Optimization and Renovation Design of Indoor Thermal Environment in Traditional Houses in Northeast Sichuan (China)—A Case Study of a Three-Section Courtyard House
Abstract
:1. Introduction
2. Methodology
2.1. General Situation and Climatic Conditions of Traditional Houses in Northeast Sichuan
2.2. Mathematical Model and Thermal Physical Parameters of Traditional Residential Buildings
2.2.1. Establishment and Parameter Settings of Traditional Residence Model
2.2.2. Heat Transfer Analysis of Traditional Residential Building Model
- (1)
- There is a functional relationship between the heat transfer process of the outdoor surface and solar radiation, the surrounding environment, and outdoor air. The expressions for the physical and mathematical models of the heat balance of the outdoor surface are as follows:
- (2)
- The heat transfer process for the exterior wall of the building was divided into three stages:
- (a)
- When the air temperature of the room (Tin) is higher than that of the wall inner surface (Tj), that is, Tin > Tj, Equation (2), the heat absorbed by the inner surface of the wall (qi), is given by
- (b)
- When the temperature of the inner surface of the wall (Tj) is higher than that of the outer surface (Ti), that is, Tj > Ti, the heat conduction (Equation (3)) of the wall material layer (qy) is
- (c)
- When the temperature of the outer wall surface (Ti) is higher than the outer air temperature (Tout), that is, Ti > Tout, Equation (4), which is the heat released by the wall’s outer surface, (qe) is
- (3)
- The physical and mathematical models of the indoor heat balance are generally modelled using four coupled heat transfer components: conduction through building units, air convection, short-wave radiation absorption and reflection, and long-wave radiation exchange. The incoming short-wave radiation originates from solar radiation entering the area through the window and the emittance of the internal light source. Long-wave radiation exchange includes the absorption and emission of low-temperature radiation sources such as surfaces, devices, and people in all other areas. In summary, the physical and mathematical models of the indoor heat balance can be expressed as
2.2.3. Physical Parameters of Building Materials
2.3. Renovation Plan of Traditional Houses
- (1)
- Renovation schemes of different primary wall materials
- (2)
- Wall reconstruction scheme of added air interlayer
- (3)
- Adding insulation materials to the wall transformation scheme
- (4)
- Wall renovation schemes for different thermal insulation positions
2.4. Measuring Platform and Measuring Instruments
3. Results and Discussion
3.1. Comparison and Verification between Measured Data and Simulated Data
3.2. Comparison of Refrigeration Energy Consumption in the Renovation Scheme of the Main Material of the Wall
3.3. Comparison of Refrigeration Energy Consumption of Wall Renovation Schemes with Added Air Interlayer
3.4. Comparison of the Refrigeration Energy Consumption of Wall Renovation Schemes with Insulation Materials
3.5. Comparative Analysis of the Refrigeration Energy Consumption of External Insulation and Internal Insulation Wall Renovation Schemes
4. Conclusions
- Compared to Case 1 and Case 2, Case 3 had the lowest building cooling energy consumption, with a total refrigeration energy consumption of only 427.7 kW·h. This indicates that when the main material of the wall is an aerated concrete block, the wall-renovation scheme has the best heat insulation and energy-saving effects.
- The refrigeration energy consumption of Case 4 in the hottest week was 422 kW·h, which was 4.3 kW·h less than that of Case 3. This indicates that the wall-renovation scheme with air interlayers exhibits better thermal insulation and energy-saving effects. This study serves as a reference for traditional house designers.
- Compared with Case 5 and Case 6, Case 7 consumed the least amount of energy in the hottest week at only 409.8 kW·h. Therefore, the XPS thermal insulation material transformation scheme has better thermal insulation and energy-saving effects.
- The refrigeration energy consumption of Case 7 was only 409.8 kW·h in the hottest week, which was 4.19% lower than that of Case 3 (without insulation materials). Therefore, selecting a central insulation scheme for an actual project results in better thermal insulation and energy-saving effects.
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Conflicts of Interest
Nomenclatures
q″αsol | Absorption of direct and diffuse solar (short wavelength) radiation by heat flow, [W/m2]; |
q″LWR | The exchange of heat radiation flux with air and the surrounding environment, [W/m2]; |
q″outdoor | Convection flux exchange between the outer surface and the outside air, [W/m2]; |
q″ko | Heat conduction flux (q/A) to the wall surface, [W/m2]; |
qi | The heat exchange intensity per unit time and area of the inner surface of the wall, [W/m2]; |
qic | The heat transferred by air to the inner surface of the wall by convective heat transfer in unit time, [W/m2]. |
qir | The heat transferred to the inner surface of the wall by means of radiant heat exchange on each surface of the heat tank in unit time, [W/m2]. |
αi | Heat transfer coefficient of the inner surface of the wall, [W/(m2·K)]. |
Tin | Air temperature in the hot box, [°C]. |
Tj | The inner surface temperature of the wall, [°C]. |
Ti | The outer surface temperature of the wall, [°C]. |
Tout | Air temperature in a cold box, [°C]. |
qy | Intensity of heat flow through the wall per unit time and per unit area, [W/m2]. |
R | Thermal conductivity resistance of the wall, [m2·K/W]. |
qe | Heat flow intensity on the surface of the wall per unit area per unit time, [W/m2]. |
αe | Heat transfer coefficient of the outer surface of the wall, [W/(m2·K)]. |
q″LWX | Net long-wave radiation energy exchanged with the room surface, [W/m2]; |
q″SW | Net shortwave radiation energy from light emission, [W/m2]; |
q″LWS | The amount of long-wave radiation emitted by equipment in the room, [W/m2]; |
q″ki | Heat gain through the wall, [W/m2]; |
q″sol | Solar radiation heat absorbed by the wall surface, [W/m2]; |
q″indoor | Convection heat transfer with indoor air, [W/m2]. |
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Name | Materials | Thickness (mm) | Density (kg/m3) | Specific Heat [J/(kg·k)] | Heat Conductivity Coefficient [W/(m·k)] |
---|---|---|---|---|---|
Roof | Tile | 10 | 1920 | 1260 | 1.59 |
Clay | 35 | 1600 | 1010 | 0.76 | |
Board | 15 | 500 | 2510 | 0.17 | |
Bamboo and earth walls | Calcicoater | 10 | 1800 | 1050 | 0.81 |
Rammed earth | 60 | 1795.6 | 884 | 0.72 | |
Calcicoater | 10 | 1800 | 1050 | 0.81 | |
Wooden exterior wall | Board | 50 | 500 | 2510 | 0.17 |
Door | Board | 50 | 500 | 2510 | 0.17 |
Floor | Limestone soil | 100 | 2000 | 1010 | 1.16 |
Stone block | 300 | 2400 | 920 | 2.04 | |
Ceiling | Board | 50 | 500 | 2510 | 0.17 |
Interior wall | Calcicoater | 10 | 1800 | 1050 | 0.81 |
Rammed earth | 10 | 1795.6 | 884 | 0.72 | |
Calcicoater | 10 | 1800 | 1050 | 0.81 |
Case | Materials (Arranged from Inside to Outside) | Thickness (mm) | Density (kg/m3) | Specific Heat [J/(kg·k)] | Heat Conductivity Coefficient [W/(m·k)] |
---|---|---|---|---|---|
Case 1 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Solid clay brick | 200 | 0.76 | 1086 | 1700 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 | |
Case 2 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Porous clay brick | 200 | 0.58 | 1062 | 1400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 | |
Case 3 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 200 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 |
Case | Materials (Arranged from Inside to Outside) | Thickness (mm) | Density (kg/m3) | Specific Heat [J/(kg·k)] | Heat Conductivity Coefficient [W/(m·k)] |
---|---|---|---|---|---|
Case 3 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 200 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 | |
Case 4 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Air space | 20 | 0.026 | 1005 | 1210 | |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 |
Case | Materials (Arranged from Inside to Outside) | Thickness (mm) | Density (kg/m3) | Specific Heat [J/(kg·k)] | Heat Conductivity Coefficient [W/(m·k)] |
---|---|---|---|---|---|
Case 5 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Mineral wool board | 20 | 0.045 | 1220 | 140 | |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 | |
Case 6 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
EPS | 20 | 0.042 | 1380 | 18 | |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 | |
Case 7 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
XPS | 20 | 0.03 | 1380 | 20 | |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 |
Case | Materials (Arranged from Inside to Outside) | Thickness (mm) | Density (kg/m3) | Specific Heat [J/(kg·k)] | Heat Conductivity Coefficient [W/(m·k)] |
---|---|---|---|---|---|
Case 7 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
XPS | 20 | 0.03 | 1380 | 20 | |
Aerated concrete block | 100 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 | |
Case 8 | Cement mortar | 10 | 0.93 | 1050 | 1800 |
XPS | 20 | 0.03 | 1380 | 20 | |
Aerated concrete block | 200 | 0.18 | 1430 | 400 | |
Cement mortar | 10 | 0.93 | 1050 | 1800 |
Equipment Name | Type Specification | Measurable Variable | Measuring Range and Accuracy |
---|---|---|---|
Temperature and humidity tester | ZA88289 | Humidity | 0–100% (±3%) |
Temperature | −40–85 °C (± 0.5 °C) | ||
Solar radiation tester | JTR05 | Radiation | 0–2000 W/m2 (±1 W/m2) |
Temperature | −40 °C–120 °C (±0.5 °C) | ||
Wind speed tester | JT1402 | Wind speed | 0–20 m/s (±0.03 m/s) |
Black globe temperature tester | JTR04 | Black globe temperature | −20–125 °C (±0.5 °C) |
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Hou, C.; Hu, W.; Jiang, Y.; Gao, W. Optimization and Renovation Design of Indoor Thermal Environment in Traditional Houses in Northeast Sichuan (China)—A Case Study of a Three-Section Courtyard House. Sustainability 2024, 16, 2921. https://doi.org/10.3390/su16072921
Hou C, Hu W, Jiang Y, Gao W. Optimization and Renovation Design of Indoor Thermal Environment in Traditional Houses in Northeast Sichuan (China)—A Case Study of a Three-Section Courtyard House. Sustainability. 2024; 16(7):2921. https://doi.org/10.3390/su16072921
Chicago/Turabian StyleHou, Chaoping, Wentao Hu, Yuefan Jiang, and Weijun Gao. 2024. "Optimization and Renovation Design of Indoor Thermal Environment in Traditional Houses in Northeast Sichuan (China)—A Case Study of a Three-Section Courtyard House" Sustainability 16, no. 7: 2921. https://doi.org/10.3390/su16072921
APA StyleHou, C., Hu, W., Jiang, Y., & Gao, W. (2024). Optimization and Renovation Design of Indoor Thermal Environment in Traditional Houses in Northeast Sichuan (China)—A Case Study of a Three-Section Courtyard House. Sustainability, 16(7), 2921. https://doi.org/10.3390/su16072921