Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process

Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet ru...
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Autor*in:	Chen, Hai-long [verfasserIn] Li, Tao [verfasserIn] Xing, Kai [verfasserIn] Li, Kun-ling [verfasserIn] Zhang, Mao-dong [verfasserIn] Li, Qing-ling [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2017

Schlagwörter:	Rubber Microwave power Microwave vulcanization The rate of temperature rising Temperature distribution

Übergeordnetes Werk:	Enthalten in: Journal of thermal analysis and calorimetry - Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969, 130(2017), 3 vom: 24. Juli, Seite 2079-2091
Übergeordnetes Werk:	volume:130 ; year:2017 ; number:3 ; day:24 ; month:07 ; pages:2079-2091

Links:	Volltext

DOI / URN:	10.1007/s10973-017-6601-0

Katalog-ID:	SPR015605337

Internformat


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245	1	0	\|a Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
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520			\|a Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone.
650		4	\|a Rubber \|7 (dpeaa)DE-He213
650		4	\|a Microwave power \|7 (dpeaa)DE-He213
650		4	\|a Microwave vulcanization \|7 (dpeaa)DE-He213
650		4	\|a The rate of temperature rising \|7 (dpeaa)DE-He213
650		4	\|a Temperature distribution \|7 (dpeaa)DE-He213
700	1		\|a Li, Tao \|e verfasserin \|4 aut
700	1		\|a Xing, Kai \|e verfasserin \|4 aut
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700	1		\|a Zhang, Mao-dong \|e verfasserin \|4 aut
700	1		\|a Li, Qing-ling \|e verfasserin \|4 aut
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912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
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912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
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912			\|a GBV_ILN_2025
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912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
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912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
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952			\|d 130 \|j 2017 \|e 3 \|b 24 \|c 07 \|h 2079-2091

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author_variant	h l c hlc t l tl k x kx k l l kll m d z mdz q l l qll
matchkey_str	article:15728943:2017----::xeietlnetgtootcnlgclodtosntmeaueitiuinnubraeil
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publishDate	2017
allfields	10.1007/s10973-017-6601-0 doi (DE-627)SPR015605337 (SPR)s10973-017-6601-0-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Chen, Hai-long verfasserin aut Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone. Rubber (dpeaa)DE-He213 Microwave power (dpeaa)DE-He213 Microwave vulcanization (dpeaa)DE-He213 The rate of temperature rising (dpeaa)DE-He213 Temperature distribution (dpeaa)DE-He213 Li, Tao verfasserin aut Xing, Kai verfasserin aut Li, Kun-ling verfasserin aut Zhang, Mao-dong verfasserin aut Li, Qing-ling verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 130(2017), 3 vom: 24. Juli, Seite 2079-2091 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091 https://dx.doi.org/10.1007/s10973-017-6601-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA 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_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_206 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_2056 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 130 2017 3 24 07 2079-2091
spelling	10.1007/s10973-017-6601-0 doi (DE-627)SPR015605337 (SPR)s10973-017-6601-0-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Chen, Hai-long verfasserin aut Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone. Rubber (dpeaa)DE-He213 Microwave power (dpeaa)DE-He213 Microwave vulcanization (dpeaa)DE-He213 The rate of temperature rising (dpeaa)DE-He213 Temperature distribution (dpeaa)DE-He213 Li, Tao verfasserin aut Xing, Kai verfasserin aut Li, Kun-ling verfasserin aut Zhang, Mao-dong verfasserin aut Li, Qing-ling verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 130(2017), 3 vom: 24. Juli, Seite 2079-2091 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091 https://dx.doi.org/10.1007/s10973-017-6601-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA 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_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_206 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_2056 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 130 2017 3 24 07 2079-2091
allfields_unstemmed	10.1007/s10973-017-6601-0 doi (DE-627)SPR015605337 (SPR)s10973-017-6601-0-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Chen, Hai-long verfasserin aut Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone. Rubber (dpeaa)DE-He213 Microwave power (dpeaa)DE-He213 Microwave vulcanization (dpeaa)DE-He213 The rate of temperature rising (dpeaa)DE-He213 Temperature distribution (dpeaa)DE-He213 Li, Tao verfasserin aut Xing, Kai verfasserin aut Li, Kun-ling verfasserin aut Zhang, Mao-dong verfasserin aut Li, Qing-ling verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 130(2017), 3 vom: 24. Juli, Seite 2079-2091 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091 https://dx.doi.org/10.1007/s10973-017-6601-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA 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_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_206 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_2056 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 130 2017 3 24 07 2079-2091
allfieldsGer	10.1007/s10973-017-6601-0 doi (DE-627)SPR015605337 (SPR)s10973-017-6601-0-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Chen, Hai-long verfasserin aut Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone. Rubber (dpeaa)DE-He213 Microwave power (dpeaa)DE-He213 Microwave vulcanization (dpeaa)DE-He213 The rate of temperature rising (dpeaa)DE-He213 Temperature distribution (dpeaa)DE-He213 Li, Tao verfasserin aut Xing, Kai verfasserin aut Li, Kun-ling verfasserin aut Zhang, Mao-dong verfasserin aut Li, Qing-ling verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 130(2017), 3 vom: 24. Juli, Seite 2079-2091 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091 https://dx.doi.org/10.1007/s10973-017-6601-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA 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_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_206 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_2056 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 130 2017 3 24 07 2079-2091
allfieldsSound	10.1007/s10973-017-6601-0 doi (DE-627)SPR015605337 (SPR)s10973-017-6601-0-e DE-627 ger DE-627 rakwb eng 660 ASE 35.00 bkl Chen, Hai-long verfasserin aut Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone. Rubber (dpeaa)DE-He213 Microwave power (dpeaa)DE-He213 Microwave vulcanization (dpeaa)DE-He213 The rate of temperature rising (dpeaa)DE-He213 Temperature distribution (dpeaa)DE-He213 Li, Tao verfasserin aut Xing, Kai verfasserin aut Li, Kun-ling verfasserin aut Zhang, Mao-dong verfasserin aut Li, Qing-ling verfasserin aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 130(2017), 3 vom: 24. Juli, Seite 2079-2091 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091 https://dx.doi.org/10.1007/s10973-017-6601-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA 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_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_206 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_2056 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 35.00 ASE AR 130 2017 3 24 07 2079-2091
language	English
source	Enthalten in Journal of thermal analysis and calorimetry 130(2017), 3 vom: 24. Juli, Seite 2079-2091 volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091
sourceStr	Enthalten in Journal of thermal analysis and calorimetry 130(2017), 3 vom: 24. Juli, Seite 2079-2091 volume:130 year:2017 number:3 day:24 month:07 pages:2079-2091
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Rubber Microwave power Microwave vulcanization The rate of temperature rising Temperature distribution
dewey-raw	660
isfreeaccess_bool	false
container_title	Journal of thermal analysis and calorimetry
authorswithroles_txt_mv	Chen, Hai-long @@aut@@ Li, Tao @@aut@@ Xing, Kai @@aut@@ Li, Kun-ling @@aut@@ Zhang, Mao-dong @@aut@@ Li, Qing-ling @@aut@@
publishDateDaySort_date	2017-07-24T00:00:00Z
hierarchy_top_id	315295422
dewey-sort	3660
id	SPR015605337
language_de	englisch
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author	Chen, Hai-long
spellingShingle	Chen, Hai-long ddc 660 bkl 35.00 misc Rubber misc Microwave power misc Microwave vulcanization misc The rate of temperature rising misc Temperature distribution Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
authorStr	Chen, Hai-long
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topic_title	660 ASE 35.00 bkl Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process Rubber (dpeaa)DE-He213 Microwave power (dpeaa)DE-He213 Microwave vulcanization (dpeaa)DE-He213 The rate of temperature rising (dpeaa)DE-He213 Temperature distribution (dpeaa)DE-He213
topic	ddc 660 bkl 35.00 misc Rubber misc Microwave power misc Microwave vulcanization misc The rate of temperature rising misc Temperature distribution
topic_unstemmed	ddc 660 bkl 35.00 misc Rubber misc Microwave power misc Microwave vulcanization misc The rate of temperature rising misc Temperature distribution
topic_browse	ddc 660 bkl 35.00 misc Rubber misc Microwave power misc Microwave vulcanization misc The rate of temperature rising misc Temperature distribution
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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hierarchy_parent_title	Journal of thermal analysis and calorimetry
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title	Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
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title_full	Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
author_sort	Chen, Hai-long
journal	Journal of thermal analysis and calorimetry
journalStr	Journal of thermal analysis and calorimetry
lang_code	eng
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author_browse	Chen, Hai-long Li, Tao Xing, Kai Li, Kun-ling Zhang, Mao-dong Li, Qing-ling
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title_sort	experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
title_auth	Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
abstract	Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone.
abstractGer	Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone.
abstract_unstemmed	Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone.
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title_short	Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process
url	https://dx.doi.org/10.1007/s10973-017-6601-0
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author2	Li, Tao Xing, Kai Li, Kun-ling Zhang, Mao-dong Li, Qing-ling
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doi_str	10.1007/s10973-017-6601-0
up_date	2024-07-03T17:19:27.834Z
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fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR015605337</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230519144907.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2017 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10973-017-6601-0</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR015605337</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10973-017-6601-0-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="082" ind1="0" ind2="4"><subfield code="a">660</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">35.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Chen, Hai-long</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process</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="520" ind1=" " ind2=" "><subfield code="a">Abstract The optical fiber temperature online monitor and the optical fiber temperature sensor were employed to measure internal temperature of sheet rubber during the microwave vulcanization process, and the infrared thermal imager was utilized to measure the temperature at the surfaces of sheet rubber. First of all, in the contrast experiment, the setting principle of microwave power was explored, the experimental results demonstrated that the rate of temperature rising within sheet rubber was higher by using high microwave power during microwave heating process, and the proper vulcanization temperature was obtained by using high and low microwave power alternately. Experimental results indicated that the output of heat during vulcanization reaction promoted the rate of temperature rising of the temperature measuring point, during the microwave vulcanization process of all experimental sheet rubber, the rate of temperature rising in the central zone of sheet rubber was higher than the rate of temperature rising in the marginal zone, the temperature distribution at the surfaces of sheet rubber presented non-uniformity, the maximum of temperature converged on the central zone of sheet rubber, and results manifested that the distribution of electric field was uneven in heating chamber. Due to the existence of heat transfer phenomenon, the area of the higher temperature zone of sheet rubber expanded gradually from the central zone to the marginal zone.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Rubber</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Microwave power</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Microwave vulcanization</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">The rate of temperature rising</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Temperature distribution</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Li, Tao</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Xing, Kai</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Li, Kun-ling</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zhang, Mao-dong</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Li, Qing-ling</subfield><subfield code="e">verfasserin</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 thermal analysis and calorimetry</subfield><subfield code="d">Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969</subfield><subfield code="g">130(2017), 3 vom: 24. Juli, Seite 2079-2091</subfield><subfield code="w">(DE-627)315295422</subfield><subfield code="w">(DE-600)2017304-0</subfield><subfield code="x">1572-8943</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:130</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:3</subfield><subfield code="g">day:24</subfield><subfield code="g">month:07</subfield><subfield code="g">pages:2079-2091</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s10973-017-6601-0</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 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Experimental investigation of technological conditions and temperature distribution in rubber material during microwave vulcanization process

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