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Article

Non-Intrusive Measurements to Incorporate the Air Renovations in Dynamic Models Assessing the In-Situ Thermal Performance of Buildings

by
María José Jiménez
1,*,
José Alberto Díaz
1,
Antonio Javier Alonso
2,
Sergio Castaño
1 and
Manuel Pérez
2
1
Energy Efficiency in Buildings R&D Unit, CIEMAT, 28040 Madrid, Spain
2
CIESOL Research Center on Solar Energy, Joint Center University of Almería-CIEMAT, 04120 Almería, Spain
*
Author to whom correspondence should be addressed.
Energies 2021, 14(1), 37; https://doi.org/10.3390/en14010037
Submission received: 13 November 2020 / Revised: 7 December 2020 / Accepted: 21 December 2020 / Published: 23 December 2020

Abstract

:
This paper reports the analysis of the feasibility to characterise the air leakage and the mechanical ventilation avoiding the intrusiveness of the traditional measurement techniques of the corresponding indicators in buildings. The viability of obtaining the air renovation rate itself from measurements of the concentration of the metabolic CO2, and the possibilities to express this rate as function of other climatic variables, are studied. N2O tracer gas measurements have been taken as reference. A Test Cell and two full size buildings, with and without mechanical ventilation and with different levels of air leakage, are considered as case studies. One-month test campaigns have been used for the reference N2O tracer gas experiments. Longer periods are available for the analysis based on CO2 concentration. When the mechanical ventilation is not active, the results indicate significant correlation between the air renovation rate and the wind speed. The agreement between the N2O reference values and the evolution of the metabolic CO2 is larger for larger initial values of the CO2 concentration. When the mechanical ventilation is active, relevant variations have been observed among the N2O reference values along the test campaigns, without evidencing any correlation with the considered boundary variables.

1. Introduction

Buildings use about 40% of the total energy produced globally and have a relevant potential in terms of energy savings and reducing the pollutant emissions to the atmosphere [1]. These issues are driving an increasing interest to foster the energy efficiency in buildings leading to the elaboration and incorporation of related regulations, stressing the demand to broaden the knowledge related to the energy performance of the buildings, and motivating many research initiatives in this area. Presently, the majority of the checks of compliance and energy performance labelling of buildings rely on design values and theoretical assessments or simulations. Nevertheless, many researches have demonstrated that the actual performance of a building can be very different from the one theoretically evaluated [2,3]. The readiness of reliable enough test procedures applicable to as built buildings for assessing their thermal performance, would contribute to eliminate the problems related to the performance gap. The need for tools identifying the sources of the performance gaps, and providing feedback to different stakeholders, is included among the research themes considered by the Energy in Buildings and Communities (EBC) Technology Collaboration Programme (TCP) of the International Energy Agency (IEA) [1]. One of the elements having a significant influence on the energy behaviour of the buildings is the building envelope. The identification of the intrinsic thermal properties characterising the as built building envelope from on board monitoring system is recently attracting the attention of many research groups in the context of international collaboration initiatives [4]. In this context, those monitoring systems with a limited set of non-intrusive measurement devices, embedded in the building, as those typically used for billing or for controlling the Heating, Ventilating and Air Conditioning (HVAC) systems are considered as on board monitoring systems. The energy performance assessment of the building envelope can be carried out through data analysis techniques that require the measurement (that can be direct or indirect) of all the effects that contribute to the energy balance in the space that is confined by the building envelope being characterised [5]. One of the contributions to this energy balance is the one from air renovations, either by mechanical or natural ventilation, or by infiltrations as consequence of cracks or material porosity [6].
There are several procedures for the experimental assessment of the air renovation rate in rooms. Some of these procedures are based on pressurisation and others are based on tracer gas techniques [7]. These traditionally applied methods that could give precise results are complex, expensive and highly intrusive for the building users and inhabitants. Additionally, these traditional techniques characterise the air renovations by a constant parameter. Some standardised procedures obtain this parameter under a pressure that is raised regarding the pressure of the building in use [8]. These constant values can introduce some degree of uncertainty on the data based dynamic modelling techniques that are applied for the thermal performance assessment of the building envelope from on-board monitoring systems [5,9,10]. Part of this uncertainty can be driven by the use of the air renovation rate as a constant parameter when actually it is a variable. A review paper that has been recently published identifies the dynamic behaviour of the air renovation rate as an issue contributing to the uncertainty in tracer gas-based methods [11]. Other authors have analysed the uncertainties due to wind in building pressurisation tests [12]. They identified errors in the rage 6–12% for wind speed in the range 6–10 ms−1 for test carried out under a standard pressure of 50 Pa, while the errors raised up to 35% and 60% for wind speeds of 6 ms−1 and 10 ms−1, respectively under a pressure of 10 Pa. When the air renovation rate is obtained according the standardised building pressurisation tests, the transformation of the pressurised value to the non-pressurised one, can introduce also certain degree of uncertainty in the dynamic models that are used for the energy performance assessment of in-use buildings. The presence of some uncertainty and variability in the air renovation rate due to infiltrations as well as mechanical ventilation, can contribute to understand and explain the behaviour of the Heat Loss Coefficient (HLC) experimentally assessed and its uncertainties [13,14].
The work reported in this paper is focused on the experimental assessment of the air renovation rate analysing the reliability of cheaper and more cost effective techniques regarding the traditional techniques based on tracer gas. The feasibility to characterise air leakage and mechanical ventilation avoiding the intrusiveness of the traditional measurement techniques is analysed. The viability to obtain the air renovation rate itself, as well as the possibilities to express it as function of other variables (such as wind speed, atmospheric pressure, etc.), are studied extending some preliminary studies [15]. Tracer gas measurements based on N2O have been used as reference. Experimental relations between the air renovations and the wind speed, the indoor-outdoor air temperature difference, and the atmospheric pressure have been analysed. The reliability of an alternative method based on the evolution of the metabolic CO2 using wall mounted sensors of CO2 concentration is evaluated. A PASLINK Test Cell [16,17] and two full size buildings are considered as case studies. First the Test Cell and a very simple single zone building, without mechanical ventilation, are considered. Afterwards, a room in an office building has been studied with and without mechanical ventilation. One-month test campaigns have been used for the reference study based on tracer gas measurements using N2O, in both buildings and the Test Cell. Longer periods are available for the analysis based on CO2 concentration.
The next sections are organised as follows: Section 2 presents the considered case studies, and briefly describes the experiment set up and the methodology applied for data analysis, Section 3 presents and discusses the results that have been obtained for the different case studies, and finally Section 4 summarises the conclusions regarding the behaviour of the air renovation rate, discusses the effect of this behaviour on the Heat Loss Coefficient (HLC) and suggest further research on this issue.

2. Materials and Methods

The next subsections included under this section describe the three considered case studies, the experiment set up, the tests carried out, and finally the methodology applied for data analysis.

2.1. Case Studies

A PASLINK Test Cell and two full size extensively monitored buildings are considered as case studies [16,17]. These buildings and the Test Cell, briefly described in Section 2.1.1, Section 2.1.2, Section 2.1.3 are at the CIEMAT’s Plataforma Solar de Almeria (PSA), in Tabernas (37.1° N, 2.4° W), Almería (Spain). They are in a rural area where the climate is semi-arid, with large day-night temperature variations.

2.1.1. PASLINK Test Cell

The PASLINK Test Cell consists in a test facility with a high-thermal-insulation test room and an auxiliary room (Figure 1a). The test room has a surface of 4.825 × 2.48 m2 and its high is 2.47 m. The Test Cell is placed in a large open area without any shading. It has an air conditioning system and measurement devices for testing full-scale building components. Its test room envelope is highly insulated by 40 cm of polystyrene and it is equipped with the Pseudo-Adiabatic Shell (PAS) Concept. This system is based on a thermopile that detects if there is heat flux through the envelope of the test room, and cancels it by means of a heating foil. The interior surface of the test room is finished with an aluminium sheet giving it thermal uniformity. The Test Cell is over a rotating device that enables it for testing in any orientation.
The south wall and the roof of the test chamber are interchangeable, which permits any vertical or horizontal building component to be installed for testing. The tests of air renovations considered in this work correspond to a reference experiment. In this case, the Test Cell incorporates a homogeneous and opaque wall in its replaceable façade.
This test was conducted in the framework of a series of tests that included several photovoltaic modules and electrocromic windows replacing a piece of the component taken as reference. The Heat Loss Coefficients of these components are obtained by subtracting the Heat Loss Coefficient obtained with the photovoltaic modules or the electrocromic windows, from the Heat Loss Coefficient obtained from the reference component. The Test Cell is designed to be very airtight. Typical air renovation rates during testing are between 0.02 and 0.05 renovations per hour [18]. The assessment of its air renovation rate is important in order to check the achieved level of air tightness and to assess the deviations from this level due to the climatic variables.

2.1.2. Single-Zone Building

This building is a small workshop with just one room, and its area is 31.83 m2 (Figure 1b) [17]. It can give experimental support to diverse research activities maintaining it empty or with low occupancy rates. It was built in 2002. It is near another twin building that is placed 2 m from its east wall. Both are built in an open area without any other obstacles around that could shade them.
This building was designed to reduce the energy demand incorporating the following passive strategies: South orientation, shading elements avoiding the solar gains in summer and maximising them in winter, the windows are double-glazed to reduce heat losses, and diagonally aligned (north-south) to facilitate the natural ventilation, thermal mass incorporated in the building envelope, external insulation and high ceilings.

2.1.3. Office Building Prototype

The so called C-DdI ARFRISOL at PSA is a one floor building with most of the regularly occupied offices facing south (Figure 1c). Its net floor area is 1007.40 m2. It was constructed in 2007 in the framework of the PSE-ARFRISOL project [19]. It is a prototype of a new plant, built on one floor longitudinal plan.
A double-wing structure, that is installed on the roof along the main axis of the building, protects it from the solar radiation. This structure integrates two different types of solar collectors. Uncovered collectors which are designed to operate as radiant coolers by night are over the wing facing north. Flat plate collectors that are designed to supply hot water for the heating, cooling and DHW systems are over the south facing wing. Small solar chimneys that provide night ventilation of the offices are constructed on the central part of this structure. The south windows are protected by an overhang that provides shade during the summertime and facilitates passive heating in winter.
This building is in use, but it must be taken into account that the experiments used for this work were carried out when the considered room was positively empty; at lunch time and also once the working day is finalised (identified every day as test 1, and test 2, respectively).

2.2. Experiment Set Up

A tracer gas device combined with a gas analyser have been used to carry out Decay experiments based on the evolution of N2O concentration in both buildings and the Test Cell.
The Test Cell and the two buildings are extensively monitored. The monitoring system records minutely read measurements of the following variables:
  • N2O concentration when the Decay experiments are being conducted.
  • Indoor and outdoor air temperatures, relative humidity, and concentration of CO2. Two sensors are installed to measure this variable. An accurate and expensive sensor used as reference, and a cheaper and less accurate sensor (Identified as CO2_ref and CO2 respectively in this document).
  • Temperature of walls, floor and glass surfaces.
  • Energy delivered by the heating system (radiant floor).
  • Electric consumption due to computers and lighting
  • Whether doors and windows are closed or “not closed”.
  • Ground temperature.
  • Beam, diffuse, global horizontal, global vertical south and global vertical north solar irradiance.
  • Longwave radiation.
One-month test campaigns for each building were considered for the analysis. These campaigns were conducted under different conditions: Dynamic heating sequence in the Test Cell maintaining a large indoor to outdoor air temperature difference, free running test in the single-zone building, and space heating maintaining the indoor air temperature in a comfort range in the office building.

2.3. Methodology

2.3.1. Analysis of the Relations between the Air Renovation Rate and Climate Variables

  • For both buildings and the Test Cell, for infiltrations and mechanical ventilation, tracer gas measurements based on N2O have been used as reference. The air renovation rate has been obtained using the Decay method [7]. Experimental relations between the air renovation rate and the following variables have been analysed.
  • The difference between the indoor and outdoor air temperatures (Ti − Te).
  • The wind speed (W).
  • The product of the wind speed and the difference between the indoor and outdoor air temperatures (W(Ti − Te)).
  • The product of the wind speed raised to two and the difference between the indoor and outdoor air temperatures (W2(Ti − Te)).
  • The atmospheric pressure (Patm).
  • The absolute value of the variation of wind speed per unit of time(|dW/dt|).

2.3.2. Analysis of Feasibility to Obtain Air Renovation Rate from Wall Mounted CO2 Sensors

Additionally, the reliability of an alternative method based on the evolution of the metabolic CO2 using wall mounted sensors of CO2 concentration is evaluated in a room of the office building. A reference value (CO2infinite) has been used, such that the variable used for the Decay method is the CO2-CO2infinite. This value was obtained as the average of the CO2 concentration in a period when the room is positively non-occupied (from 9 pm to 7 am), starting when the Decay curve has reached its asymptotic value. An error obtained as the percentage of deviation regarding the reference value (based on N2O), has been represented as function of the maximum value of the CO2 concentration at the beginning of the decay method curve.

3. Results and Discussion

A reference value has been obtained for each of the considered case studies. These reference values have been obtained using a N2O tracer gas applying the Decay method. The measurements carried out for the different case studies, presented in Figure 2, evidence that the air renovation rates are different for the different case studies.
The air renovation rates obtained from these tests are:
  • PASLINK Test Cell: 0.056 renovations/hour.
  • Single-zone building: 0.308 renovations/hour.
  • Office building without mechanical ventilation: 0.825 renovations/hour.
  • Office building with the mechanical ventilation active: 2.12 renovations/hour.
The dependence of these infiltration rates on the considered climate variables, and the feasibility to obtain them from the concentration of the metabolic CO2, is discussed in the next subsections.

3.1. PASLINK Test Cell. Infiltrations

As expected, very low infiltration rates have been obtained for all the tests carried out in the PASLINK Test Cell. These results are shown in Figure 3 and Table 1. In this case, the infiltration rate does not show any relevant correlation with the indoor to outdoor air temperature difference (Figure 3a). This correlation also is not relevant with the atmospheric pressure (Figure 3d). However, the air infiltration rate presents some correlation with other considered variables. It shows significant linear dependency on the wind speed (Figure 3e), and the dependency is remarkable on the absolute value of the variation of the wind speed per unit of time (Figure 3f).

3.2. Single-Zone Building. Infiltrations

The results obtained for the single zone building are summarised in Table 2. This table shows that the air renovation rate (n) presents a large variation in the range 0.16–0.97 renov/hour. Its average is 0.37 renov/hour, and its standard deviation is 0.26 renov/hour. Figure 4a,c,e,g,i) shows that the n value has evident correlation with all the considered boundary variables except the atmospheric pressure (Figure 4g). The most relevant correlation detected is regarding the wind speed (Figure 4c). The absolute value of the variation of the wind speed per unit of time is also relevant (Figure 4i).

3.3. Office Building Prototype

3.3.1. Infiltrations

The results obtained for the studied room are summarised in Figure 4b,d,f,h,j and Table 3. Considering the analysis based on N2O, the air renovation rate (n) presents some variation. However, the observed variation is not so large as in the single-zone building. The n value is between 0.61 and 0.75 renov/hour. Its average is 0.67 renov/hour, and it standard deviation is 0.05 renov/hour. Figure 4b,d,f,h,j shows that the n value has relevant correlation with all the considered boundary variables except the indoor to outdoor air temperature difference and the atmospheric pressure. The most relevant correlation detected is regarding the wind speed (Figure 4d).
It is noticeable the different behaviour observed for the dependence of the n value with the indoor-outdoor temperature difference in this heated room regarding the single zone free running building. The n value for the heated office does not show relevant dependence with this variable (Figure 4b). This behaviour is also observed in the Test Cell, also heated during the test campaign, that does not show relevant dependence with this variable (Figure 3a). However, a linear tendency is seen for the free running single-zone building (Figure 4a). This different behaviour could be explained by the different ranges of indoor-outdoor air temperature differences in the case studies (Figure 3a and Figure 4a,b).
Acceptable agreement is observed for the values obtained using the metabolic CO2 ref concentration, measured with the wall-mounted sensors, regarding the reference n values based on N2O (Table 3 and Figure 5a). The agreement is very poor when the less accurate CO2 sensor is used (Table 3 and Figure 5a). This behaviour is explained by taking into account that the office has just one user, and consequently, the level of CO2 concentration produced by the metabolic activity is very low, which is leading to relevant uncertainties in the estimations of the n values if the used sensor does not have enough resolution. These uncertainties show a decreasing tendency when the CO2 concentration increases (Figure 5b). Taking into account this behaviour a better performance of this sensor is foreseen for larger CO2 concentrations that would be present in rooms with more occupants. This issue will be further investigated.

3.3.2. Mechanical Ventilation

The results obtained for the studied room are summarised in Table 4 and Table 5. Considering the analysis based on N2O, the air renovation rate (n) presents a large variation. It is between 0.95 and 3.08 renov/hour. Its average is 1.98 renov/hour which is very close to the design value (2 renov/hour), and it standard deviation is 0.59 renov/hour. However, the n value does not show relevant correlation with any of the considered boundary variables. The observed large spread could be caused by the instability of the electricity that powers the mechanical ventilation system that transmits such instability to the ventilation rate. Other effects, such as hysteresis of the mechanical components of the ventilation system could contribute to produce the detected variations. The causes of the detected large spread will be further investigated in future research works.
Large uncertainties are observed for the values obtained using the metabolic CO2 concentration measured with the wall-mounted sensors (Table 4 and Table 5 and Figure 6). These uncertainties are remarkably larger than those observed for the same room without mechanical ventilation (Figure 5). This high uncertainty is attributed the low level of metabolic CO2 concentration produced by just one user. This issue also leads to large uncertainties in the air renovation rate obtained for the same room without mechanical ventilation using the less accurate sensor (Figure 5b). However, such uncertainty is worsened in the case of mechanical ventilation taking into account that the time interval available for each calculation of the n value is shortened regarding the case of not using mechanical ventilation.

4. Conclusions

This section summarises the conclusions regarding the behaviour of the air renovation rate and discusses the effect of this behaviour on the experimental assessment of the Heat Transfer Coefficient (HLC).
The following conclusions are extracted regarding the air renovation rate from the different tests carried out:
  • When the mechanical ventilation is not active: Significant correlation between air renovation rate and the wind speed has been observed in both buildings and the Test Cell. The agreement between the values obtained using N2O and the evolution of metabolic CO2 increases when the starting value of CO2 concentration increases.
  • When the mechanical ventilation is active: Large variations have been observed among the different values obtained along the test campaign using N2O tracer gas. However, these values do not show any correlation with any of the considered climate variables. Consequently, the observed spread has been used to estimate an uncertainty of the air renovations rate. The measurements based on CO2 concentrations do not show good agreement to the values obtained using N2O tracer gas. This issue will be further investigated, but in principle it is attributed to the low level of CO2 measured along the analysed test campaign when the mechanical ventilation is active. This explanation is in agreement with previous works carried out regarding the air renovation in the same building [15].
The behaviour observed in the air renovation rate, showing large variability considering infiltrations and also considering mechanical ventilation, contributes to understand the behaviour of the HLC experimentally assessed and its uncertainties. The following text summarises the conclusions extracted from this work and some ideas for further research, regarding the influence of the air renovation rate on the behaviour of the Heat Loss Coefficient (HLC):
  • Regarding infiltrations, the dependencies of the n value with the wind speed and its variation per unit of time in absolute value, can explain some variability of the HLC and some uncertainty when it is assumed as a constant value. Further analysis of this wind dependence is an interesting issue regarding future research works that could lead to a wind dependent HTC reducing the uncertainties of this coefficient in experimental assessments.
  • The behaviour observed in the n value for the case of mechanical ventilation leads to conclude that the experimental assessment of an HLC assuming n as constant could lead to some degree of uncertainty. The work presented in this paper has not identified any variable that could contribute to model such variability reducing the associated uncertainty. This issue is identified as a relevant topic regarding future research.

Author Contributions

Measurements, S.C.; Data curation, A.J.A. and J.A.D.; Data analysis, elaboration of graphs and synthesis of results, A.J.A., J.A.D. and M.P.; writing—review and editing M.J.J. and M.P., Methodology and writing—original draft preparation, M.J.J. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the Spanish National Research Agency (Agencia Estatal de Investigación) through the In-Situ-BEPAMAS project, reference PID2019-105046RB-I00. Additionally, the operation of the test facilities that supported this study was partially funded by the Spanish Ministry of Economy, Industry and Competitiveness through ERDF funds (SolarNOVA-II project Ref. ICTS-2017-03-CIEMAT-04).

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. EBC Executive Committtee. Strategic Plan 2019–2024. Energy in Buildings and Communities Technology Collaboration Programm; International Energy Agency: Paris, France, 2019. [Google Scholar]
  2. Tian, W.; Heo, Y.; de Wilde, P.; Li, Z.; Yan, D.; Park, C.S.; Feng, X.; Augenbroe, G. A review of uncertainty analysis in building energy assessment. Renew. Sustain. Energy Rev. 2018, 93, 285–301. [Google Scholar] [CrossRef] [Green Version]
  3. Kampelis, N.; Gobakis, K.; Vagias, V.; Kolokotsa, D.; Standardi, L.; Isidori, D.; Cristalli, C.; Montagnino, F.M.; Paredes, F.; Muratore, P.; et al. Evaluation of the performance gap in industrial, residential & tertiary near-Zero energy buildings. Energy Build. 2017, 148, 58–73. [Google Scholar] [CrossRef] [Green Version]
  4. Annex 71 of the Programme “(EBC)” of the IEA on EBC Annex 71. Building Energy Performance Assessment Based on In-Situ Measurements. 2016–2021. Available online: http://www.iea-ebc.org/projects/project?AnnexID=71 (accessed on 4 December 2020).
  5. Jiménez, M.J. IEA, EBC annex 58, report of subtask 3, part 1. In Thermal Performance Characterization Based on Full Scale Testing–Description of the Common Exercises and Physical Guidelines; Jiménez, M.J., Ed.; KU Leuven: Leuven, Belgium, 2016; ISBN 9789460189876. Available online: http://www.iea-ebc.org/Data/publications/EBC_Annex_58_Final_Report_ST3a.pdf (accessed on 3 November 2020).
  6. Marin, M.; Vlase, S.; Paun, M. Considerations on double porosity structure for micropolar bodies. AIP Adv. 2015, 5, 037113. [Google Scholar] [CrossRef] [Green Version]
  7. Sherman, M.H. On the estimation of multizone ventilation rates from tracer gas measurements. Build. Environ. 1989, 24, 355–362. [Google Scholar] [CrossRef] [Green Version]
  8. ISO 9972:2015. Thermal Performance of Buildings–Determination of Air Permeability of Buildings–Fan Pressurization Method; ISO: Geneva, Switzerland, 2015. [Google Scholar]
  9. Olazo-Gómez, Y.; Herrada, H.; Castaño, S.; Arce, J.; Xamán, J.P.; Jiménez, M.J. Data-based RC dynamic modelling to assessing the in-situ thermal performance of buildings. Analysis of several key aspects in a simplified reference case toward the application at on-board monitoring level. Energies 2020, 13, 4800. [Google Scholar] [CrossRef]
  10. Díaz-Hernández, H.P.; Torres-Hernández, P.R.; Aguilar-Castro, K.M.; Macias-Melo, E.V.; Jiménez, M.J. Data-based RC dynamic modelling incorporating physical criteria to obtain the HLC of in-use buildings: Application to a case study. Energies 2020, 13, 313. [Google Scholar] [CrossRef] [Green Version]
  11. Remion, G.; Moujalled, B.; El Mankibi, M. Review of tracer gas-based methods for the characterization of natural ventilation performance: Comparative analysis of their accuracy. Build. Environ. 2019, 160, 106180. [Google Scholar] [CrossRef]
  12. Carrié, F.R.; Leprince, V. Uncertainties in building pressurisation tests due to steady wind. Energy Build. 2016, 116, 656–665. [Google Scholar] [CrossRef]
  13. Farmer, D.; Johnston, D.; Miles-Shenton, D. Obtaining the heat loss coefficient of a dwelling using its heating system (integrated coheating). Energy Build. 2016, 117, 1–10. [Google Scholar] [CrossRef]
  14. Marshall, A.; Fitton, R.; Swan, W.; Farmer, D.; Johnston, D.; Benjaber, M.; Ji, Y. Domestic building fabric performance: Closing the gap between the in situ measured and modelled performance. Energy Build. 2017, 150, 307–317. [Google Scholar] [CrossRef]
  15. Enríquez, R.; Bravo, D.; Díaz, J.A.; Jiménez, M.J. Mechanical ventilation performance assessment in several office buildings by means of Big Data techniques. In Proceedings of the 36th AIVC Conference “Effective Ventilation in High Performance Buildings”, Madrid, Spain, 23–24 September 2015; ISBN 2-930471-45-X. [Google Scholar]
  16. Baker, P.H.; van Dijk, H.A.L. PASLINK and dynamic outdoor testing of building components. Build. Environ. 2008, 43, 127–128. [Google Scholar] [CrossRef]
  17. Castaño, S.; Guzmán, J.D.; Jiménez, M.J.; Heras, M.R. LECE-UiE3-CIEMAT. In Report of Subtask 1a: Inventory of Full Scale Test Facilities for Evaluation of Building Energy Performances. IEA EBC Annex 58; Janssens, A., Ed.; KU Leuven: Leuven, Belgium, 2016; ISBN 9789460189906. [Google Scholar]
  18. Jiménez, M.J.; Porcar, B.; Heras, M.R. Estimation of UA and gA values of building components from outdoor tests in warm and moderate weather conditions. Solar Energy 2008, 82, 573–587. [Google Scholar] [CrossRef]
  19. Olmedo, R.; Sánchez, M.N.; Enríquez, R.; Jiménez, M.J.; Heras, M.R. ARFRISOL Buildings-UIE3-CIEMAT. In Report of Subtask 1a: Inventory of Full Scale Test Facilities for Evaluation of Building Energy Performances. IEA EBC Annex 58; Janssens, A., Ed.; KU Leuven: Leuven, Belgium, 2016; ISBN 9789460189906. [Google Scholar]
Figure 1. Buildings considered as case studies: (a) PASLINK Test Cell; (b) Single-zone building; (c) Office building.
Figure 1. Buildings considered as case studies: (a) PASLINK Test Cell; (b) Single-zone building; (c) Office building.
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Figure 2. Decay method based on N2O as tracer gas, applied to the three case studies: (a) PASLINK Test Cell (08/10/2018–11/10/2018); (b) Single-zone building 24/02/2016; (c) Office building without mechanical ventilation (10/02/2017); (d) Office building with mechanical ventilation (02/02/2017).
Figure 2. Decay method based on N2O as tracer gas, applied to the three case studies: (a) PASLINK Test Cell (08/10/2018–11/10/2018); (b) Single-zone building 24/02/2016; (c) Office building without mechanical ventilation (10/02/2017); (d) Office building with mechanical ventilation (02/02/2017).
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Figure 3. PASLINK Test Cell. Relations between the air renovation rate and the climatic variables. N2O tracer gas measurement taken as reference. (a) Indoor to outdoor air temperature difference; (b) product of the indoor to outdoor air temperature difference and the wind speed; (c) product of the indoor to outdoor air temperature difference and the wind speed raised to two; (d) atmospheric pressure; (e) wind speed; (f) absolute value of the variation of wind sped per unit of time.
Figure 3. PASLINK Test Cell. Relations between the air renovation rate and the climatic variables. N2O tracer gas measurement taken as reference. (a) Indoor to outdoor air temperature difference; (b) product of the indoor to outdoor air temperature difference and the wind speed; (c) product of the indoor to outdoor air temperature difference and the wind speed raised to two; (d) atmospheric pressure; (e) wind speed; (f) absolute value of the variation of wind sped per unit of time.
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Figure 4. Relations between the air renovations and the climatic variables. Left: single-zone building. Right: Room of the office building. (a,b) Indoor to outdoor air temperature difference; (c,d) wind speed; (e,f) product of the indoor to outdoor air temperature difference and the wind speed; (g,h) product of the indoor to outdoor air temperature difference and the wind speed raised to two; (i,j) absolute value of the variation of the wind sped per unit of time.
Figure 4. Relations between the air renovations and the climatic variables. Left: single-zone building. Right: Room of the office building. (a,b) Indoor to outdoor air temperature difference; (c,d) wind speed; (e,f) product of the indoor to outdoor air temperature difference and the wind speed; (g,h) product of the indoor to outdoor air temperature difference and the wind speed raised to two; (i,j) absolute value of the variation of the wind sped per unit of time.
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Figure 5. Office number 1, analysis of infiltrations. Percentage of error of the results obtained from the Decay method using the metabolic CO2 concentration and considering as reference the value obtained from the N2O tracer gas. (a) Using the CO2 reference sensor; (b) using the cheaper CO2 sensor.
Figure 5. Office number 1, analysis of infiltrations. Percentage of error of the results obtained from the Decay method using the metabolic CO2 concentration and considering as reference the value obtained from the N2O tracer gas. (a) Using the CO2 reference sensor; (b) using the cheaper CO2 sensor.
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Figure 6. Office number 1, tests with mechanical ventilation active. Percentage of error of the results obtained from the Decay method using the metabolic CO2 concentration and considering as reference the value obtained from the N2O tracer gas. (a) Using the CO2 reference sensor; (b) using the cheaper CO2 sensor.
Figure 6. Office number 1, tests with mechanical ventilation active. Percentage of error of the results obtained from the Decay method using the metabolic CO2 concentration and considering as reference the value obtained from the N2O tracer gas. (a) Using the CO2 reference sensor; (b) using the cheaper CO2 sensor.
Energies 14 00037 g006
Table 1. PASLINK Test Cell. Experimentally determined air infiltration rates and climate variables.
Table 1. PASLINK Test Cell. Experimentally determined air infiltration rates and climate variables.
Daysnr2Ti − TeWW(Ti − Te)W2(Ti − Te)Patm
(N2O) 1(N2O) 1
In 2018(ren/h)(·)(°C)(m/s)[m/s] [°C][(m/s)2] [°C](mbar)
24/09–26/090.10220.983412.23.0736.39145.7960
27/09–29/090.05430.977816.71.4822.4683.9957
02/10–04/100.05360.991719.41.0518.2045.9900
05/10–07/100.05030.998316.80.9113.4528.3954
08/10–11/100.05600.993619.51.4828.3590.3949
12/10–14/100.05430.982912.71.3815.9442.4954
23/10–25/100.04580.936710.41.179.5227.8960
26/10–29/100.05740.988216.91.3323.4572.9941
29/10–01/110.05200.997918.80.9818.1138.6944
1 The (N2O) indicates that the values included in the column were obtained using the N2O tracer gas.
Table 2. Single-zone building. Experimentally determined air infiltration rates and climate variables.
Table 2. Single-zone building. Experimentally determined air infiltration rates and climate variables.
nr2Ti − TeWW(Ti − Te)W2(Ti − Te)Patm
Day(N2O) 1(N2O) 1
(ren/h)(·)(°C)(m/s)[m/s] [°C][(m/s)2] [°C](mbar)
09/02/20160.740.9756−2.499.20−21.88−214.9956
10/02/20160.600.9125−0.7910.27−9.58−121.6954
11/02/20160.500.97080.289.272.6625.8951
12/02/20160.970.9942−0.6111.55−7.07−87.0951
15/02/20160.220.97769.443.7532.07157.8952
16/02/20160.190.987412.072.4525.3978.9960
17/02/20160.310.95509.544.4839.96201.3955
18/02/20160.160.99659.573.0429.71107.1955
19/02/20160.220.99369.684.4442.93213.0958
22/02/20160.160.96666.582.8418.4078.8958
23/02/20160.170.997610.422.2118.2646.1959
24/02/20160.310.99356.304.7326.75131.4952
25/02/20160.220.960810.123.8229.83141.6952
1 The (N2O) indicates that the values included in the column were obtained using the N2O tracer gas.
Table 3. Office number 1. Experimentally determined air infiltration rates, climate variables and deviations between the results obtained using the metabolic CO2 concentration and the N2O tracer gas.
Table 3. Office number 1. Experimentally determined air infiltration rates, climate variables and deviations between the results obtained using the metabolic CO2 concentration and the N2O tracer gas.
nnnr2r2r2Ti − TeWW(Ti − Te)W2(Ti − Te)PatmCO2ref.maxErrorCO2maxError
Day(N2O) 1(CO2) 1(CO2_ref) 1(N2O) 1(CO2) 1(CO2_ref) 1 (CO2_ref) 1 (CO2) 1
(ren/h)(ren/h)(ren/h)(·)(·)(·)(°C)(m/s)[m/s] [°C][(m/s)2] [°C](mbar)(ppm)(%)(ppm)(%)
09/02/20170.720.070.720.99940.03340.963913.030.8510.513.58005060.242691.0
10/02/20170.830.570.780.99940.75640.986413.833.1843.5161.59495175.143631.4
14/02/20170.880.640.820.99970.75200.992312.473.4642.6161.79616296.947027.3
15/02/20170.770.380.780.99910.79000.990912.963.3743.0156.59666452.245850.1
16/02/20170.840.380.740.99960.80520.991312.913.2240.9149.396553811.345454.3
21/02/20170.860.480.780.99900.61570.98889.774.1040.0178.09566159.543044.8
01/03/20170.690.050.590.99410.04460.96779.671.2610.919.895757014.742793.3
1 The (N2O), (CO2) and (CO2_ref) indicate that the values included in the column refer to the measurements using the N2O tracer gas, the CO2 or the CO2_ref devices respectively.
Table 4. Office number 1, test 1 for each day. Experimentally determined air infiltration rates when the mechanical ventilation is active, climate variables and deviations between the results obtained using the metabolic CO2 concentration and the N2O tracer gas.
Table 4. Office number 1, test 1 for each day. Experimentally determined air infiltration rates when the mechanical ventilation is active, climate variables and deviations between the results obtained using the metabolic CO2 concentration and the N2O tracer gas.
nnnr2r2r2Ti − TeWW(Ti − Te)W2(Ti − Te)PatmCO2ref.maxErrorCO2maxError
Day(N2O) 1(CO2) 1(CO2_ref) 1(N2O) 1(CO2) 1(CO2_ref) 1 (CO2_ref) 1 (CO2) 1
(ren/h)(ren/h)(ren/h)(·)(·)(·)(°C)(m/s)[m/s] [°C][(m/s)2] [°C](mbar)(ppm)(%)(ppm)(%)
31/01/20172.410.410.650.99830.70640.98192.121.062.33.29535377348983
01/02/20172.411.100.760.99820.80000.98722.082.194.511.69555646846354
02/02/20172.120.260.730.99630.58890.98526.211.6410.118.69536466551688
03/02/20172.70−0.980.970.99840.25340.94051.975.049.954.595654364433136
07/02/20172.610.631.050.99710.82460.99410.304.610.83.79587166052076
08/02/20172.450.070.500.99590.04270.96945.743.9122.398.98006128048697
09/02/20172.500.610.810.99730.76530.97957.633.8929.7128.68006156845476
10/02/20172.310.300.910.99540.63790.97899.501.7616.944.59496116148887
13/02/20173.08−0.111.230.99930.00150.98236.443.8124.5111.894755860436104
14/02/20172.610.140.680.99660.27000.94877.322.9221.471.99596137447095
15/02/20172.410.140.690.99730.20150.98947.774.3233.6159.19646637152594
16/02/20172.39−0.040.610.99590.01330.96829.065.7452.0323.796561974446102
17/02/20171.510.330.710.99650.71700.98899.602.0719.950.89626405349878
21/02/20172.411.340.600.99350.61930.96128.138.4868.9605.39576067546144
22/02/20172.260.540.580.99550.75010.97385.635.9433.4207.49546977447376
23/02/20171.57−0.650.770.99840.05420.97516.174.8729.9166.594865451433142
24/02/20171.540.090.520.99950.05880.97766.921.399.518.89506846660394
02/03/20172.640.020.470.99800.00140.97941.471.572.34.49555878246199
1 The (N2O), (CO2) and (CO2_ref) indicate that the values included in the column refer to the measurements using the N2O tracer gas, the CO2 or the CO2_ref devices respectively.
Table 5. Office number 1, test 2 for each day. Experimentally determined air infiltration rates when the mechanical ventilation is active, climate variables and deviations between the results obtained the using the metabolic CO2 concentration and the N2O tracer gas.
Table 5. Office number 1, test 2 for each day. Experimentally determined air infiltration rates when the mechanical ventilation is active, climate variables and deviations between the results obtained the using the metabolic CO2 concentration and the N2O tracer gas.
nnnr2r2r2Ti − TeWW(Ti − Te)W2(Ti − Te)PatmCO2ref.maxErrorCO2maxError
Day(N2O) 1(CO2) 1(CO2_ref) 1(N2O) 1(CO2) 1(CO2_ref) 1 (CO2_ref) 1 (CO2) 1
(ren/h)(ren/h)(ren/h)(·)(·)(·)(°C)(m/s)[m/s] [°C][(m/s)2] [°C](mbar)(ppm)(%)(ppm)(%)
31/01/20172.110.291.420.99790.76980.99116.752.1214.132.69545443348986
01/02/20171.96−0.291.210.99490.35620.98235.471.115.58.095552938443115
02/02/20172.000.121.100.99600.53960.98946.081.036.27.89545354547094
06/02/20172.250.560.980.99490.71540.98352.363.376.424.79604905647075
07/02/20171.34−0.170.860.99880.18740.99014.103.3013.753.295751936461113
08/02/20171.330.431.040.99970.68810.99168.911.6514.030.08005152245868
13/02/20170.950.040.760.98260.09700.91288.902.5522.469.29515772040996
17/02/20171.220.711.070.97670.84580.920811.912.6531.294.49615451249542
20/02/20170.950.511.380.99920.77410.910411.297.2281.3618.89585314440947
22/02/20171.120.390.990.98440.79940.99588.213.5429.0121.89525631147365
23/02/20171.420.411.070.99830.76820.99519.871.7416.934.19485592548671
24/02/20171.360.301.330.98000.18490.99359.481.029.312.4951565244078
02/03/20171.460.831.600.99650.30750.98936.541.337.913.2954547943943
1 The (N2O), (CO2) and (CO2_ref) indicate that the values included in the column refer to the measurements using the N2O tracer gas, the CO2 or the CO2_ref devices respectively.
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Jiménez, M.J.; Díaz, J.A.; Alonso, A.J.; Castaño, S.; Pérez, M. Non-Intrusive Measurements to Incorporate the Air Renovations in Dynamic Models Assessing the In-Situ Thermal Performance of Buildings. Energies 2021, 14, 37. https://doi.org/10.3390/en14010037

AMA Style

Jiménez MJ, Díaz JA, Alonso AJ, Castaño S, Pérez M. Non-Intrusive Measurements to Incorporate the Air Renovations in Dynamic Models Assessing the In-Situ Thermal Performance of Buildings. Energies. 2021; 14(1):37. https://doi.org/10.3390/en14010037

Chicago/Turabian Style

Jiménez, María José, José Alberto Díaz, Antonio Javier Alonso, Sergio Castaño, and Manuel Pérez. 2021. "Non-Intrusive Measurements to Incorporate the Air Renovations in Dynamic Models Assessing the In-Situ Thermal Performance of Buildings" Energies 14, no. 1: 37. https://doi.org/10.3390/en14010037

APA Style

Jiménez, M. J., Díaz, J. A., Alonso, A. J., Castaño, S., & Pérez, M. (2021). Non-Intrusive Measurements to Incorporate the Air Renovations in Dynamic Models Assessing the In-Situ Thermal Performance of Buildings. Energies, 14(1), 37. https://doi.org/10.3390/en14010037

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