Thermal analysis of oblique stagnation point flow with slippage on second-order fluid
Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an inco...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Awan, Aziz Ullah [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Schlagwörter: |
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| Anmerkung: |
© Akadémiai Kiadó, Budapest, Hungary 2021 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of thermal analysis and calorimetry - Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969, 147(2021), 5 vom: 13. Apr., Seite 3839-3851 |
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| Übergeordnetes Werk: |
volume:147 ; year:2021 ; number:5 ; day:13 ; month:04 ; pages:3839-3851 |
| Links: |
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| DOI / URN: |
10.1007/s10973-021-10760-z |
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| Katalog-ID: |
SPR046211373 |
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| 245 | 1 | 0 | |a Thermal analysis of oblique stagnation point flow with slippage on second-order fluid |
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| 520 | |a Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. | ||
| 650 | 4 | |a Oblique stagnation point flow |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Second-grade fluid |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Buongiorno model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Slip effects |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Aziz, Mashal |4 aut | |
| 700 | 1 | |a Ullah, Naeem |4 aut | |
| 700 | 1 | |a Nadeem, Sohail |4 aut | |
| 700 | 1 | |a Abro, Kashif Ali |0 (orcid)0000-0003-0867-642X |4 aut | |
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10.1007/s10973-021-10760-z doi (DE-627)SPR046211373 (SPR)s10973-021-10760-z-e DE-627 ger DE-627 rakwb eng Awan, Aziz Ullah verfasserin aut Thermal analysis of oblique stagnation point flow with slippage on second-order fluid 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Akadémiai Kiadó, Budapest, Hungary 2021 Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. Oblique stagnation point flow (dpeaa)DE-He213 Second-grade fluid (dpeaa)DE-He213 Buongiorno model (dpeaa)DE-He213 Slip effects (dpeaa)DE-He213 Aziz, Mashal aut Ullah, Naeem aut Nadeem, Sohail aut Abro, Kashif Ali (orcid)0000-0003-0867-642X aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 147(2021), 5 vom: 13. Apr., Seite 3839-3851 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:147 year:2021 number:5 day:13 month:04 pages:3839-3851 https://dx.doi.org/10.1007/s10973-021-10760-z 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_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_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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 147 2021 5 13 04 3839-3851 |
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10.1007/s10973-021-10760-z doi (DE-627)SPR046211373 (SPR)s10973-021-10760-z-e DE-627 ger DE-627 rakwb eng Awan, Aziz Ullah verfasserin aut Thermal analysis of oblique stagnation point flow with slippage on second-order fluid 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Akadémiai Kiadó, Budapest, Hungary 2021 Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. Oblique stagnation point flow (dpeaa)DE-He213 Second-grade fluid (dpeaa)DE-He213 Buongiorno model (dpeaa)DE-He213 Slip effects (dpeaa)DE-He213 Aziz, Mashal aut Ullah, Naeem aut Nadeem, Sohail aut Abro, Kashif Ali (orcid)0000-0003-0867-642X aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 147(2021), 5 vom: 13. Apr., Seite 3839-3851 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:147 year:2021 number:5 day:13 month:04 pages:3839-3851 https://dx.doi.org/10.1007/s10973-021-10760-z 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_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_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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 147 2021 5 13 04 3839-3851 |
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10.1007/s10973-021-10760-z doi (DE-627)SPR046211373 (SPR)s10973-021-10760-z-e DE-627 ger DE-627 rakwb eng Awan, Aziz Ullah verfasserin aut Thermal analysis of oblique stagnation point flow with slippage on second-order fluid 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Akadémiai Kiadó, Budapest, Hungary 2021 Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. Oblique stagnation point flow (dpeaa)DE-He213 Second-grade fluid (dpeaa)DE-He213 Buongiorno model (dpeaa)DE-He213 Slip effects (dpeaa)DE-He213 Aziz, Mashal aut Ullah, Naeem aut Nadeem, Sohail aut Abro, Kashif Ali (orcid)0000-0003-0867-642X aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 147(2021), 5 vom: 13. Apr., Seite 3839-3851 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:147 year:2021 number:5 day:13 month:04 pages:3839-3851 https://dx.doi.org/10.1007/s10973-021-10760-z 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_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_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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 147 2021 5 13 04 3839-3851 |
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10.1007/s10973-021-10760-z doi (DE-627)SPR046211373 (SPR)s10973-021-10760-z-e DE-627 ger DE-627 rakwb eng Awan, Aziz Ullah verfasserin aut Thermal analysis of oblique stagnation point flow with slippage on second-order fluid 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Akadémiai Kiadó, Budapest, Hungary 2021 Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. Oblique stagnation point flow (dpeaa)DE-He213 Second-grade fluid (dpeaa)DE-He213 Buongiorno model (dpeaa)DE-He213 Slip effects (dpeaa)DE-He213 Aziz, Mashal aut Ullah, Naeem aut Nadeem, Sohail aut Abro, Kashif Ali (orcid)0000-0003-0867-642X aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 147(2021), 5 vom: 13. Apr., Seite 3839-3851 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:147 year:2021 number:5 day:13 month:04 pages:3839-3851 https://dx.doi.org/10.1007/s10973-021-10760-z 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_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_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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 147 2021 5 13 04 3839-3851 |
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10.1007/s10973-021-10760-z doi (DE-627)SPR046211373 (SPR)s10973-021-10760-z-e DE-627 ger DE-627 rakwb eng Awan, Aziz Ullah verfasserin aut Thermal analysis of oblique stagnation point flow with slippage on second-order fluid 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Akadémiai Kiadó, Budapest, Hungary 2021 Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. Oblique stagnation point flow (dpeaa)DE-He213 Second-grade fluid (dpeaa)DE-He213 Buongiorno model (dpeaa)DE-He213 Slip effects (dpeaa)DE-He213 Aziz, Mashal aut Ullah, Naeem aut Nadeem, Sohail aut Abro, Kashif Ali (orcid)0000-0003-0867-642X aut Enthalten in Journal of thermal analysis and calorimetry Dordrecht [u.a.] : Springer Science + Business Media B.V., 1969 147(2021), 5 vom: 13. Apr., Seite 3839-3851 (DE-627)315295422 (DE-600)2017304-0 1572-8943 nnns volume:147 year:2021 number:5 day:13 month:04 pages:3839-3851 https://dx.doi.org/10.1007/s10973-021-10760-z 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_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_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_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_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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 147 2021 5 13 04 3839-3851 |
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Awan, Aziz Ullah @@aut@@ Aziz, Mashal @@aut@@ Ullah, Naeem @@aut@@ Nadeem, Sohail @@aut@@ Abro, Kashif Ali @@aut@@ |
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| author |
Awan, Aziz Ullah |
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Awan, Aziz Ullah misc Oblique stagnation point flow misc Second-grade fluid misc Buongiorno model misc Slip effects Thermal analysis of oblique stagnation point flow with slippage on second-order fluid |
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Thermal analysis of oblique stagnation point flow with slippage on second-order fluid Oblique stagnation point flow (dpeaa)DE-He213 Second-grade fluid (dpeaa)DE-He213 Buongiorno model (dpeaa)DE-He213 Slip effects (dpeaa)DE-He213 |
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misc Oblique stagnation point flow misc Second-grade fluid misc Buongiorno model misc Slip effects |
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thermal analysis of oblique stagnation point flow with slippage on second-order fluid |
| title_auth |
Thermal analysis of oblique stagnation point flow with slippage on second-order fluid |
| abstract |
Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. © Akadémiai Kiadó, Budapest, Hungary 2021 |
| abstractGer |
Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. © Akadémiai Kiadó, Budapest, Hungary 2021 |
| abstract_unstemmed |
Abstract It is well-established fact that thermal resistance models are highly effective passive devices to transfer large quantities of heat for predicting the thermal performance. In the present investigation, we analyzed the thermal analysis of an unsteady oblique stagnation point flow of an incompressible second-grade fluid on a stretching surface with some slip effects. The governing equations of the model under consideration are presented. The governing PDEs are altered into nonlinear ODEs by utilizing non-similar and similar variables and then solved numerically. The analysis further reveals that these solutions sustain in a definite domain of corresponding parameters. Moreover, the variations in temperature and velocity are presented in graphical form to show the influence of controlling parameters. The numerical details of the heat transfer rate for the several thermophysical parameters and skin friction are illustrated in tabular form. The increment in the local second-grade parameter causes the Sherwood number to decrease. The value of the Nusselt number enhances if we decrease the value of the local second-grade parameter. © Akadémiai Kiadó, Budapest, Hungary 2021 |
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Thermal analysis of oblique stagnation point flow with slippage on second-order fluid |
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https://dx.doi.org/10.1007/s10973-021-10760-z |
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Aziz, Mashal Ullah, Naeem Nadeem, Sohail Abro, Kashif Ali |
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10.1007/s10973-021-10760-z |
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2024-07-03T21:05:54.525Z |
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| score |
7.39946 |