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Error associated with assuming a finite regular geometry as an infinite one for modeling of transient heat and mass transfer processes

机译:与将瞬态传热和传质过程建模的有限规则几何假设为无限规则几何相关的误差

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Error (ε) due to assuming a finite regular geometry as an infinite one was determined for transient heat and mass transfer processes. Dimensionless numbers Fourier (Fo) and Biot (Bi), and geometrical properties (type, shape, and size) were the possible effective parameters on ε. Types of geometries used were slab (circle, square, and rectangle) and rod (cylinder and square). The error decreased with decreasing Fo, with the ε-curves shifting in parallel to the Fo-axis in the decreasing direction with increasing Bi. And Bi≥100 was found to be infinite for all geometries. The error for circle and square slab geometries was same at all Bi. The size of the dimension through which the transfer occurs did not affect the error in all geometries. However, the size of the dimensions, through which the transfer occurs was neglected, affected the error in squared slabs. It increased with decreasing ratio of width over length, e.g. In the order of square slab and rectangular slab of 1 x 2, 1x5, and 1x10. The error was same for the cylindrical and square rods for Bi = 0.01 and 0.1. For Bi≥1, square rod had greater ε values than cylindrical rod at the same Fo-Bi. An error chart was constructed as a function of Fo, Bi, and geometrical properties that can be used to determine the error due to assuming a finite slab and rod geometry as an infinite one during transient heat or mass transfer processes.
机译:对于瞬态传热和传质过程,确定了由于假设有限规则几何为无限而导致的误差(ε)。傅立叶(Fo)和比奥(Bi)的无因次数以及几何性质(类型,形状和大小)是ε上可能的有效参数。使用的几何类型为平板(圆形,正方形和矩形)和棒状(圆柱和正方形)。误差随着Fo的减小而减小,随着Bi的增大,ε曲线平行于Fo轴沿减小的方向移动。并且发现Bi≥100对于所有几何形状都是无限的。所有Bi的圆和正方形平板几何形状的误差都相同。进行转移的尺寸大小不会影响所有几何形状中的误差。但是,忽略了发生转移的尺寸大小,影响了方板的误差。它随着宽度与长度之比的减小而增加,例如。顺序为1 x 2、1x5和1x10的方形平板和矩形平板。对于Bi = 0.01和0.1,圆柱棒和方棒的误差相同。对于Bi≥1,在相同的Fo-Bi下,方棒的ε值大于圆柱棒的ε值。根据Fo,Bi和几何特性构造了一个误差图,可将其用于确定误差,这是由于在瞬态热或传质过程中假设有限的平板和棒几何形状为无穷大。

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