Intense Fast Neutron Sources Using a Superconducting Electron Linac - - PowerPoint PPT Presentation

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Intense Fast Neutron Sources Using a Superconducting Electron Linac - - PowerPoint PPT Presentation

High Power Liquid Lead-bismuth Targetry for Intense Fast Neutron Sources Using a Superconducting Electron Linac M. Mamtimin, J. Diemer, T.L. Grimm, F.Y. Odeh, and V.N. Starovoitova Niowave, Inc. S.A. Maloy and K.A. Woloshun Los Alamos National


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SLIDE 1

High Power Liquid Lead-bismuth Targetry for Intense Fast Neutron Sources Using a Superconducting Electron Linac

  • M. Mamtimin, J. Diemer, T.L. Grimm, F.Y. Odeh, and V.N. Starovoitova

Niowave, Inc. S.A. Maloy and K.A. Woloshun Los Alamos National Laboratory

mayir@niowaveinc.com

This project is partially supported by DOE under grant DE-SC0011355

High Power Targetry Workshop, June 2018

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SLIDE 2

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Outline

❖ About Niowave ❖ Uranium Target Assembly ❖ Hybrid Subcritical Testbed ❖ High Power Target

❖ Physics ❖ Target Material

❖ High Power Target Design

❖ Stagnant LBE target ❖ Forced flow LBE target ❖ LBE + NU target

❖ Corrosion Studies ❖ Summary and Future Work

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SLIDE 3

Niowave, Inc.

  • Niowave is a world-wide leader in research, development, manufacturing

and operation of superconducting electron linear accelerators.

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Turn-key Systems

  • Superconducting Linac
  • Helium Cryoplant
  • Microwave Power
  • End Station
  • Licensing

End Stations

Beam Energy ~9 MeV Average Beam Power 10-100 kW Duty Cycle 10-100% Closed-loop Cooling Capacity 40-110 W @ 4 K

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SLIDE 4

Niowave’s Commercial Markets

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Sterilization & Advanced Manufacturing

Eliminate dirty bomb material

Medical & Industrial Radioisotopes

Domestic supply without nuclear reactor or highly-enriched uranium

Nuclear Energy Advanced Technologies

Domestic fast neutron irradiation and advanced reactor development < 9 MeV > 9 MeV 9 MeV

Superconducting Electron Linacs

Radiography & Active Interrogation

Cargo inspection for contraband and shielded nuclear bombs > 9 MeV

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SLIDE 5

Niowave’s Subcritical Assembly

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NU LEU Neutron source coupler

E-beam power 40 MeV, 530 kW Neutron source 8.5×1014 n/s LEU fuel loading 10 kgU keff 0.95 Fission power 210 kW

  • Subcritical uranium target

assembly (UTA)

  • Water cooled pool type

thermal assembly

  • Low enriched uranium
  • Driven by SEL and high

power neutron target

  • Licensed by NRC
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SLIDE 6

Outer Core Reflector Internal Radial Reflector Inner Core Sample Irradiation C Neutron Source

C

Internal Axial Reflector Internal Structure Shield z(cm) ~1 ~5 ~20 ~30 r(cm) ~30 ~15 ~10 LBE beam

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Hybrid Subcritical Testbed

Pump LBE Ar LBE NU Beam

High power target

  • Nuclear Reactors
  • Domestic fast neutron irradiation facility
  • Reactor Materials
  • Radiation and corrosion resistant materials
  • Nuclear Fuel Cycle
  • Commercial closed-loop nuclear fuel cycle
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SLIDE 7

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Photoneutron Production

n

Electrons are accelerated Electrons brake and produce bremsstrahlung photons e- Photons cause photonuclear reactions and liberate neutrons

n n n n n n

Niowave’s Superconducting Linear Electron Accelerator High Power Neutron Target

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SLIDE 8

Target Material

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  • High conversion efficiency (high Z)
  • High melting point (if the converter is solid)
  • If liquid, low melting point and good

thermomechanical properties Lead-bismuth eutectic (LBE):

  • Z=82(45%),83(55%)
  • Tmelt = 124°C

Isotope Eth(MeV) Peak Value (mb)

2H

2.22 2.5

9Be

1.67 5

184W

7.41 440

208Pb

7.37 620

209Bi

7.46 530

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SLIDE 9

Target Design

  • Stagnant LBE
  • Feasibility studies
  • Low power demonstration
  • Forced flow LBE
  • Liquid metal pump
  • A fast neutron flux of 1014 n/cm2/s
  • For small scale material studies (~ 10 mm3)
  • LBE with uranium
  • Low power prototype
  • Higher neutron production yield

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SLIDE 10

Stagnant LBE Target

10 Ee, MeV Power, W Average Flux, #/cm^2/s Peak Flux, #/cm^2/s 10 500 1.63E+08 8.30E+08 20 1200 1.02E+11 3.10E+11 35 1600 2.97E+11 7.50E+11

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SLIDE 11

ANSYS Thermal Analysis

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At 40 MeV 5 kW: SS window stress is above yield

At 40 MeV 5 kW: Max LBE T= 663 °C; Flow Rate = 15 cm/s Max SS T = 503 C Max SS Y = 179 MPa

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SLIDE 12

Liquid Metal Pump

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0.0 100.0 200.0 300.0 400.0 500.0 600.0 700.0 800.0 900.0 1000.0 50 100 150 200 250 300 350

Temperature Rise ( C) Flow rate (lb/min)

50 kW LBE Temperaure Rise

  • Better heat removal
  • Higher power operation
  • Minimum LBE temperature rise

Liquid metal mechanical pump Ferro fluid shaft seal Sealed LBE container Band heater Impeller LBE outlet LBE inlet

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SLIDE 13

Windowless LBE Target

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  • Eliminates thin SS window
  • High power operation
  • Allows better coupling
  • Versatile:
  • Neutron source
  • Xray source
  • Positron target

electrons

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SLIDE 14

LBE with Uranium

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  • Higher neutron production due to

(γ,xn) and (γ,f) reactions

  • Gram quantities of uranium will

increase peak neutron flux by a factor of 4

Electron

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SLIDE 15

Corrosion Studies

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  • LBE is corrosive:
  • Corrosion studies in up to 700 C LBE
  • Bimetal structures for high temperature components
  • Forced flow corrosion test station (erosion and corrosion)
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SLIDE 16

Summary

  • Liquid metal based target development
  • Various high power neutron targets were designed,

built, and tested

  • Radiation damage, corrosion, and erosion issues

are being addressed

  • Versatility can be leveraged towards nuclear

energy community and basic nuclear physics research

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