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    连续梯度BCC骨架孔隙率分布对复合相变材料熔化特性的影响

    Effect of Continuous Porosity Gradients in BCC Lattices on Melting Characteristics of Composite Phase Change Materials

    • 摘要: 针对侧壁恒温加热条件下复合相变材料熔化不均及远端底部熔化滞后的问题,建立连续梯度体心立方(BCC)金属骨架/石蜡复合相变材料三维瞬态数值模型。在平均孔隙率和热端局部孔隙率相同的条件下,构建N05-BCC、N10-BCC和N20-BCC结构,考察孔隙率沿程分布规律对熔化特性的影响,并与均匀U-BCC结构进行比较。结果表明,孔隙率分布对熔化初期影响较小,主要通过调节中后期金属骨架导热路径及液相流动空间影响熔化过程。N10-BCC/PCM的完全熔化时间为5314.5 s,较U-BCC/PCM缩短23.69%,其远端底部测点的相变结束时刻及局部相变持续时间均为三种梯度结构中的最小。结果说明,连续梯度结构的强化效果取决于孔隙率沿程分布所形成的金属导热路径与液相流动空间之间的匹配,而非梯度指数的简单增大。

       

      Abstract: To address the nonuniform melting and delayed melting at the far-end bottom region of composite phase change materials under constant-temperature sidewall heating, a three-dimensional transient numerical model was developed for a paraffin-based composite phase change material incorporating a continuous-gradient body-centered cubic (BCC) metallic lattice. Three continuous-gradient structures, N05-BCC, N10-BCC, and N20-BCC, were constructed with the same overall average porosity and local porosity near the heated wall. The effects of the porosity distribution along the heat-flow direction on melting characteristics were investigated and compared with those of a uniform BCC structure (U-BCC). The results show that the porosity distribution has only a minor effect during the early melting stage, whereas it mainly influences the middle and late stages by regulating the heat-conduction paths of the metallic lattice and the flow space available to the liquid phase. The complete melting time of N10-BCC/PCM is 5314.5 s, which is 23.69% shorter than that of U-BCC/PCM. Moreover, among the three graded structures, N10-BCC/PCM exhibits the earliest phase-change completion and the shortest local phase-change duration at the far-end bottom monitoring point. These results indicate that the enhancement achieved by continuous-gradient structures depends on the balance between metallic heat-conduction pathways and liquid-flow space established by the spatial porosity distribution, rather than simply on increasing the gradient exponent.

       

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