Magnetohydrodynamics double-diffusive natural convection and entropy generation in novel E-shaped enclosure

IF 6.4 2区 工程技术 Q1 MECHANICS International Communications in Heat and Mass Transfer Pub Date : 2025-05-01 Epub Date: 2025-03-18 DOI:10.1016/j.icheatmasstransfer.2025.108873
Ammar Abdulkadhim , Naseer H. Hamza , Hameed K. Hamzah , Azher M. Abed , Farooq H. Ali
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The enclosure had been filled by electrically conducting fluid with Prandtl number of <span><math><mfenced><mrow><mo>Pr</mo><mo>=</mo><mn>0.024</mn></mrow></mfenced></math></span>. Additionally, Hartmann number and Darcy number kept constant at as <span><math><mfenced><mrow><mi>Ha</mi><mo>=</mo><mn>20</mn></mrow><mrow><mi>Da</mi><mo>=</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>5</mn></mrow></msup></mrow></mfenced><mo>.</mo></math></span> The studied parameters are the inclination of the magnetic field that varied as <span><math><mfenced><mrow><mi>γ</mi><mo>=</mo><msup><mn>0</mn><mo>°</mo></msup></mrow><msup><mn>15</mn><mo>°</mo></msup><msup><mn>30</mn><mo>°</mo></msup><msup><mn>45</mn><mo>°</mo></msup><msup><mn>60</mn><mo>°</mo></msup><mrow><msup><mn>75</mn><mo>°</mo></msup><mspace></mspace><mtext>and</mtext><mspace></mspace><msup><mn>90</mn><mo>°</mo></msup></mrow></mfenced></math></span>. Additionally, the enclosure its self is orientated as <span><math><mfenced><mrow><mi>λ</mi><mo>=</mo><msup><mn>0</mn><mo>°</mo></msup></mrow><msup><mn>45</mn><mo>°</mo></msup><msup><mn>90</mn><mo>°</mo></msup><msup><mn>135</mn><mo>°</mo></msup><msup><mn>180</mn><mo>°</mo></msup><msup><mn>225</mn><mo>°</mo></msup><msup><mn>270</mn><mo>°</mo></msup><mrow><msup><mn>315</mn><mo>°</mo></msup><mspace></mspace><mtext>and</mtext><mspace></mspace><msup><mn>360</mn><mo>°</mo></msup></mrow></mfenced></math></span>. The Rayleigh number are varied as <span><math><mfenced><mrow><mi>Ra</mi><mo>=</mo><msup><mn>10</mn><mn>3</mn></msup><mo>−</mo><msup><mn>10</mn><mn>6</mn></msup></mrow></mfenced></math></span>. The buoyancy ratio had been varied as <span><math><mfenced><mrow><mi>N</mi><mo>=</mo><mn>0</mn></mrow><mn>2</mn><mn>4</mn><mn>6</mn><mn>8</mn><mn>10</mn></mfenced><mspace></mspace></math></span>and Lewis number is varied as <span><math><mfenced><mrow><mi>Le</mi><mo>=</mo><mn>1</mn><mo>−</mo><mn>10</mn></mrow></mfenced></math></span>. Additionally, the inner circular body is varied <span><math><mfenced><mrow><mo>−</mo><mn>0.3</mn><mo>≤</mo><mi>δ</mi><mo>≤</mo><mo>+</mo><mn>0.3</mn></mrow></mfenced></math></span>. The results show that applied the magnetic field in the vertical direction <span><math><mfenced><mrow><mi>γ</mi><mo>=</mo><msup><mn>90</mn><mo>°</mo></msup></mrow></mfenced></math></span> helped in enhancing the heat transfer and lower entropy generation while at <span><math><mfenced><mrow><mi>γ</mi><mo>=</mo><msup><mn>0</mn><mo>°</mo></msup></mrow></mfenced></math></span> helped in better mass transfer. Additionally, in spite inclining the enclosure at <span><math><mfenced><mrow><mi>λ</mi><mo>=</mo><msup><mn>270</mn><mo>°</mo></msup></mrow></mfenced></math></span> contributed in lower entropy generation but it led to lower heat and mass transfer rate. At zero buoyancy ratio number <span><math><mfenced><mrow><mi>N</mi><mo>=</mo><mn>0</mn></mrow></mfenced></math></span>, there is no impact of Lewis number on heat transfer rate. However, when buoyancy ratio number into <span><math><mfenced><mrow><mi>N</mi><mo>=</mo><mn>10</mn></mrow></mfenced></math></span>, it is noted that increasing Lewis number from <span><math><mfenced><mrow><mi>Le</mi><mo>=</mo><mn>1</mn></mrow></mfenced></math></span> into <span><math><mfenced><mrow><mi>Le</mi><mo>=</mo><mn>10</mn></mrow></mfenced></math></span>, leads to decreases <em>Nu</em> by 52.17 %. Similar behavior is noted for the entropy generation while Sherwood number increases with the increasing of Lewis number regardless the value of buoyancy ratio number. Lastly, the position of the inner body and its role in heat and mass transfer is highly impacted by the Rayleigh number. It is obtained that at low <em>Ra</em>, the best position for heat transfer is at <span><math><mi>δ</mi><mo>=</mo><mo>−</mo><mn>0.2</mn></math></span> while at high <em>Ra</em>, the best position is at <span><math><mi>δ</mi><mo>=</mo><mo>−</mo><mn>0.3</mn></math></span>. Additionally, at high <em>Ra</em>, the entropy generation decreases as the inner body moved in the positive direction.</div></div>","PeriodicalId":332,"journal":{"name":"International Communications in Heat and Mass Transfer","volume":"164 ","pages":"Article 108873"},"PeriodicalIF":6.4000,"publicationDate":"2025-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Communications in Heat and Mass Transfer","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0735193325002982","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/3/18 0:00:00","PubModel":"Epub","JCR":"Q1","JCRName":"MECHANICS","Score":null,"Total":0}
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Abstract

A CFD interpretation is presented to analyze the double-diffusive natural convection along with the entropy generation inside inclined E-shaped enclosure with wavy wall under the influence of magnetic field. The existence of inner heated circular body had been included in this study that it solved numerically using finite element formulation. The enclosure wavy wall is kept at the same hot temperature of the inner heated body while the vertical wall of the enclosure is kept at cold temperature and the rest of the horizontal walls are thermally insulated. The enclosure had been filled by electrically conducting fluid with Prandtl number of Pr=0.024. Additionally, Hartmann number and Darcy number kept constant at as Ha=20Da=105. The studied parameters are the inclination of the magnetic field that varied as γ=0°15°30°45°60°75°and90°. Additionally, the enclosure its self is orientated as λ=0°45°90°135°180°225°270°315°and360°. The Rayleigh number are varied as Ra=103106. The buoyancy ratio had been varied as N=0246810and Lewis number is varied as Le=110. Additionally, the inner circular body is varied 0.3δ+0.3. The results show that applied the magnetic field in the vertical direction γ=90° helped in enhancing the heat transfer and lower entropy generation while at γ=0° helped in better mass transfer. Additionally, in spite inclining the enclosure at λ=270° contributed in lower entropy generation but it led to lower heat and mass transfer rate. At zero buoyancy ratio number N=0, there is no impact of Lewis number on heat transfer rate. However, when buoyancy ratio number into N=10, it is noted that increasing Lewis number from Le=1 into Le=10, leads to decreases Nu by 52.17 %. Similar behavior is noted for the entropy generation while Sherwood number increases with the increasing of Lewis number regardless the value of buoyancy ratio number. Lastly, the position of the inner body and its role in heat and mass transfer is highly impacted by the Rayleigh number. It is obtained that at low Ra, the best position for heat transfer is at δ=0.2 while at high Ra, the best position is at δ=0.3. Additionally, at high Ra, the entropy generation decreases as the inner body moved in the positive direction.
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新型e形外壳的磁流体力学双扩散自然对流和熵生成
提出了一种计算流体力学(CFD)方法,分析了在磁场影响下,波浪壁倾斜的e型壳体内的双扩散自然对流和熵的产生。本研究考虑了内加热圆体的存在,采用有限元公式进行了数值求解。所述箱体波浪形壁保持与内受热体相同的热温度,所述箱体垂直壁保持冷温度,其余水平壁保温。用普朗特数Pr=0.024的导电流体填充。Hartmann数和Darcy数保持不变,Ha=20Da=10−5。研究参数为γ=0°15°30°45°60°75°和90°时的磁场倾角。此外,外壳本身定向为λ=0°45°90°135°180°225°270°315°和360°。瑞利数的变化范围为Ra=103 ~ 106。浮力比变化为N=0246810,路易斯数变化为Le=1−10。此外,内圆体变化为−0.3≤δ≤+0.3。结果表明,在垂直方向γ=90°处施加磁场有利于强化传热,熵产更小,而在垂直方向γ=0°处施加磁场有利于更好的传质。此外,虽然λ=270°倾斜的外壳有助于降低熵产,但它导致较低的传热传质率。在零浮力比数N=0时,路易斯数对换热速率没有影响。而当浮力比数变为N=10时,Lewis数由Le=1增加到Le=10, Nu降低了52.17%。当舍伍德数随刘易斯数的增加而增加时,无论浮力比数的大小如何,熵产也有相似的行为。最后,内体的位置及其在传热传质中的作用受到瑞利数的高度影响。结果表明:低Ra时,最佳换热位置为δ=−0.2,高Ra时,最佳换热位置为δ=−0.3。此外,在高Ra时,随着内体向正方向移动,熵产减小。
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来源期刊
CiteScore
11.00
自引率
10.00%
发文量
648
审稿时长
32 days
期刊介绍: International Communications in Heat and Mass Transfer serves as a world forum for the rapid dissemination of new ideas, new measurement techniques, preliminary findings of ongoing investigations, discussions, and criticisms in the field of heat and mass transfer. Two types of manuscript will be considered for publication: communications (short reports of new work or discussions of work which has already been published) and summaries (abstracts of reports, theses or manuscripts which are too long for publication in full). Together with its companion publication, International Journal of Heat and Mass Transfer, with which it shares the same Board of Editors, this journal is read by research workers and engineers throughout the world.
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