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Preferential Hydrogen Diffusion from Zircaloy-2 Cladding to an Inner Zr Barrier Zachary Campbell, Edite M. Grendze, Ian Hamilton, Michael Toomey Faculty Advisor: David Bahr, Mysore Dayananda Industrial Sponsor: Dan Lutz Project Background GNF has expressed interest in modeling to predict diffusion, precipitation, and dissolution of hydrogen in Zircaloy-2 nuclear fuel cladding during dry storage. To assist in this effort, the following data were obtained from hydrogen- charged Zircaloy-2 samples. Samples were heated and then cooled from 400°C to 200°C over 1, 2, 4, and 15 days. An isothermal test at 440°C for 32 days was also performed. The samples were then analyzed using stereological techniques. No precipitate reorientation was observed and the hydride direction was circumferential as in the as - received samples. The denuded zone thickness grew and then shrank with increasing cooling time. A loss of hydrogen from 340 ppm in the as-received sample to 300 ppm in a 15-day sample was observed by hydrogen analysis. Heat Treatments Microscopy Acknowledgements Results & Model MSE 430-440: Materials Processing and Design Denuded zone thickness versus heat treatment time for various concentrations. Phase diagram: hydrogen concentration versus temperature. Note terminal solid solubility line. (Sugisaki, et. al.) Four samples of varying hydrogen content were received for testing. This work is sponsored by GE-Hitachi Global Nuclear Fuels, Wilmington, NC. Zircaloy-2 is an alloy of 98.8% Zr and 1.2% Sn with trace Fe, Cr and Ni used for nuclear fuel cladding in boiling water reactors. The precipitation of hydrides in Zircaloy-2 can lead to embrittlement and eventual failure of the cladding. Due to the high temperatures reached in the reactor, the metal corrodes, and hydrogen is emitted. This hydrogen diffuses into the cladding and a zirconium hydride phase precipitates once the terminal solid solubility of hydrogen is reached. After spent nuclear fuel rods have been cooled in a spent fuel pool, they are moved into dry storage containers for more permanent disposal. During insertion into the dry storage casks, the temperature within the cask peaks at approximately 400°C, then cools to 350°C. Previous research (Courty, et al.) suggests that after reaching the solid solubility limit, hydrides prefer to precipitate on the edge of the cladding. If orientated radially, the hydrides can be detrimental to the structural integrity of the cladding edge. Denuded zone thickness varies with length of heat treatment. The data does not have a linear fit. The data suggests that hydride precipitation is more favorable in the liner of the samples. Initially, the hydrides prefer to precipitate on the liner-cladding edge and the denuded zone grows. As the sample cools over time, the hydrides super saturate the liner- cladding interface. Precipitation becomes more preferred in the cladding and the denuded zone shrinks. This is supported by images of sample quenched from 400°C where an even distribution of hydrides was observed. A model was created based on efforts by Courty, et al. to predict hydrogen loss in spent fuel cladding during dry storage. Results from LECO analysis were used to find an appropriate dissolution activation energy to match results for H loss.after a fifteen day controlled cool from 400°C to 200°C Comparisons were made between the developed model and quantitative metallographic analysis. Model results did not align with metallographic analysis. The team would like to thank Paul Cantonwine, Jameson Root, John Holaday, Lisa Rueschloff, Andrew Kustas, and Kevin Chaput for their assistance and guidance on this project. Samples were encapsulated in glass ampoules to allow for heat treatment in an inert environment. Five total heat treatments were performed: a 32-day isothermal heat treatment at 440°C, and four step- wise slow cools from 400°C-200°C over a period of 15, 4, 2, and 1 days. The samples were imaged using back scattered electron detection at maximum contrast and 15 kV to clearly show the hydrides. Hydrides were generally circumferentially oriented, with a thicker band of hydrides in the zirconium - Zircaloy-2 boundary. SEM micrographs of hydrides in 320 ppm sample, as-received (left) and after a 16-day heat treatment (right). Further research is recommended on the effects of terminal solid solubility on temperature at concentrations above 80 ppm. Currently, hydrogen loss out of the sample is not considered in any other published research. Further tests need to be completed to monitor both hydride distribution and hydrogen leaving the sample after heat treatments of various lengths. Longer heat treatment times, more representative of long-term storage, should also be considered while monitoring the denuded zone thickness. Serial sectioning of samples, as well as further metallurgical analysis is also recommended to get a more accurate picture of the microstructure through the length of the sample tube. Recommendations Stereology Sealed ends of borosilicate ampoules. Samples are visible, measuring approximately ⅛ by 1/16 inch. Quantitative metallographic analysis was used in conjunction with stereology to calculate the volume fraction of delta hydrides and surface area of hydrides per unit volume of cladding. An area lacking in hydrides known as the denuded zone was also monitored. References Evaluation of the Technical Basis for Extended Dry Storage and Transportation of Used Nuclear Fuel - Executive Summary. (2010). United States Nuclear Waste Technical Review Board Dunavant, R., Lutz, D., & Cantonwine, P. (2013). Performance Considerations for Used BWR Fuel in Dry Storage and Transportation. Courty, O., Motta, A., & Hales, J. (2014). Modeling and simulation of hydrogen behavior in Zircaloy-4 fuel cladding. Journal of Nuclear Materials, 311-320. Underwood, E. (1970). Quantitative stereology. Reading, Mass.: Addison-Wesley Publishing Company. Sugisaki, M., Hashizume, K., & Hatano, Y. (n.d.). Estimation of hydrogen redistribution in Zircaloy cladding of spent fuel under thermal conditions of dry storage and evaluation of its influence on mechanical properties of the cladding. The Zircaloy-2 samples were analyzed with energy dispersive x-ray spectroscopy and confirmed to have the correct composition. SEM micrographs of sample liner (left) and cladding (right). The isothermal heat treatment temperature was selected based on the terminal solid solubility temperature. Since samples with a range of hydrogen content were provided, a median temperature of 440°C was chosen. Tubular samples were sectioned and tested along the length of the tube for hydrogen content using testing. Variation in hydrogen content from one end to the other is due to a temperature gradient during loading. LECO testing of a sample before and after heat treatment showed loss of hydrogen. The sample went from 340 ppm in the as-received condition to 300 ppm after a 15-day heat treatment.

Preferential Hydrogen Diffusion from Zircaloy-2 Cladding to an ......nuclear fuel cladding during dry storage. To assist in this effort, the following data were obtained from hydrogen-charged

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  • Preferential Hydrogen Diffusion from Zircaloy-2 Cladding to an Inner Zr BarrierZachary Campbell, Edite M. Grendze, Ian Hamilton, Michael ToomeyFaculty Advisor: David Bahr, Mysore DayanandaIndustrial Sponsor: Dan Lutz

    Project Background

    GNF has expressed interest in modeling to predict diffusion, precipitation, and dissolution of hydrogen in Zircaloy-2nuclear fuel cladding during dry storage. To assist in this effort, the following data were obtained from hydrogen-charged Zircaloy-2 samples. Samples were heated and then cooled from 400°C to 200°C over 1, 2, 4, and 15 days. Anisothermal test at 440°C for 32 days was also performed. The samples were then analyzed using stereologicaltechniques. No precipitate reorientation was observed and the hydride direction was circumferential as in the as -received samples. The denuded zone thickness grew and then shrank with increasing cooling time. A loss of hydrogenfrom 340 ppm in the as-received sample to 300 ppm in a 15-day sample was observed by hydrogen analysis.

    Heat Treatments

    Microscopy

    Acknowledgements

    Results & Model

    MSE 430-440: Materials Processing and Design

    Denuded zone thickness versus heat treatment time for various concentrations.

    Phase diagram: hydrogen concentration versus temperature. Note terminal solid solubility line. (Sugisaki, et. al.)

    Four samples of varyinghydrogen content werereceived for testing.

    This work is sponsored by GE-Hitachi Global Nuclear Fuels, Wilmington, NC.

    ● Zircaloy-2 is an alloy of 98.8% Zr and 1.2% Snwith trace Fe, Cr and Ni used for nuclear fuelcladding in boiling water reactors. Theprecipitation of hydrides in Zircaloy-2 can lead toembrittlement and eventual failure of the cladding.

    ● Due to the high temperatures reached in thereactor, the metal corrodes, and hydrogen isemitted. This hydrogen diffuses into the claddingand a zirconium hydride phase precipitates oncethe terminal solid solubility of hydrogen is reached.

    ● After spent nuclear fuel rods have been cooled ina spent fuel pool, they are moved into dry storagecontainers for more permanent disposal. Duringinsertion into the dry storage casks, thetemperature within the cask peaks atapproximately 400°C, then cools to 350°C.

    ● Previous research (Courty, et al.) suggests thatafter reaching the solid solubility limit, hydridesprefer to precipitate on the edge of the cladding.

    ● If orientated radially, the hydrides can bedetrimental to the structural integrity of thecladding edge.

    Denuded zone thickness varies with length of heattreatment. The data does not have a linear fit. Thedata suggests that hydride precipitation is morefavorable in the liner of the samples. Initially, thehydrides prefer to precipitate on the liner-claddingedge and the denuded zone grows. As the samplecools over time, the hydrides super saturate the liner-cladding interface. Precipitation becomes morepreferred in the cladding and the denuded zoneshrinks. This is supported by images of samplequenched from 400°C where an even distribution ofhydrides was observed.A model was created based on efforts by Courty, etal. to predict hydrogen loss in spent fuel claddingduring dry storage. Results from LECO analysiswere used to find an appropriate dissolutionactivation energy to match results for H loss.after afifteen day controlled cool from 400°C to 200°CComparisons were made between the developedmodel and quantitative metallographic analysis.Model results did not align with metallographicanalysis.

    The team would like to thank Paul Cantonwine,Jameson Root, John Holaday, Lisa Rueschloff,Andrew Kustas, and Kevin Chaput for their assistanceand guidance on this project.

    Samples wereencapsulated in glassampoules to allow forheat treatment in aninert environment.

    Five total heat treatmentswere performed: a 32-dayisothermal heat treatmentat 440°C, and four step-wise slow cools from400°C-200°C over aperiod of 15, 4, 2, and 1days.

    The samples were imaged using back scatteredelectron detection at maximum contrast and 15 kVto clearly show the hydrides. Hydrides weregenerally circumferentially oriented, with a thickerband of hydrides in the zirconium - Zircaloy-2boundary.

    SEM micrographs of hydrides in 320 ppm sample, as-received (left) and after a 16-day heat treatment (right).

    ● Further research is recommended on the effectsof terminal solid solubility on temperature atconcentrations above 80 ppm.

    ● Currently, hydrogen loss out of the sample is notconsidered in any other published research.Further tests need to be completed to monitorboth hydride distribution and hydrogen leavingthe sample after heat treatments of variouslengths. Longer heat treatment times, morerepresentative of long-term storage, should alsobe considered while monitoring the denuded zonethickness.

    ● Serial sectioning of samples, as well as furthermetallurgical analysis is also recommended to geta more accurate picture of the microstructurethrough the length of the sample tube.

    Recommendations

    Stereology

    Sealed ends of borosilicate ampoules. Samples are visible, measuring approximately ⅛ by 1/16 inch.

    Quantitative metallographic analysis was used in conjunction with stereology to calculate the volume fraction of delta hydrides and surface area of hydrides per unit volume of cladding. An area lacking in hydrides known as the denuded zone was also monitored.

    ReferencesEvaluation of the Technical Basis for Extended Dry Storage and Transportation of Used Nuclear Fuel- Executive Summary. (2010). United States Nuclear Waste Technical Review Board

    Dunavant, R., Lutz, D., & Cantonwine, P. (2013). Performance Considerations for Used BWR Fuel inDry Storage and Transportation.

    Courty, O., Motta, A., & Hales, J. (2014). Modeling and simulation of hydrogen behavior in Zircaloy-4fuel cladding. Journal of Nuclear Materials, 311-320.

    Underwood, E. (1970). Quantitative stereology. Reading, Mass.: Addison-Wesley PublishingCompany.

    Sugisaki, M., Hashizume, K., & Hatano, Y. (n.d.). Estimation of hydrogen redistribution in Zircaloycladding of spent fuel under thermal conditions of dry storage and evaluation of its influence onmechanical properties of the cladding.

    The Zircaloy-2 samples were analyzed with energydispersive x-ray spectroscopy and confirmed tohave the correct composition.

    SEM micrographs of sample liner (left) and cladding (right).

    The isothermal heat treatment temperature wasselected based on the terminal solid solubilitytemperature. Since samples with a range ofhydrogen content were provided, a mediantemperature of 440°C was chosen.

    Tubular samples were sectioned and tested alongthe length of the tube for hydrogen content usingtesting. Variation in hydrogen content from one endto the other is due to a temperature gradient duringloading.

    LECO testing of a sample before and after heattreatment showed loss of hydrogen. The samplewent from 340 ppm in the as-received conditionto 300 ppm after a 15-day heat treatment.

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