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首页> 外文期刊>International journal of numerical methods for heat & fluid flow >Semi-analytical unsteady heat conduction in large plane walls with heat convection exchange: The transversal method of lines (TMOL) in the 'small time' sub-domain
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Semi-analytical unsteady heat conduction in large plane walls with heat convection exchange: The transversal method of lines (TMOL) in the 'small time' sub-domain

机译:具有热对流交换的大平面壁中的半解析非稳态热传导:“小时间”子域中的线横向方法(TMOL)

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Purpose The purpose of this study is to address one-dimensional, unsteady heat conduction in a large plane wall exchanging heat convection with a nearby fluid under small time conditions.Design/methodology/approach The Transversal Method of Lines (TMOL) was used to reformulate the unsteady, one-dimensional heat conduction equation in the space coordinate and time into a transformed quasi-steady, one-dimensional heat conduction equation in the space coordinate housing the time as an embedded parameter. The resulting ordinary differential equation of second order with heat convection boundary conditions is solved analytically with the method of undetermined coefficients.Findings Semi-analytical TMOL dimensionless temperature profiles of compact form with/without regressed terms are obtained for the whole spectrum of Biot number (0 Bi ) in the small time sub-domain. In addition, a new large time sub-domain is redefined, that is, setting a smaller critical dimensionless time or critical Fourier number (cr) = 0.18.Originality/value The computed dimensionless center, surface and mean temperature profiles in the large plane wall accounting for all Biot number (0 Bi ) in the small time sub-domain (cr) = 0.18 exhibit excellent quality while carrying reasonable relative errors for engineering applications. The exemplary level of accuracy indicates that the traditional evaluation of the center, surface and mean temperatures with the standard infinite series retaining a large number of terms is no longer necessary.
机译:目的本研究的目的是解决大平面壁在短时间条件下与附近流体进行热对流交换时的一维非稳态热传导。设计/方法/方法使用线的横向方法(TMOL)来重新表述将空间坐标和时间中的非稳态一维热传导方程转换为以时间为嵌入参数的空间坐标中的转换后的准稳态一维热传导方程。通过不确定系数的方法解析求解了具有热对流边界条件的二阶常微分方程。发现对于整个毕奥数(0,0

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