Advances in Ejecta Diagnostics at LLNL
Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagno...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Steele, P. T. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2017 |
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| Schlagwörter: |
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| Anmerkung: |
© Society for Experimental Mechanics, Inc (outside the US) 2017 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of dynamic behavior of materials - Berlin [u.a.] : Springer, 2015, 3(2017), 2 vom: 31. Mai, Seite 253-264 |
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| Übergeordnetes Werk: |
volume:3 ; year:2017 ; number:2 ; day:31 ; month:05 ; pages:253-264 |
| Links: |
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| DOI / URN: |
10.1007/s40870-017-0119-1 |
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| Katalog-ID: |
SPR037949896 |
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| 520 | |a Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. | ||
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| 650 | 4 | |a Mie scattering |7 (dpeaa)DE-He213 | |
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| 700 | 1 | |a Jacoby, B. A. |4 aut | |
| 700 | 1 | |a Compton, S. M. |4 aut | |
| 700 | 1 | |a Sinibaldi, J. O. |4 aut | |
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10.1007/s40870-017-0119-1 doi (DE-627)SPR037949896 (SPR)s40870-017-0119-1-e DE-627 ger DE-627 rakwb eng Steele, P. T. verfasserin aut Advances in Ejecta Diagnostics at LLNL 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Society for Experimental Mechanics, Inc (outside the US) 2017 Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. Asay foils (dpeaa)DE-He213 Mie scattering (dpeaa)DE-He213 Ejecta (dpeaa)DE-He213 Jacoby, B. A. aut Compton, S. M. aut Sinibaldi, J. O. aut Enthalten in Journal of dynamic behavior of materials Berlin [u.a.] : Springer, 2015 3(2017), 2 vom: 31. Mai, Seite 253-264 (DE-627)815914458 (DE-600)2806649-2 2199-7454 nnns volume:3 year:2017 number:2 day:31 month:05 pages:253-264 https://dx.doi.org/10.1007/s40870-017-0119-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2017 2 31 05 253-264 |
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10.1007/s40870-017-0119-1 doi (DE-627)SPR037949896 (SPR)s40870-017-0119-1-e DE-627 ger DE-627 rakwb eng Steele, P. T. verfasserin aut Advances in Ejecta Diagnostics at LLNL 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Society for Experimental Mechanics, Inc (outside the US) 2017 Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. Asay foils (dpeaa)DE-He213 Mie scattering (dpeaa)DE-He213 Ejecta (dpeaa)DE-He213 Jacoby, B. A. aut Compton, S. M. aut Sinibaldi, J. O. aut Enthalten in Journal of dynamic behavior of materials Berlin [u.a.] : Springer, 2015 3(2017), 2 vom: 31. Mai, Seite 253-264 (DE-627)815914458 (DE-600)2806649-2 2199-7454 nnns volume:3 year:2017 number:2 day:31 month:05 pages:253-264 https://dx.doi.org/10.1007/s40870-017-0119-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2017 2 31 05 253-264 |
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10.1007/s40870-017-0119-1 doi (DE-627)SPR037949896 (SPR)s40870-017-0119-1-e DE-627 ger DE-627 rakwb eng Steele, P. T. verfasserin aut Advances in Ejecta Diagnostics at LLNL 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Society for Experimental Mechanics, Inc (outside the US) 2017 Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. Asay foils (dpeaa)DE-He213 Mie scattering (dpeaa)DE-He213 Ejecta (dpeaa)DE-He213 Jacoby, B. A. aut Compton, S. M. aut Sinibaldi, J. O. aut Enthalten in Journal of dynamic behavior of materials Berlin [u.a.] : Springer, 2015 3(2017), 2 vom: 31. Mai, Seite 253-264 (DE-627)815914458 (DE-600)2806649-2 2199-7454 nnns volume:3 year:2017 number:2 day:31 month:05 pages:253-264 https://dx.doi.org/10.1007/s40870-017-0119-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2017 2 31 05 253-264 |
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10.1007/s40870-017-0119-1 doi (DE-627)SPR037949896 (SPR)s40870-017-0119-1-e DE-627 ger DE-627 rakwb eng Steele, P. T. verfasserin aut Advances in Ejecta Diagnostics at LLNL 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Society for Experimental Mechanics, Inc (outside the US) 2017 Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. Asay foils (dpeaa)DE-He213 Mie scattering (dpeaa)DE-He213 Ejecta (dpeaa)DE-He213 Jacoby, B. A. aut Compton, S. M. aut Sinibaldi, J. O. aut Enthalten in Journal of dynamic behavior of materials Berlin [u.a.] : Springer, 2015 3(2017), 2 vom: 31. Mai, Seite 253-264 (DE-627)815914458 (DE-600)2806649-2 2199-7454 nnns volume:3 year:2017 number:2 day:31 month:05 pages:253-264 https://dx.doi.org/10.1007/s40870-017-0119-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2017 2 31 05 253-264 |
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Steele, P. T. @@aut@@ Jacoby, B. A. @@aut@@ Compton, S. M. @@aut@@ Sinibaldi, J. O. @@aut@@ |
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Advances in Ejecta Diagnostics at LLNL Asay foils (dpeaa)DE-He213 Mie scattering (dpeaa)DE-He213 Ejecta (dpeaa)DE-He213 |
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Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. © Society for Experimental Mechanics, Inc (outside the US) 2017 |
| abstractGer |
Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. © Society for Experimental Mechanics, Inc (outside the US) 2017 |
| abstract_unstemmed |
Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging. © Society for Experimental Mechanics, Inc (outside the US) 2017 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR037949896</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230328194535.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2017 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s40870-017-0119-1</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR037949896</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s40870-017-0119-1-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Steele, P. T.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Advances in Ejecta Diagnostics at LLNL</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Society for Experimental Mechanics, Inc (outside the US) 2017</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Renewed interest in ejecta experiments at Lawrence Livermore National Laboratory has motivated reinvestigation and refinement of historical ejecta diagnostics as well as development of new diagnostics. Two diagnostics are discussed here: Asay foils and the multi-wavelength extinction diagnostic. Both are capable, in theory, of measuring ejecta mass or density as a function of time, but they work in fundamentally different ways and rely upon different assumptions. Significant changes have been made in the design of historical Asay foil assemblies. Associated experiments and modeling efforts are described. Ultimately, a miniaturized assembly has been made and tested that works in any orientation and produces data matching larger, historical designs. The ongoing development of the multi-wavelength extinction diagnostic is also described. The goal of this diagnostic is not just to measure ejecta mass but also the temporal evolution of the ejecta particle size distribution. Preliminary modeling and experiments are encouraging.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Asay foils</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Mie scattering</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ejecta</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jacoby, B. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Compton, S. M.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sinibaldi, J. O.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of dynamic behavior of materials</subfield><subfield code="d">Berlin [u.a.] : Springer, 2015</subfield><subfield code="g">3(2017), 2 vom: 31. Mai, Seite 253-264</subfield><subfield code="w">(DE-627)815914458</subfield><subfield code="w">(DE-600)2806649-2</subfield><subfield code="x">2199-7454</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:3</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:2</subfield><subfield code="g">day:31</subfield><subfield code="g">month:05</subfield><subfield code="g">pages:253-264</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s40870-017-0119-1</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" 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