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HEAF Modeling in Fire Dynamics Simulator (FDS) Dr. Jason Floyd (Jensen Hughes) In cooperation with: Dr. Kevin McGrattan (NIST)

HEAF Modeling in Fire Dynamics Simulator (FDS)

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Page 1: HEAF Modeling in Fire Dynamics Simulator (FDS)

HEAF Modeling in Fire Dynamics Simulator (FDS)

Dr. Jason Floyd (Jensen Hughes)

In cooperation with:Dr. Kevin McGrattan (NIST)

Page 2: HEAF Modeling in Fire Dynamics Simulator (FDS)

HEAF Research Working Group Update – April 6th, 2021

FDS Model Validation Qualifiers

• The videos used in this presentation are intended to be used for model validation only and do not depict specific in plant HEAF operating experience

• WG members are using data generated by the NRC only test program

• The CFD simulations depicted in this presentation are intended to represent the specific conditions which were selected and tested at the KEMA facility for the HEAF Phase II NRC testing

• Different conditions and fault locations are represented in OpEx and will be addressed in both modeling and PRA application space

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Page 3: HEAF Modeling in Fire Dynamics Simulator (FDS)

6900 V26,600 A4.1 s120 MJ

GE Magne-Blast Switchgear Cabinet

Page 4: HEAF Modeling in Fire Dynamics Simulator (FDS)
Page 5: HEAF Modeling in Fire Dynamics Simulator (FDS)

Tungsten Slug Calorimeter

Page 6: HEAF Modeling in Fire Dynamics Simulator (FDS)

Modified Plate Thermometer

Page 7: HEAF Modeling in Fire Dynamics Simulator (FDS)

Modeling Assumptions:

• Fixed volumetric heat source• 75% of specified heat is radiated using

2000 solid angles; gray gas assumption• Lagrangian particles represent molten

aluminum emitted at Al vaporization temperature

• Steel enclosure ruptures at 1350 °C• Target plates and slugs modeled as 10

cm by 10 cm obstructions

• t2 dependence for mass loss rate• 10 % of the mass loss is aluminum

vapor• 90 % are Lagrangian particles

emitted at the Al melting temperature that can later evaporate

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Conclusion

• This FDS effort is maturing however there are many assumptions that need to be justified by a source term code such as Aria including;• Radiative fraction of the heat source• Particle size distribution

• At the current stage of the FDS modeling effort, simulations of the configurations different from the MV SWGR tests are expected to yield large uncertainties in the results due to the lack of source term characterization

• Model must be made more robust and faster• The use of the FDS at this stage of the project for the development of the ZOIs

recognizes large uncertainties in the results for differing conditions