Neutronics modeling of activation diagnostics in SPARC
POSTER
Abstract
The SPARC tokamak, now under construction in Devens, Massachusetts, is slated to operate with a
maximum of 140 MW of DT fusion power and thus a total neutron rate of approximately 5 × 10^19 n/s
(Creely et al. 2020). Activation diagnostics have been used with success on both TFTR and JET during DT
operation to measure time-integrated fusion power in combination with other diagnostics (Jarvis et al. 1991)
(Nieschmidt, 1986). SPARC plans to use activation diagnostics in combination with fission-chamber based
flux monitors to measure fusion energy during both DD and DT operation. The Monte-Carlo neutronics
code OpenMC is used to model the neutron flux in various locations in the device in order to assess possible
activation foil locations as well as predict the induced activity. A realistic SPARC geometry is used with
several different neutron source configurations in order to asses the sensitivity of the system to source geom-
etry and energy spectrum. A target activity of 100 μCuries is used to design the activation foil geometry.
Various possible activation foil materials are then analyzed including Silicon-28, Zirconium-90, and Iron-56.
maximum of 140 MW of DT fusion power and thus a total neutron rate of approximately 5 × 10^19 n/s
(Creely et al. 2020). Activation diagnostics have been used with success on both TFTR and JET during DT
operation to measure time-integrated fusion power in combination with other diagnostics (Jarvis et al. 1991)
(Nieschmidt, 1986). SPARC plans to use activation diagnostics in combination with fission-chamber based
flux monitors to measure fusion energy during both DD and DT operation. The Monte-Carlo neutronics
code OpenMC is used to model the neutron flux in various locations in the device in order to assess possible
activation foil locations as well as predict the induced activity. A realistic SPARC geometry is used with
several different neutron source configurations in order to asses the sensitivity of the system to source geom-
etry and energy spectrum. A target activity of 100 μCuries is used to design the activation foil geometry.
Various possible activation foil materials are then analyzed including Silicon-28, Zirconium-90, and Iron-56.
Presenters
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John L Ball
Massachusetts Institute of Technology, MIT
Authors
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John L Ball
Massachusetts Institute of Technology, MIT
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Shon P Mackie
MIT, Department of Physics
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Roy A Tinguely
Massachusetts Institute of Technology, MIT