Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility
The Marangoni forced convective inclined magnetohydrodynamic flow is examined. Marangoni forced convection depends on the differences in surface pressure computed by magnetic field, temperature, and concentration gradient. Casson nanoliquid flow by an infinite disk is considered. Viscous dissipation...
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| Format: | Article |
| Language: | English |
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MDPI AG
2020-04-01
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| Series: | Entropy |
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| Online Access: | https://www.mdpi.com/1099-4300/22/4/433 |
| _version_ | 1827718901141602304 |
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| author | Muhammad Adil Sadiq Tasawar Hayat |
| author_facet | Muhammad Adil Sadiq Tasawar Hayat |
| author_sort | Muhammad Adil Sadiq |
| collection | DOAJ |
| description | The Marangoni forced convective inclined magnetohydrodynamic flow is examined. Marangoni forced convection depends on the differences in surface pressure computed by magnetic field, temperature, and concentration gradient. Casson nanoliquid flow by an infinite disk is considered. Viscous dissipation, heat flux, and Joule heating are addressed in energy expressions. Thermophoresis and Brownian motion are also examined. Entropy generation is computed. The physical characteristics of entropy optimization with Arrhenius activation energy are discussed. Nonlinear PDE’s are reduced to highly nonlinear ordinary systems with appropriate transformations. A nonlinear system is numerically computed by the NDSolve technique. The salient characteristics of velocity, temperature, concentration, entropy generation, and Bejan number are explained. The computational results of the heat-transfer rate and concentration gradient are examined through tables. Velocity and temperature have reverse effects for the higher approximation of the Marangoni number. Velocity is a decreasing function of the Casson fluid parameter. Temperature is enhanced for higher radiation during reverse hold for concentration against the Marangoni number. The Bejan number and entropy generation have similar effects for Casson fluid and radiation parameters. For a higher estimation of the Brinkman number, the entropy optimization is augmented. |
| first_indexed | 2024-03-10T20:32:19Z |
| format | Article |
| id | doaj.art-caa9ce645a1c4aeeba80d53d06615f2e |
| institution | Directory Open Access Journal |
| issn | 1099-4300 |
| language | English |
| last_indexed | 2024-03-10T20:32:19Z |
| publishDate | 2020-04-01 |
| publisher | MDPI AG |
| record_format | Article |
| series | Entropy |
| spelling | doaj.art-caa9ce645a1c4aeeba80d53d06615f2e2023-11-19T21:18:25ZengMDPI AGEntropy1099-43002020-04-0122443310.3390/e22040433Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and IrreversibilityMuhammad Adil Sadiq0Tasawar Hayat1Department of Mathematics, DCC-KFUPM Box 5084, Dhahran 31261, Saudi ArabiaDepartment of Mathematics, Quaid-I-Azam University, Islamabad 45320, PakistanThe Marangoni forced convective inclined magnetohydrodynamic flow is examined. Marangoni forced convection depends on the differences in surface pressure computed by magnetic field, temperature, and concentration gradient. Casson nanoliquid flow by an infinite disk is considered. Viscous dissipation, heat flux, and Joule heating are addressed in energy expressions. Thermophoresis and Brownian motion are also examined. Entropy generation is computed. The physical characteristics of entropy optimization with Arrhenius activation energy are discussed. Nonlinear PDE’s are reduced to highly nonlinear ordinary systems with appropriate transformations. A nonlinear system is numerically computed by the NDSolve technique. The salient characteristics of velocity, temperature, concentration, entropy generation, and Bejan number are explained. The computational results of the heat-transfer rate and concentration gradient are examined through tables. Velocity and temperature have reverse effects for the higher approximation of the Marangoni number. Velocity is a decreasing function of the Casson fluid parameter. Temperature is enhanced for higher radiation during reverse hold for concentration against the Marangoni number. The Bejan number and entropy generation have similar effects for Casson fluid and radiation parameters. For a higher estimation of the Brinkman number, the entropy optimization is augmented.https://www.mdpi.com/1099-4300/22/4/433mixed convectionrotating coneviscous fluidBejan numberentropy generationthermal radiation |
| spellingShingle | Muhammad Adil Sadiq Tasawar Hayat Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility Entropy mixed convection rotating cone viscous fluid Bejan number entropy generation thermal radiation |
| title | Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility |
| title_full | Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility |
| title_fullStr | Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility |
| title_full_unstemmed | Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility |
| title_short | Characterization of Marangoni Forced Convection in Casson Nanoliquid Flow with Joule Heating and Irreversibility |
| title_sort | characterization of marangoni forced convection in casson nanoliquid flow with joule heating and irreversibility |
| topic | mixed convection rotating cone viscous fluid Bejan number entropy generation thermal radiation |
| url | https://www.mdpi.com/1099-4300/22/4/433 |
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