纺织学报 ›› 2026, Vol. 47 ›› Issue (05): 72-80.doi: 10.13475/j.fzxb.20250805701

• 纤维材料 • 上一篇    下一篇

MXene改性对正十八烷-海藻酸钠相变微胶囊非等温结晶动力学的影响

曹祥玺1,2, 李博1,2, 孙艳丽1,2(), 姚倩1,2, 刘哲1,2, 陆少峰1,2   

  1. 1 西安工程大学 纺织科学与工程学院, 陕西 西安 710048
    2 西安工程大学 功能性纺织材料及制品教育部重点实验室, 陕西 西安 710048
  • 收稿日期:2025-08-27 修回日期:2026-03-07 出版日期:2026-05-15 发布日期:2026-07-10
  • 通讯作者: 孙艳丽(1989—),女,讲师,博士。主要研究方向为功能与智能纺织品。E-mail:sunyanli@xpu.edu.cn
  • 作者简介:曹祥玺(2002—),男,硕士生。主要研究方向为功能与智能纺织品。
  • 基金资助:
    陕西省教育厅科学研究计划项目(25JS052);泉州市引进高层次人才团队项目(24KGDW0036);陕西省自然科学基础研究计划项目(2023-JC-QN-0423);功能性纺织材料及制品教育部重点实验室开放课题(2024FTMP027);福厦泉国家自主创新示范区发展战略新兴产业和未来产业项目

Influence of MXene modification on non-isothermal crystallization kinetics of n-octadecane-sodium alginate phase change microcapsules

CAO Xiangxi1,2, LI Bo1,2, SUN Yanli1,2(), YAO Qian1,2, LIU Zhe1,2, LU Shaofeng1,2   

  1. 1 School of Textile Science and Engineering, Xi'an Polytechnic University, Xi'an, Shaanxi 710048, China
    2 Key Laboratory of Functional Textile Material and Product, Ministry of Education, Xi'an Polytechnic University, Xi'an, Shaanxi 710048, China
  • Received:2025-08-27 Revised:2026-03-07 Published:2026-05-15 Online:2026-07-10

摘要:

相变材料存在储热效率不足、调温时间有限等问题,这些均与其结晶行为密切相关。为提升热管理效能,采用二维纳米材料MXene改性相变微胶囊,调控其结晶行为以提升蓄热调温性能。通过乳液静电喷雾技术,以正十八烷为芯材、海藻酸钠为壁材,MXene改性制备了复合相变微胶囊。借助差示扫描量热仪(DSC)测试其在 5、10、15、20 ℃/min 4种降温速率下的非等温结晶行为,并运用 Jeziorny 法、莫志深法与 Kissinger 法开展动力学分析。结果表明,在相同降温速率下,随着 MXene 质量分数的增加,微胶囊的半结晶时间(t1/2)、冷却函数(F(T))及结晶活化能(ΔE)均呈现先下降后上升的趋势,其中,添加4% MXene的微胶囊相较于未改性样品,其t1/2缩短了约30%、F(T)值平均降低约42%,活化能下降约28%,说明适量MXene可有效提升非等温结晶速率,促进结晶过程并降低结晶能垒。MXene作为异相成核剂,其二维片层结构为结晶提供了成核位点,提升了复合相变微胶囊的结晶动力学行为。

关键词: 复合相变微胶囊, 正十八烷, 海藻酸钠, MXene, 非等温结晶, 结晶活化能, 蓄热调温纺织品

Abstract:

Objective Thermal energy storage and thermoregulatory textiles utilizing phase change materials (PCMs) can autonomously regulate micro-environment temperatures through phase transition processes, thereby significantly improving wear comfort and attracting considerable research interest. However, issues such as limited latent heat capacity and constrained regulation duration impede their broader development and application. These limitations are inherently linked to the crystallization behavior of PCMs. In order to address these limitations and further advance the thermal management performance of PCM-based textiles, this work systematically investigates the crystallization kinetics of MXene-incorporated phase-change microcapsules, as MXene exhibits exceptional thermal conductivity that can effectively accelerate thermal response and regulate the crystallization behavior of phase-change materials.

Method The microcapsules were synthesized by emulsion electrostatic spraying techniques, employing n-octadecane as the core, sodium alginate as the wall material, and MXene as an enhancer. The non-isothermal crystallization behavior of microcapsules doped with varying MXene contents was investigated using differential scanning calorimetry (DSC) at distinct cooling rates (Φ=5, 10, 15, 20 ℃/min). Additionally, crystallization kinetics were analyzed by the Jeziorny method, the Mo method, and the Kissinger equation to quantify crystallization mechanisms and activation energy.

Results The DSC results showed that with the increase of Φ, little difference appeared in the initial crystallization temperature of the same microcapsule, but the crystallization peak temperature decreased by 1-2 ℃, the peak width of the crystallization peak becames larger, and the half-crystallization time (t1/2) decreased significantly, indicating that the crystallization rate increased with the increase of the cooling rate. In MXene-modified microcapsules, the addition of 0-4% MXene increases the crystallization peak temperature. The results indicated that for a given cooling rate Φ, an increase in MXene content led to a situation where half-crystallization time (t1/2), cooling function (F(T)), and crystallization activation energy initially decreased before subsequently increasing. This suggests that adding MXene would enhance the crystallinity of microcapsules, whereas 5% MXene loading, it began to suppress the crystallization rate. This phenomenon occurred because the confined MXene acted as a nucleation catalyst during the initial microcapsule crystallization, facilitating crystal nucleation and growth on its surface. When the MXene content exceeds 4%, a rigid network would develop within the system, significantly hindering further crystal growth. Notably, microcapsules containing 4% MXene exhibited approximately 30% reduction in t1/2, a 42% decrease in the average F(T), and about a 28% reduction in activation energy relative to unmodified samples. These findings suggest that MXene mass concentration from 0% to 4% can significantly accelerate non-isothermal crystallization, facilitate nucleation, and lower the energy barrier for crystallization. As a heterogeneous nucleating agent, MXene's two-dimensional lamellar architecture provides nucleation sites, thereby enhancing the crystallization kinetics and thermal properties of the microencapsulated PCMs.

Conclusion Non-isothermal crystallization kinetics demonstrate that, at cooling rates of 5, 10, 15, 20 ℃/min, the optimal dosage of MXene modifiers can effectively decrease the activation energy required for the nucleation and growth of crystalline phases in microcapsules, thereby accelerating their crystallization kinetics. Consequently, analyzing the non-isothermal crystallization behavior offers valuable insights into optimizing the crystallization properties of phase change microcapsules, which can enhance their thermal storage capacity and thermoregulatory performance. This research provides useful reference for the development of high-efficiency thermoregulating and heat-storage textiles.

Key words: composite phase change microcapsule, n-octadecane, sodium alginate, MXene, non-isothermal crystallization, crystallization activation energy, thermal energy storage and temperature regulation textiles

中图分类号: 

  • TS101.3

图1

相变微胶囊的SEM照片"

图2

元素映射图像"

图3

不同降温速率下相变微胶囊的DSC曲线"

表1

不同降温速率下相变微胶囊的非等温结晶参数"

样品
名称
降温速率/
(℃·min-1)
T0/℃ Tp/℃ Te/℃ ΔHc/
(J·g-1)
S0 5 28.16 22.83 10.33 79.69
10 28.05 22.06 8.30 82.35
15 27.82 21.25 7.25 83.73
20 27.75 20.67 6.35 84.25
S2 5 28.67 23.50 10.91 74.87
10 28.33 22.83 9.66 75.15
15 28.50 22.50 9.25 75.98
20 28.85 22.33 7.33 76.66
S4 5 28.13 24.08 11.33 75.17
10 28.33 23.50 10.65 76.26
15 28.25 23.00 9.50 77.68
20 28.38 23.67 7.33 78.97
S5 5 27.67 21.58 10.17 78.06
10 27.83 20.17 9.67 78.67
15 27.75 19.05 8.13 79.68
20 27.66 18.25 6.35 81.95

图4

非等温结晶的结晶度随时间变化关系"

图5

相变微胶囊的t1/2-Φ曲线"

图6

相变微胶囊的lg[-ln(1-Xt )]-lgt曲线"

表2

基于Jeziorny法非等温结晶参数"

样品
名称
降温速率/
(℃·min-1)
n Zt Zc
S0 5 2.00 0.34 0.81
10 2.24 0.42 0.92
15 2.43 0.12 0.87
20 2.99 0.64 0.98
S2 5 1.96 0.32 0.80
10 2.21 0.23 0.86
15 2.14 0.58 0.96
20 2.39 0.83 0.99
S4 5 2.43 0.51 0.87
10 2.28 0.20 0.85
15 2.75 0.54 0.96
20 2.76 0.81 0.99
S5 5 2.47 1.12 1.02
10 2.20 0.20 0.85
15 2.26 0.05 0.82
20 2.19 0.25 0.93

图7

不同降温速率下相变微胶囊的lgβ-lgt曲线"

表3

基于Mo法的相变微胶囊的非等温结晶参数"

样品名称 相对结晶度/% F(T) α
S0 20 0.921 0.96
40 0.952 1.02
60 0.990 1.09
80 1.107 0.98
S2 20 0.468 1.47
40 0.580 1.32
60 0.732 1.45
80 0.990 1.37
S4 20 0.315 1.45
40 0.460 1.43
60 0.631 1.36
80 0.943 1.21
S5 20 0.692 0.95
40 0.791 1.03
60 0.883 1.08
80 0.993 1.12

图8

冷却函数与相对结晶度的变化关系"

图9

不同降温速率下样品ln(Φ/Tp2)-1/Tp曲线"

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