Difference between revisions of "TF NEUP 2011"
Line 45: | Line 45: | ||
#"Fission chambers for CANDU SDS neutronic trip applications", V. Mohindrs, M. Vartolomei, and A. McDonald, 28th Annual Canadian Nuclear Society (CNS) conference, June 3-6, 2007New Brunswick, Canada [[Media:Virender_CANDU2007.pdf]] | #"Fission chambers for CANDU SDS neutronic trip applications", V. Mohindrs, M. Vartolomei, and A. McDonald, 28th Annual Canadian Nuclear Society (CNS) conference, June 3-6, 2007New Brunswick, Canada [[Media:Virender_CANDU2007.pdf]] | ||
#GE builds fission chambers http://www.ge-mcs.com/en/nuclear-reactor-instrumentation/neutron-monitoring-instrumentation/ex-core-fission.html | #GE builds fission chambers http://www.ge-mcs.com/en/nuclear-reactor-instrumentation/neutron-monitoring-instrumentation/ex-core-fission.html | ||
− | + | #GEs thermal neutron device for in core http://www.ge-mcs.com/en/nuclear-reactor-instrumentation/neutron-monitoring-instrumentation/moveable-detectors.html | |
[[Forest_Proposals]] | [[Forest_Proposals]] |
Revision as of 05:26, 15 October 2011
Project Summary
We propose to develop a gaseous detector sensitive to fast (100 keV - 100 MeV) neutrons which may be used to monitor the neutron flux in nuclear reactors. The monitoring of a reactor core's neutron flux has been a long standing problem due to the high neutron and gamma intensity.
Neutron fluxes in reactors
according to http://www.bnl.gov/bnlweb/history/HFBR_main.asp
a 40 MW reactor at Brookhaven's High Flux Beam Reactor (HBFR) produced a neutron flux of
for experiments. The neutron flux was a maximum outside the core because the neutrons were directed tangentially to the core instead of radially.1e11 to 1e12 neutrons per cm^2 per second may be more typical
Let's assume this flux is an upper limit for a detector to measure neutron fluxes in a reactor core. The pulse width of a regular GEM detector is
sec. Because of the high gain a signal may be observed over a surface area of 3 cm^2 (10 cm by 300 \times 10^{-3} cm ). A GEM detector with this active area would only be able to count neutron fluxes of if the detector efficiency was 100 %. A detector efficiency of 10^{-5} would be able to see rates of 10^{11}.
The pulse width of a standard ionization chamber is on the order of 300 nsec, so a standard GEm detector would only be able to have a factor of 6 higher rate than a typical ionization/fission chamber.
Path to work accomplishments
Deliverables and outcomes
1.) Neutron sensitive ionization chamber (no position readout)
Time Frame
Budget
Each year
2 grad students ($50k)
2 faculty summer months ($20k)
Beam time: electron experiment which produces isotropic neutrons. Compare neutron rates seen by several know detectors to the rate from the THGEM based detector.
Bibliography
- File:NEUP Pre-app RFP.pdf
- "Fission chambers for CANDU SDS neutronic trip applications", V. Mohindrs, M. Vartolomei, and A. McDonald, 28th Annual Canadian Nuclear Society (CNS) conference, June 3-6, 2007New Brunswick, Canada Media:Virender_CANDU2007.pdf
- GE builds fission chambers http://www.ge-mcs.com/en/nuclear-reactor-instrumentation/neutron-monitoring-instrumentation/ex-core-fission.html
- GEs thermal neutron device for in core http://www.ge-mcs.com/en/nuclear-reactor-instrumentation/neutron-monitoring-instrumentation/moveable-detectors.html