河南大学化学与分子科学学院 开封 475004
pc@henu.edu.cn
zhangwenkai@henu.edu.cn
收稿:2026-03-25,
录用:2026-04-10,
网络首发:2026-06-08,
纸质出版:2026-07-20
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张曼曼, 王驰宇, 王慧娟, 樊文豪, 叶子凡, 高稍轩, 孟献瑞, 彭闯, 张文凯. 非平衡相分离驱动的温敏水凝胶时间可调光学响应. 高分子通报, 2026, 39(7), 1204–1215.
Zhang, M. M.; Wang, C. Y.; Wang, H. J.; Fan, W. H.; Ye, Z. F.; Gao, S. X.; Meng, X. R.; Peng, C.; Zhang, W. K. Nonequilibrium phase separation‑driven temporally tunable optical response in thermoresponsive hydrogels. Polym. Bull. (in Chinese), 2026, 39(7), 1204–1215.
张曼曼, 王驰宇, 王慧娟, 樊文豪, 叶子凡, 高稍轩, 孟献瑞, 彭闯, 张文凯. 非平衡相分离驱动的温敏水凝胶时间可调光学响应. 高分子通报, 2026, 39(7), 1204–1215. DOI: 10.14028/j.cnki.1003-3726.2026.26.054.
Zhang, M. M.; Wang, C. Y.; Wang, H. J.; Fan, W. H.; Ye, Z. F.; Gao, S. X.; Meng, X. R.; Peng, C.; Zhang, W. K. Nonequilibrium phase separation‑driven temporally tunable optical response in thermoresponsive hydrogels. Polym. Bull. (in Chinese), 2026, 39(7), 1204–1215. DOI: 10.14028/j.cnki.1003-3726.2026.26.054.
温敏水凝胶的光学响应通常由平衡相行为决定,而对溶剂交换过程中产生的非平衡效应仍缺乏系统性的认识。本研究以P(NIPAM-
co
-AAm)水凝胶为模型体系,考察其在水–乙醇混合溶剂中的透光率随时间的变化行为。在相同终态温度与溶剂组成条件下,不同处理方式得到的光学状态存在明显差异。水溶胀态样品直接进入高温乙醇环境时,乙醇向内扩散在凝胶内部形成瞬时组成梯度,使局部区域进入LCST敏感区间并发生相分离,出现短时浑浊;而先完成溶剂交换再升温时,体系始终处于均一溶剂环境,保持透明。通过分析透光率–时间曲线,提取相分离时间
τ
p
与恢复时间
τ
rel
,发现两者随乙醇浓度显著变化,其比值由约11.7降低至1.5,对应由长时间维持浑浊到快速恢复透明的转变。冷冻干燥扫描电子显微镜与原位光学显微结果表明,不同处理路径对应的结构形貌存在明显差异。通过调控乙醇浓度或环境温度,可在数十秒至数千秒范围内连续调节相分离特征时间,实现对光学响应时间的精准控制,为动态光学调控材料的设计提供了可行思路。
The optical response of thermoresponsive hydrogels is typically governed by equilibrium phase behavior
whereas the nonequilibrium effects arising from solvent exchange processes remain insufficiently understood. In this study
we used P(NIPAM-
co
-AAm) hydrogels as a model system to investigate the temporal evolution of transmittance in water-ethanol mixed solvents. Under identical final-state temperatures and solvent compositions
distinct optical states were observed depending on the treatment pathway. When a water-swollen sample is directly introduced i
nto a high-temperature ethanol environment
the inward diffusion of ethanol generates transient compositional gradients within the gel
causing localized regions to enter the LCST-sensitive range and undergo phase separation
resulting in temporary turbidity. In contrast
when solvent exchange was completed prior to heating
the system remained in a homogeneous solvent environment and remained transparent. Analysis of the transmittance-time curves revealed the characteristic phase separation time
τ
p
and recovery time
τ
rel
both of which varied significantly with ethanol concentration
with their ratio decreasing from approximately 11.7 to 1.5
corresponding to a transition from prolonged turbidity to rapid recovery of transparency. Cryo-SEM and
in situ
optical microscopy results revealed distinct structural morphologies depending on the treatment pathway. The phase separation characteristic time can be continuously tuned from tens to thousands of seconds by varying the ethanol concentration or temperature
allowing precise regulation of the optical response time and offering a promising strategy for dynamic optical materials.
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