Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions
Entropy generation in thermal convection with differentially discrete heat boundary conditions at various Rayleigh numbers (Ra) are numerically investigated using the lattice Boltzmann method. We mainly focused on the effects of Ra and discrete heat boundary conditions on entropy generation in therm...
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doaj-75521f4042a64d7b92d8432151508f6a2020-11-24T22:45:48ZengMDPI AGEntropy1099-43002018-05-0120535110.3390/e20050351e20050351Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary ConditionsZhengdao Wang0Yikun Wei1Yuehong Qian2Shanghai Institute of Applied Mathematics and Mechanics, Shanghai University, Shanghai 200072, ChinaState-Province Joint Engineering Lab of Fluid Transmission System Technology, Faculty of Mechanical Engineering and Automation, Zhejiang Sci-Tech University, Hangzhou 310018, ChinaSchool of Mathematical Science, Soochow University, Suzhou 215006, ChinaEntropy generation in thermal convection with differentially discrete heat boundary conditions at various Rayleigh numbers (Ra) are numerically investigated using the lattice Boltzmann method. We mainly focused on the effects of Ra and discrete heat boundary conditions on entropy generation in thermal convection according to the minimal entropy generation principle. The results showed that the presence of the discrete heat source at the bottom boundary promotes the transition to a substantial convection, and the viscous entropy generation rate (Su) generally increases in magnitude at the central region of the channel with increasing Ra. Total entropy generation rate (S) and thermal entropy generation rate (Sθ) are larger in magnitude in the region with the largest temperature gradient in the channel. Our results also indicated that the thermal entropy generation, viscous entropy generation, and total entropy generation increase exponentially with the increase of Rayleigh number. It is noted that lower percentage of single heat source area in the bottom boundary increases the intensities of viscous entropy generation, thermal entropy generation and total entropy generation. Comparing with the classical homogeneous thermal convection, the thermal entropy generation, viscous entropy generation, and total entropy generation are improved by the presence of discrete heat sources at the bottom boundary.http://www.mdpi.com/1099-4300/20/5/351entropyRayleighdiscrete boundary conditionsheat transferlattice Boltzmann method |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Zhengdao Wang Yikun Wei Yuehong Qian |
spellingShingle |
Zhengdao Wang Yikun Wei Yuehong Qian Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions Entropy entropy Rayleigh discrete boundary conditions heat transfer lattice Boltzmann method |
author_facet |
Zhengdao Wang Yikun Wei Yuehong Qian |
author_sort |
Zhengdao Wang |
title |
Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions |
title_short |
Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions |
title_full |
Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions |
title_fullStr |
Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions |
title_full_unstemmed |
Numerical Study on Entropy Generation in Thermal Convection with Differentially Discrete Heat Boundary Conditions |
title_sort |
numerical study on entropy generation in thermal convection with differentially discrete heat boundary conditions |
publisher |
MDPI AG |
series |
Entropy |
issn |
1099-4300 |
publishDate |
2018-05-01 |
description |
Entropy generation in thermal convection with differentially discrete heat boundary conditions at various Rayleigh numbers (Ra) are numerically investigated using the lattice Boltzmann method. We mainly focused on the effects of Ra and discrete heat boundary conditions on entropy generation in thermal convection according to the minimal entropy generation principle. The results showed that the presence of the discrete heat source at the bottom boundary promotes the transition to a substantial convection, and the viscous entropy generation rate (Su) generally increases in magnitude at the central region of the channel with increasing Ra. Total entropy generation rate (S) and thermal entropy generation rate (Sθ) are larger in magnitude in the region with the largest temperature gradient in the channel. Our results also indicated that the thermal entropy generation, viscous entropy generation, and total entropy generation increase exponentially with the increase of Rayleigh number. It is noted that lower percentage of single heat source area in the bottom boundary increases the intensities of viscous entropy generation, thermal entropy generation and total entropy generation. Comparing with the classical homogeneous thermal convection, the thermal entropy generation, viscous entropy generation, and total entropy generation are improved by the presence of discrete heat sources at the bottom boundary. |
topic |
entropy Rayleigh discrete boundary conditions heat transfer lattice Boltzmann method |
url |
http://www.mdpi.com/1099-4300/20/5/351 |
work_keys_str_mv |
AT zhengdaowang numericalstudyonentropygenerationinthermalconvectionwithdifferentiallydiscreteheatboundaryconditions AT yikunwei numericalstudyonentropygenerationinthermalconvectionwithdifferentiallydiscreteheatboundaryconditions AT yuehongqian numericalstudyonentropygenerationinthermalconvectionwithdifferentiallydiscreteheatboundaryconditions |
_version_ |
1725687435821580288 |