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The stage of nonisothermal nucleation of supercritical particles of a new phase under nonstationary conditions of particle diffusion growth and heat transfer to a medium

机译:在粒子扩散生长和向介质传热的非平稳条件下,新相超临界粒子的非等温成核阶段

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An analytical theory has been formulated for the stage of nonisothermal nucleation of supercritical particles in a metastable medium with instantaneously generated initial supersaturation. The theory takes into account the nonuniformities of metastable substance concentration and temperature, which result from the nonstationary diffusion of the substance to growing particles and the nonstationary transfer of the heat of the phase transition from the particles to the medium. The formulated theory extends the approach based on the concept of excluded volume that has recently been used in the theory of the stage of nucleation under isothermal conditions. This approach implies that the nucleation intensity of new particles is suppressed in spherical diffusion regions with certain sizes that surround previously nucleated supercritical particles and remaining unchanged in the rest of the medium. It has been shown that, when self-similar solutions are used for nonstationary equations of substance diffusion to particles and heat transfer from the particles, the ratio between the excluded volume and the particle volume is independent of particle size, thereby enabling one to analytically solve the integral equation for the excluded volume throughout a system as a time function at the stage of nucleation. The main characteristics of the phase transition have been found for the end of the stage of nucleation. Comparison has been carried out with the characteristics obtained in terms of the isothermal and nonisothermal nucleation theory upon uniform vapor consumption and heat dissipation (the mean-field approximation of vapor supersaturation and temperature).
机译:已经建立了一种分析理论,用于在瞬态产生的初始过饱和的亚稳态介质中超临界粒子的非等温成核阶段。该理论考虑了亚稳态物质浓度和温度的不均匀性,这是由于物质向生长颗粒的非平稳扩散以及相变热从颗粒向介质的非平稳传递所致。公式化理论扩展了基于排除体积概念的方法,该概念最近已在等温条件下的成核阶段理论中使用。这种方法意味着在球形扩散区域中,新粒子的成核强度受到抑制,球形扩散区域的某些尺寸围绕着先前成核的超临界粒子,并在其余介质中保持不变。已经表明,当自相似解用于物质扩散到颗粒和从颗粒传热的非平稳方程时,排除体积与颗粒体积之比与颗粒大小无关,从而使人们能够解析地求解整个系统中排除体积的积分方程,作为成核阶段的时间函数。在成核阶段的末期发现了相变的主要特征。比较了等温和非等温成核理论在均匀的蒸汽消耗和热耗散(蒸汽过饱和度和温度的平均场近似)方面获得的特性。

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