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    <article-meta>
      <title-group>
        <article-title>The development of a model for predicting the stability boundaries of natural circulation process</article-title>
      </title-group>
      <contrib-group>
        <aff id="aff0">
          <label>0</label>
          <institution>V.V. Andreev, E.E. Orekhova</institution>
          ,
          <addr-line>N.P. Tarasova, Yu.S. Perevezentseva</addr-line>
        </aff>
      </contrib-group>
      <abstract>
        <p>The concept of safety for facilities comprising nuclear power plants implies in large the use of passive systems. One of the main passive systems in a nuclear power plant is a system for cooling the reactor core with its action based on gravitational forces. In this regard, the importance of such a physical process as natural circulation is increasing with the development of nuclear power facilities. However, this system has not only advantages but some drawbacks as well. These are the emergence of instability in the two-phase coolant flow, pulsations of thermohydraulic parameters, possible circulation reversal and stagnation. This paper deals with the study of a generalized model of the natural circulation stability. The said model is designed to simplify the design engineering of power equipment. This model will also enable the operating personnel to predict the operating limits of the equipment and remain within the coolant stability bounds. This paper presents a model for predicting the stability boundaries of natural circulation process.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>Nuclear energy is currently one of the most promising
power sources. The importance of passive safety systems
is increasing with the development of the nuclear industry.
The main advantage of these systems is the independence
of their functioning of external energy sources and as a
consequence the simplification of their design. One of the
important reactor systems is a passive heat removal system
required to cool the core. This system is based on the fluid
motion due to difference in specific gravities. The motion
occurs without any forcing equipment (no pumps) and
represents the coolant circulation generated by the action
of natural forces. Moreover, equipment operated with the
natural coolant circulation is characterized by reduced
installation noise, overall dimensions and the power
consumption for self-supply. But notwithstanding these
advantages the system has some drawbacks as well,
namely, the occurrence of instability in the two-phase
coolant flow during the reactor core cooling, pulsations of
thermohydraulic parameters and possible circulation
reversal and stagnation.</p>
    </sec>
    <sec id="sec-2">
      <title>2. Instability of two-phase flows</title>
      <p>
        In natural-convection loops with the two-phase coolant
condition the flow instabilities are noted, which are
manifested themselves through a periodic change in the
main thermohydraulic parameters of the flow under
constant external conditions. Such unstable flow regime
may result in deteriorating reliability of thermal power
equipment. Periodic repeated fluctuations in the flow rate
of the coolant in the loop may cause the premature loss of
the equipment serviceability, the wall material destruction,
low-frequency vibrations affecting the operation of the
plant as a whole. Furthermore, the loop instability imposes
restrictions on permissible limits of the thermal power;
therefore, the determination of areas with stable operation
of natural circulation loops at low pressures is a very
urgent task [
        <xref ref-type="bibr" rid="ref1 ref2">1,2</xref>
        ].
      </p>
      <p>Destabilizing mechanisms are often associated with
design features of a plant using a two-phase flow; the
instability may be caused by the availability of a volume
equalizer, a hydraulic accumulator or some peculiarities of
performances of elements.
3.</p>
    </sec>
    <sec id="sec-3">
      <title>Geyser instability</title>
      <p>The results of experimental studies have shown that
one of the main types of instability at low pressures and
flow rates of the coolant is the flow instability caused by
the surge of the coolant boiling in the lifting section of
the circulation loop. This type of instability is
characterized by periodic emission of a two-phase mixture
from the lifting section followed by filling the circulation
path with water.</p>
      <p>The geysering-type instability was named so because
of its resemblance to natural geysers, which are
characterized by periodic emissions of a steam-water
mixture from the depths of the Earth.</p>
      <p>
        Such geyser instability was first studied in vertical
pipes closed from below and filled with water [
        <xref ref-type="bibr" rid="ref3 ref4">3,4</xref>
        ]. When
a pipe is heated with some heat flow in the lower part the
water boiling begins. In low-pressure systems it results in
the sudden increase of steam generation and the rapid
discharge of the steam-water mixture into an expansion
vessel thereto the pipe is connected. Liquid which is not
warmed up to the saturation temperature is discharged
from the vessel into the pipe. The system returns to the
non-boiling state. The cycle is further repeated [
        <xref ref-type="bibr" rid="ref5 ref6">5,6</xref>
        ].
      </p>
      <p>The cycle consists of the following several stages:
1) energy accumulation;
2) the coolant boiling at a temperature slightly above the
saturation temperature;
3) the emission of a steam-water jet;
4) the return to the initial state.
4.</p>
    </sec>
    <sec id="sec-4">
      <title>Methods and techniques for prediction of the coolant flow regimes</title>
      <p>This paper is concerned with the study of the process
of natural circulation and its stability using a few different
methods in order to create a single generalized system. The
following methods have been applied in the work:
experimental method, calculation method using
computational codes of hydrodynamics, method using
artificial neural networks. The results obtained using the
said methods are combined to create a generalized model.
This model shall enable to predict the system behavior, to
determine the limiting boundary conditions for the stable
operation of the system.
5.</p>
    </sec>
    <sec id="sec-5">
      <title>Experimental research methods</title>
      <p>Experimental studies were carried out at the
Department of Nuclear Reactors and Power Plants,
Institute of Nuclear Energy and Technical Physics, Nizhny
Novgorod State Technical University n.a. R.E. Alekseev.</p>
      <p>The experiments were carried out at atmospheric
pressure. The system operating modes at atmospheric
pressure simulate the emergency cooling process for a
nuclear plant.</p>
      <p>The scheme of the stand is shown in Fig. 1.</p>
      <p>The experiments were conducted as follows:
measurement of the initial water temperatures in the
circulation loop;
measurement of the initial temperature in the cooling
loop;
measurement of the cooling water flow rate;
setting of the heater power;
activation of the data recording and archiving.</p>
      <p>Parameters read out:
heater power;
refrigerator power;
coolant temperature at the inlet and outlet of the
heating section;
duct wall temperature along the height of the lifting
region:
˗ cooling water temperature at the outlet of the
refrigerator
˗ differential pressure at the downcomer region
˗ steam content at the outlet of the heated duct.</p>
      <p>Upon setting the pulsation mode the following
parameters were recorded: the pulsation frequency and
duration, the pressure drop, the coolant temperature at the
outlet of the heated section and the pulsation
commencement temperature.</p>
    </sec>
    <sec id="sec-6">
      <title>Experimental data processing results</title>
      <p>Fig. 2 shows the curve of the natural circulation
stability obtained as a result of the experimental data
processing.</p>
      <p>The curve has a left branch bent to the relative
temperature axis, a pronounced minimum and a right
branch. The operating mode characterized by the right
branch includes an interval of the unstable operation of the
system. Therefore, the left branch is of particular interest
in the results obtained.</p>
      <p>
        Similar results in regard to the natural circulation
stability have been found in the literature and are shown in
Fig. 3 [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ]
      </p>
      <p>Based on the experimental data obtained and found in
the literature a technique has been elaborated for creating
a generalized model to predict the natural circulation
stability.</p>
    </sec>
    <sec id="sec-7">
      <title>7. Experimental computational system for studying the natural coolant circulation</title>
      <p>The generalized model is a set of lines showing the
boundary conditions for the existence of a stable system
constructed on the Q-T axes. Such a combination of
boundary conditions is unique for a specific technical
system and enables to determine the limits for stable
operation of the equipment. The combination of boundary
conditions is a family of curves of a characteristic form:
the left branch of the family is bent at a certain angle to the
temperature axis (T), this angle depends on the geometry
of the contour. The salient point (kink) moves depending
on the conditions thereunder the coolant is located. The
suggested model is shown in Fig. 4</p>
      <p>The introduction of generalized coordinates enables us
to modify the model under study and reduce it to a simpler
form:</p>
    </sec>
    <sec id="sec-8">
      <title>8. Generalized model of stability boundaries for systems with natural coolant circulation</title>
      <p>The generalized model is the summary of results
obtained using experimental methods, computer
simulation and artificial neural networks. This model
enables to predict the limiting densities of heat flows
therewith the system will still be stable and the coolant
boundary temperature at the inlet to the heated section
upon exceeding thereof the system will become unstable.
This model enables to simplify the procedure of the design
and engineering of heat exchange equipment based on the
principle of natural circulation. The methodology for
constructing such a generalized model is shown in Fig. 5.</p>
    </sec>
    <sec id="sec-9">
      <title>9. Application of numerical methods for simulation of natural circulation process</title>
      <p>Experimentally obtained results are used to simulate
systems using computational fluid dynamics. To apply the
computational fluid dynamics method, it is necessary to
construct a geometric model of the system under study, to
construct a calculation - grid model based on the geometric
model, to create a mathematical model.
10. Methodology for conducting experiments to
study the natural coolant circulation by
computational simulation methods</p>
      <p>To conduct numerical experiment, it is necessary:
to create the geometry of the loop under study;
to create a finite - element model;
to identify physical and mathematical models of
processes studied;
11. Description of a geometric model used for
numerical experiments</p>
      <p>The geometric model is a combination of several
components:
- the hot coolant circulation path corresponding to the
test stand;
- the coolant circulation path in the refrigerator
corresponding to the test stand;
- metal walls of the refrigerator.</p>
      <p>All geometrical parameters of the computer model
correspond to the natural test-stand under study. The
computer geometric model is shown in Fig. 6.</p>
      <p>∂xi
where ρ is the density, ui is the projection of the velocity
onto the axis under study, t is time; xi is the coordinate
thereon the flow is studied.</p>
      <p>- the motion equation:</p>
      <p>∂(∂uti ) + u j ∂∂(xuij) = − ρ1 ∂∂xpi + ρ1 ∂∂(σxijj ) + Ji ,
where indices i =1,2,3 shall be the coordinate axis index; j
is the summation index; Ji is the external force acting on
the system (gravity force)
- the energy equation:
∂h r
ρ = −div(q) +ω</p>
      <p>
        ∂τ
where q⃗ shall be projections of the heat flow density onto
the coordinate axes; ω are internal heat sources.
13. Application of artificial neural networks for
simulation of the natural circulation process
Based on the results obtained using the above methods
artificial neural networks (ANNs) are simulated. An ANN
of the multilayer perceptron type is used in this work. [
        <xref ref-type="bibr" rid="ref9">9</xref>
        ]
When simulating ANN, the coolant characteristics of the
geometry and state are taken as input parameters. The
output parameters are the corrected value of the boundary
heat flow and temperature thereat the instability occurs as
well as the value of tg(ɑ) characterizing the position of the
curve in space. The ANN simulation scheme is shown in
Fig. 7.
      </p>
      <p>Fig. 7. Scheme of ANN used for generalized model creation
f(Г) is characteristic of the circulation duct; f(У) is
characteristic of the coolant state conditions; tg(ɑ), Qпр, tпр are
output ANN data - system stability parameters</p>
      <p>When developing a model using artificial neural
networks the results of personal experiments have been
used as well as the results found in reference data.</p>
      <p>It may be noted that in the obtained dependences there
is a sharp ascending and descending section. To avoid
ambiguity, two neural networks have been simulated: one
for each section. However, we lack of knowledge on on
the upper limit of each network use because of few
experimental data available.</p>
      <p>Networks of the multilayer perceptron type with
different numbers of neurons in the intermediate layer and
several different activation functions have been studied
during the simulation.</p>
      <p>The analysis of simulated networks is given in
Appendix B. Find below the results obtained with a neural
network having minimal errors.</p>
      <p>A set of points has been obtained in the course of the
simulation. A boundary stability curve of the natural
circulation process corresponds to each point in the spatial
coordinate system. It is noted that the said points are on
one curve in space and represent an integral system (fig.
9).
15. Conclusion</p>
      <p>This paper is concerned with the study of the stability
boundaries for the natural coolant circulation process. The
purpose of the work is to develop a generalized model
which enables to predict the stability without reference to
a specific geometry, installation or conditions of the
system operation. This purpose has been achieved.</p>
      <p>The following has been achieved in the course of the
work performance:
1. The methodology has been elaborated for conducting
full-scale experiments to study the stability limits of
geyser instability under the natural coolant circulation
using a thermophysical test stand.
2. The methodology has been elaborated for the use of
artificial neural networks to predict the stability of the
natural circulation process.
3. The generalized model of the natural circulation
stability has been developed.</p>
      <p>The results obtained may be applied to elaborate
technical and organizational measures for process
management. This model may also be used to predict the
maximum operating conditions of the power equipment
with natural coolant circulation.</p>
    </sec>
    <sec id="sec-10">
      <title>Acknowledgements</title>
      <p>This work was supported by the RFBR, grant №
1907-00455.</p>
    </sec>
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