BULLETIN OF THE CHINESE CERAMIC SOCIETY ›› 2026, Vol. 45 ›› Issue (3): 755-770.DOI: 10.16552/j.cnki.issn1001-1625.2025.1143
• Glass • Previous Articles Next Articles
YAN Hongying1,2(
), YAN Jingping2,3, JIANG Fangling2, ZHENG Qiuju1(
), DENG Lu2(
)
Received:2025-11-17
Revised:2026-01-11
Online:2026-03-20
Published:2026-04-10
Contact:
ZHENG Qiuju, DENG Lu
CLC Number:
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.
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 |
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 |
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 |
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 |
Fig.5 Relationship between Fnet descriptor and experimental density (a), glass transition temperature (b), CTE (c), Young’s modulus (d), hardness (e)[14]
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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