硅酸盐通报 ›› 2026, Vol. 45 ›› Issue (3): 755-770.DOI: 10.16552/j.cnki.issn1001-1625.2025.1143
闫洪滢1,2(
), 严静萍2,3, 蒋芳玲2, 郑秋菊1(
), 邓路2(
)
收稿日期:2025-11-17
修订日期:2026-01-11
出版日期:2026-03-20
发布日期:2026-04-10
通信作者:
郑秋菊,博士,教授。E-mail:qlzhengqj@163.com;作者简介:闫洪滢(2003—),女,硕士研究生。主要从事玻璃材料结构和化学稳定性的研究。E-mail:10431251384@stu.qlu.edu.cn
基金资助:
YAN Hongying1,2(
), YAN Jingping2,3, JIANG Fangling2, ZHENG Qiuju1(
), DENG Lu2(
)
Received:2025-11-17
Revised:2026-01-11
Published:2026-03-20
Online:2026-04-10
摘要:
复杂的非晶态结构和热力学亚稳态特征导致研究人员对玻璃材料结构-性能映射关系的理解仍面临挑战,因此,构效关系研究成为新型高性能玻璃研制的核心难题之一。定量结构-性质关系(QSPR)分析法通过建立数学模型将材料的微观结构与宏观性能相关联,为新型玻璃材料的研究提供了可以突破传统试错法局限的新途径。本文系统综述了QSPR分析法在玻璃材料领域中的最新研究进展:首先,梳理了从数据获取、描述符提取到模型构建的完整研究流程;其次,聚焦描述符体系的分类,阐述了自该方法首次提出后描述符体系在结构、能量和动力学机制方面的发展演化;随后,进一步总结了QSPR分析法在硅酸盐玻璃、磷酸盐玻璃及其他类型玻璃中成功预测力学、热学及化学稳定性等性能的案例,论证了其在实际材料设计中的有效性。最后分析了当前研究在描述符物理意义与数据质量方面面临的挑战,并展望了未来通过多尺度融合与多方法联用的改进策略,以推动QSPR分析法从解释工具向精准设计平台的转变。
中图分类号:
闫洪滢, 严静萍, 蒋芳玲, 郑秋菊, 邓路. 定量结构-性质关系分析法在玻璃材料领域的研究进展[J]. 硅酸盐通报, 2026, 45(3): 755-770.
YAN Hongying, YAN Jingping, JIANG Fangling, ZHENG Qiuju, DENG Lu. Research Progress of Quantitative Structure-Property Relationship Analysis Method in the Field of Glass Materials[J]. BULLETIN OF THE CHINESE CERAMIC SOCIETY, 2026, 45(3): 755-770.
图3 实验测量的密度(a)、硬度(b)、玻璃化转变温度(c),以及使用配位数为结构输入,探究用于评估玻璃网络整体强度的结构描述符Fnet与密度(d)、硬度(e)、玻璃化转变温度(f)的相关性,以及使用Q n 为结构输入,探究Fnet与密度(g)、硬度(h)、玻璃化转变温度(i)的相关性[43]
Fig.3 Experimentally measured density (a), hardness (b), glass transition temperature (c) and use coordination number as structure input to explore correlation between structural descriptor Fnet, which is used to evaluate the overall strength of glass network, and density (d), hardness (e), glass transition temperature (f), and use Q n as structural input to explore correlation between Fnet and density (g), hardness (h), glass transition temperature (i)[43]
| Item | Fnet | R2 |
|---|---|---|
| Density | BSdc/Tm with MNC | 0.865 |
| BSdc with MNC | 0.838 | |
| SBS/Tm | 0.813 | |
| Tg | EF/Tm with MNC | 0.732 |
| EF with MNC | 0.711 | |
| CTE | SBS with MNC | 0.973 |
| SBS/Tm with MNC | 0.972 | |
| BSdm with MNC | 0.971 | |
| BSdm/Tm with MNC | 0.943 | |
| Young’s modulus | EF/Tm | 0.988 |
| EF/Tm with MNC | 0.953 | |
| EF | 0.987 | |
| EF with MNC | 0.958 | |
| Hardness | EF | 0.933 |
| EF/Tm | 0.925 | |
| EF/Tm with MNC | 0.844 |
表1 Fnet描述符对于密度、玻璃化转变温度、热膨胀系数、杨氏模量和硬度的R2的值[14]
Table 1 Fnet descriptor provides values R2 for density, glass transition temperature, CTE, Young’s modulus and hardness[14]
| Item | Fnet | R2 |
|---|---|---|
| Density | BSdc/Tm with MNC | 0.865 |
| BSdc with MNC | 0.838 | |
| SBS/Tm | 0.813 | |
| Tg | EF/Tm with MNC | 0.732 |
| EF with MNC | 0.711 | |
| CTE | SBS with MNC | 0.973 |
| SBS/Tm with MNC | 0.972 | |
| BSdm with MNC | 0.971 | |
| BSdm/Tm with MNC | 0.943 | |
| Young’s modulus | EF/Tm | 0.988 |
| EF/Tm with MNC | 0.953 | |
| EF | 0.987 | |
| EF with MNC | 0.958 | |
| Hardness | EF | 0.933 |
| EF/Tm | 0.925 | |
| EF/Tm with MNC | 0.844 |
| Structure | Density | Hardness | Tg | CTE | Young’s modulus | ηP | ηAl | ηSi |
|---|---|---|---|---|---|---|---|---|
| CN | 1 | 1/R'M | RAl | 1/R'M | 1 | 1/R'p | R | R |
| Q n | R'M | 1/R'M | 1 | 1/R'M | 1 | 1/R'p | R | R |
表2 SAP系列与硅酸盐玻璃中不同性质相关的Ccoe系数[43]
Table 2 Ccoe coefficients associated with different properties in SAP series and silicate glass[43]
| Structure | Density | Hardness | Tg | CTE | Young’s modulus | ηP | ηAl | ηSi |
|---|---|---|---|---|---|---|---|---|
| CN | 1 | 1/R'M | RAl | 1/R'M | 1 | 1/R'p | R | R |
| Q n | R'M | 1/R'M | 1 | 1/R'M | 1 | 1/R'p | R | R |
Development stage | Descriptor | Key improvement | Advantage | Limitation |
|---|---|---|---|---|
| Early model | Fnet-BE[ | Combination of CN and BE | Pioneering the fusion of energy and structural parameters. | Dependent on MD simulation, limited application scope |
| Energy-related developments | Fnet-SBS[ | Optimized energy parameters: Replace BE with SBS and introduce MNC | Parameter optimization, significantly enhanced correlation | Dependent on experimental bond energy data |
| Fnet-FE[ | Substitution of EF with formation energy | Good correlation in silicate systems, high prediction accuracy | Strong dependency on FE data, high computational cost | |
| Fnet-CSE[ | Using electronegativity to replace bond energy, Ccoe is introduced | No experimental input required, strong cross-system applicability | Al CN prediction deviation, neglect of covalent effects | |
| Average metal oxide dissociation energy[ | Integration of metal-oxygen bond strengths and CN | Direct-correlation with dissolution energy barrier, excellent prediction performance | Strong dependency on CN accuracy | |
| Structure-related developments | Three-scale Fnet[ | Based on multi-scale structural descriptor: CN, Q n, and ring size | Validation of multi-scale QSPR strategy | Dependent on MD simulation, high computational cost |
| Topological indices descriptor[ | Quantification of spatial connectivity complexity in silicate networks | Highly correlated with various properties | Sensitive to methods of model construction | |
| Kinetics-related developments | Fnet-variants[ | Replace the fixed value mij by the NC-based dynamic factor | Identified optimal descriptor forms for different properties | Relatively complex parameters |
| Average self-diffusion coefficient of the molten state[ | Independent of bond energy parameters | Insensitive to thermal history, good stability | Neglect of external factors such as interface reactions |
表3 QSPR在玻璃材料领域的混合型描述符
Table 3 QSPR hybrid descriptors in the field of glass materials
Development stage | Descriptor | Key improvement | Advantage | Limitation |
|---|---|---|---|---|
| Early model | Fnet-BE[ | Combination of CN and BE | Pioneering the fusion of energy and structural parameters. | Dependent on MD simulation, limited application scope |
| Energy-related developments | Fnet-SBS[ | Optimized energy parameters: Replace BE with SBS and introduce MNC | Parameter optimization, significantly enhanced correlation | Dependent on experimental bond energy data |
| Fnet-FE[ | Substitution of EF with formation energy | Good correlation in silicate systems, high prediction accuracy | Strong dependency on FE data, high computational cost | |
| Fnet-CSE[ | Using electronegativity to replace bond energy, Ccoe is introduced | No experimental input required, strong cross-system applicability | Al CN prediction deviation, neglect of covalent effects | |
| Average metal oxide dissociation energy[ | Integration of metal-oxygen bond strengths and CN | Direct-correlation with dissolution energy barrier, excellent prediction performance | Strong dependency on CN accuracy | |
| Structure-related developments | Three-scale Fnet[ | Based on multi-scale structural descriptor: CN, Q n, and ring size | Validation of multi-scale QSPR strategy | Dependent on MD simulation, high computational cost |
| Topological indices descriptor[ | Quantification of spatial connectivity complexity in silicate networks | Highly correlated with various properties | Sensitive to methods of model construction | |
| Kinetics-related developments | Fnet-variants[ | Replace the fixed value mij by the NC-based dynamic factor | Identified optimal descriptor forms for different properties | Relatively complex parameters |
| Average self-diffusion coefficient of the molten state[ | Independent of bond energy parameters | Insensitive to thermal history, good stability | Neglect of external factors such as interface reactions |
图5 Fnet描述符分别与实验密度(a)、玻璃化转变温度(b)、热膨胀系数(c)、杨氏模量(d)、硬度(e)的相关性[14]
Fig.5 Relationship between Fnet descriptor and experimental density (a), glass transition temperature (b), CTE (c), Young’s modulus (d), hardness (e)[14]
图6 初始溶解速率r0与Fnet(a)、Fnet 和网络连接性修正因子(b)、桥氧百分比(c)、整体网络连接性(d)的相关性[50]
Fig.6 Correlation between initial dissolution rate r0 and Fnet(a), Fnet and modified network connectivity (b), bridge oxygen percentage (c), overall network connectivity (d)[50]
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