Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids
Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experi...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Malinarič, Svetozár [verfasserIn] Dieška, Peter [verfasserIn] Krupa, Peter [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2012 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: International journal of thermophysics - New York, NY : Springer Science + Business Media B.V., 1980, 33(2012), 3 vom: 29. Feb., Seite 528-539 |
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| Übergeordnetes Werk: |
volume:33 ; year:2012 ; number:3 ; day:29 ; month:02 ; pages:528-539 |
| Links: |
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| DOI / URN: |
10.1007/s10765-012-1173-5 |
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| Katalog-ID: |
SPR013106635 |
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| 520 | |a Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. | ||
| 650 | 4 | |a Modified dynamic plane source method |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Polymethylmethacrylate |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Thermal conductivity |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Thermal diffusivity |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Transient plane source method |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Dieška, Peter |e verfasserin |4 aut | |
| 700 | 1 | |a Krupa, Peter |e verfasserin |4 aut | |
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10.1007/s10765-012-1173-5 doi (DE-627)SPR013106635 (SPR)s10765-012-1173-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Malinarič, Svetozár verfasserin aut Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. Modified dynamic plane source method (dpeaa)DE-He213 Polymethylmethacrylate (dpeaa)DE-He213 Thermal conductivity (dpeaa)DE-He213 Thermal diffusivity (dpeaa)DE-He213 Transient plane source method (dpeaa)DE-He213 Dieška, Peter verfasserin aut Krupa, Peter verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 33(2012), 3 vom: 29. Feb., Seite 528-539 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:33 year:2012 number:3 day:29 month:02 pages:528-539 https://dx.doi.org/10.1007/s10765-012-1173-5 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 33.00 ASE AR 33 2012 3 29 02 528-539 |
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10.1007/s10765-012-1173-5 doi (DE-627)SPR013106635 (SPR)s10765-012-1173-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Malinarič, Svetozár verfasserin aut Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. Modified dynamic plane source method (dpeaa)DE-He213 Polymethylmethacrylate (dpeaa)DE-He213 Thermal conductivity (dpeaa)DE-He213 Thermal diffusivity (dpeaa)DE-He213 Transient plane source method (dpeaa)DE-He213 Dieška, Peter verfasserin aut Krupa, Peter verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 33(2012), 3 vom: 29. Feb., Seite 528-539 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:33 year:2012 number:3 day:29 month:02 pages:528-539 https://dx.doi.org/10.1007/s10765-012-1173-5 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 33.00 ASE AR 33 2012 3 29 02 528-539 |
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10.1007/s10765-012-1173-5 doi (DE-627)SPR013106635 (SPR)s10765-012-1173-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Malinarič, Svetozár verfasserin aut Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. Modified dynamic plane source method (dpeaa)DE-He213 Polymethylmethacrylate (dpeaa)DE-He213 Thermal conductivity (dpeaa)DE-He213 Thermal diffusivity (dpeaa)DE-He213 Transient plane source method (dpeaa)DE-He213 Dieška, Peter verfasserin aut Krupa, Peter verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 33(2012), 3 vom: 29. Feb., Seite 528-539 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:33 year:2012 number:3 day:29 month:02 pages:528-539 https://dx.doi.org/10.1007/s10765-012-1173-5 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 33.00 ASE AR 33 2012 3 29 02 528-539 |
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10.1007/s10765-012-1173-5 doi (DE-627)SPR013106635 (SPR)s10765-012-1173-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Malinarič, Svetozár verfasserin aut Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. Modified dynamic plane source method (dpeaa)DE-He213 Polymethylmethacrylate (dpeaa)DE-He213 Thermal conductivity (dpeaa)DE-He213 Thermal diffusivity (dpeaa)DE-He213 Transient plane source method (dpeaa)DE-He213 Dieška, Peter verfasserin aut Krupa, Peter verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 33(2012), 3 vom: 29. Feb., Seite 528-539 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:33 year:2012 number:3 day:29 month:02 pages:528-539 https://dx.doi.org/10.1007/s10765-012-1173-5 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 33.00 ASE AR 33 2012 3 29 02 528-539 |
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10.1007/s10765-012-1173-5 doi (DE-627)SPR013106635 (SPR)s10765-012-1173-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Malinarič, Svetozár verfasserin aut Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. Modified dynamic plane source method (dpeaa)DE-He213 Polymethylmethacrylate (dpeaa)DE-He213 Thermal conductivity (dpeaa)DE-He213 Thermal diffusivity (dpeaa)DE-He213 Transient plane source method (dpeaa)DE-He213 Dieška, Peter verfasserin aut Krupa, Peter verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 33(2012), 3 vom: 29. Feb., Seite 528-539 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:33 year:2012 number:3 day:29 month:02 pages:528-539 https://dx.doi.org/10.1007/s10765-012-1173-5 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 33.00 ASE AR 33 2012 3 29 02 528-539 |
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Malinarič, Svetozár @@aut@@ Dieška, Peter @@aut@@ Krupa, Peter @@aut@@ |
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| author |
Malinarič, Svetozár |
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Malinarič, Svetozár ddc 530 bkl 33.00 misc Modified dynamic plane source method misc Polymethylmethacrylate misc Thermal conductivity misc Thermal diffusivity misc Transient plane source method Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids |
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Malinarič, Svetozár |
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530 ASE 33.00 bkl Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids Modified dynamic plane source method (dpeaa)DE-He213 Polymethylmethacrylate (dpeaa)DE-He213 Thermal conductivity (dpeaa)DE-He213 Thermal diffusivity (dpeaa)DE-He213 Transient plane source method (dpeaa)DE-He213 |
| topic |
ddc 530 bkl 33.00 misc Modified dynamic plane source method misc Polymethylmethacrylate misc Thermal conductivity misc Thermal diffusivity misc Transient plane source method |
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ddc 530 bkl 33.00 misc Modified dynamic plane source method misc Polymethylmethacrylate misc Thermal conductivity misc Thermal diffusivity misc Transient plane source method |
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ddc 530 bkl 33.00 misc Modified dynamic plane source method misc Polymethylmethacrylate misc Thermal conductivity misc Thermal diffusivity misc Transient plane source method |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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International journal of thermophysics |
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International journal of thermophysics |
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(DE-627)319584321 (DE-600)2016169-4 |
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Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids |
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(DE-627)SPR013106635 (SPR)s10765-012-1173-5-e |
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Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids |
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Malinarič, Svetozár |
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International journal of thermophysics |
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International journal of thermophysics |
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eng |
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2012 |
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Malinarič, Svetozár Dieška, Peter Krupa, Peter |
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530 ASE 33.00 bkl |
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Elektronische Aufsätze |
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Malinarič, Svetozár |
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10.1007/s10765-012-1173-5 |
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530 |
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verfasserin |
| title_sort |
modified dynamic plane source method for measuring thermophysical parameters of solids |
| title_auth |
Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids |
| abstract |
Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. |
| abstractGer |
Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. |
| abstract_unstemmed |
Abstract The authors proposed and experimentally verified a new method of measurements of thermal conductivity and thermal diffusivity of homogeneous and isotropic materials with thermal conductivities of <%${2\,{\rm W} \cdot{\rm m}^{-1} \cdot{\rm K}^{-1}}%$ . The theoretical model and the experimental arrangement of the method, referred to as the modified dynamic plane source method, are described. The influence of the floating temperature of the heat sink was analyzed and included into the evaluation. The method was both theoretically and experimentally compared with other transient methods, namely, transient plane source and extended dynamic plane source methods. Two different polymethylmethacrylate materials were measured at laboratory temperature using all three methods, obtaining results with coefficients of variation of <2 % and 5 % for the thermal conductivity and thermal diffusivity, respectively. In addition, the sensor calibration and the sources of measurement uncertainty are outlined. |
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Modified Dynamic Plane Source Method for Measuring Thermophysical Parameters of Solids |
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https://dx.doi.org/10.1007/s10765-012-1173-5 |
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Dieška, Peter Krupa, Peter |
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10.1007/s10765-012-1173-5 |
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2024-07-03T17:30:12.998Z |
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| score |
7.3985195 |