Numerical Analysis of the Effect of Floor Depression on the Extent of Thermal Interaction with the Ground and Energy Management Using a Vegetable Cold Store as an Example
Abstract
:1. Introduction
2. Materials and Methods
2.1. Research Object
2.2. Measuring Equipment
2.3. Calculation Methods and Tools
3. Results
3.1. Validation of the Computational Model
3.2. Verification of the Calculation Model
3.3. Heat Exchange with the Ground and Energy Balance of Cold Storage Facilities—Existing Condition
3.4. Heat Exchange with the Ground and Energy Balance of Cold Storage—Theoretical Variant with Floor Recessed into the Ground
4. Discussion
5. Conclusions
Author Contributions
Funding
Data Availability Statement
Conflicts of Interest
Nomenclature
ΔQ | increase in internal energy of the element (J) |
C | total heat capacity of the element (J·K−1) |
Δθ | element temperature increase (K) |
v | element volume (m3) |
c | specific heat of the element material (J·kg−1·K−1) |
ρ | material density (kg·m−3) |
i | element number |
Φixiyiz,… | heat flux flowing between element ix and iy and iz and neighboring elements (W) |
heat flux density (heat flow density) (W·m−2) | |
λ | thermal conductivity coefficient of the element material (W·m−1·K−1) |
∇ | Hamilton’s vector operator |
temperature gradient (K·m−1) | |
ΣΦ | the sum of heat flows between individual elements (J) |
θk+1 | temperature at time step k + 1 (K) |
θk | temperature at time step k (K) |
Δτ | time step (s) |
mi | measured parameter |
n | number of measured data |
si | calculated parameter |
mean value of measured parameters | |
p | number of adjustable model parameters |
NMBE | normalized mean bias error |
CV(RMSE) | coefficient of variation of the root mean square error |
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Specification | Unit | Value | |
---|---|---|---|
loamy clay | volumetric weight | kg·m−3 | 1600 |
specific heat | J·kg−1·K−1 | 1000 | |
thermal conductivity coefficient | W·m−1·K−1 | 1.80 | |
humus | volumetric weight | kg·m−3 | 1800 |
specific heat | J·kg−1·K−1 | 1260 | |
thermal conductivity coefficient | W·m−1·K−1 | 0.90 | |
polystyrene | volumetric weight | kg·m−3 | 20 |
specific heat | J·kg−1·K−1 | 1500 | |
thermal conductivity coefficient | W·m−1·K−1 | 0.04 | |
concrete | volumetric weight | kg·m−3 | 2300 |
specific heat | J·kg−1·K−1 | 1000 | |
thermal conductivity coefficient | W·m−1·K−1 | 2.30 | |
gravel ballast | volumetric weight | kg·m−3 | 1800 |
specific heat | J·kg−1·K−1 | 840 | |
thermal conductivity coefficient | W·m−1·K−1 | 0.90 | |
steel | volumetric weight | kg·m−3 | 7900 |
specific heat | J·kg−1·K−1 | 460 | |
thermal conductivity coefficient | W·m−1·K−1 | 17.00 |
Data Type | Uncertainty Index | FEMP 3.0 | ASHRAE G14-2014 | IPMVP |
---|---|---|---|---|
Hourly criteria (%) | NMBE | ±10 | ±10 | ±5 |
CV (RMSE) | ±30 | ±30 | ±20 |
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Sokołowski, P.; Jakubowski, T.; Nawalany, G.; Atilgan, A.; Syrotyuk, S. Numerical Analysis of the Effect of Floor Depression on the Extent of Thermal Interaction with the Ground and Energy Management Using a Vegetable Cold Store as an Example. Energies 2024, 17, 5. https://doi.org/10.3390/en17010005
Sokołowski P, Jakubowski T, Nawalany G, Atilgan A, Syrotyuk S. Numerical Analysis of the Effect of Floor Depression on the Extent of Thermal Interaction with the Ground and Energy Management Using a Vegetable Cold Store as an Example. Energies. 2024; 17(1):5. https://doi.org/10.3390/en17010005
Chicago/Turabian StyleSokołowski, Paweł, Tomasz Jakubowski, Grzegorz Nawalany, Atilgan Atilgan, and Serhiy Syrotyuk. 2024. "Numerical Analysis of the Effect of Floor Depression on the Extent of Thermal Interaction with the Ground and Energy Management Using a Vegetable Cold Store as an Example" Energies 17, no. 1: 5. https://doi.org/10.3390/en17010005
APA StyleSokołowski, P., Jakubowski, T., Nawalany, G., Atilgan, A., & Syrotyuk, S. (2024). Numerical Analysis of the Effect of Floor Depression on the Extent of Thermal Interaction with the Ground and Energy Management Using a Vegetable Cold Store as an Example. Energies, 17(1), 5. https://doi.org/10.3390/en17010005