Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K

Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data h...
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Gespeichert in:

Autor*in:	Siwach, Rajesh K. [verfasserIn] Sharma, V. K. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2011

Schlagwörter:	Aromatic hydrocarbons Connectivity parameter of third degree Excess isentropic compressibilities Isentropic compressibilities Speeds of sound Tetrahydropyran

Übergeordnetes Werk:	Enthalten in: International journal of thermophysics - New York, NY : Springer Science + Business Media B.V., 1980, 32(2011), 6 vom: 31. Mai, Seite 1188-1201
Übergeordnetes Werk:	volume:32 ; year:2011 ; number:6 ; day:31 ; month:05 ; pages:1188-1201

Links:	Volltext

DOI / URN:	10.1007/s10765-011-0997-8

Katalog-ID:	SPR01310487X

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520			\|a Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values.
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912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
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
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
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912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
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912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2116
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2119
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2144
912			\|a GBV_ILN_2147
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912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
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allfields	10.1007/s10765-011-0997-8 doi (DE-627)SPR01310487X (SPR)s10765-011-0997-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Siwach, Rajesh K. verfasserin aut Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values. Aromatic hydrocarbons (dpeaa)DE-He213 Connectivity parameter of third degree (dpeaa)DE-He213 Excess isentropic compressibilities (dpeaa)DE-He213 Isentropic compressibilities (dpeaa)DE-He213 Speeds of sound (dpeaa)DE-He213 Tetrahydropyran (dpeaa)DE-He213 Sharma, V. K. verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 32(2011), 6 vom: 31. Mai, Seite 1188-1201 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201 https://dx.doi.org/10.1007/s10765-011-0997-8 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 32 2011 6 31 05 1188-1201
spelling	10.1007/s10765-011-0997-8 doi (DE-627)SPR01310487X (SPR)s10765-011-0997-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Siwach, Rajesh K. verfasserin aut Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values. Aromatic hydrocarbons (dpeaa)DE-He213 Connectivity parameter of third degree (dpeaa)DE-He213 Excess isentropic compressibilities (dpeaa)DE-He213 Isentropic compressibilities (dpeaa)DE-He213 Speeds of sound (dpeaa)DE-He213 Tetrahydropyran (dpeaa)DE-He213 Sharma, V. K. verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 32(2011), 6 vom: 31. Mai, Seite 1188-1201 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201 https://dx.doi.org/10.1007/s10765-011-0997-8 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 32 2011 6 31 05 1188-1201
allfields_unstemmed	10.1007/s10765-011-0997-8 doi (DE-627)SPR01310487X (SPR)s10765-011-0997-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Siwach, Rajesh K. verfasserin aut Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values. Aromatic hydrocarbons (dpeaa)DE-He213 Connectivity parameter of third degree (dpeaa)DE-He213 Excess isentropic compressibilities (dpeaa)DE-He213 Isentropic compressibilities (dpeaa)DE-He213 Speeds of sound (dpeaa)DE-He213 Tetrahydropyran (dpeaa)DE-He213 Sharma, V. K. verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 32(2011), 6 vom: 31. Mai, Seite 1188-1201 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201 https://dx.doi.org/10.1007/s10765-011-0997-8 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 32 2011 6 31 05 1188-1201
allfieldsGer	10.1007/s10765-011-0997-8 doi (DE-627)SPR01310487X (SPR)s10765-011-0997-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Siwach, Rajesh K. verfasserin aut Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values. Aromatic hydrocarbons (dpeaa)DE-He213 Connectivity parameter of third degree (dpeaa)DE-He213 Excess isentropic compressibilities (dpeaa)DE-He213 Isentropic compressibilities (dpeaa)DE-He213 Speeds of sound (dpeaa)DE-He213 Tetrahydropyran (dpeaa)DE-He213 Sharma, V. K. verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 32(2011), 6 vom: 31. Mai, Seite 1188-1201 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201 https://dx.doi.org/10.1007/s10765-011-0997-8 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 32 2011 6 31 05 1188-1201
allfieldsSound	10.1007/s10765-011-0997-8 doi (DE-627)SPR01310487X (SPR)s10765-011-0997-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Siwach, Rajesh K. verfasserin aut Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values. Aromatic hydrocarbons (dpeaa)DE-He213 Connectivity parameter of third degree (dpeaa)DE-He213 Excess isentropic compressibilities (dpeaa)DE-He213 Isentropic compressibilities (dpeaa)DE-He213 Speeds of sound (dpeaa)DE-He213 Tetrahydropyran (dpeaa)DE-He213 Sharma, V. K. verfasserin aut Enthalten in International journal of thermophysics New York, NY : Springer Science + Business Media B.V., 1980 32(2011), 6 vom: 31. Mai, Seite 1188-1201 (DE-627)319584321 (DE-600)2016169-4 1572-9567 nnns volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201 https://dx.doi.org/10.1007/s10765-011-0997-8 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 32 2011 6 31 05 1188-1201
language	English
source	Enthalten in International journal of thermophysics 32(2011), 6 vom: 31. Mai, Seite 1188-1201 volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201
sourceStr	Enthalten in International journal of thermophysics 32(2011), 6 vom: 31. Mai, Seite 1188-1201 volume:32 year:2011 number:6 day:31 month:05 pages:1188-1201
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Aromatic hydrocarbons Connectivity parameter of third degree Excess isentropic compressibilities Isentropic compressibilities Speeds of sound Tetrahydropyran
dewey-raw	530
isfreeaccess_bool	false
container_title	International journal of thermophysics
authorswithroles_txt_mv	Siwach, Rajesh K. @@aut@@ Sharma, V. K. @@aut@@
publishDateDaySort_date	2011-05-31T00:00:00Z
hierarchy_top_id	319584321
dewey-sort	3530
id	SPR01310487X
language_de	englisch
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author	Siwach, Rajesh K.
spellingShingle	Siwach, Rajesh K. ddc 530 bkl 33.00 misc Aromatic hydrocarbons misc Connectivity parameter of third degree misc Excess isentropic compressibilities misc Isentropic compressibilities misc Speeds of sound misc Tetrahydropyran Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K
authorStr	Siwach, Rajesh K.
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topic_title	530 ASE 33.00 bkl Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K Aromatic hydrocarbons (dpeaa)DE-He213 Connectivity parameter of third degree (dpeaa)DE-He213 Excess isentropic compressibilities (dpeaa)DE-He213 Isentropic compressibilities (dpeaa)DE-He213 Speeds of sound (dpeaa)DE-He213 Tetrahydropyran (dpeaa)DE-He213
topic	ddc 530 bkl 33.00 misc Aromatic hydrocarbons misc Connectivity parameter of third degree misc Excess isentropic compressibilities misc Isentropic compressibilities misc Speeds of sound misc Tetrahydropyran
topic_unstemmed	ddc 530 bkl 33.00 misc Aromatic hydrocarbons misc Connectivity parameter of third degree misc Excess isentropic compressibilities misc Isentropic compressibilities misc Speeds of sound misc Tetrahydropyran
topic_browse	ddc 530 bkl 33.00 misc Aromatic hydrocarbons misc Connectivity parameter of third degree misc Excess isentropic compressibilities misc Isentropic compressibilities misc Speeds of sound misc Tetrahydropyran
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title	Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K
ctrlnum	(DE-627)SPR01310487X (SPR)s10765-011-0997-8-e
title_full	Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K
author_sort	Siwach, Rajesh K.
journal	International journal of thermophysics
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author_browse	Siwach, Rajesh K. Sharma, V. K.
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class	530 ASE 33.00 bkl
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author-letter	Siwach, Rajesh K.
doi_str_mv	10.1007/s10765-011-0997-8
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title_sort	sound speeds and excess isentropic compressibilities of ternary mixtures of tetrahydropyran and aromatic hydrocarbons at 308.15 k
title_auth	Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K
abstract	Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values.
abstractGer	Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values.
abstract_unstemmed	Abstract Speeds of sound, uijk, of tetrahydropyran (THP) (i) + benzene (j) + toluene or o- or p-xylene (k), and tetrahydropyran (i)+toluene (j) + o- or p-xylene (k) ternary mixtures have been measured over the entire mole fraction range at 308.15 K and atmospheric pressure. The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). It has been observed that %${(\kappa_S)_{ijk}}%$ values predicted by the Moelwyn–Huggins concept compare well with corresponding experimental values.
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title_short	Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K
url	https://dx.doi.org/10.1007/s10765-011-0997-8
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doi_str	10.1007/s10765-011-0997-8
up_date	2024-07-03T17:29:30.527Z
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The speed-of-sound data have been used to calculate isentropic compressibilities, %${(\kappa_S)_{ijk}}%$ , and excess isentropic compressibilities, %${(\kappa_S^{\rm E})_{ijk}}%$ . The %${(\kappa_S^{\rm E})_{ijk}}%$ values for the investigated mixtures are correlated with the Redlich–Kister equation to estimate ternary adjustable parameters and standard deviations. The Moelwyn–Huggins concept (Huggins, Polymer 12:357, 1971) of interaction between the surfaces of components of binary mixtures has been extended to predict excess isentropic compressibilities of ternary mixtures by employing the concept of connectivity parameters of the third degree of a molecule (which in turn depends on its topology). 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Sound Speeds and Excess Isentropic Compressibilities of Ternary Mixtures of Tetrahydropyran and Aromatic Hydrocarbons at 308.15 K

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