Editorial: Editor’s challenge in heat transfer mechanisms and applications: 2022

L. Dombrovsky
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Abstract

In the study of many heat transfer processes, it is necessary to consider the interaction of heat conduction, natural or forced convection, and heat transfer by thermal radiation. The greatest difficulties in the computational modeling of combined heat transfer are related to time-consuming calculations of radiative transfer in absorbing and scattering media. Such media are, for example, gases or liquids with suspended particles, as well as dispersed materials and solids with microcracks or bubbles. Natural objects of study include the Earth’s atmosphere and ocean, snow and ice, powders or dust, ordinary sand, and even biological tissues with optically heterogeneous living cells. In thermal engineering, these are combustion products containing soot and fly ash particles, porous ceramics and heatshielding materials, particles in thermochemical reactors, and melt droplets from a possible severe nuclear reactor accident. Thermal radiation has a wide spectral range in which the optical properties of substances and materials are usually substantially dependent on the radiation wavelength. Therefore, in order to calculate the contribution of thermal radiation to heat transfer, radiative transfer calculations must be carried out for a large set of different wavelengths. In the numerical solution of transient heat transfer problems, such calculations, carried out at each time step, are the main factor influencing the computation time. It is also important that the numerical solution of the integrodifferential radiative transfer equation (RTE) regarding the radiation intensity, which is dependent not only on the coordinates but also on the direction, is a very complex procedure (Coelho, 2014). This means that the use of simple but sufficiently accurate models of radiative transfer in scattering media is absolutely essential for solving many problems of combined heat transfer. Fortunately, heat transfer problems (unlike optical diagnostics problems) have a number of physical features that allow simpler mathematical models. Note that we are usually dealing with multiple scattering of radiation in a medium when the angular distribution of the radiation in a single scattering is irrelevant. In this case, the so-called transport approximation can be used (Dombrovsky, 2012); the integral term in RTE is missing and the scattering anisotropy is taken into account by a transport scattering coefficient. The high accuracy of the transport approximation has been confirmed for diverse problems (Dombrovsky, 2010; Dombrovsky, 2019). OPEN ACCESS
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社论:编者在传热机制和应用方面的挑战:2022
在许多传热过程的研究中,需要考虑热传导、自然对流或强制对流以及热辐射传热的相互作用。复合传热计算建模的最大困难是吸收介质和散射介质中辐射传递的耗时计算。例如,这种介质是带有悬浮颗粒的气体或液体,以及带有微裂纹或气泡的分散材料和固体。研究的自然对象包括地球的大气和海洋、雪和冰、粉末或灰尘、普通的沙子,甚至是具有光学异质活细胞的生物组织。在热能工程中,这些是含有烟尘和飞灰颗粒的燃烧产物,多孔陶瓷和隔热材料,热化学反应堆中的颗粒,以及可能发生严重核反应堆事故的熔融液滴。热辐射具有很宽的光谱范围,其中物质和材料的光学特性通常在很大程度上取决于辐射波长。因此,为了计算热辐射对传热的贡献,必须对一组大的不同波长进行辐射传递计算。在瞬态传热问题的数值解中,这种在每个时间步进行的计算是影响计算时间的主要因素。同样重要的是,关于辐射强度的积分微分辐射传递方程(RTE)的数值解是一个非常复杂的过程,它不仅取决于坐标,而且取决于方向(Coelho, 2014)。这意味着在散射介质中使用简单但足够精确的辐射传递模型对于解决许多联合传热问题是绝对必要的。幸运的是,传热问题(与光学诊断问题不同)具有许多物理特征,可以使用更简单的数学模型。注意,当单次散射中辐射的角分布无关紧要时,我们通常处理的是介质中辐射的多次散射。在这种情况下,可以使用所谓的输运近似(Dombrovsky, 2012);RTE中缺少积分项,散射各向异性由输运散射系数来考虑。输运近似的高精度已被证实适用于各种问题(Dombrovsky, 2010;Dombrovsky, 2019)。开放获取
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