; ΔI is a geometrical factor, it can be calculated by the following equation, i.e.,
h1=L1/R, h2=L2/R, here, L1 and L2 are the distances from target to the front surface and the rear surface of the sensitive volume of the counter, respectively. M1/2 is the percentage of the counts of the half area of the calculated recoil proton spectrum in high energy part to the total counts.
The main framework of the recoil proton proportional counter
Preliminary design for diagnostic of neutron flux in NT-TBM(CN HCSB)
Development of low detection efficiency and wide dynamic range 235U FC operated in campbelling or current mode. Development of 238U FC. Development of electronics(low noise). Development of compact ~1011 n/s DT neutron source for NFMcalibration. Plan