杰弗里流经具有活化能和粘性耗散的拉伸里加板的洞察力:熔化传热机制

Mubashar Javed
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摘要

本文强调了阿伦尼乌斯活化能以及杰弗里流体在里加板上的粘性耗散的重要性。里加板基本上是一种由磁铁和电极阵列组成的执行器,它在一个平面上解决了流体流动过程中导电性较弱的问题。为了确保新颖性,我们在厚度可变的非线性拉伸里加板上加入了可靠的熔化热表面条件,以研究传热特征。此外,本研究还保留了停滞点。为了获得非线性常微分方程系统,采用了适当的变换。利用一种著名的半分析技术(同调分析法)来获得常用无量纲方程的序列解。图解分析了几个相关参数对速度、热量和浓度分布的影响。对阻力系数和热传导率进行了物理评估和图解。对速度和相关边界层厚度的分析对修正哈特曼数的强度产生了越来越大的影响。无量纲反应速率和内热/放热反应参数的增加导致拉伸里加板上的热通量增加。埃克特数越高,热分布越大,而热边界层厚度则呈相反趋势。施密特数越高,浓度边界层厚度越大,而浓度分布则越小。在强烈熔化过程中,速度分布会增加。据分析,较高的无量纲活化能参数是造成浓度场增大的原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Insight of Jeffrey flow over a stretching Riga plate with activation energy and viscous dissipation: Melting heat transfer regime
Present article highlights the significance of Arrhenius activation energy along with viscous dissipation in Jeffrey fluid over a Riga plate. Riga plate is basically an actuator made up of array of magnets and electrodes scaled on a plane surface to tackle the weaker electrical conductivity during fluid flow. In order to ensure the novelty, a reliable melting heat surface condition has been incorporated on nonlinear stretching Riga plate of variable thickness to reconnoiter features of heat transfer. Moreover, stagnation point has been retained in this study. Adequate transformations are employed in order to attain system of nonlinear ordinary differential equations. A well known semi analytical technique (Homotopy analysis method) is utilized to obtain series solutions of prevailing dimensionless equations. Influence of several apposite parameters on velocity, thermal and concentration distributions is analyzed graphically. Physical evaluation and graphical sketch is presented for drag force coefficient and rate of heat transfer. Analysis of velocity as well as associated boundary layer thickness gives the growing up impact for the strength of modified Hartmann number. Enhancement of dimensionless reaction rate and endothermic/exothermic reaction parameter results in increment for heat flux over stretching Riga plate. Increase in thermal distribution takes place for higher Eckert number while thermal boundary layer thickness depicts opposite trend in this case. Concentration boundary layer thickness enhances while concentration profile declines for higher Schmidt number. Velocity distribution is found to be incremented for intense melting process. Higher dimensionless activation energy parameter is analyzed to be responsible for growing up concentration field.
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