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Article

Determination of the Optimal Order of Grey-Box Models for Short-Time Prediction of Buildings’ Thermal Behavior

1
Laboratory of civil engineering and geo-environment, Lille University, 59650 Villeneuve d’Ascq, France
2
School of Civil Engineering, Tongji University, Shanghai 200092, China
3
Modeling Center, Lebanese University, Hadath 99000, Lebanon
*
Authors to whom correspondence should be addressed.
Buildings 2019, 9(9), 198; https://doi.org/10.3390/buildings9090198
Submission received: 25 July 2019 / Revised: 26 August 2019 / Accepted: 27 August 2019 / Published: 29 August 2019

Abstract

:
The use of grey-box models for short-time forecasting of buildings’ thermal behavior requires the determination of the models’ order since this order could influence the grey-box models’ performance. This paper presents an analysis of the optimal order of these models for different thermal conditions. The novelty of this work consists of considering the influence of the heating conditions on the determination of the performances of grey-box models. The analysis is based on experimental tests that were conducted in a room with different thermal conditions, related to the variation of the heating power. Experimental results were used for the determination of the optimal grey-box models’ order that minimizes the gap between the experimental results and the grey-box forecasting. Results show that the optimal grey-box models’ order depends on the buildings’ thermal conditions, but generally lies between two and three with an error less than 0.2 °C and a fit percent greater than 90%.

1. Introduction

Building energy simulation models (white models) require a good understanding of the thermal behavior of buildings [1]. Since the use of these models requires detailed information about the buildings’ components, equipment and use, as well as large computation capacities [2,3], alternative thermal models were proposed for the thermal modelling of buildings such as the black-box models [4,5] and grey-box models [6,7].
The grey-box models provide some advantages in the buildings’ thermal modeling process, in particular, ease of their use and the possibility to link their parameters to global buildings’ physical characteristics, such as the heat resistance and the mass capacity. These models can be used for different purposes such as control of the indoor environment [8,9], forecasting energy consumption, and evaluating buildings’ energy performance [10,11,12]. However, their practical use is subjected to the difficulty of the determination of their optimal order. This issue was investigated recently in some papers [6,13]. For unoccupied buildings, Bacher and Madson [14] showed that the performances of the grey-box were not improved by increasing the model order beyond 3. Hedgaard and Peterson [13] showed that the second and third-order models produce a good short-time forecasting of the building’s thermal behavior. Fonti et al. [15] used experimental studies to analyze the accuracy of grey-box models for the short-term prediction of a building. Results showed that the second-order models provide the required accuracy. Reynders et al. [16] carried out an identification study to determine suitable reduced-order models for predicting the thermal response of a residential building. They found out that best predictions were obtained with the third-order grey-box model.
Generally, the grey-box models’ order is presumed independent of the power supply conditions. In recent research [17], it was shown that the heating conditions should be considered in the determination of the optimal order of the grey-box models and that the data dynamics affect the performance of grey-box models. This paper discusses this issue using experimental tests conducted in various heating conditions for the investigation of the influence of these conditions on the optimal order of the grey-box model.

2. Methodology

Tests were carried out in a room submitted to various thermal conditions. The indoor temperature, as well as the external temperature, were recorded. Tests were conducted with three values of the indoor heating power (zero, 900 W and 1500 W). The results of each test were then used for the analysis of the grey-box models’ performances for three forecasting times: 15, 30, and 60 min. Analyses were conducted with four values of the grey-box order: 1, 2, 3 and 4 (Figure 1). The optimal order of the grey-box model for each experiment was then determined by comparing the numerical simulations to recorded data.
Numerical simulations were performed using MATLAB software.

2.1. Grey Box Modeling

Grey box models combine building physics and statistics. Physical knowledge derived from the buildings’ dynamics is formulated by stochastic differential equations in the state space form [15]. Statistical measurements present information embedded in the collected data.
dX ( t ) = A ( θ ) X ( t ) + B ( θ ) U ( t ) +   σ ( θ ) dw   ,   Y ( t ) = C ( θ ) X ( t ) + D ( θ ) U ( t ) +   ε
Sun radiation is considered zero due to the absence of windows. Parameters θ were estimated using MATLAB software. The model structures are derived from (RC) networks, analogue to the electric circuit.
The parameters of the model represent different thermal properties of the building. This includes thermal resistances: R, Re, Ri, Rm, and Rf.
The heat capacities of different parts of the building are represented by: C, Ci, Cfe and Cfi and Cm.
Finally, the input vector consists of Te and the internal energy sources which are presented by Qs and Qh.
An example of a simple model (1R1C) is given here. By applying the dynamic heating balance equation, we get:
C dTi dt = 1 R ( Te Ti ) + heating   source ,   C dTi dt = 1 R ( Te Ti ) + Qs + Qh
Same methodology was applied for the other orders.

2.2. Parameters Estimation

The model’s parameters were determined using ‘Greyest’ function in ‘Matlab’. This function provides the maximum likelihood using the following algorithms: The Gauss-Newton direction, the Levenberg-Marquardt and the steepest descent gradient [15,18].
Initialization of parameters was calculated by applying the French thermal code (RT 2005–2012), see Appendix A [11,19,20]. Table 1 presents the initial values of the parameters defining buildings’ characteristics.
The performance of the model is evaluated by (i) the root-mean-square error (RMSE-values); (ii) the final prediction errors (FPE); (iii) the level of fit (FIT) or normalized root mean square error (NRMSE) and (iv) the auto-correlation of the residuals [21]. The error distribution ‘e’ between the predicted and recorded temperatures is also determined (e is evaluated by subtracting the predicted value from the recorded one than a distribution analysis was carried out.).
A sensitivity study was performed by calculating the Sobol index to verify that all estimated models’ parameters are necessary for the predictions. This method allows measuring the overall impact of a parameter in the output of the model. When the Sobol index is high (close to 1), the parameter has a strong impact on the model.
Saltelli [22] and Jansen [23] proposed the following expression for the Sobol index:
  ST i   = 1 2 N w = 1 N ( Y b Y ci ) 2 Var ( Y a   ,   Y b ) ,
The model comparative criterion (Y) is the Root Mean Squared Error (RMSE, Equation (4)) between the predicted data and the reference data. The quasi-random LHS (Latin hypercube sampling) type method is used to accelerate the convergence. All parameters vary by plus or minus 30% of their adjusted value (values after learning).
RMSE   = i = 1 n ( y i y ^ i ) 2 n ,
For each dataset, the most performing order are investigated. A parameter cannot be identified correctly if its variation does not impact output values. Therefore, it is necessary to have high values of the total Sobol index for all parameters to validate the model architecture.

3. Experimental Data

A smart monitoring system was installed in a room of a research building ‘A4’ at Lille University in the north of France. The room is formed of two façades and two internal walls without windows. The following experiments were conducted (Table 2):
-
Experiment A: The room was submitted only to external thermal condition without any indoor heating power.
-
Experiment B: The room was submitted to the external thermal conditions as well as to an indoor 900 W heating power.
-
Experiment C: The room was submitted to the external thermal conditions as well as to an indoor 1500 W heating power.
Figure 2 shows the variation of the indoor temperature for low and high heating levels. This graph indicates that for 4 hours high heating, 18 minutes (min) has been needed for a variation of 1 °C, while 30 min is needed for low heating. By decreasing the heating time of 2 hours, 12 min are needed for a variation of 1 °C at 1500 W heating. We noticed that for high heating, 25 min are needed to achieve a variation of 1 °C for the difference between the indoor and outdoor temperatures, while 40 min are needed for low heating. By decreasing the heating time of 2 hours, 15 min is needed for a variation of 1 °C at 1500 W heating. Consequently, it is necessary to execute prediction for 15 min, 30 min, and 60 min to cover the phase of façade heating exchange.

4. Results and Discussion

For each dataset, the prediction is executed for 15, 30 and 60 min for the first, second, third and fourth order. To simplify the comparison, results will be presented in terms of RMSE and fit percent to determine the best performing models and to evaluate the impact of the dynamics of data on the predictions quality.

4.1. Sensitivity Analysis

Sensitivity analysis was conducted to confirm the significant role of chosen parameters [24]. Table 3 presents the result of this analysis. It shows that all parameters have an important influence on forecasting values. Figure 3 indicates that for tests B and C, the "Ri" parameter is among the two highest indices. This parameter represents the thermal resistance of indoor air in the building. It shows that this phenomenon has a preponderant impact on the thermal behavior of the building.
We noticed that for test B, Ci and Cfe have low total Sobol indices comparing to other parameters (0.07 and 0.09), but their values are not negligible. This can be referred to the subjection of these parameters to a small amplitude of variation (± 30%) compared to the dispersion observed in a real building.
This sensitivity analysis showed that the totality of identified parameters had an important role in predicting the building’s thermal behavior.

4.2. Experiment A (Heating Power = 0)

Table 4 illustrates the influence of the order of grey-box model on the quality of temperature predictions at 15 minutes. It could be observed that the optimal order of the grey-box model is equal to 2 (RMSE equal to 0.0616), with a slight difference with orders 1 and 3, which have RMSEs equal to 0.0656 and 0.0648, respectively. Table 5 and Table 6 illustrate the influence of the order of grey-box model on the quality of temperature predictions at 30 and 60 minutes. This influence is similar to that of 15 minutes. Since by increasing the model order above 1, the improvement in the temperature prediction is negligible, order 1 could be retained for this dataset as the simplest structure. Models of fourth order did not converge for all predictions because this experiment does not include any excitation source. Similar results were provided by Reynders et al. [16].
Figure 4 shows the error distribution corresponding to the first order. It could be observed that about 99% of the data have an error of less than 0.5 °C for 15, 30, and 60 min predictions. Model of order one can be used effectively for 1-hour prediction (large-step forecasting), which is considered adequate for heating control.

4.3. Experiment B (Heating Power = 900 W)

Table 7, Table 8 and Table 9 illustrate the influence of the grey-box models’ order on the temperature predictions at 15, 30, and 60 minutes. It could be observed that the optimal order is equal to 3, with a slight difference with order 2. Models of first order do not converge for all predictions. This result is similar to the those obtained in [25], because this order is not sufficient to explain the data dynamics.
Models of fourth order become more sensitive and complex for this set of data.
Figure 5 shows the error distribution corresponding to the third order. It could be observed that about 99% of the data have an error of less than 0.5 °C for 15- and 30-min predictions and 97% for 60-min predictions.
Figure 6 illustrates the residuals’ auto-correlation for order 3 obtained with a lag of 25. The yellow interval shows a 99% limit of confidence, which indicates that this model describes well the building dynamics.

4.4. Experiment C (Heating Power = 1500 W)

Table 10, Table 11 and Table 12 illustrate the influence of the order of the grey-box model on the temperature predictions at 15, 30 and 60 minutes. It could be observed that the optimal order is equal to 2, with a slight difference with orders 3 and 4. Results show that this dataset explains the best the building’s dynamics since all models’ orders present satisfactory performances with the greatest fit percentage and the lowest RMSE. This confirms the results obtained in [15], where the order 2 was the most performing order with RMSE less than 0.5 °C and fit percent equal to 94% for 1-hour prediction.
Figure 7 shows the error distribution corresponding to the second order. It could be observed that about 99% of the data have an error of less than 0.5 °C for 15- and 30-min predictions and 97% for 60-min predictions.
Figure 8 shows the residuals’ auto-correlation for order 2 with a lag of 25. The yellow interval indicates a 99% limit of confidence. This figure indicates that this model describes the building dynamics well.
By analyzing the previous results, we noticed that the choice of the model’s order depended on the data dynamics. The prediction for the most reliable order for all the data sets present performing results for short term forecasting. Dynamic data with heating at 1500 W reveal the most buildings’ dynamics. We can notice the need for an automated process combining many datasets and grey-box models able to determine the most performing order for the best dataset revealing the real dynamics of the building.

5. Conclusions

This paper presented a method for the determination of the optimal order of the grey-box models used in forecasting building’s thermal behavior in different thermal conditions. Experiments were conducted in a monitored room with three values of the heating power. These experiments were used for the analysis of the influence of the order of the grey-box models on the quality of the short-time forecasting of the indoor temperature. Results show that the optimal order of the grey-box models depends on the buildings’ thermal conditions, but generally lies between 2 and 3 with an error less than 0.2 °C and a fit percent greater than 90% for all prediction times. Analyses indicate that in the case of dynamic heating, the first order is not sufficient for the identification process. This study reveals a need for data in different heating conditions to determine the optimal order of the grey-box models.

Author Contributions

Conceptualization, N. A. and I.S.; Methodology, N.A. and I.S.; Software, N.A.; Analysis, N.A., I.S., H.M. and R.Y.; Writing-Original Draft Preparation, N.A.; Writing-Review and Editing, I.S.

Acknowledgments

This research received funding from the University of Lille, the French University Agency (AUF) and the Lebanese National Council for Scientific Research CNRS-L.

Conflicts of Interest

The authors declare no conflict of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

Nomenclature

X(t)State vector of the dynamic system, temperature of building’s components
U(t)Vector of measured inputs (outdoor temperature, sun radiation and heating power).
WRandom function of time (Wiener process).
Y(t)Measured output.
ε Measurement error.
θEstimated parameter
TiIndoor air temperature,
TfTemperature of building envelope
TfeTemperature of the external building façade
TfiTemperature of the internal building façade
TmTemperature of internal wall
R:Resistance between indoor and outdoor medium
ReConvection resistance of outdoor air
Ri, RmConvection resistance of indoor air
Rf:Conduction resistance of the façade
CEquivalent mass capacity for building
CiAir mass capacity,
CfEnvelope mass capacity
CfeExternal capacity of the façade
CfiInternal capacity of the façade
CmMass capacity of internal walls
TeOutdoor temperature
QsSolar energy gain
QhHeating energy gain
RMSERoot-mean-square error
FPEFinal prediction error
FITLevel of fit
NRMSENormalized root mean square error
eError
STiTotal Sobol index
NNumber of samples
Yb, YaVectors of output data in which all parameters vary
YciOutput vector in which all parameters vary except the ith
yiPredicted temperature
y i ^ Reference temperature
nNumber of samples.

Appendix A

Many methods exist to initialize the parameters. Here we used the standard values ​​of the RT2012, the bylaw of 9 November, 2006, on DPE calculation methods (Standard, 2006) and on-site observations.
Necessary information obtained by "on-site observation":
-
Year of construction or renovation
-
Type of use (offices, shops, etc.)
-
Heated surface (Sh)
-
Surface of vertical walls (Sm)
-
External exchange surface (Sext)
-
Internal exchange surface (Sint)
-
Indoor air volume (Vint)
-
Coefficients of internal convection (hint) and external (hext), supposed constant.
Information to look for in RT 2012:
-
Daily capacity (Cq in kJ / K.m2) according to the inertia class (Table A1 and Table A2).
-
The impact of the furniture on the air capacity (Mob = 20 kJ / K.m2 for non-empty buildings and zero otherwise).
Information to be found in the decree of 9 November, 2006, on DPE calculation methods:
-
Conductivity of the outer walls: "Uwall", "Uslab" and "Uroof", depending on the year of construction (Table A3).
Here are the formulas to initialize each parameter: (Table A3 and Table A4)
C i = ρ air   ×   C air   ×   V int + Mob   ×   S h ,   C f = C q   ×   S h ,
R i = 1 h int   ×   S int   ,   R e = 1 h ext   ×   S ext ,   R m = 1 U wall   ×   S m
Table A1. Inertia classes for building.
Table A1. Inertia classes for building.
Low FloorHigh Floor Vertical WallInertia Class
heavyheavyheavyvery heavy
-heavyheavyheavy
heavy-heavyheavy
heavyheavy-heavy
--heavyaverage
-heavy-average
Table A2. Daily capacity.
Table A2. Daily capacity.
Daily Inertia ClassDaily Capacity Cm (KJ/K)Exchange Surface Am(m2)
Very heavy80 × Abuild2.5 × Abuild
light110 × Abuild2.5 × Abuild
average165 × Abuild2.5 × Abuild
heavy260 × Abuild3 × Abuild
very light370 × Abuild 3 × Abuild
Table A3. Conductivity values.
Table A3. Conductivity values.
Construction DateH1H2H3
Joule EffectOtherJoule EffectOtherJoule EffectOther
From 1948 to 19742.52.52.5
From 1975 to 197711.051.11
From 1978 to 19820.810.841.050.891.11
From 1983 to 19880.70.80.740.840.780.89
From 1989 to 20000.450.50.470.530.50.56
From 2001 to 20050.40.40.47
From 20060.360.360.4
Table A4. Coefficient of internal and external convection.
Table A4. Coefficient of internal and external convection.
Wall PositionEmissivityhinthext
NormalShelteredSevere
Vertical0.98.1318.212.533.3
Vertical03.2914.99.133.3
External ceiling0.99.4322.214.350
External ceiling04.5918.911.150
External floor 0.96.67202020
External floor01.78202020
Internal horizontal 0.98---
Internal horizontal03---

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Figure 1. Resistor-Capacitor networks for the four models.
Figure 1. Resistor-Capacitor networks for the four models.
Buildings 09 00198 g001
Figure 2. Variation of indoor and outdoor temperature while heating: (a) 4 hours heating at 1500 W; (b) 4 hours heating at 900 W; (c) 2 hours heating at 1500 W.
Figure 2. Variation of indoor and outdoor temperature while heating: (a) 4 hours heating at 1500 W; (b) 4 hours heating at 900 W; (c) 2 hours heating at 1500 W.
Buildings 09 00198 g002aBuildings 09 00198 g002b
Figure 3. Results of sensibility analysis: (a)Test A; (b) Test B; (c) Test C.
Figure 3. Results of sensibility analysis: (a)Test A; (b) Test B; (c) Test C.
Buildings 09 00198 g003
Figure 4. Error distribution for experiment A-order 1: (a) 15 min prediction; (b) 30 min prediction (c) 60 min prediction.
Figure 4. Error distribution for experiment A-order 1: (a) 15 min prediction; (b) 30 min prediction (c) 60 min prediction.
Buildings 09 00198 g004
Figure 5. Error distribution for experiment B-order 3: (a) 15 min prediction; (b) 30 min prediction (c) 60 min prediction.
Figure 5. Error distribution for experiment B-order 3: (a) 15 min prediction; (b) 30 min prediction (c) 60 min prediction.
Buildings 09 00198 g005
Figure 6. Residual autocorrelation—Experiment B—order 3.
Figure 6. Residual autocorrelation—Experiment B—order 3.
Buildings 09 00198 g006
Figure 7. Error distribution for experiment C-order 2: (a) 15 min prediction; (b) 30 min prediction (c) 60 min prediction.
Figure 7. Error distribution for experiment C-order 2: (a) 15 min prediction; (b) 30 min prediction (c) 60 min prediction.
Buildings 09 00198 g007
Figure 8. Residual autocorrelation—Experiment C—order 2.
Figure 8. Residual autocorrelation—Experiment C—order 2.
Buildings 09 00198 g008
Table 1. Initial values for the estimated parameters.
Table 1. Initial values for the estimated parameters.
Estimated ParameterValue
Ci (J/K)1.47 × 105
Cfe (J/K)1.77 × 108
Cfi (J/K)9.36 × 106
Cm (J/K)4.54 × 106
Ri, Rm (K/W)1.82 × 10−2
Re (K/W)3 × 10−3
Rf (K/W)1.1 × 10−1
Table 2. Conducted experiments.
Table 2. Conducted experiments.
ExperimentIndoor Heating Power (W)
A0
B900
C1500
Table 3. Calculated total Sobol index.
Table 3. Calculated total Sobol index.
ResultFree-Floating (Test A)Heating - 900W
(Test B)
Heating - 1500W
(Test C)
ParameterCRCiCfeCfiRiReRfCiCfRiRe
STi0.980.990.070.090.240.600.120.180.620.850.720.59
Table 4. Fifteen-minute prediction results for expirment A.
Table 4. Fifteen-minute prediction results for expirment A.
Result1R1C2R2C3R3C4R4C
Fit percent95.1195.3595.1210.09
RMSE0.06560.06160.06481.2004
Table 5. Thirty-minute prediction results for experiment A.
Table 5. Thirty-minute prediction results for experiment A.
Result1R1C2R2C3R3C4R4C
Fit percent91.8692.9191.97-
RMSE0.10860.09490.1072-
Table 6. Sixty-minute prediction results for experiment A.
Table 6. Sixty-minute prediction results for experiment A.
Result1R1C2R2C3R3C4R4C
Fit percent87.8390.2488.05-
RMSE0.16250.13040.1594-
Table 7. Fifteen-minute prediction results for experiment B.
Table 7. Fifteen-minute prediction results for experiment B.
Result1R1C2R2C3R3C4R4C
Fit percent-93.9795.4344.15
RMSE-0.12040.09171.1170
Table 8. Thirty-minute prediction results for experiment B.
Table 8. Thirty-minute prediction results for experiment B.
Result1R1C2R2C3R3C4R4C
Fit percent-87.692.9836.52
RMSE-0.24800.14041.2697
Table 9. Sixty-minute prediction results for experiment B.
Table 9. Sixty-minute prediction results for experiment B.
Result1R1C2R2C3R3C4R4C
Fit percent-80.6590.7131.25
RMSE-0.38690.18571.3751
Table 10. Fifteen-minute prediction results for experiment C.
Table 10. Fifteen-minute prediction results for experiment C.
Result1R1C2R2C3R3C4R4C
Fit percent93.3697.295.796.18
RMSE0.23490.09900.15230.1353
Table 11. Thirty-minute prediction results for experiment C.
Table 11. Thirty-minute prediction results for experiment C.
Result1R1C2R2C3R3C4R4C
Fit percent83.3495.5690.792.17
RMSE0.58950.15720.32910.2769
Table 12. Sixty-minute prediction results for experiment C.
Table 12. Sixty-minute prediction results for experiment C.
Result1R1C2R2C3R3C4R4C
Fit percent71.4993.5484.7187.59
RMSE1.00900.22850.54100.4392

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Attoue, N.; Shahrour, I.; Mroueh, H.; Younes, R. Determination of the Optimal Order of Grey-Box Models for Short-Time Prediction of Buildings’ Thermal Behavior. Buildings 2019, 9, 198. https://doi.org/10.3390/buildings9090198

AMA Style

Attoue N, Shahrour I, Mroueh H, Younes R. Determination of the Optimal Order of Grey-Box Models for Short-Time Prediction of Buildings’ Thermal Behavior. Buildings. 2019; 9(9):198. https://doi.org/10.3390/buildings9090198

Chicago/Turabian Style

Attoue, Nivine, Isam Shahrour, Hussein Mroueh, and Rafic Younes. 2019. "Determination of the Optimal Order of Grey-Box Models for Short-Time Prediction of Buildings’ Thermal Behavior" Buildings 9, no. 9: 198. https://doi.org/10.3390/buildings9090198

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