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A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based on a Mirror Status Workshop Berkeley, CA. Sept. 8-9, 2008 25 Participants - 6 Labs. and 5 Universities - Japan & Russia T. C. Simonen, Chair Renews Workshop March 2-6, 2009
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Page 1: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap

(DTNS) One Element in an Urgently Needed

Comprehensive Fusion Materials Program

Based on a Mirror Status Workshop Berkeley, CA. Sept. 8-9, 2008

25 Participants - 6 Labs. and 5 Universities - Japan & Russia

T. C. Simonen, ChairRenews Workshop March 2-6, 2009

Page 2: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

The Simple Axisymmetric Mirror A Physics & Engineering Game Changer

• Simple magnet geometry stabilized by plasma exhaust– Physics established: Novosibirsk GDT Device – 60% beta, Te, classical– Extrapolates to a Dynamic Trap D-T Neutron Source (DTNS)– ~ 2 MW/m2 Neutron Flux, ~2 m2 Area, ~100 Liter Volume– Simple Geometry, Ease of Construction & Maintenance– Addresses Greenwald Gaps 10 & 13 and Initiative 7 Neutron Source

Page 3: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

3

GDT at Novosibirsk, Russia12 m Long with Large End Tanks to Decouple Te

Page 4: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

One Version of DTNS Showing Magnets, Shielding ,Neutral Beams, and Material Samples

(Bobouch, Fusion Science & Tech. 41 (2002) p44)

Page 5: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Neutron Flux Scales With Te to 4 MW/m2(for various NBI energies)

Page 6: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

DTNS Could Produce ITER-Like Neutron Energy Spectra

(Fischer, A.Moslang, A.Ivanov, FE&D 48 (2000) p.307)

Page 7: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

DTNS Would Operate at Higher Magnetic Field, Neutral Beam Energy, and Power than GDT

GDT Achieved DTNS Design

Beta (%) 60 60

Beam Power (MW) 4 30

Beam Energy (kV) 20 80

Ion Energy (keV) 10 40

Electron Temp (eV) 230 750

Density (10e20 m-3) 1 4

Energy Confinement Time (ms)

2 2

Pulse Duration 5 ms cw

Page 8: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

DTNS Has Two Test Zones

• Neutron Flux concentrates in regions of beam ion Turning Points– One Zone could test many material samples– One Zone could test Sub-components

Page 9: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Small Material Sample Test Assembly(Holds ~8,000 Temp. Controlled Specimens)

ref: U. Fisher, A. Moslang, A.A. Ivanov, FE&D 48 (2000) p307

Page 10: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Monte Carlo Calculation Indicates Uniform Radial-Axial Neutron Flux

(r-uniformity < 5%/cm, z-uniformity < 0.1%/cm)

Page 11: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Materials Testing Neutron Sources RTNS

D-T

82-87

IFMIF

D+Li

DTNS

D-T

FDF/CTF

D-T

Neutron Power

(MW)

20 W ? 2+ 100-300

30-160

Flux (MW/m2) 0.2 1.5 2+ 2 - 3

1 - 3

Area (m2) .0001 0.01 2 70

15

Tritium (kg/FPY) ~0 0 0.15 ~2 to 20 without breeding

Cost ($M) FY08 1000 325-650 ?

1500

Page 12: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Summary– The DTNS is an Attractive D-T Neutron Source That Closes Gaps 10 & 13

and Initiative 7 for Materials Testing

• ITER-Like Neutron Energy Spectrum

• Produces 1-4 MW/m2

• Provides ~2 m2 Test Area

• Provides ~100 Liter Test Volume

• Uniformity < 5%/cm

Page 13: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Suggested Next Steps

• Collaboration with Novosibirsk GDT– Diagnostics (Thomson Scattering, …)– GDT-Upgrade (4 MW to 10 MW)

• Theory-Modeling to– Extrapolate to DTNS (Te, MHD, DCLC, TPM )– Seek More Efficient Design (end cells)– Deploy US Theory Capabilities (e.g. UTexas, LLNL,

LANL, Lehigh, etc, etc)• Initiate DTNS Design• Construct DTNS (could be phased)

Page 14: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

Additional Benefits of DTNS Activity

• DTNS Physics Has Much in Common with Other Confinement Systems

• Tests Existing Modeling Capability in Very Simple Geometry

• More Efficient DTNS (end cells) Leads to a Fusion-Fission Hybrid

• Benefits Outside Magnetic Fusion

• Fosters International Collaboration

Page 15: A Materials Evaluation Neutron Source Based on the Gas Dynamic Trap (DTNS) One Element in an Urgently Needed Comprehensive Fusion Materials Program Based.

References

• Gas dynamic trap as high power 14 MeV neutron source, P.A Bagryansky , et. al. Fusion Engineering and Design 70 (2004), p13-33

• Assessment of the gas dynamic trap mirror facility as intense neutron source for fusion material test irradiations, U. Fischer, A. Moslang, A.A. Ivanov, Fusion Engineering and Design, 48 (2000) p307-325


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