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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta>
      <issn pub-type="ppub">1613-0073</issn>
    </journal-meta>
    <article-meta>
      <title-group>
        <article-title>Model of the Building Envelope the Thermophysical Characteristics Determining Process</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Vitalii Babak</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Oleg Dekusha</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Svitlana Kovtun</string-name>
          <email>sveta_kovtun@ukr.net</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Leonid Shcherbak</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Sergiy Kobzar</string-name>
          <email>SKobzar@nas.gov.ua</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Workshop</string-name>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>General Energy Institute of National Academy of Sciences of Ukraine</institution>
          ,
          <addr-line>172, Antonovich str, Kyiv, 03150</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Institute of Engineering Thermophysics of NAS of Ukraine</institution>
          ,
          <addr-line>2a, Marii Kapnist str., Kyiv, 03057</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>Thermophysical properties are a key factor in controlling heat losses and as a result in assessing the building's energy efficiency. For control heat losses one of the main thermophysical characteristics is the specific thermal resistance of the building envelope, which is defined as the resistance of individual characteristic zones of the envelope taking into account their area. Various calculation methods, physical and dynamics (CFD) modeling and experimental studies are used to determine thermal resistance. This work combines all the above-mentioned approaches to control the thermophysical characteristics of the building. In the work, a computer simulation of the process of complex radiative and convective-conductive heat exchange during the control of the thermophysical characteristics of the building envelope was carried out, taking into account the locations of the sensors and the influence of their parameters on the control result. Validation of the CFD model was performed using experimental data and shown good convergence of the obtained results. In work also shown practical application of the CFD model for the analysis of the sensor's parameters influence on the thermophysical characteristics control of the building envelope. Computer model, CFD model, thermophysical characteristics, heat flux, control of the thermal Proceedings ITTAP'2023: 3rd International Workshop on Information Technologies: Theoretical and Applied Problems, November 22-24, Proceedings</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>resistance, heat flux sensors</p>
    </sec>
    <sec id="sec-2">
      <title>1. Introduction</title>
      <p>
        Thermophysical properties are a key factor in controlling heat losses and as a result in assessing the
building's energy efficiency [
        <xref ref-type="bibr" rid="ref1 ref2">1,2</xref>
        ]. For control heat losses one of the main thermophysical characteristics
is the specific thermal resistance of the building envelope, which is defined as the resistance of
individual characteristic zones of the envelope taking into account their area [
        <xref ref-type="bibr" rid="ref3 ref4">3,4</xref>
        ]. Various calculation
methods [
        <xref ref-type="bibr" rid="ref3 ref4">3,4</xref>
        ], physical and mathematical models [
        <xref ref-type="bibr" rid="ref5 ref6">5,6</xref>
        ], computational fluid dynamics (CFD) modeling
[
        <xref ref-type="bibr" rid="ref7 ref8">7,8</xref>
        ] and experimental studies [
        <xref ref-type="bibr" rid="ref10 ref11 ref9">9,10,11</xref>
        ] are used to determine thermal resistance. Experimental studies
of thermophysical characteristics of the building envelope defined by the ISO 9869 standard [
        <xref ref-type="bibr" rid="ref9">9</xref>
        ] have a
number of significant drawbacks, among which the following should be highlighted: long duration of
measurements (at least 72 hours) [
        <xref ref-type="bibr" rid="ref12">12</xref>
        ] if necessary, the experiment can be extended; the need to use a
large number of sensors to obtain a representative result [
        <xref ref-type="bibr" rid="ref13 ref14">13,14</xref>
        ]; limitation of climate parameters for
measurements [
        <xref ref-type="bibr" rid="ref11 ref15">11, 15</xref>
        ]. Significant uncertainties of the measurement results can be caused by large
number of influencing factors such as geometric dimensions and orientation of the building [
        <xref ref-type="bibr" rid="ref16">16</xref>
        ],
location of sensors [
        <xref ref-type="bibr" rid="ref11 ref9">9,11</xref>
        ], external climatic conditions [
        <xref ref-type="bibr" rid="ref11 ref15 ref16">11,15, 16</xref>
        ]. CFD modeling expands the range
of solvable tasks, which are the basis for improving building envelope designs and developing optimal
      </p>
      <p>2020 Copyright for this paper by its authors.
CEUR</p>
      <p>
        ceur-ws.org
operation modes of the ventilation and heating system [
        <xref ref-type="bibr" rid="ref14 ref8">8,14</xref>
        ]. For variation of ventilation systems
operating modes CFD-models have become one of the main tools [
        <xref ref-type="bibr" rid="ref17 ref18">17, 18</xref>
        ]. But the created CFD models
necessarily require validation according to experimental data [
        <xref ref-type="bibr" rid="ref18">18</xref>
        ].
      </p>
      <p>This work combines all the above-mentioned approaches to control the thermophysical
characteristics of the building envelope taking into account the locations of the sensors and the influence
of their parameters on the control result.</p>
    </sec>
    <sec id="sec-3">
      <title>2. Analysis of the object and the research problem</title>
      <p>The aim of the research is to determine the distribution of the internal thermal field during the control
of the thermophysical characteristics of the building envelope in typical structures by using the
computer modeling results under the influence of external factors taking into account the locations and
the influence of the sensors parameters.</p>
      <p>Figure 1 shows a schematic illustration of the object under study, in particular the section of the
building envelope, on which influence the external and internal fields, and also the heat flux sensor.
The thermophysical properties of the building envelope are related to the external climatic and internal
thermal fields, the heat transfer process.</p>
      <p>The stochastic part of the climatic component   ( ,  ,  ) of the atmospheric meteorological field
characterizes its corresponding fluctuations.</p>
      <p>The thermophysical characteristics and properties of the building envelope are generally described
by the appropriate transformation operator Υ under the action of an external field. Thus, in general,
the internal (in the middle of the building envelope) random field is described by the following
expression:
{  ( ;  1;  ) = Υ[  ( ;  ;  )],  ∈  ,  1 = ( 1,  1,  1) ∈  1 ⊂  ,  ∈  } (3)
The tuple of control parameters  = ( ;  ;  ) includes the coefficient of thermal conductivity
(thermal resistance), relative humidity, emission coefficient, which in general are functions of the above
parameters of the fields.</p>
      <p>The following assumptions were used to obtain the results of a computer experiment with the aim
of verifying the mathematical model of the internal thermal field based on the measurement data.</p>
      <p>Using the hypothesis of a fixed state of the atmosphere during the computer experiment, the
specified parameters of the climatic component were considered numerical values. For more detailed
analysis, the building envelope is divided into characteristic measurement zones for analysis using
computer models. One of such characteristic zones is the insulated section of the wall facade without
the presence of heating devices.</p>
    </sec>
    <sec id="sec-4">
      <title>3. CFD model of heat exchange in the characteristic zone of the building</title>
      <p>envelope</p>
    </sec>
    <sec id="sec-5">
      <title>3.1. Description of the model</title>
      <p>The simulation was carried out using the ANSYS CFX software. The model includes fluid and solid
computational domains. The liquid domain is a layer of air. The geometry of the studied object was
constructed using the ANSYS Design Manager. Since one of the modeling tasks is to assess the effect
of sensors on the distribution of the thermal field on the surface of the building envelope structure
during tests, heat flux sensors were introduced into the model as separate elements installed on the wall.
Also, to match the calculation grid, separate zones were formed in the solid area, which coincide in size
with the heat flux sensors. The general appearance of the 3D model is shown in Fig. 2.</p>
      <p>For perform CFD modeling, an unstructured combined calculation grid was used, built using the
ANSYS CFX Mesh generator (Fig. 3). The calculated grid consisted of 2053866 elements and 1446712
nodes. It should be noted that each heat flux sensor consisted of 43200 elements and 51667 nodes.</p>
      <p>Material Thickness, m Thermal conductivity, W/(m·K)</p>
      <p>PUF 0.03 0.0346</p>
      <sec id="sec-5-1">
        <title>Concrete blocks 0.40 0.5200</title>
        <p>The characteristics of heat flux sensors are defined in the publication [23]</p>
        <p>Complex conductive, convective and radiative heat exchange is considered in the model, which
makes it possible to analyze in detail the factors influencing the results of control the thermophysical
characteristics of the building envelope (Fig. 4).</p>
        <p>
          As can be seen from the figures, there is an increase in speed in the upper and middle sensor zones
in the wall layer, but the air speed does not exceed 0.2 m/s, which does not have a significant impact
on the measurement results [
          <xref ref-type="bibr" rid="ref7 ref8">7,8,25</xref>
          ]. It should be noted that the air properties include a radiation
absorption coefficient equal to 0.01.
        </p>
        <p>The temperature distribution in the "XZ" plane is shown in Fig. 7.</p>
        <p>Figure 7 The temperature field in the "XZ" plane that passes through the heat flux sensors.</p>
        <p>As noted earlier, important in the analysis is the influence of the presence of sensors on the heat flux
measurement results. For this, cross-sections on the area "ZX" and "XY" were constructed, which pass
through the center of the q9 sensor. The change in the temperature field of the wall surface due to the
installation of the q9 sensor is shown in Fig. 8.</p>
        <p>The temperature distributions on the axes of the heat flux sensor q9 and near it are shown in Fig. 9.</p>
        <p>For the CFD model validation an experiment conducted on a characteristic zone of the wall section
(Fig. 10). Heat flux was measured by bimetallic heat flux sensors (Ni-Const). Type L thermocouples
were used to measure temperature. Calibration of heat flux sensors was carried out by the radiation
method [23]. L-type thermocouples with individual calibration were used as sensors for measuring the
external temperature [26].</p>
        <p>An information and measurement system with the following characteristics was used to register the
signals of temperature and heat flux sensors [26]:
• 8-channel ADC with 16-bit bit rate and 10 Hz conversion frequency;
• adjustment and calibration of the dynamic range;
• support for the RS-485 industrial interface and addressing, which makes it possible to create a
measuring network.</p>
        <p>The time of one measurement cycle was set to 30 s.</p>
        <p>From the analysis of the Table 2 it was found that the deviation between the results of CFD modeling
and experimental data did not exceed 0.3 K for the temperature and 0.3 W/m² for the heat flux, which
indicates a good convergence of the obtained results and the adequacy of the created CFD model.</p>
      </sec>
    </sec>
    <sec id="sec-6">
      <title>4. CFD model practical application</title>
      <p>One of the advantages of proposed CFD model lays in the inclusion of the heat flux sensors with
corresponding physical parameters. Which gives possibility for the analysis of the sensor’s parameters
influence on the thermophysical characteristics control of the building envelope.</p>
      <p>For this task, the emission coefficient of the q9 sensor was changed to 0.71, which corresponds to
the value of the TES1-12703 sensor described in the article [24], while all other parameters of the model
remain unchanged.</p>
      <p>Figure 11 shows the temperature distribution on the axes of the heat flux sensor and along it.</p>
      <p>From the data presented in Table 3, it follows that the change in the emission factor led to a
difference in the results of simulation and experiment by more than 2 W/m². An assessment of the effect
on the direct result of determining the thermal resistance of the enclosing structure was carried out. For
this, the results in all four cases were compared. The value of the thermal resistance is calculated
according to the following expression (4):</p>
      <p>The comparison of the obtained results was carried out by calculating the relative deviation
according to the following expression (5):
 
=   −  (4)</p>
      <p>DEV = |</p>
      <p>
        −  | ∙ 100 %, (5)
where Rc is the theoretical value calculated according to the ISO 9869 [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ].
      </p>
      <p>The results of the comparison are shown in Table 4</p>
      <sec id="sec-6-1">
        <title>Comparison of the results of experimental studies and modeling</title>
        <p>Value, (m2K)/W</p>
      </sec>
      <sec id="sec-6-2">
        <title>Deviation, %</title>
        <p>Rc</p>
        <p>Based on the results of the comparison, the deviation for this case is 17.51%.</p>
      </sec>
    </sec>
    <sec id="sec-7">
      <title>5. Conclusions</title>
      <p>In the work, a computer simulation of the process of complex radiative and convective-conductive
heat exchange during the control of the thermophysical characteristics of the building envelope was
carried out, taking into account the locations of the sensors and the influence of their parameters on the
control result. A general description of the heat exchange process of the building envelope using a
mathematical model of an external random field, its transformation operator, which is characterized by
the thermophysical properties of the building envelope and the resulting internal random field, is given.</p>
      <p>As a result of computer CFD modeling, the distribution of the temperature and the air velocity field
of the internal thermal field was obtained, which made it possible to establish the absence of increased
turbulence in the area where the heat flux sensors are located. According to the results of validation of
the created CFD model using experimental data, it was found that the deviation does not exceed 0.3 K
for temperature and 0.3 W/m² for heat flux.</p>
      <p>The work also shows the case when the emission coefficient of the sensor is reduced by 0.16 units,
the difference in the values of the heat flux through the zone of its installation is more than 2 W/m². At
the same time, the deviation of the result of control the thermal resistance of the building envelope is
17.51%.</p>
      <p>Therefore, the use of the created CFD model is promising from the point of view of the analysis of
the process of controlling the thermophysical characteristics of the building envelope, taking into
account the influence of both external factors and the applied tools for in-situ tests.</p>
    </sec>
    <sec id="sec-8">
      <title>6. Acknowledgements</title>
      <p>These researches have been performed within of the scientific program «Information technology for
energy audit of buildings as a component of the energy security of the country».</p>
    </sec>
    <sec id="sec-9">
      <title>7. References</title>
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