青花椒堆积对流干燥过程堆积层孔隙率宏细观跨尺度演变特征

    Multi-scale Evolution of Porosity in a Zanthoxylum schinifolium Stack during Convective Drying: From Macro to Micro-scale Characteristics

    • 摘要: 针对青花椒干燥过程中孔隙率动态变化特征不明导致工艺优化与结构设计依据不足的问题,该研究采用试验分析与数值模拟相结合的方法,从宏细观跨尺度角度揭示青花椒堆积孔隙率演变规律。结果表明:孔隙率变化范围为0.345~0.591,初始阶段(0~120 min,湿基含水率Mc≥34.46%),层厚L变化较小(从0.2 mm降至0.1938 mm)仅下降3.1%,压差ΔP波动较小(432.3~513.9 Pa);主干燥阶段(120~390 min,10.45%≤湿基含水率Mc≤34.46%)孔隙率显著降低,压差ΔP下降剧烈35.2%,果体收缩明显;终阶段(干燥时间t>390 min,湿基含水率Mc≤10.45%,青花椒堆积层局部出现“开口”现象,层厚L反常膨胀0.018 mm,并建立ε-Mc数学模型(决定系数R2=0.9778)。结合数值模拟表明,堆积层的传热始于底部中心,并优先沿壁面向上、向内扩散(稳态温度70.1 ℃),此热扩散路径与青花椒堆积层在实际干燥中“开口”的先后顺序吻合,单粒传热分3个阶段:热量突破壳层阶段(热量突破壳层向籽传递热量,花椒壳收缩形变微小);内部传热主导阶段(花椒籽内部逐渐升温,花椒壳收缩量逐渐增大);趋近热平衡阶段(花椒籽内部温度趋于稳定,花椒壳形变量达到峰值0.487 mm)。研究为青花椒干燥工艺优化及传热传质机理研究提供了理论依据。

       

      Abstract: Aiming at the problem that the unclear dynamic characteristics of porosity during the drying process of Zanthoxylum schinifolium lead to insufficient basis for process optimization and structural design, this study adopts a method combining experimental analysis and numerical simulation to reveal the evolution law of porosity in Zanthoxylum schinifolium bulk from a multi-scale perspective.The results show that the porosity varies in the range of 0.345-0.591.In the initial stage(0-120 min, Mc≥34.46%), the layer thickness L changes slightly (from 0.2 mm to 0.1938 mm, a decrease of only 3.1%), and the pressure difference ΔP fluctuates slightly (432.3-513.9 Pa). In the main drying stage (120-390 min, 10.45%≤Mc≤34.46%), the porosity decreases significantly, the pressure difference ΔP drops sharply by 35.2%, and the fruit body contracts obviously. In the final stage (t>390 min, Mc≤10.45%,and the Zanthoxylum schinifolium bulk layer shows a "cracking" phenomenon locally), the layer thickness L abnormally expands by 0.018 mm. Meanwhile, an ε-Mc mathematical model is established (R2=0.9778). Combined with numerical simulation, it is shown that the heat transfer in the bulk layer starts from the bottom center and preferentially diffuses upward and inward along the wall (steady-state temperature 70.1℃). This heat diffusion path coincides with the order of "cracking" in the Zanthoxylum schinifolium bulk layer in practice. The heat transfer of a single particle is divided into three stages: the shell-breaking heat transfer stage (heat breaks through the shell to transfer heat to the seed, and the Zanthoxylum schinifolium shell undergoes slight contraction deformation); the internal heat transfer dominant stage (the Zanthoxylum schinifolium seed gradually warms up, and the contraction of the Zanthoxylum schinifolium shell gradually increases); and the heat balance approaching stage (the internal temperature of the Zanthoxylum schinifolium seed tends to stabilize, and the deformation of the Zanthoxylum schinifolium shell reaches its peak value of 0.487 mm). This study provides a theoretical basis for the optimization of the Zanthoxylum schinifolium drying process and the research on heat and mass transfer mechanisms.

       

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