Impact of Thermal Mass, Window Performance, and Window–Wall Ratio on Indoor Thermal Dynamics in Public Buildings
Abstract
1. Introduction
2. Methodology
2.1. Simulation Process
2.1.1. The Physical Model
2.1.2. Building Envelope Parameters
2.1.3. Heating Power of Personnel, Lights, and Equipment
2.2. Evaluation Indicator
2.3. Validation
3. Results and Discussion
3.1. Study Overview and Analysis Scope
3.2. The Daily Average Maximum Temperature
3.3. The Daily Average Minimum Temperature
3.4. The Daily Average Temperature Fluctuation
3.5. The Attenuation Coefficient
3.6. The Occurrence of Extreme Superheat Temperatures During the Operational Period
3.7. The Cooling Load
4. Conclusions
- With the increase in thermal mass, the daily average maximum temperature increases by 0.33–0.96 °C. The daily average maximum temperature of the double-glazed window increased by 0–0.30 °C compared to the single-glazed window. With the increase in WWRs, the daily average maximum temperature increased by 1.43–1.67 °C. At this time, the influence of thermal mass on the daily average maximum temperature decreases, while the influence of window performance on the daily average maximum temperature increases. High WWRs can cause excessive indoor temperatures, especially for buildings using single-glazed windows.
- The daily average minimum temperature of heavy thermal mass is 0.14–0.31 °C and 0.45–0.94 °C higher than that of medium and light thermal mass, respectively. With the increase in WWRs, the daily average minimum temperature of the double-glazed window increased by 0.21–1.98%, while the daily average minimum temperature of the single-glazed window decreased by 0.06–2.24%. The increase in WWRs weakens the effect of thermal mass on the daily average minimum temperature. Light thermal mass, the single-glazed window, and high WWRs contribute to the building’s nighttime heat dissipation.
- With the increase in thermal mass, the daily average Tflu increased by 0.18–0.29%, and the influence was weak. Compared with the double-glazed window, the daily average Tflu of the single-glazed window increased significantly by 2.56–22.14%. With the increase in WWRs, the daily average Tflu also increased significantly (2.33–44.18%). In Qingdao’s summer, buildings with single-glazed windows and high WWRs are more conducive to improving thermal comfort.
- With the increase in thermal mass and WWRs, the attenuation coefficient increases by 0.18–0.24% and 2.18–40.72%, respectively, while the attenuation coefficient of the single-glazed window is 0.02–0.15 higher than that of the double-glazed window, which is more likely to cause indoor overheating. However, from the point of view of the occurrence time of different temperatures during the operational period, when the WWRs ≥ 50%, the single-glazed window shows better performance than the double-glazed window, and the extreme temperature occurrence time is reduced by 0.81–14.63%.
- When the refrigeration system is turned on, the increase in WWR leads to an increase in the cooling load (14.30–30.56%). In double-glazed buildings, the cooling load decreases by 0.07–1.04% with the increase in thermal mass; in single-glazed buildings, when WWRs < 50%, the cooling load decreases by 0.13–0.86% with the increase of thermal mass. When WWRs ≥ 50%, the cooling load increases by 0.02–0.38% with the increase in thermal mass. Controlling WWRs is the key to energy conservation, and light thermal mass is recommended for buildings with high WWRs and single-glazed windows.
Author Contributions
Funding
Data Availability Statement
Conflicts of Interest
References
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Type | Layer | Thickness (δ), m | Total Thickness (δ), m | Overall Heat Transfer Coefficient (U), W·m−2K−1 |
---|---|---|---|---|
Celling | Expanded polystyrene board | 0.02 | 0.155 | 0.224 |
Reinforced concrete | 0.12 | |||
Cement mortar | 0.015 | |||
Interior wall | Gypsum | 0.012 | 0.074 | 0.652 |
Insulation | 0.050 | |||
Gypsum | 0.012 | |||
Light thermal mass | Plaster | 0.015 | 0.285 | 0.833 |
Insulation | 0.030 | |||
Brick | 0.240 | |||
Medium thermal mass | Plaster | 0.015 | 0.320 | 0.485 |
Insulation | 0.065 | |||
Brick | 0.240 | |||
Heavy thermal mass | Plaster | 0.015 | 0.355 | 0.339 |
Insulation | 0.100 | |||
Brick | 0.240 |
Type | Double 14011 | Single 102 |
---|---|---|
Thickness of glass (δ), mm | 26 (6/16/4) | 6 |
Overall heat transfer coefficient (U), W·m−2K−1 | 1.240 | 5.69 |
Solar radiation transmissivity | 0.354 | 0.823 |
Solar radiation reflectivity | 0.321 | 0.072 |
Visible light transmissivity | 0.529 | 0.855 |
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Cheng, R.; Zhang, N.; Zhang, W.; Sun, Y.; Yin, B.; Gao, W. Impact of Thermal Mass, Window Performance, and Window–Wall Ratio on Indoor Thermal Dynamics in Public Buildings. Buildings 2025, 15, 1757. https://doi.org/10.3390/buildings15101757
Cheng R, Zhang N, Zhang W, Sun Y, Yin B, Gao W. Impact of Thermal Mass, Window Performance, and Window–Wall Ratio on Indoor Thermal Dynamics in Public Buildings. Buildings. 2025; 15(10):1757. https://doi.org/10.3390/buildings15101757
Chicago/Turabian StyleCheng, Ran, Nan Zhang, Wengan Zhang, Yinan Sun, Bing Yin, and Weijun Gao. 2025. "Impact of Thermal Mass, Window Performance, and Window–Wall Ratio on Indoor Thermal Dynamics in Public Buildings" Buildings 15, no. 10: 1757. https://doi.org/10.3390/buildings15101757
APA StyleCheng, R., Zhang, N., Zhang, W., Sun, Y., Yin, B., & Gao, W. (2025). Impact of Thermal Mass, Window Performance, and Window–Wall Ratio on Indoor Thermal Dynamics in Public Buildings. Buildings, 15(10), 1757. https://doi.org/10.3390/buildings15101757